Re: Block Universes

2014-03-08 Thread Jesse Mazer
On Fri, Mar 7, 2014 at 8:37 PM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 I guess I'm supposed to take that as a yes? You do agree that A's world
 line is actually shorter than C's (even though it is depicted as longer)
 because A's proper time along it is less than C's from parting to meeting?
 Correct? Strange how resistant you are to ever saying you agree when we
 actually do agree. Remember we are not counting points here, at least I'm
 not, we are trying to find the truth


I'm not resistant in general, I have said I agree to a number of
agree/disagree questions you asked in the past. But in this one case I was
expressing irritation because from your question it seemed pretty obvious
you either hadn't read, or hadn't paid any attention to, my discussion of
lengths in the post you were responding to. If you really, really can't
deduce my opinion on this from statements like this:

in terms of proper times C  B  A which is the opposite of how it works
with spatial lengths

or:

in spatial terms a straight line is the SHORTEST path between two points,
but in spacetime a straight (constant-velocity) worldline is the one with
the LARGEST proper time between points

...then just tell me why you think these statements are ambiguous and I
will then tell you whether I agree that A's world line is actually shorter
than C's (even though it is depicted as longer) because A's proper time
along it is less than C's from parting to meeting. But if reading those
statements does answer your question, then I would suggest that part of
trying to find the truth is actually reading through the responses you
get, not skimming/skipping over parts of it.




 First, note you don't actually have to calculate anything. A and C just
 compare clocks when they meet and that gives the actual world line lengths.


Sure, but I'm talking about the theoretical analysis.



 But, if you want to calculate to predict what that comparison will be,
 then you have to be careful to do it correctly.

 C can't just use the Pythagorean theorem on A's world line from his
 perspective on the x and y distances, he has to use it on the time
 dimension as well squareroot((y2-y1)^2 + (x2-x1)^2 - c(t2-t1)^2).


You have the right idea, although that formula (with c^2 rather than c)
actually calculates proper length on a spacelike interval, if you want
proper time on a timelike interval the equivalent formula would be
squareroot((t2-t1)^2 - (1/c)^2*(x2-x1)^2 - (1/c)^2*(y2-y1)^2). And since we
were talking about a 2D spacetime diagram where all motion was along a
single spatial axis, I dropped the y-coordinate, and as I mentioned I was
also assuming units where c=1, like years for time and light-years for
distance. That's why I just wrote the formula as sqrt((t2 - t1)^2 - (x2 -
x1)^2).



 It is the subtraction of this time term that will reduce the length of the
 slanting blue lines of A and B to THEIR PROJECTIONS ON C'S OWN WORLDLINE.


That statement appears wrong, although you'd have to give me a definition
of what you mean by projections on C's own worldline for me to be sure.
It seems to me that by the normal definition of projection, projecting
one of the slanted blue line segments onto the C's vertical worldline would
give a new segment parallel to the vertical axis, whose length is just
equal to the vertical separation between the ends of the original slanted
blue segment. If so, the length of that sort of projection is NOT equal
to the proper time of the original slanted blue segment, instead it's equal
to the coordinate time between its endpoints, in C's rest frame.

For example, looking at the diagram at
http://www.jessemazer.com/images/tripletparadox.jpg , let's say the bottom
blue segment on A's worldline begins in 2001 in C's rest frame, and ends in
2008, and it has a velocity of 0.6c. In that case, by the normal meaning of
projection, projecting this segment onto C's vertical worldline would
just create a vertical segment that goes from 2001 to 2008, and thus has a
coordinate time of 7 years (and for any vertical segment of a worldline
parallel to the time coordinate axis, proper time is supposed to be equal
to coordinate time). But because of time dilation, the proper time along
the original blue segment (before it was projected to make it vertical)
is less than the coordinate time by a factor of sqrt(1 - (0.8c/c)^2) =
sqrt(1 - 0.64) = sqrt(0.36) = 0.6, so relativity says the correct proper
time along that original slanted blue segment is 7*0.6 = 4.2 years. Do you
agree or disagree with these numbers?





 I think that is what you are saying as well, but my point is that that
 NULLIFIES any effect on the length of the world lines by the SLANTING of
 the blue lines NO MATTER WHAT THEIR LENGTHS, and LEAVES ONLY the effects of
 the red curves.



No, you're simply wrong about this. Let's actually do a numerical example.
Suppose that both A and B go through the same sequence of 3 accelerations:

ACCELERATION 1: starting from 

Re: Block Universes

2014-03-08 Thread Jesse Mazer
On Sat, Mar 8, 2014 at 9:31 AM, Jesse Mazer laserma...@gmail.com wrote:


 And B's worldline consists of the following five segments:

 Segment 1 (blue): Remaining at rest in C's frame, from t=1999 to t=2009
 Segment 2 (red): ACCELERATION 1 from t=2009 to t=2011
 Segment 3 (blue): Moving inertially at 0.6c in the +x direction, from
 t=2011 to t=2013
 Segment 4 (red): ACCELERATION 2 from t=2013 to t=2017
 Segment 5 (blue): Moving inertially at 0.6c in the -x direction, from
 t=2017 to t=2019
 Segment 6 (red): ACCELERATION 3 from t=2019 to t=2019


Correction--that last line for B's worldline should read

Segment 6 (red): ACCELERATION 3 from t=2019 to t=2021

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Re: Block Universes

2014-03-08 Thread Edgar L. Owen
Jesse,

OK, Assume c=1 and start with your sqrt((t2 - t1)^2 - (x2 - x1)^2) to 
calculate what you say is the proper time on a time-like interval. Using 
your method, which I assume is correct I do see that A's proper time will 
be greater than B's. The reason is basically that A has to travel further 
in space to get from t1 to t2 and consequently must also travel less far in 
time. Correct?


To confirm, consider a simplified twin example with only straight lines so 
we can ignore accelerations. A remains at rest with a straight vertical 
line from t1 to t3. B travels away from t1 in a straight oblique line, 
reverses direction midpoint (call this t2) and travels in a straight 
oblique line back to t3.

The two halves of B's trip are symmetric (have the same velocities away 
from and back towards A) therefore B's proper time, calculated by A, will 
be = 2 x sqrt((t2 - t1)^2 - (x2 - x1)^2).  In other words we have to 
multiply by 2 to get the proper time of B for the entire trip. Correct?


OK, now consider another case with A and B just moving with constant 
relative motion and their world lines crossing at t1 and then diverging. 
There is NO acceleration.

In this case using the Lorentz transform both A and B will observe each 
other's time running slow relative to their own. And using your formula 
above both A and B will also observe each other's proper times SLOWED 
RELATIVE TO THEIR OWN.

But doesn't this mean that since A and B get different results about each 
other's proper times that this method of calculating proper times is NOT 
INVARIANT, and thus is not actually calculating proper times which you say 
are invariant?

I agree that this method correctly calculates how A and B observe each 
other's clock times, but not sure that's the same as the other's actual 
proper times.

Edgar



On Saturday, March 8, 2014 9:31:24 AM UTC-5, jessem wrote:



 On Fri, Mar 7, 2014 at 8:37 PM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 I guess I'm supposed to take that as a yes? You do agree that A's world 
 line is actually shorter than C's (even though it is depicted as longer) 
 because A's proper time along it is less than C's from parting to meeting? 
 Correct? Strange how resistant you are to ever saying you agree when we 
 actually do agree. Remember we are not counting points here, at least I'm 
 not, we are trying to find the truth


 I'm not resistant in general, I have said I agree to a number of 
 agree/disagree questions you asked in the past. But in this one case I was 
 expressing irritation because from your question it seemed pretty obvious 
 you either hadn't read, or hadn't paid any attention to, my discussion of 
 lengths in the post you were responding to. If you really, really can't 
 deduce my opinion on this from statements like this:

 in terms of proper times C  B  A which is the opposite of how it works 
 with spatial lengths

 or:

 in spatial terms a straight li
 ...

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Re: Block Universes

2014-03-08 Thread Jesse Mazer
On Sat, Mar 8, 2014 at 2:03 PM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 OK, Assume c=1 and start with your sqrt((t2 - t1)^2 - (x2 - x1)^2) to
 calculate what you say is the proper time on a time-like interval. Using
 your method, which I assume is correct I do see that A's proper time will
 be greater than B's. The reason is basically that A has to travel further
 in space to get from t1 to t2 and consequently must also travel less far in
 time. Correct?


It's true in C's rest frame that A travels a greater distance than B, but
this needn't be true if you used a different frame. For example, if you
analyze the problem using an inertial frame D in which A is at rest during
the first blue leg of his trip, then A and B should travel the same
distance between departing and reuniting, because neither ever turns around
and travels in the wrong direction in this frame, they are both always at
rest in this frame or traveling in the -x direction towards the position in
this frame where they will reunite. So if you imagine that A and B are cars
that are driving along a piece of flat ground at rest in frame D, and both
start out with odometers reading 0 when A first departs from B, then A and
B's odometer will show the same reading when they reunite, since they have
both traveled in a consistent direction (but varying speed) along the same
straight road between the position in frame D where they departed and the
position where they reunited.






 To confirm, consider a simplified twin example with only straight lines so
 we can ignore accelerations. A remains at rest with a straight vertical
 line from t1 to t3. B travels away from t1 in a straight oblique line,
 reverses direction midpoint (call this t2) and travels in a straight
 oblique line back to t3.

 The two halves of B's trip are symmetric (have the same velocities away
 from and back towards A) therefore B's proper time, calculated by A, will
 be = 2 x sqrt((t2 - t1)^2 - (x2 - x1)^2).  In other words we have to
 multiply by 2 to get the proper time of B for the entire trip. Correct?


Yes, that's correct.




 OK, now consider another case with A and B just moving with constant
 relative motion and their world lines crossing at t1 and then diverging.
 There is NO acceleration.

 In this case using the Lorentz transform both A and B will observe each
 other's time running slow relative to their own. And using your formula
 above both A and B will also observe each other's proper times SLOWED
 RELATIVE TO THEIR OWN.

 But doesn't this mean that since A and B get different results about each
 other's proper times that this method of calculating proper times is NOT
 INVARIANT, and thus is not actually calculating proper times which you say
 are invariant?



The method gives an invariant answer for the proper time between any two
specific events on an inertial worldline, events which are known to have
coordinates (x1,t1) and (x2,t2) in whatever frame you're using.  But in
your example, they haven't agreed on a specific pair of points on each
worldline to calculate the proper time between. Suppose their worldlines
cross at the moment of their births, when they are both 0 years old, and
subsequently they move apart with arelative velocity of 0.6c so the time
dilation factor is 0.8c. If A wants to use his own rest frame to predict
how old B will be at the same moment that A turns 20, he is picking the
event b1 on B's worldline that is SIMULTANEOUS IN A's REST FRAME with A
turning 20, and calculate the proper time between the event of B's birth
and b1, which is 16. On the other hand, if B wants to use his own rest
frame to predict how old he'll be at the same moment that A turns 20, he
must pick the event b2 on B's worldline that is SIMULTANEOUS IN B'S REST
FRAME with A turning 20, and calculate the proper time between B's birth
and b2, which is 25. Both frames agree that the proper time between B's
birth and b1 is 16, and that the proper time between B's birth and b2 is
25, they just disagree about whether b1 or b2 is simultaneous with A
turning 20. So that's why they disagree about whether A is older or younger
than B at any specified point on A's worldline, like A turning 20 (and of
course the logic works the same if you specify a point on B's worldline and
ask about A's age at the same moment). Of course, this sort of ambiguity
about what events to choose doesn't arise in a twin-paradox type scenario
where the twins depart from each other at one specific point on their
worldlines, and reunite at some other specific point on their worldlines.

If you want further evidence that the method gives an invariant answer, you
can use the Lorentz transformation to check that this is so. Pick two
events on the worldline of an inertial clock of arbitrary velocity in the
frame you're using, and assume that the spacetime origin is chosen so that
the first event is labeled with coordinates x1=0, t1=0. Then the second
event can be anything (so long as the 

Re: Block Universes

2014-03-08 Thread Edgar L. Owen
Jesse,

PS: And in your nice long numerical example, which I thank you for, it 
seems to me what you are doing is calculating the proper time length of 
every segment of A's trip in terms of C's proper time. Isn't that correct?

But if so aren't you in fact establishing a 1:1 correlation of proper times 
between A and C with your method?

And isn't that what you keep telling me CAN'T BE DONE?

Edgar



On Saturday, March 8, 2014 9:31:24 AM UTC-5, jessem wrote:



 On Fri, Mar 7, 2014 at 8:37 PM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 I guess I'm supposed to take that as a yes? You do agree that A's world 
 line is actually shorter than C's (even though it is depicted as longer) 
 because A's proper time along it is less than C's from parting to meeting? 
 Correct? Strange how resistant you are to ever saying you agree when we 
 actually do agree. Remember we are not counting points here, at least I'm 
 not, we are trying to find the truth


 I'm not resistant in general, I have said I agree to a number of 
 agree/disagree questions you asked in the past. But in this one case I was 
 expressing irritation because from your question it seemed pretty obvious 
 you either hadn't read, or hadn't paid any attention to, my discussion of 
 lengths in the post you were responding to. If you really, really can't 
 deduce my opinion on this from statements like this:

 in terms of proper times C  B  A which is the opposite of how it works 
 with spatial lengths

 or:

 in spatial terms a stra
 ...

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Re: Block Universes

2014-03-08 Thread Jesse Mazer
On Sat, Mar 8, 2014 at 3:11 PM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 PS: And in your nice long numerical example, which I thank you for, it
 seems to me what you are doing is calculating the proper time length of
 every segment of A's trip in terms of C's proper time. Isn't that correct?


No, it's in terms of coordinate time in C's rest frame. C's proper time
can only be defined between pairs of events on C's own worldline. Of course
if C is inertial as in this example, then the coordinate time of events on
C's worldline is the same as the proper time between those events, but it
doesn't make sense to talk about C's proper time between events that are
NOT on C's worldline.




 But if so aren't you in fact establishing a 1:1 correlation of proper
 times between A and C with your method?

 And isn't that what you keep telling me CAN'T BE DONE?


You can of course define a correlation in proper times of separated clocks
A and B if you specify what frame's definition of simultaneity you want to
use. Then you can find a pair of events a1 and b1 that are simultaneous in
this frame, and a pair of events a2 and b2 that are simultaneous in this
frame, and compare the proper time on A's worldline between a1 and a2 with
the proper time on B's worldline between b1 and b2. But this sort of
correlation will differ depending on what frame you choose (because the
simultaneous events will differ), and what can't be done is find any basis
in relativity for saying that one frame's correlation represents the real
correlation while other frames' do not.

Jesse

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Re: Block Universes

2014-03-07 Thread Edgar L. Owen
Jesse,

Finally hopefully getting a minute to respond to at least some of your 
posts.

I'm looking at the two 2 world line diagram on your website and I would 
argue that the world lines of A and B are exactly the SAME LENGTH due to 
the identical accelerations of A and B rather than different lengths as you 
claim.

The length of a world line is the PROPER TIME along that world line. Thus 
the length of a world line is INVARIANT. It is the length of the world line 
according to its proper clock and NOT the length according to C's clock 
which is what this diagram shows.

So to calculate the length of A's and B's world lines in C's frame (which 
this diagram represents) we must take the apparent lengths as shown from 
C's frame view on the diagram, and SHORTEN each section by the apparent 
slowing of ITS CLOCK relative to C's CLOCK.

In other words, the proper time LENGTHS of A's and B's world lines will NOT 
be as they appear in this diagram which displays their apparent length's 
relative to C's proper clock. To get the actual length we have to use the 
readings of A's and B's clock and shorten their apparent lengths by that 
amount.

When we do this all the blue segments of A's and B's world lines become 
parallel to C's and thus add no length to A's or B's world lines. This is 
what we would expect since the pure NON-accelerated relative motion of the 
blue segments doesn't add length to a world line.

So when we subtract the apparent length differences of the blue lines all 
we are left with is the red ones which are equal.

Thus the actual LENGTHS of A's and B's world lines are equal. And the only 
effects which add length to world lines are in fact accelerations as I 
claimed.

The point is that the TRAJECTORIES in spacetime of world lines from some 
frame like C's in this diagram do NOT properly represent the invariant 
LENGTHS of those world lines. Because to get the invariant proper time 
length we must shorten those trajectories by the apparent clock slowing 
along it to get the actual proper clock interval from start to finish.

So when we do this we find that the different LENGTHS of world lines 
between any two spacetime points are due ONLY TO ACCELERATIONS OR 
GRAVITATION as I previously stated. 

Do you agree?


Edgar




On Thursday, March 6, 2014 12:01:53 PM UTC-5, jessem wrote:



 On Thu, Mar 6, 2014 at 11:02 AM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Liz,

 Sure, but aren't the different lengths of world lines due only to 
 acceleration and gravitational effects? So aren't you saying the same thing 
 I was?

 Isn't that correct my little Trollette? (Note I wouldn't have included 
 this except in response to your own Troll obsession.)

 Anyway let's please put our Troll references aside and give me an honest 
 scientific answer for a change if you can... OK?

 It would be nice to get an answer from Brent or Jesse as well if they 
 care to chime in..



 In the case of the traditional twin paradox where one accelerates between 
 meetings while the other does not, the one that accelerates always has the 
 greater path length through spacetime, so in this case they are logically 
 equivalent. But you can have a case in SR (no gravity) where two observers 
 have identical accelerations (i.e. each acceleration lasts the same 
 interval of proper time and involves the same proper acceleration 
 throughout this interval), but because different proper times elapse 
 *between* these accelerations, they end up with worldlines with different 
 path lengths between their meetings (and thus different elapsed aging)...in 
 an online discussion a while ago someone drew a diagram of such a case that 
 I saved on my website:

 http://www.jessemazer.com/images/tripletparadox.jpg

 In this example A and B have identical red acceleration phases, but A will 
 have aged less than B when they reunite (you can ignore the worldline of C, 
 who is inertial and naturally ages more than either of them).

 You can also have cases in SR where twin A accelerates more than B 
 (defined in terms of the amount of proper time spent accelerating, or the 
 value of the proper acceleration experienced during this time, or both), 
 but B has aged less than A when they reunite, rather than vice versa. As 
 always the correct aging is calculated by looking at the overall path 
 through spacetime in some coordinate system, and calculating its length 
 (proper time) with an equation that's analogous to the one you'd use to 
 calculate the spatial length of a path on a 2D plane.

 Jesse


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Re: Block Universes

2014-03-07 Thread Jesse Mazer
On Fri, Mar 7, 2014 at 4:02 PM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 Finally hopefully getting a minute to respond to at least some of your
 posts.

 I'm looking at the two 2 world line diagram on your website and I would
 argue that the world lines of A and B are exactly the SAME LENGTH due to
 the identical accelerations of A and B rather than different lengths as you
 claim.

 The length of a world line is the PROPER TIME along that world line. Thus
 the length of a world line is INVARIANT. It is the length of the world line
 according to its proper clock and NOT the length according to C's clock
 which is what this diagram shows.


I don't understand what you mean by the length according to C's
clock--are you just talking about the numbers on the vertical time axis,
2000-2020? That axis represents the coordinate time in C's rest frame, and
obviously the coordinate time between 2000 at the bottom of the diagram
and 2020 at the top is 20 years regardless of what path you're talking
about, so I don't see how it makes sense to call this the length of any
particular path. But you can also use C's rest frame to assign x and t
coordinates to the endpoints of any straight blue segment, x1 and t1 for
one endpoint and x2 and t2 for the other, and then C can calculate the
proper time along that segment as squareroot[(t2 - t1)^2 - (x2 - x1)^2] and
get the correct INVARIANT answer (note that I am using units of light-years
and years where c=1 so it doesn't appear in the equation, otherwise the
second term in the square root would have to be (1/c^2)*(x2 - x1)^2).

What the diagram is trying to show is that even though the different paths
have identical red acceleration curves, they have different SPATIAL
lengths, i.e. the length you'd measure if you printed out the diagram and
laid a flexible cloth tape measure along each path to measure the distance
ALONG THE PATH between the point at the bottom of the diagram where the
paths diverge and the point at the top where they rejoin. It is true that
if you just look at the spatial lengths of each path on the diagram, the
ratio between the spatial lengths doesn't actually match up with the ratio
between the proper times that would be calculated using relativity. If you
use any Cartesian spatial coordinate system to draw x-y axes on the
diagram, then you can use this coordinate system to assign x and y
coordinates to the endpoints of any straight blue segment, x1 and y1 for
one endpoint and x2 and y2 for the other, and then calculate the spatial
length of that segment using the Pythagorean theorem: squareroot[(y2 -
y1)^2 + (x2 - x1)^2]. Note that you ADD the squares of the two terms in
parentheses when calculating spatial length, but my earlier equation showed
that you SUBTRACT the square of the two terms in parentheses when
calculating proper time, which explains why this sort of spatial path
length on a spacetime diagram can be misleading. For example, in spatial
terms a straight line is the SHORTEST path between two points, but in
spacetime a straight (constant-velocity) worldline is the one with the
LARGEST proper time between points.

Nevertheless, the math for calculating the invariant spatial path length
using a Cartesian coordinate system is closely analogous to the math for
calculating the invariant proper time using an inertial frame. The diagrams
show the spatial length of the paths being different despite identical red
acceleration segments, and this remains true if you actually calculate
proper time, even though in terms of proper times C  B  A which is the
opposite of how it works with spatial lengths. If you assign time
coordinates to the beginning and end of each acceleration phase, and you
specify the proper acceleration involved, then you can calculate the proper
time along elapsed on each worldline during both the acceleration phases
(using the relativistic rocket equations given at
http://math.ucr.edu/home/baez/physics/Relativity/SR/rocket.html ) as well
as the proper time during the constant-velocity phases (using the method I
mentioned above with squareroot[(t2 - t1)^2 - (x2 - x1)^2] for each
segment). If you do this, you do find that in a detailed numerical version
of the scenario in the diagram, A ELAPSES LESS TOTAL PROPER TIME THAN B
DESPITE HAVING IDENTICAL ACCELERATIONS. I can give the detailed
calculations using the relativistic rocket equations if you want, or you
can just take my word for it.




 So to calculate the length of A's and B's world lines in C's frame (which
 this diagram represents) we must take the apparent lengths as shown from
 C's frame view on the diagram, and SHORTEN each section by the apparent
 slowing of ITS CLOCK relative to C's CLOCK.


Yes, that would be another way to calculate proper time along the blue
constant-velocity segments: just take the times t2 and t1 of the beginning
and end of each segment in C's frame, and multiply by the time dilation
factor which depends on the speed v in C's frame during 

Re: Block Universes

2014-03-07 Thread Edgar L. Owen
Jesse,

Do you understand why the world line that is depicted as LONGER in the 
typical world line diagram is ACTUALLY SHORTER?

E.g. in your diagram do you understand why even though A's world line looks 
longer than C's world line, it is ACTUALLY SHORTER?

Edgar





On Friday, March 7, 2014 5:15:57 PM UTC-5, jessem wrote:




 On Fri, Mar 7, 2014 at 4:02 PM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 Finally hopefully getting a minute to respond to at least some of your 
 posts.

 I'm looking at the two 2 world line diagram on your website and I would 
 argue that the world lines of A and B are exactly the SAME LENGTH due to 
 the identical accelerations of A and B rather than different lengths as you 
 claim.

 The length of a world line is the PROPER TIME along that world line. Thus 
 the length of a world line is INVARIANT. It is the length of the world line 
 according to its proper clock and NOT the length according to C's clock 
 which is what this diagram shows.


 I don't understand what you mean by the length according to C's 
 clock--are you just talking about the numbers on the vertical time axis, 
 2000-2020? That axis represents the coordinate time in C's rest frame, and 
 obviously the coordinate time between 2000 at the bottom of the diagram 
 and 2020 at the top is 20 years regardless of what path you're talking 
 about, so I don't see how it makes sense to call this the length of any 
 particular path. But you can also use C's 
 ...

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Re: Block Universes

2014-03-07 Thread Jesse Mazer
On Fri, Mar 7, 2014 at 7:20 PM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 Do you understand why the world line that is depicted as LONGER in the
 typical world line diagram is ACTUALLY SHORTER?

 E.g. in your diagram do you understand why even though A's world line
 looks longer than C's world line, it is ACTUALLY SHORTER?

 Edgar


Are you actually reading my posts carefully all the way through, or just
skimming them or something? I spent a whole extended section of my post
discussing just this point, read it again:

'It is true that if you just look at the spatial lengths of each path on
the diagram, the ratio between the spatial lengths doesn't actually match
up with the ratio between the proper times that would be calculated using
relativity. If you use any Cartesian spatial coordinate system to draw x-y
axes on the diagram, then you can use this coordinate system to assign x
and y coordinates to the endpoints of any straight blue segment, x1 and y1
for one endpoint and x2 and y2 for the other, and then calculate the
spatial length of that segment using the Pythagorean theorem:
squareroot[(y2 - y1)^2 + (x2 - x1)^2]. Note that you ADD the squares of the
two terms in parentheses when calculating spatial length, but my earlier
equation showed that you SUBTRACT the square of the two terms in
parentheses when calculating proper time, which explains why this sort of
spatial path length on a spacetime diagram can be misleading. For example,
in spatial terms a straight line is the SHORTEST path between two points,
but in spacetime a straight (constant-velocity) worldline is the one with
the LARGEST proper time between points.

Nevertheless, the math for calculating the invariant spatial path length
using a Cartesian coordinate system is closely analogous to the math for
calculating the invariant proper time using an inertial frame. The diagrams
show the spatial length of the paths being different despite identical red
acceleration segments, and this remains true if you actually calculate
proper time, even though in terms of proper times C  B  A which is the
opposite of how it works with spatial lengths.'









 On Friday, March 7, 2014 5:15:57 PM UTC-5, jessem wrote:




 On Fri, Mar 7, 2014 at 4:02 PM, Edgar L. Owen edga...@att.net wrote:

 Jesse,

 Finally hopefully getting a minute to respond to at least some of your
 posts.

 I'm looking at the two 2 world line diagram on your website and I would
 argue that the world lines of A and B are exactly the SAME LENGTH due to
 the identical accelerations of A and B rather than different lengths as you
 claim.

 The length of a world line is the PROPER TIME along that world line. Thus
 the length of a world line is INVARIANT. It is the length of the world line
 according to its proper clock and NOT the length according to C's clock
 which is what this diagram shows.


 I don't understand what you mean by the length according to C's
 clock--are you just talking about the numbers on the vertical time axis,
 2000-2020? That axis represents the coordinate time in C's rest frame, and
 obviously the coordinate time between 2000 at the bottom of the diagram
 and 2020 at the top is 20 years regardless of what path you're talking
 about, so I don't see how it makes sense to call this the length of any
 particular path. But you can also use C's
 ...

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Re: Block Universes

2014-03-07 Thread LizR
This is why time has a minus sign in SR. (I believe the usual way this
informally is put is that the space-traveller trades space for time.)


On 8 March 2014 13:26, Jesse Mazer laserma...@gmail.com wrote:


 On Fri, Mar 7, 2014 at 7:20 PM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 Do you understand why the world line that is depicted as LONGER in the
 typical world line diagram is ACTUALLY SHORTER?

 E.g. in your diagram do you understand why even though A's world line
 looks longer than C's world line, it is ACTUALLY SHORTER?

 Edgar


 Are you actually reading my posts carefully all the way through, or just
 skimming them or something? I spent a whole extended section of my post
 discussing just this point, read it again:

 'It is true that if you just look at the spatial lengths of each path on
 the diagram, the ratio between the spatial lengths doesn't actually match
 up with the ratio between the proper times that would be calculated using
 relativity. If you use any Cartesian spatial coordinate system to draw x-y
 axes on the diagram, then you can use this coordinate system to assign x
 and y coordinates to the endpoints of any straight blue segment, x1 and y1
 for one endpoint and x2 and y2 for the other, and then calculate the
 spatial length of that segment using the Pythagorean theorem:
 squareroot[(y2 - y1)^2 + (x2 - x1)^2]. Note that you ADD the squares of the
 two terms in parentheses when calculating spatial length, but my earlier
 equation showed that you SUBTRACT the square of the two terms in
 parentheses when calculating proper time, which explains why this sort of
 spatial path length on a spacetime diagram can be misleading. For example,
 in spatial terms a straight line is the SHORTEST path between two points,
 but in spacetime a straight (constant-velocity) worldline is the one with
 the LARGEST proper time between points.

 Nevertheless, the math for calculating the invariant spatial path length
 using a Cartesian coordinate system is closely analogous to the math for
 calculating the invariant proper time using an inertial frame. The diagrams
 show the spatial length of the paths being different despite identical red
 acceleration segments, and this remains true if you actually calculate
 proper time, even though in terms of proper times C  B  A which is the
 opposite of how it works with spatial lengths.'









 On Friday, March 7, 2014 5:15:57 PM UTC-5, jessem wrote:




 On Fri, Mar 7, 2014 at 4:02 PM, Edgar L. Owen edga...@att.net wrote:

 Jesse,

 Finally hopefully getting a minute to respond to at least some of your
 posts.

 I'm looking at the two 2 world line diagram on your website and I would
 argue that the world lines of A and B are exactly the SAME LENGTH due to
 the identical accelerations of A and B rather than different lengths as you
 claim.

 The length of a world line is the PROPER TIME along that world line.
 Thus the length of a world line is INVARIANT. It is the length of the world
 line according to its proper clock and NOT the length according to C's
 clock which is what this diagram shows.


 I don't understand what you mean by the length according to C's
 clock--are you just talking about the numbers on the vertical time axis,
 2000-2020? That axis represents the coordinate time in C's rest frame, and
 obviously the coordinate time between 2000 at the bottom of the diagram
 and 2020 at the top is 20 years regardless of what path you're talking
 about, so I don't see how it makes sense to call this the length of any
 particular path. But you can also use C's
 ...

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Re: Block Universes

2014-03-07 Thread Edgar L. Owen
Jesse,

I guess I'm supposed to take that as a yes? You do agree that A's world 
line is actually shorter than C's (even though it is depicted as longer) 
because A's proper time along it is less than C's from parting to meeting? 
Correct? Strange how resistant you are to ever saying you agree when we 
actually do agree. Remember we are not counting points here, at least I'm 
not, we are trying to find the truth

First, note you don't actually have to calculate anything. A and C just 
compare clocks when they meet and that gives the actual world line lengths.

But, if you want to calculate to predict what that comparison will be, then 
you have to be careful to do it correctly.

C can't just use the Pythagorean theorem on A's world line from his 
perspective on the x and y distances, he has to use it on the time 
dimension as well squareroot((y2-y1)^2 + (x2-x1)^2 - c(t2-t1)^2). It is the 
subtraction of this time term that will reduce the length of the slanting 
blue lines of A and B to THEIR PROJECTIONS ON C'S OWN WORLDLINE.

I think that is what you are saying as well, but my point is that that 
NULLIFIES any effect on the length of the world lines by the SLANTING of 
the blue lines NO MATTER WHAT THEIR LENGTHS, and LEAVES ONLY the effects of 
the red curves.

This must be the case because NON-accelerated relative motion DOES NOT 
affect proper time rates. This is because it is exactly the same from the 
perspective of A and C moving relative to each other, thus it cannot affect 
the lengths of their world lines.

I'm trying to parse your last paragraph. Your diagram shows ONLY how A's 
and B's world lines appear in C's comoving frame. It does NOT show the 
proper LENGTHS of A's and B's world lines. I think we agree the lengths 
depicted are NOT the actual world line lengths.

I claim the blue slanting lines of A and B, one set longer than the other, 
have NO EFFECT on the actual lengths of A's and B's world lines. Because 
when we calculate just their proper lengths subtracting the time term as I 
do above, their proper lengths reduce to their VERTICAL PROJECTIONS on C's 
vertical world line. In other words there is no difference in proper time 
rates of A, B or C during the intervals of the slanting blue lines.

Thus, in my view, we are left with ONLY the effects of the curving red 
accelerations, and these are exactly the same for A and B. And when the 
lengths of those red acceleration segments are calculated we find that A's 
and B's world lines will both be SHORTER than C's world line AND by the 
SAME AMOUNT and that A's and B's world line lengths will be EQUAL due only 
to their equal accelerations.


Perhaps to make this clearer consider just two blue lines of A and B 
slanted with respect to each other and crossing at P. From A's perspective 
B's line will be slanted, but from B's perspective A's line will be slanted 
in the other direction by an equal amount AND since this is NON-accelerated 
inertial motion only, both views are EQUALLY VALID. When we do the 
Pythagorean world line length calculation we get EXACTLY THE SAME RESULTS 
from both frame views. So both world line lengths are exactly equal.

Thus slanted blue lines of ANY LENGTH have NO EFFECT AT ALL on world line 
lengths, and only curved red line accelerations do.

If you disagree I can give you another example.

Edgar



On Friday, March 7, 2014 7:26:38 PM UTC-5, jessem wrote:


 On Fri, Mar 7, 2014 at 7:20 PM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 Do you understand why the world line that is depicted as LONGER in the 
 typical world line diagram is ACTUALLY SHORTER?

 E.g. in your diagram do you understand why even though A

 ...

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Re: Block Universes

2014-03-06 Thread Edgar L. Owen
Liz,

Sure, but aren't the different lengths of world lines due only to 
acceleration and gravitational effects? So aren't you saying the same thing 
I was?

Isn't that correct my little Trollette? (Note I wouldn't have included this 
except in response to your own Troll obsession.)

Anyway let's please put our Troll references aside and give me an honest 
scientific answer for a change if you can... OK?

It would be nice to get an answer from Brent or Jesse as well if they care 
to chime in..

Edgar


On Wednesday, March 5, 2014 3:56:56 PM UTC-5, Liz R wrote:

 On 6 March 2014 09:12, Edgar L. Owen edga...@att.net javascript:wrote:

 Jesse,

 PS: It is well known that accelerations and gravitation are the ONLY 
 causes that produce real actual age rate changes. These real actual age 
 rate changes are real and actual because 1. ALL OBSERVERS AGREE on them 
 when they meet up and check them, and 2.BECAUSE THEY ARE PERMANENT.


 Having your worldlines be different lengths in spacetime will also cause 
 differences in actual age, as Brent has explained (with diagrams).

 Consistently ignoring this point and others like it is one reason most 
 people here consider you a troll, so please try to address it.



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Re: Block Universes

2014-03-06 Thread Edgar L. Owen
Jesse,

Yes, from the point any two observers in the same inertial frame 
synchronize clocks, their clocks will be synchronized in p-time BUT ONLY 
FROM THEN ON (we can't know if they were previously synchronized unless we 
know their acceleration histories). And only SO LONG AS they continue in 
the same inertial frame OR undergo symmetric accelerations. 

Same ages is just a way to ensure synchronized clocks at the birth event 
and make examples simpler. It has nothing to do with p-time synchrony per 
se.

So in your next paragraph your and Jimbo's proper clocks ARE synchronized 
in p-time from then on under the conditions stated.

But I don't understand the rest of your example since you just stated that 
we are to ignore their PREVIOUS and SUBSEQUENT acceleration histories to 
preserve the synchronies but then you start giving an example with 
accelerations, which will obviously change their synchrony UNLESS they are 
symmetric. You seem to claim that the accelerations are symmetric but you 
keep describing them as stopping in different frames at different times 
which indicates they are NOT symmetric.

The only way to ensure the accelerations are symmetric is for both A and B 
to have the same proper accelerations at the same proper times AFTER they 
synchronize clocks. Are you doing that? If not you are not using MY method.

Also you seem to be switching from synchronized proper clocks which I 
assumed did NOT reflect actual ages to ACTUAL AGES which doesn't work.

I used actual ages synchronized at birth (twins) to avoid that kind of 
misunderstanding.

Edgar

 





On Wednesday, March 5, 2014 4:23:54 PM UTC-5, jessem wrote:




 On Wed, Mar 5, 2014 at 2:42 PM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 Yes, but respectfully, what I'm saying is that your example doesn't 
 represent my method OR results.

 In your example of A and B separated but moving at the same velocity and 
 direction, and C and D separated but moving at the same velocity and 
 direction, BUT the two PAIRS moving at different velocities, AND where B 
 and C happen to pass each other at the same point in spacetime here is my 
 result.

 Assuming the acceleration/gravitation histories of A and B are the same 
 and they are twins; AND the acceleration/gravitation histories of C and D 
 are the same and they are twins, then A(t1)=B(t1)=C(t2)=D(t2) which is 
 clearly transitive between all 4 parties.



 You earlier agreed that if two observers are at rest relative to each 
 other, then if they synchronize clocks in their rest frame, their clocks 
 will also be synchronized in p-time from then on. In your post at 
 http://www.mail-archive.com/everything-list%40googlegroups.com/msg48404.htmlyou
  responded to
 ...

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Re: Block Universes

2014-03-06 Thread Jesse Mazer
On Thu, Mar 6, 2014 at 11:02 AM, Edgar L. Owen edgaro...@att.net wrote:

 Liz,

 Sure, but aren't the different lengths of world lines due only to
 acceleration and gravitational effects? So aren't you saying the same thing
 I was?

 Isn't that correct my little Trollette? (Note I wouldn't have included
 this except in response to your own Troll obsession.)

 Anyway let's please put our Troll references aside and give me an honest
 scientific answer for a change if you can... OK?

 It would be nice to get an answer from Brent or Jesse as well if they care
 to chime in..



In the case of the traditional twin paradox where one accelerates between
meetings while the other does not, the one that accelerates always has the
greater path length through spacetime, so in this case they are logically
equivalent. But you can have a case in SR (no gravity) where two observers
have identical accelerations (i.e. each acceleration lasts the same
interval of proper time and involves the same proper acceleration
throughout this interval), but because different proper times elapse
*between* these accelerations, they end up with worldlines with different
path lengths between their meetings (and thus different elapsed aging)...in
an online discussion a while ago someone drew a diagram of such a case that
I saved on my website:

http://www.jessemazer.com/images/tripletparadox.jpg

In this example A and B have identical red acceleration phases, but A will
have aged less than B when they reunite (you can ignore the worldline of C,
who is inertial and naturally ages more than either of them).

You can also have cases in SR where twin A accelerates more than B
(defined in terms of the amount of proper time spent accelerating, or the
value of the proper acceleration experienced during this time, or both),
but B has aged less than A when they reunite, rather than vice versa. As
always the correct aging is calculated by looking at the overall path
through spacetime in some coordinate system, and calculating its length
(proper time) with an equation that's analogous to the one you'd use to
calculate the spatial length of a path on a 2D plane.

Jesse

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Re: Block Universes

2014-03-06 Thread Edgar L. Owen
Jesse,

You are right about velocity intervals I think, but I do think there will 
be a mathematically rigorous way to compare the proper time correlation of 
any two observers from all frame views of that correlation and I do think 
they will cluster around my results. Each frame view will certainly give us 
an EXACT value for the difference in proper times between A and B and I 
think it will be possible to compare those in a meaningful way to see how 
they cluster WITHOUT weighting them.

In any case this is a peripheral though interesting subject..

Edgar

On Wednesday, March 5, 2014 4:41:17 PM UTC-5, jessem wrote:



 On Wed, Mar 5, 2014 at 2:52 PM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 Yes, the views are infinite on several axes, but that can be addressed 
 simply by enumerating views at standard intervals on those axes.


 But velocity intervals which are equal when the velocit
 ...

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Re: Block Universes

2014-03-06 Thread Edgar L. Owen
Jesse,

I don't think this is correct. It is meaningless to try to TAKE THE FRAME 
VIEW OF ALL FRAME VIEWS. That's not the correct way to look at it.

What we do is to take all frame views of any ONE proper time correlation. 
Every frame view will give one and only one EXACT answer of how close those 
proper times are to being equal. Once that's done we have the whole 
picture. We DO NOT HAVE TO TAKE FRAME VIEWS OF THOSE FRAME VIEWS because we 
already have ALL the frame views of that one situation.

Edgar



On Wednesday, March 5, 2014 5:01:10 PM UTC-5, jessem wrote:



 On Wed, Mar 5, 2014 at 4:47 PM, LizR liz...@gmail.com javascript:wrote:

 If you have a continuum of inertial frames with velocities ranging from 
 +c to -c in all possible directions, how are you going to integrate over 
 them? Isn't there a measure problem over an uncountably infinite set?



 There's no inherent problem with defining measures on uncountably infinite 
 sets--for example, a bell curve is a continuous probability measure defined 
 over the infinite real number line from -infinity to +infinity, which can 
 be integrated over any specific range to define a probability that a result 
 will fall in that range. But as I've said, the problem is that although you 
 can define a measure over all frames in relativity, if it looks like a 
 uniform distribution when you state the velocity of each frame relative to 
 a particular reference frame A, then it will be a non-uniform distribution 
 when you state the velocity of each frame relative to a different reference 
 frame B, so any such measure will be privileging one frame from the start.

 Jesse


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Re: Block Universes

2014-03-06 Thread Jesse Mazer
On Thu, Mar 6, 2014 at 11:32 AM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 Yes, from the point any two observers in the same inertial frame
 synchronize clocks, their clocks will be synchronized in p-time BUT ONLY
 FROM THEN ON (we can't know if they were previously synchronized unless we
 know their acceleration histories). And only SO LONG AS they continue in
 the same inertial frame OR undergo symmetric accelerations.

 Same ages is just a way to ensure synchronized clocks at the birth event
 and make examples simpler. It has nothing to do with p-time synchrony per
 se.

 So in your next paragraph your and Jimbo's proper clocks ARE synchronized
 in p-time from then on under the conditions stated.

 But I don't understand the rest of your example since you just stated that
 we are to ignore their PREVIOUS and SUBSEQUENT acceleration histories to
 preserve the synchronies but then you start giving an example with
 accelerations, which will obviously change their synchrony UNLESS they are
 symmetric.


I clearly stated that the reason I was giving an example of accelerations
was in case you DIDN'T accept the clocks were synchronized in p-time in my
example with Jimbo, which ignored my and Jimbo's past acceleration
histories and ages. My words were:

OK, I don't think it should be necessary to specify acceleration histories
or ages if you agree with my statement about me and Jimbo above, but if you
disagree with that statement I can give details about each pair's past
history, though it makes the example a bit more complicated.

Since you do accept my statement about p-time simultaneity in the Jimbo
example, then there's really no NEED to assume anything about A/B and C/D's
past accelerations being symmetric, we can just assume that at some point
before the experiment happened, A and B came to rest in frame F and
synchronized their clocks in frame F, and C and D came to rest in frame F'
and synchronized their clocks in frame F', and subsequently their x(t) and
T(t) functions in frame F were as I described. However, in the rest of your
post you are responding to my example of a history where A and B had
symmetrical accelerations before the experiment, and so did C and D, so I
will discuss that example; maybe it makes the statements about p-time
simultaneity conceptually clearer to think of their history that way,
although if you think it'd be simpler I'd also be just as happy to make the
assumption above that each pair synchronized clocks after they came to rest
in the same frame.




 You seem to claim that the accelerations are symmetric but you keep
 describing them as stopping in different frames at different times which
 indicates they are NOT symmetric.



In my example both accelerations were totally symmetric in the frames where
the twins started out at rest next to each other with synchronized clocks.
A and B's accelerations were totally symmetric in the unprimed frame F
where they started out both at rest at position x=12.5, and C and D's
accelerations were totally symmetric in the primed frame F' where they
started out both at rest at position x'=7.5. Of course since C and D
stopped accelerating simultaneously in the primed frame F' (at time t'=-12
in F'), they stopped accelerating at different times in the unprimed frame
F which I had used to describe their x(t) and T(t) functions, but surely
your criteria for symmetrical accelerations is just that there is ONE
specific frame where all their proper accelerations are simultaneous,
namely the frame where they started out at rest and next to each other with
synchronized clocks? Assuming that's your criteria, then F' is that one
specific frame for C and D (and note that according to relativity, C and
D's proper times T also remain synchronized in frame F' at all coordinate
times), and F is that one specific frame for A and B (and A and B's proper
times T also remain synchronized in F at all coordinate times).




 The only way to ensure the accelerations are symmetric is for both A and B
 to have the same proper accelerations at the same proper times AFTER they
 synchronize clocks. Are you doing that? If not you are not using MY method.


Yes, I was doing that. In my example I said that in the unprimed frame F, A
and B were originally at rest at position x=12.5, with both having the same
ages, and let's say that their proper time clocks have been set to read T =
-18 years at the moment they were born. Since they were right next to each
other with the same ages and their proper time clocks both showing a time
that's just their age minus 18, naturally their clocks were originally
synchronized. Then they accelerated in a completely symmetrical way in
frame F, with all changes in acceleration being simultaneous in F,
including the event of their both ceasing their acceleration and coming to
rest again in F, which happened at t=-12 in F.



 Also you seem to be switching from synchronized proper clocks which I
 assumed did NOT reflect actual ages 

Re: Block Universes

2014-03-06 Thread meekerdb

On 3/6/2014 9:01 AM, Jesse Mazer wrote:



On Thu, Mar 6, 2014 at 11:02 AM, Edgar L. Owen edgaro...@att.net 
mailto:edgaro...@att.net wrote:


Liz,

Sure, but aren't the different lengths of world lines due only to 
acceleration and
gravitational effects? So aren't you saying the same thing I was?

Isn't that correct my little Trollette? (Note I wouldn't have included this 
except
in response to your own Troll obsession.)

Anyway let's please put our Troll references aside and give me an honest 
scientific
answer for a change if you can... OK?

It would be nice to get an answer from Brent or Jesse as well if they care 
to chime
in..



In the case of the traditional twin paradox where one accelerates between meetings while 
the other does not, the one that accelerates always has the greater path length through 
spacetime, so in this case they are logically equivalent. But you can have a case in SR 
(no gravity) where two observers have identical accelerations (i.e. each acceleration 
lasts the same interval of proper time and involves the same proper acceleration 
throughout this interval), but because different proper times elapse *between* these 
accelerations, they end up with worldlines with different path lengths between their 
meetings (and thus different elapsed aging)...in an online discussion a while ago 
someone drew a diagram of such a case that I saved on my website:


http://www.jessemazer.com/images/tripletparadox.jpg

In this example A and B have identical red acceleration phases, but A will have aged 
less than B when they reunite (you can ignore the worldline of C, who is inertial and 
naturally ages more than either of them).


Right.  And you could also replace A's path with the broken line path formed by two clocks 
passing one another in opposite directions and just handing off the time reading (as in 
the diagram I posted earlier) so that there was no acceleration involved at all, yet the 
path would still have less proper time elapse than B's.


Brent



You can also have cases in SR where twin A accelerates more than B (defined in terms 
of the amount of proper time spent accelerating, or the value of the proper acceleration 
experienced during this time, or both), but B has aged less than A when they reunite, 
rather than vice versa. As always the correct aging is calculated by looking at the 
overall path through spacetime in some coordinate system, and calculating its length 
(proper time) with an equation that's analogous to the one you'd use to calculate the 
spatial length of a path on a 2D plane.


Jesse
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Re: Block Universes

2014-03-06 Thread LizR
On 7 March 2014 06:01, Jesse Mazer laserma...@gmail.com wrote:


 On Thu, Mar 6, 2014 at 11:02 AM, Edgar L. Owen edgaro...@att.net wrote:

 Liz,

 Sure, but aren't the different lengths of world lines due only to
 acceleration and gravitational effects? So aren't you saying the same thing
 I was?


I'm ignoring gravitation for the sake of simplicity, so the differences in
length of world lines is indeed due to acceleration. However the time
difference is not directly caused by acceleration, which was my point. The
same acceleration can be used to produce different lengths of world line,
for example one twin can go back and forth within the solar system while
the other one accelerates to near light-speed and travels to a nearby star
and back. The resulting time difference will always be related to the
lengths of the world lines, (which in special relativity is an absolute
measure everyone will agree on).

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Re: Block Universes

2014-03-06 Thread Jesse Mazer
Just realized in retrospect that it was a very confusing choice of
terminology to use reference frame to refer to the frame that's used to
label other frame's relative velocities--I was thinking of the idea that
other frame's velocities are labeled in reference to this one choice of
frame, but somehow it didn't occur to me that reference frame is a
synonym for frame of reference, which is what ALL frames are called. So I
edited my post below to use the term index frame instead, since I'm
indexing other frames by their velocity relative to this frame:

On Thu, Mar 6, 2014 at 12:51 PM, Jesse Mazer laserma...@gmail.com wrote:


 I don't know what you mean by the frame view of all frame views. I agree
 that for a given pair of clocks A and B that are at rest relative to each
 other and synchronized in their rest frame, each frame has only ONE answer
 to how much clock A is ahead of B (a number which can be zero if the frame
 in question is their rest frame, and can also be negative if the frame in
 question sees clock A as having a time that's behind clock B's time). But
 if we want to LABEL each such frame by velocity (so we can do an integral
 or sum over frames with different velocities to take the average), then we
 must use some specific index frame, and label the velocity of every other
 frame relative to the index frame. So for example if a given frame X has a
 velocity of 0.9c relative to a pair of clocks that are 2 light-year apart
 in their own rest frame, then in X they are out-of-sync by 2*0.9 = 1.8
 years. If we use as our index frame the rest frame of the clocks
 themselves, then X is labeled with v=0.9c since that's its velocity
 relative to the index frame, and thus our amount out of sync as a function
 of v function will have a value of 1.8 at v=0.9c. On the other hand, if we
 use as our index frame a frame moving at 0.8c relative to the clocks,
 then frame X will have to be labeled with v=0.357c since that's its
 velocity relative to the new index frame--it's still the same frame X, and
 it still has the same amount-out-of-sync of 1.8, but it just has a
 different velocity label. So using this index frame, our amount out of
 sync as a function of v function will have a value of 1.8 at v=0.357c.

 Point is, depending on the index frame we use to define the v of every
 other frame, our amount out of sync as a function of v function will look
 different, and thus if we integrate over that function to find some sort of
 average value for the amount the clocks are out of sync, or just do an
 average over a finite number of values of the function at regular intervals
 of v, then we'll get different answers depending on what index frame we
 chose.

 Jesse


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Re: Block Universes

2014-03-05 Thread Edgar L. Owen
Jesse,

First I see no conclusion that demonstrates INtransitivity here or any 
contradiction that I asked for. Did I miss that?

But that really doesn't matter because second, you are NOT using MY method 
because you are using ANOTHER coordinate clock FRAME rather than the frame 
views of the parties of their OWN age relationships.

So whatever proof you think you have, it is not a proof about my method.

So, in spite of what you claim you just seem to be trying to prove there is 
no simultaneity of VIEWS of age relationships rather than addressing the 
ACTUAL age relationships of the parties themselves which is my whole point.

Edgar

.

On Tuesday, March 4, 2014 8:03:57 PM UTC-5, jessem wrote:



 On Tue, Mar 4, 2014 at 5:45 PM, Jesse Mazer laser...@gmail.comjavascript:
  wrote:


  
 I promise you the example has nothing to do with any frames other than 
 the ones in which each pair is at rest. Again, the only assumptions about 
 p-time that I make in deriving the contradiction are:

 ASSUMPTION 1. If two observers are at rest in the same inertial frame, 
 then events on their worldlines that are simultaneous in their rest frame 
 are also simultaneous in p-time

 ASSUMPTION 2. If two observers cross paths at a single point in spacetime 
 P, and observer #1's proper time at P is T1 while observer #2's proper time 
 at P is T2, then the event of observer #1's clock showing T1 is 
 simultaneous in p-time with the event of observer #2's clock showing T2.

 ASSUMPTION 3. p-time simultaneity is transitive

 That's it! I make no other assumptions about p-time simultaneity. But if 
 you want to actually see how the contradiction is derived, there's really 
 no shortcut besides looking at the math. If you are willing to do that, can 
 we just start with the last 2 questions I asked about the scenario? Here's 
 what I asked again, with a few cosmetic modifications:

 Please have another look at the specific numbers I gave for x(t), 
 coordinate position as a function of coordinate time, and T(t), proper time 
 as a function of coordinate time, for each observer (expressed using the 
 inertial frame where A and B are at rest, and C and D are moving at 0.8c), 
 and then tell me if you agree or disagree with the following two statements:

 For A: x(t) = 25, T(t) = t
 For B: x(t) = 0, T(t) = t
 For C: x(t) = 0.8c * t, T(t) = 0.6*t
 For D: x(t) = [0.8c * t] + 9, T(t) = 0.6*t - 12

 --given the x(t) functions for B and C, we can see that they both pass 
 through the point in spacetime with coordinates x=0, t=0. Given their T(t) 
 functions, we can see that B has a proper time T=0 at those coordinates, 
 and C also has a proper time T=0 at those coordinates. Therefore, by 
 ASSUMPTION 1 above, the event of B's proper time clock reading T=0 is 
 simultaneous in p-time with the event of C's proper time clock reading T=0. 
 Agree or disagree?

 --given the x(t) functions for A and D, we can see that they both pass 
 through the point in spacetime with coordinates x=25, t=20. Given their 
 T(t) functions, we can see that A has a proper time T=20 at those 
 coordinates, and D has a proper time T=0 at those coordinates. Therefore, 
 by ASSUMPTION 1 above, the event of A's proper time clock reading T=20 is 
 simultaneous in p-time with the event of D's proper time clock reading T=0. 
 Agree or disagree?


 Another little correction--in the last two paragraphs there, where I said 
 Therefore, by ASSUMPTION 1 above, I should have written ASSUMPTION 2, 
 since in both cases I was deriving p-time simultaneity from the fact that 
 two clock readings happened at the same point in spacetime.

 Jesse


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Re: Block Universes

2014-03-05 Thread Edgar L. Owen
Jesse,

Here's another point for you to ponder:

You claim that all frame views are equally valid. What would you say the 
weighted mean of all frame views is? I would suspect that it converges 
towards my solution. It is clear from your own analysis that it does 
converge to my solution as separation and relative motion diminishes, so I 
strongly suspect it converges towards my solution in all cases.

Correct? And if so I would argue that this also tends to validate my 
solution as the actual correct 1:1 correlation of proper ages, even though 
I agree completely that all observers cannot direct observe this 
correlation...

In fact this is tantalizingly similar to the notion of a wavefunction 
representing the probabilities of all possible locations of a particle. If 
we take all possible frame views as a continuous 'wavefunction' of the 
actual age correlation can we begin to assign probabilities based on their 
weighted mean, and if so isn't that going to be my solution?

Edgar


On Tuesday, March 4, 2014 8:03:57 PM UTC-5, jessem wrote:



 On Tue, Mar 4, 2014 at 5:45 PM, Jesse Mazer laser...@gmail.comjavascript:
  wrote:


 div

 ...

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Re: Block Universes

2014-03-05 Thread Jesse Mazer
On Wed, Mar 5, 2014 at 8:19 AM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 First I see no conclusion that demonstrates INtransitivity here or any
 contradiction that I asked for. Did I miss that?


No, I was just asking if you agreed with those two steps, which show that
different pairs of readings are simultaneous using ASSUMPTION 2. If you
agreed with those, I would show that several further pairs of readings must
also be judged simultaneous in p-time using ASSUMPTION 1, and then all
these individual simultaneity judgments would together lead to a
contradiction via the transitivity assumption, ASSUMPTION 3. I already laid
this out in the original Alice/Bob/Arlene/Bart post, but since you
apparently didn't understand that post I wanted to go over everything more
carefully with the exact x(t) and T(t) functions given, and every point
about simultaneity stated more carefully.

I thought you would be more likely to answer if I just gave you two
statements to look over and verify rather than a large collection of them,
but if you are going to stubbornly refuse to answer the opening questions
until I lay out the whole argument, here it is in full:

ASSUMPTION 1. If two observers are at rest in the same inertial frame, then
events on their worldlines that are simultaneous in their rest frame are
also simultaneous in p-time

ASSUMPTION 2. If two observers cross paths at a single point in spacetime
P, and observer #1's proper time at P is T1 while observer #2's proper time
at P is T2, then the event of observer #1's clock showing T1 is
simultaneous in p-time with the event of observer #2's clock showing T2.

ASSUMPTION 3. p-time simultaneity is transitive

Please have another look at the specific numbers I gave for x(t),
coordinate position as a function of coordinate time, and T(t), proper time
as a function of coordinate time, for each observer (expressed using the
inertial frame where A and B are at rest, and C and D are moving at 0.8c),
and then tell me if you agree or disagree with the following two statements:

For A: x(t) = 25, T(t) = t
For B: x(t) = 0, T(t) = t
For C: x(t) = 0.8c * t, T(t) = 0.6*t
For D: x(t) = [0.8c * t] + 9, T(t) = 0.6*t - 12

STATEMENT 1. Given the x(t) functions for B and C, we can see that they
both pass through the point in spacetime with coordinates x=0, t=0. Given
their T(t) functions, we can see that B has a proper time T=0 at those
coordinates, and C also has a proper time T=0 at those coordinates.
Therefore, by ASSUMPTION 2 above, the event of B's proper time clock
reading T=0 is simultaneous in p-time with the event of C's proper time
clock reading T=0. Agree or disagree?

STATEMENT 2. Given the x(t) functions for A and D, we can see that they
both pass through the point in spacetime with coordinates x=25, t=20. Given
their T(t) functions, we can see that A has a proper time T=20 at those
coordinates, and D has a proper time T=0 at those coordinates. Therefore,
by ASSUMPTION 2 above, the event of A's proper time clock reading T=20 is
simultaneous in p-time with the event of D's proper time clock reading T=0.
Agree or disagree?

STATEMENT 3. At t=0 in this frame, both A and B have a proper time of T=0;
these readings are simultaneous in this frame. Since A and B are both at
rest in this frame, by ASSUMPTION 1 above, the event of A's proper time
clock reading T=0 is simultaneous in p-time with the event of B's proper
time clock reading T=0. Agree or disagree?

STATEMENT 4. C's worldline passes through the point x=0, t=0, and at this
point C's proper time clock reads T=0. D's worldline passes through the
point  x=25, t=20, and at this point D's proper time clock reads T=0. These
events are not simultaneous in this frame, but using the Lorentz
transformation we can see that they ARE simultaneous in the frame where C
and D are at rest. Therefore, by ASSUMPTION 1 above, the event of C's
proper time clock reading T=0 is simultaneous in p-time with the event of
D's proper time clock reading T=0. Agree or disagree?

Note: This statement is perhaps the subtlest if you aren't too familiar
with the math of SR--in case you didn't know, the Lorentz transformation is
used when we know the coordinates x,t of an event in one inertial frame,
and we want to find the coordinates x',t' of the SAME event in a second
inertial frame which is moving at speed v relative to the first (a good
intro to various aspects of SR including the Lorentz transform can be found
at http://en.wikibooks.org/wiki/Special_Relativity ). Assuming that the
spatial origins of the two frames coincide when t=0 in the first frame and
t'=0 in the second, and assuming that the first frame subsequently sees the
origin of the second frame moving at speed v along the first frame's
x-axis, the transformation equations are:

x' = gamma*(x - v*t)
t' = gamma*(t - (v*x)/c^2 )

Where gamma is the commonly-used relativistic factor 1/sqrt(1 - (v/c)^2).
So with v=0.8c in this example, gamma works out to 1/sqrt(1 - 0.64) =

Re: Block Universes

2014-03-05 Thread Jesse Mazer
On Wed, Mar 5, 2014 at 8:38 AM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 Here's another point for you to ponder:

 You claim that all frame views are equally valid. What would you say the
 weighted mean of all frame views is?


Weighted how? I can't see any weighing that doesn't itself depend on
privileging one frame over others. For example, suppose I label frames
using velocity relative to my rest frame, and use a uniform distribution on
velocity values as my weight function, which implies that the collection of
frames with velocities between 0.1c and 0.1c + dV will have the same total
weight as the collection of frames with velocities between 0.9c and 0.9c +
dV, since these are equal-sized velocity intervals (for example, if
dV=0.05c then we are looking at the frames from 0.1c to 0.15c, and the
frames from 0.9c to 0.95c). But if we look at all the frames in these two
intervals, and translate from their velocities relative to ME to their
velocities relative to another frame B that is moving at say 0.8c relative
to me, then these two bunches of frames do NOT occupy equal-sized velocity
intervals when we look at their velocities relative to frame B (an interval
from 0.1c to 0.15c in my frame translates to the interval from -0.761c to
-0.739c in B's frame, while an interval of 0.9c to 0.95c in my frame
translates to an interval from 0.357c to 0.625c in B's frame). So if we
weigh them equally using MY velocity labels, that would translate to an
unequal weighing relative to B's velocity labels, so we are privileging my
frame's definitions over the definitions of other frames like B.




 I would suspect that it converges towards my solution. It is clear from
 your own analysis that it does converge to my solution as separation and
 relative motion diminishes, so I strongly suspect it converges towards my
 solution in all cases.

 Correct? And if so I would argue that this also tends to validate my
 solution as the actual correct 1:1 correlation of proper ages, even though
 I agree completely that all observers cannot direct observe this
 correlation...

 In fact this is tantalizingly similar to the notion of a wavefunction
 representing the probabilities of all possible locations of a particle. If
 we take all possible frame views as a continuous 'wavefunction' of the
 actual age correlation can we begin to assign probabilities based on their
 weighted mean, and if so isn't that going to be my solution?


This doesn't really help your case unless you can find a weight function
for the continuous infinity of different possible frames that doesn't
itself privilege one frame's definitions from the start.

Jesse

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Re: Block Universes

2014-03-05 Thread Edgar L. Owen
Jesse,

Yes, you are right. I phrased it incorrectly.

What I meant to say was not that each individual view was somehow weighted, 
but that all views considered together would tend to cluster around my 
results for any distance and motion difference pairs. In other words there 
would be a lot more views that were close to my solution, than views that 
were far from my solution. And that we can see this because, as you 
yourself pointed out, as distance separation and relative motion 
differences decrease all other frame views DO tend to converge on my 
results.

Thus the aggregate WEIGHT OF ALL VIEWS tends to converge on my solution, 
which is what I meant to say. Sort of like a Bell curve distribution with a 
point at top representing my solution

Would you agree to that?

Edgar

On Wednesday, March 5, 2014 11:00:19 AM UTC-5, jessem wrote:



 On Wed, Mar 5, 2014 at 8:38 AM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 Here's another point for you to ponder:

 You claim that all frame views are equally valid. What would you say the 
 weighted mean of all frame views is?


 Weighted how? I can't see any weighing that doesn't itself depend on 
 privileging one frame over others. For example, suppose I label frames 
 using velocity relative to my rest frame, and use a uniform distribution on 
 velocity values as my weight function, which implies that the collection of 
 frames with velocities between 0.1c and 0.1c + dV will have the same total 
 weight as the collection of frames with velocities between 0.9c and 0.9c + 
 dV, since these are equal-sized velocity intervals (for example, if 
 dV=0.05c then we are looking at the frames from 0.1c to 0.15c, and the 
 frames from 0.9c to 0.95c). But if we look at all the frames in these two 
 intervals, and translate from their velocities relative to ME to their 
 velocities relative to another frame B that is moving at say 0.8c relative 
 to me, then these two bunches of frames do NOT occupy equal-sized velocity 
 intervals when we look at their velocities relative to frame B (an interval 
 from 0.1c to 0.15c in my frame translates to the interval from -0.761c to 
 -0.739c in B's frame, while an interval of 0.9c to 0.95c in my frame 
 translates to an interval from 0.357c to 0.625c in B's frame). So if we 
 weigh them equally using MY velocity labels, that would translate to an 
 unequal weighing relative to B's velocity labels, so we are privileging my 
 frame's definitions over the definitions of other frames like B.


  

 I would suspect that it converges towards my solution. It is clear from 
 your own analysis that it does converge to my solution as separation and 
 relative motion diminishes, so I strongly suspect it converges towards my 
 solution in all cases.

 Correct? And if so I would argue that this also tends to validate my 
 solution as the actual correct 1:1 correlation of proper ages, even though 
 I agree completely that all observers cannot direct observe this 
 correlation...

 In fact this is tantalizingly similar to the notion of a wavefunction 
 representing the probabilities of all possible locations of a particle. If 
 we take all possible frame views as a continuous 'wavefunction' of the 
 actual age correlation can we begin to assign probabilities based on their 
 weighted mean, and if so isn't that going to be my solution?


 This doesn't really help your case unless you can find a weight function 
 for the continuous infinity of different possible frames that doesn't 
 itself privilege one frame's definitions from the start.

 Jesse


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Re: Block Universes

2014-03-05 Thread Jesse Mazer
On Wed, Mar 5, 2014 at 1:27 PM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 Yes, you are right. I phrased it incorrectly.

 What I meant to say was not that each individual view was somehow
 weighted, but that all views considered together would tend to cluster
 around my results for any distance and motion difference pairs.


Too vague. What does all views considered together mean mathematically,
if not a weighted average using some specific weighting function?



 In other words there would be a lot more views that were close to my
 solution, than views that were far from my solution.


How do you count more when there are a continuous infinity of frame's
views? The only way to count different subsets of an infinite set is
using some sort of measure function (see
https://en.wikipedia.org/wiki/Measure_(mathematics) ), which is equivalent
to a weighting function--whatever you choose to call it, the idea would be
that if you want to compare the number or weight of frames with
velocity between v1 and v2 (the velocities defined relative to some other
specific frame, of course) vs. the number or weight with velocity
between v3 and v4, you use a measure/weight function W(v) which gives a
value for every specific frame velocity v, and you integrate the function
W(v) from v1 to v2, and compare the result to integrating W(v) between v3
and v4 (and if you want to do a weighted average of some specific
quantity Q(v) that varies from one frame to another, like the amount by
which two clocks are out-of-sync, you would integrate Q(v)*W(v) over the
frame velocity interval over which you want the weighted average of Q).




 And that we can see this because, as you yourself pointed out, as distance
 separation and relative motion differences decrease all other frame views
 DO tend to converge on my results.

 Thus the aggregate WEIGHT OF ALL VIEWS tends to converge on my solution,
 which is what I meant to say. Sort of like a Bell curve distribution with a
 point at top representing my solution

 Would you agree to that?



In the case of two clocks at rest and synchronized in a common frame, the
only convergence I think we agree on is if you consider a series of cases
where the distance between the two clocks approaches 0, or where the
velocity of the frame whose opinion you're considering relative to the rest
frame of the two clocks approaches 0 (which may be what you meant by as
distance separation and relative motion differences decrease all other
frame views DO tend to converge on my results). If you are talking about a
FIXED value for the distance between two clocks in their rest frame, and
doing a weighted average of larger and larger sets of different frame's
opinions about the time difference between the two clocks (eventually
including frames with a very large velocity relative to the clocks), then
what value this average would converge to would depend entirely on the
weighting function. As I said a weighting function that looks uniform in
one frame (equal velocity intervals have equal weight when you integrate
over the integral) will look non-uniform in other frames, so I can't see a
way to define a weighting function that doesn't privilege one frame at the
outset.

Jesse

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Re: Block Universes

2014-03-05 Thread Edgar L. Owen
Jesse,

Yes, but respectfully, what I'm saying is that your example doesn't 
represent my method OR results.

In your example of A and B separated but moving at the same velocity and 
direction, and C and D separated but moving at the same velocity and 
direction, BUT the two PAIRS moving at different velocities, AND where B 
and C happen to pass each other at the same point in spacetime here is my 
result.

Assuming the acceleration/gravitation histories of A and B are the same and 
they are twins; AND the acceleration/gravitation histories of C and D are 
the same and they are twins, then A(t1)=B(t1)=C(t2)=D(t2) which is clearly 
transitive between all 4 parties.

We don't know what t1 and t2 are because you haven't specified their 
acceleration histories or birth dates, but whatever they are the equation 
above will hold.

The problem is that your careful analysis simply DOES NOT use MY method 
which depends on the actual real physical causes (acceleration histories) 
to deternine 1:1 age correlations between any two observers. It uses YOUR 
method to prove the standard lack of simultaneity between VIEWS of pairs of 
actual physical events. This is a WELL KNOWN result of relativity WITH 
WHICH I AGREE!

But for the nth time, my method concentrates on the ACTUAL RELATIONSHIP, 
rather than VIEWS of that actual relationship.

This is a simple, well accepted logical distinction which most certainly 
applies here to the ACTUAL age correlations of people..

If a man and a wife love each other that is a real actual physical 
relationship. The fact that someone else thinks they don't love each other 
may well be his real VIEW, but it does NOT change or affect the ACTUAL love 
between the man and his wife.

No matter how many times I state this it doesn't seem to sink in

Edgar



On Wednesday, March 5, 2014 10:36:10 AM UTC-5, jessem wrote:


 On Wed, Mar 5, 2014 at 8:19 AM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 First I see no conclusion that demonstrates INtransitivity here or any 
 contradiction that I asked for. Did I miss that?


 No, I was just asking if you agreed with those two steps, which show that 
 different pairs of readings are simultaneous using ASSUMPTION 2. If you 
 agreed with those, I would show that several further pairs of readings must 
 also be judged simultaneous in p-time using ASSUMPTION 1, and then all 
 these individual simultaneity judgments would together lead to a 
 contradiction via the transitivity assumption, ASSUMPTION 3. I already laid 
 this out in the original Alice/Bob/Arlene/Bart post, but since you 
 apparently didn't understand that post I wanted to go over everything more 
 carefully with the exact x(t) and T(t) functions given, and every point 
 about simultaneity stated more carefully.

 I thought you would be more likely to answer if I just gave you two 
 statements to look over and verify rather than a large collection of them, 
 but if you are going to stubbornly refuse to answer the opening questions 
 until I lay out the whole argument, here it is in full:/d
 ...

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Re: Block Universes

2014-03-05 Thread Edgar L. Owen
Jesse,

Yes, the views are infinite on several axes, but that can be addressed 
simply by enumerating views at standard intervals on those axes. Or you 
could equally integrate over the continuous functions. 

Considered together simply means you plot the correlation each frame view 
(at the standard intervals as above) gives and see how they cluster. Which 
I'm pretty sure will be around my result.

You don't need to view the resulting graph from any frame as you seem to 
suggest, because the graph is OF the actual all frame view results.

For every frame you simply calculate the apparent lack of simultaneity 
between two events Nonsiimultaneity=(t1-t2) and plot it relative to the 
simultaneity that my method claims is actual.

Edgar



On Wednesday, March 5, 2014 2:13:24 PM UTC-5, jessem wrote:



 On Wed, Mar 5, 2014 at 1:27 PM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 Yes, you are right. I phrased it incorrectly.

 What I meant to say was not that each individual view was somehow 
 weighted, but that all views considered together would tend to cluster 
 around m

 ...

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Re: Block Universes

2014-03-05 Thread Edgar L. Owen
Jesse,

PS: It is well known that accelerations and gravitation are the ONLY causes 
that produce real actual age rate changes. These real actual age rate 
changes are real and actual because 1. ALL OBSERVERS AGREE on them when 
they meet up and check them, and 2.BECAUSE THEY ARE PERMANENT.

Relativity agrees on this when the parties MEET. All my method does is to 
give a method to calculate these real actual changes BEFORE they meet, when 
the parties are still separated or in relative motion or acceleration or 
gravitation.

This is incredibly simple to understand if you can just escape the notion 
that all VIEWS of an age relationship are somehow the same as the ACTUAL 
relationship itself. The views DO differ and these VIEWS ARE VALID VIEWS, 
but they don't affect the actual RELATIONSHIP THEY ARE VIEWING which is 
what my method calculates.

Again, this is a difference in INTERPRETATIONS of relativity. It does NOT 
contradict the equations of relativity itself. It simply uses the one that 
describes the actual relationship rather than ones that describe VIEWS of 
that relationship.

Aren't you at least able to understand what I'm saying even if you don't 
agree with it? I see no evidence you are even able to do that

Edgar



On Wednesday, March 5, 2014 2:13:24 PM UTC-5, jessem wrote:



 On Wed, Mar 5, 2014 at 1:27 PM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 Yes, you are right. I phrased it incorrectly.

 What I meant to say was not that each individual view was somehow 
 weighted, but that all views considered together would tend to cluster 
 around m

 ...

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Re: Block Universes

2014-03-05 Thread LizR
On 6 March 2014 09:12, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 PS: It is well known that accelerations and gravitation are the ONLY
 causes that produce real actual age rate changes. These real actual age
 rate changes are real and actual because 1. ALL OBSERVERS AGREE on them
 when they meet up and check them, and 2.BECAUSE THEY ARE PERMANENT.


Having your worldlines be different lengths in spacetime will also cause
differences in actual age, as Brent has explained (with diagrams).

Consistently ignoring this point and others like it is one reason most
people here consider you a troll, so please try to address it.

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Re: Block Universes

2014-03-05 Thread Jesse Mazer
On Wed, Mar 5, 2014 at 2:42 PM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 Yes, but respectfully, what I'm saying is that your example doesn't
 represent my method OR results.

 In your example of A and B separated but moving at the same velocity and
 direction, and C and D separated but moving at the same velocity and
 direction, BUT the two PAIRS moving at different velocities, AND where B
 and C happen to pass each other at the same point in spacetime here is my
 result.

 Assuming the acceleration/gravitation histories of A and B are the same
 and they are twins; AND the acceleration/gravitation histories of C and D
 are the same and they are twins, then A(t1)=B(t1)=C(t2)=D(t2) which is
 clearly transitive between all 4 parties.



You earlier agreed that if two observers are at rest relative to each
other, then if they synchronize clocks in their rest frame, their clocks
will also be synchronized in p-time from then on. In your post at
http://www.mail-archive.com/everything-list%40googlegroups.com/msg48404.htmlyou
responded to one of my questions in this way:

'Yes is the answer to your question if two clocks are at rest relative to
one another and synchronized according to the definition of simultaneity
in their mutual rest frame, do you automatically assume this implies they
are synchronized in p-time? '

You didn't say anything about their ages having to be equal, or about their
needing to have had identical acceleration histories before this. For
example, if I and some stranger named Jimbo are at rest relative to each
other in an inertial frame in flat SR spacetime (no gravity), and in this
frame my 37th birthday is simultaneous with Jimbo's 20th birthday, then if
I set my clock to T=0 on my 37th birthday and he sets his clock to T=0 on
his 20th birthday, isn't this sufficient to demonstrate that our clocks
will be synchronized in p-time from then on (provided we both remain at
rest in this frame), regardless of how either of us may have accelerated
*before* we came to rest in this frame? (assuming of course that I came to
rest before my 37th birthday, and Jimbo came to rest before his 20th)

Even if you somehow don't agree with this, I can easily fill in some
details about the past history of my example to give A/B and C/D
symmetrical accelerations, if you wish--see below.




 We don't know what t1 and t2 are because you haven't specified their
 acceleration histories or birth dates, but whatever they are the equation
 above will hold.


OK, I don't think it should be necessary to specify acceleration histories
or ages if you agree with my statement about me and Jimbo above, but if you
disagree with that statement I can give details about each pair's past
history, though it makes the example a bit more complicated.

Say that in the frame F where A and B are at rest during the period I
described, A and B were originally at rest at position x=12.5, with both
having the same ages, and let's say that their proper time clocks have been
set to read T = -18 years at the moment they were born (it is the custom in
their society to have their proper time clock tell how far from voting age
they are, so for example when they turn 15 their clock reads T=-3, when
they turn 28 their clock reads T=10, etc.). Then each of them
simultaneously began to accelerate in opposite directions with a fixed
proper acceleration of 1 light year/year^2, and after each had traveled a
distance of 6.25 light years from their starting position in this frame,
they began to decelerate (i.e. turn their rockets around and accelerate in
the opposite direction, lowering their speed in this frame) at the same
proper acceleration of 1 light year/year^2. After they each had traveled
another 6.25 light years and come to rest in this frame, they stopped
decelerating and simply remained at rest. Each of them will have then
traveled a distance of 12.5 light years from their original starting
position of x=12.5 light years, with A at position x=25 light years, and B
at position x=0 light years. Hopefully you agree that because their
accelerations are completely symmetrical in the frame where they were
originally at rest with the same ages, in this frame identical ages will
still be simultaneous after they finish the acceleration/deceleration phase
and come to rest. So, let's just say that they come to rest simultaneously
at t=-12 in this frame, and at this moment their clocks both read T=-12,
meaning they are both turning 6 at the moment they stop accelerating. After
this, their x(t) and T(t) functions are just as I described.

As for C and D, let's switch over to the frame F' where THEY are at rest
during the period I describe, whose coordinates I had previously labeled as
x' and t' (and given the Lorentz transformation equations for converting
from x,t to x',t'). Say that in frame F', they were both originally at rest
at position x'=7.5, again with both having the same ages, and both having
their proper time clocks read a time of T 

Re: Block Universes

2014-03-05 Thread Jesse Mazer
On Wed, Mar 5, 2014 at 2:52 PM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 Yes, the views are infinite on several axes, but that can be addressed
 simply by enumerating views at standard intervals on those axes.


But velocity intervals which are equal when the velocities are defined
relative to one frame are not equal when the velocities are defined
relative to a different frame. I already mentioned an example where if a
frame 1 has velocity v=0.1c relative to me and another frame 2 has velocity
v=0.15c relative to me, then the interval between them is 0.05c from my
perspective, and likewise if a frame 3 has velocity v=0.9c relative to me
and another frame 4 has velocity v=0.95c relative to me, then they have the
same interval of 0.05c from my perspective; but for another observer moving
at v=0.8c relative to me, frame 1 has a velocity of -0.761c and frame 2 has
a velocity of -0.739c (so the interval between 1 and 2 is 0.022 for this
observer), whereas frame 3 has a velocity of 0.357c and frame 4 has a
velocity of 0.625c (so the interval between 3 and 4 is 0.268c for this
observer, more than ten times larger than the interval between 1 and 2).
These velocities are calculated using the relativistic velocity formula at
http://math.ucr.edu/home/baez/physics/Relativity/SR/velocity.html where u =
-0.8c is my velocity relative to the second observer, and v is the velocity
of any given frame 1,2,3, or 4 relative to me.

Point is, if your intervals are equal relative to one frame but unequal
relative to all other frames, then you are privileging a particular frame's
perspective from the start.



 Or you could equally integrate over the continuous functions.


As I said, the only way to do this is to use some sort of weight/measure
function, and a weight/measure function which is uniform when plotted
against velocity in one frame will be non-uniform when plotted against
velocity in other frames, so there doesn't seem to be a way of picking such
a function that doesn't privilege one frame from the start.




 Considered together simply means you plot the correlation each frame view
 (at the standard intervals as above) gives and see how they cluster. Which
 I'm pretty sure will be around my result.


The will cluster around the judgment of whatever frame you choose to
privilege from the start, either by your definition of equal intervals or
by your weighting/measure function. So, using this to conclude anything
about the actual correlation would just be another piece of circular
reasoning.

Jesse





 You don't need to view the resulting graph from any frame as you seem to
 suggest, because the graph is OF the actual all frame view results.

 For every frame you simply calculate the apparent lack of simultaneity
 between two events Nonsiimultaneity=(t1-t2) and plot it relative to the
 simultaneity that my method claims is actual.

 Edgar



 On Wednesday, March 5, 2014 2:13:24 PM UTC-5, jessem wrote:



 On Wed, Mar 5, 2014 at 1:27 PM, Edgar L. Owen edga...@att.net wrote:

 Jesse,

 Yes, you are right. I phrased it incorrectly.

 What I meant to say was not that each individual view was somehow
 weighted, but that all views considered together would tend to cluster
 around m

 ...

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Re: Block Universes

2014-03-05 Thread LizR
If you have a continuum of inertial frames with velocities ranging from +c
to -c in all possible directions, how are you going to integrate over them?
Isn't there a measure problem over an uncountably infinite set?

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Re: Block Universes

2014-03-05 Thread Jesse Mazer
On Wed, Mar 5, 2014 at 3:12 PM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 PS: It is well known that accelerations and gravitation are the ONLY
 causes that produce real actual age rate changes. These real actual age
 rate changes are real and actual because 1. ALL OBSERVERS AGREE on them
 when they meet up and check them, and 2.BECAUSE THEY ARE PERMANENT.


No, they produce real actual differences in TOTAL ELAPSED PROPER TIME
BETWEEN MEETINGS, which all frames agree on. This tells us nothing about
the moment-by-moment rates of each clock between meetings, unless you are
simply talking about the AVERAGE ticking rate between meetings (and all
frames do agree on the ratio between two clock's AVERAGE ticking rate
between meetings, since the average ticking rate for clock #1 between
meetings in any frame is [proper time elapsed on #1 between meetings /
coordinate time between meetings] and the average ticking rate for clock #2
is [proper time elapsed on #2 between meetings / coordinate time between
meetings], thus the ratio of the two averages is [proper time elapsed on #1
between meetings / proper time elapsed on #2 between meetings] which all
frames will agree on).



 Relativity agrees on this when the parties MEET. All my method does is to
 give a method to calculate these real actual changes BEFORE they meet, when
 the parties are still separated or in relative motion or acceleration or
 gravitation.


It gives a method which is based on simply ASSUMING FROM THE START that
the clock rates behave a certain way between the meetings, without ever
deriving or demonstrating this from more basic premises. Even a fellow
presentist could easily disagree with your assumptions, and you would have
no ARGUMENT for convincing him that your assumptions are correct, using
starting premises that you both could agree on.

And as always, my example with two pairs of twins demonstrates that your
methods lead to a direct contradiction where two different ages of A have
to labeled simultaneous in p-time--if you disagree, the only intellectually
honest way to show I'm wrong is to go through my numbered STATEMENTs
about p-time simultaneity, and tell me which is the first that is not a
valid inference using your method.




 This is incredibly simple to understand if you can just escape the notion
 that all VIEWS of an age relationship are somehow the same as the ACTUAL
 relationship itself. The views DO differ and these VIEWS ARE VALID VIEWS,
 but they don't affect the actual RELATIONSHIP THEY ARE VIEWING which is
 what my method calculates.

 Again, this is a difference in INTERPRETATIONS of relativity. It does NOT
 contradict the equations of relativity itself. It simply uses the one that
 describes the actual relationship rather than ones that describe VIEWS of
 that relationship.

 Aren't you at least able to understand what I'm saying even if you don't
 agree with it? I see no evidence you are even able to do that


I understand that your method gives a way of deciding which events are
simultaneous in p-time in your theory, it just that:

a) I don't think you have any argument for the validity of your method that
doesn't simply assume p-time simultaneity works the way you want it to from
the start, something that even another presentist who believes in absolute
simultaneity could reasonably disagree with

b) I think your method can be used to derive a contradiction, even though
you don't understand that yet and seem to be refusing to engage with the
nitty-gritty details of my example.

Jesse




 On Wednesday, March 5, 2014 2:13:24 PM UTC-5, jessem wrote:



 On Wed, Mar 5, 2014 at 1:27 PM, Edgar L. Owen edga...@att.net wrote:

 Jesse,

 Yes, you are right. I phrased it incorrectly.

 What I meant to say was not that each individual view was somehow
 weighted, but that all views considered together would tend to cluster
 around m

 ...

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Re: Block Universes

2014-03-05 Thread Jesse Mazer
On Wed, Mar 5, 2014 at 4:47 PM, LizR lizj...@gmail.com wrote:

 If you have a continuum of inertial frames with velocities ranging from +c
 to -c in all possible directions, how are you going to integrate over them?
 Isn't there a measure problem over an uncountably infinite set?



There's no inherent problem with defining measures on uncountably infinite
sets--for example, a bell curve is a continuous probability measure defined
over the infinite real number line from -infinity to +infinity, which can
be integrated over any specific range to define a probability that a result
will fall in that range. But as I've said, the problem is that although you
can define a measure over all frames in relativity, if it looks like a
uniform distribution when you state the velocity of each frame relative to
a particular reference frame A, then it will be a non-uniform distribution
when you state the velocity of each frame relative to a different reference
frame B, so any such measure will be privileging one frame from the start.

Jesse

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Re: Block Universes

2014-03-05 Thread LizR
On 6 March 2014 11:01, Jesse Mazer laserma...@gmail.com wrote:

 On Wed, Mar 5, 2014 at 4:47 PM, LizR lizj...@gmail.com wrote:

 If you have a continuum of inertial frames with velocities ranging from
 +c to -c in all possible directions, how are you going to integrate over
 them? Isn't there a measure problem over an uncountably infinite set?


 There's no inherent problem with defining measures on uncountably infinite
 sets--for example, a bell curve is a continuous probability measure defined
 over the infinite real number line from -infinity to +infinity, which can
 be integrated over any specific range to define a probability that a result
 will fall in that range. But as I've said, the problem is that although you
 can define a measure over all frames in relativity, if it looks like a
 uniform distribution when you state the velocity of each frame relative to
 a particular reference frame A, then it will be a non-uniform distribution
 when you state the velocity of each frame relative to a different reference
 frame B, so any such measure will be privileging one frame from the start.

 Ah, yes, I know you can integrate some continuous function from + to -
infinity, but I was assuming that cases like Bell curves were privileging
one particular point (e.g. starting from or centred on 0) - but I guess I
got that wrong.

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Re: Block Universes

2014-03-04 Thread Edgar L. Owen
Jesse,

I'm interested in finding the truth, not in assigning blame.

The important thing is we both now agree that there IS ALWAYS A CORRELATION 
OF ACTUAL AGES between any two observers.

The difference is I think it's an EXACT correlation, and you think that 
it's ALMOST EXACT except for cases of extreme separation or motion.

I think we have to analyze the age correlation from a POV that preserves 
the actual relationship of the accelerations that are the ONLY cause of age 
rate differences. Whereas you think we have to consider all possible views 
irrespective of whether they properly preserve the relationship of causes 
of age rate differences. My method provides an EXACT correlation. Your 
method provides an ALMOST EXACT correlation in all but extreme cases.


Also now that I have pointed out the error in your Alice, Bob, Arlene, Bart 
example do you agree my method does produce consistent, unambiguous and 
transitive 1:1 correlations of proper ages among all observers?


To address your new questions:

Do you deny acceleration and gravitation produce real actual slowings of 
clock rates and thus of real actual aging rates? Of course we can VIEW 
these slowings differently from different frames, but the ACTUAL effects 
they produce on the observer who experiences them are exact. It is these 
exact actual effects that my method explains, and yours doesn't. We know 
these effects are real and actual when twins meet up with different ages. 
Thus we know they were ALSO REAL AND ACTUAL BEFORE the twins met. That is 
pure simple logic.

How many times do I have to explain. The twins exchange flight plans for 
EXACT SAME ACCLERATIONS AT THE EXACT SAME TIMES before they part. This 
ABSOLUTELY ENSURES that their age rates will slow EXACTLY THE SAME during 
their trip. There is no way around that. Another observer can VIEW that 
differently but from the POV of the twins themselves it IS EXACT AND 
ABSOLUTE. Thus it is clear to anyone that to properly analyze the REAL 
ACTUAL CORRELATION OF THE TWINS' AGES WE MUST PRESERVE THE REAL ACTUAL 
RELATIONSHIP OF THE ACCELERATIONS THAT ARE THE ONLY CAUSE OF AGE RATE 
CHANGES.

Jeez, how difficult is that to understand? And your different frame to 
exchange flight plans in is an oxymoron because it would make their actual 
symmetric flight plans appear to be NON symmetric. Only a pair of idiots 
would do that

You are just endlessly repeating what you read in some relativity textbook 
without using simple logic to determine its proper application

Edgar







On Monday, March 3, 2014 5:51:25 PM UTC-5, jessem wrote:



 On Mon, Mar 3, 2014 at 3:45 PM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 No, it was you that said there was NO correlation.


 Jeez Edgar, you really need to work on your reading comprehension. I just 
 got through AGREEING that I had said that there wasn't a correlation, but I 
 explained that this was because I was using correlation in the way YOU 
 had consistently been using it up until now, to refer to a 1:1 correlation 
 in which each proper age of a twin is matched up to one unique proper age 
 of the other twin. The archive at 
 http://www.mail-archive.com/everything-list@googlegroups.com/ has a 
 better search function than google's archive (returning individual posts 
 rather than threads), so I searched for posts from Edgar L. Owen with 
 correlate or correlation in them, results here:


 http://www.mail-archive.com/search?a=1l=everything-list%40googlegroups.comhaswords=correlatefrom=Edgar+L.+Owennotwords=subject=datewithin=1ddate=order=datenewestsearch=Search
  


 http://www.mail-archive.com/search?a=1l=everything-list%40googlegroups.comhaswords=correlationfrom=Edgar+L.+Owennotwords=subject=datewithin=1ddate=order=datenewestsearch=Search

 Earliest posts on the block time thread I could find in these searches 
 (that were directed at me, and not some other poster) were these from Feb. 
 12 and 13 (shown in order below), where you can see from the quotes that 
 you were talking specifically about 1:1 correlations that map clock times 
 of one to specific clock times of the other:


 http://www.mail-archive.com/everything-list%40googlegroups.com/msg48613.html

 So all observers are always in the same p-time moment. Now it's just a 
 matter of correlating their clock times to see which clock times occurred 
 in any particular current moment of p-time.


 http://www.mail-archive.com/everything-list%40googlegroups.com/msg48716.html

 Do you see how this mutual agreed on understanding of how each's clock 
 time varies in the other's frame always allows each to correlate their own 
 comoving clock time with the comoving (own) clock time of the other? In 
 other words for A to always know what B's clock time was reading when A's 
 clock time was reading t, and for B to always know what A's clock time was 
 reading when B's clock time was reading t'?


 

Re: Block Universes

2014-03-04 Thread Jesse Mazer
On Tue, Mar 4, 2014 at 12:19 PM, Jesse Mazer laserma...@gmail.com wrote:

 So you are just going to COMPLETELY IGNORE my response, which pointed out
 that your supposed error relied on using the ambiguous phrase B's and
 C's proper ages are simultaneous in p-time because they are at the same
 place in spacetime to describe my views, and interpreting it in a way that
 I would never had agreed with? Again, this phrase could be interpreted two
 possible ways:

 1. If B's proper age at this point in spacetime in T, then C's proper age
 at this point in spacetime must be T as well (i.e. their proper ages are
 simultaneous in the sense that they must reach the same age
 simultaneously).

 2. If B and C's worldlines both pass through a specific point in spacetime
 P, and B's age is T1 when she passes through P, while C's age is T2 when
 she passes through P, then B must be at age T1 simultaneously with C being
 at age T2 (i.e. whatever two specific ages they have at P, they must reach
 those two ages simultaneously, even if the two ages are different)



Minor typo in #1 there, it should read If B's proper age at this point in
spacetime is T, not in T.

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Re: Block Universes

2014-03-04 Thread Edgar L. Owen
Jesse,

You ask me to choose between 1. and 2.

1. If B's proper age at this point in spacetime is T, then C's proper age 
at this point in spacetime must be T as well (i.e. their proper ages are 
simultaneous in the sense that they must reach the same age 
simultaneously).

2. If B and C's worldlines both pass through a specific point in spacetime 
P, and B's age is T1 when she passes through P, while C's age is T2 when 
she passes through P, then B must be at age T1 simultaneously with C being 
at age T2 (i.e. whatever two specific ages they have at P, they must reach 
those two ages simultaneously, even if the two ages are different)


First I assume that by passing through the same point in spacetime you 
mean that the worldlines cross at P simultaneously by the operational 
definition of no light delay.

1. is true only in a SYMMETRIC case. In the symmetric case they would have 
the same ages as they pass through the same point P, but in that case they 
have the same ages during the WHOLE trip so no big surprise.

2. is true in all cases. The actual ages T1 and T2 at which they 
simultaneously cross will stand in a 1:1 correlation, but ONLY AT THAT 
POINT P because their ages could be different due to acceleration 
differences either before or after.

There are two equivalent ways they can confirm their actual 1:1 age 
correlations in both (all cases) when they cross paths.

First they can directly observe this 1:1 correlation by simply looking at 
each other's clocks as they pass. Normally this is not possible if two 
observers have relative motion with respect to each other, but in this case 
there is no time delay and the looking only takes a SINGLE MOMENT OF TIME, 
so even though the time RATES of each other's proper clocks are dilated in 
each other's frames, each can still actually read the correct proper time 
on the other's clock as they cross.

(One might initially think it is impossible to read each others' clocks 
correctly due to the dilation of relative motion, or even if they passed 
with different accelerations, but this is not true in the case where they 
read as they cross. Each proper clock is ALWAYS reading the actual proper 
age. The apparent dilation effect is just due to the longer interval it 
takes for signals from that clock to reach the observer. But the signals 
received always display the real and actual proper age of the clock WHEN 
the signals were sent. So in the crossing case where there is only a single 
signal with NO time delay the clock reading received = the actual clock 
reading when the signal was sent.

Note that this analysis points out that all proper clocks continually show 
the actual proper age of the clock when the signal was sent. So that real 
actual age is REALLY OUT THERE. Your imaginary 1:1 correlation problem just 
doesn't take into proper account the transmission time from the clock to 
the receiver. Just subtract the transmission time and you will get the 
actual 1:1 age correlation between when any proper age signal was sent and 
what proper time it was received.)

Second they CAN CONFIRM the actual age correlation in ALL cases simply by 
exchanging light messages as they cross telling each other their actual 
ages which is an equivalent method. As they cross the light signal has no 
appreciable delay so whatever actual age they report will correlate to the 
actual age the other receives the signal.

In this way crossing observers CAN UNambiguously determine the 1:1 
correlation of their actual ages even if they are in relative motion.

With this understanding your 1. is true of symmetric cases, and 2. is true 
of all cases...

Edgar






On Tuesday, March 4, 2014 12:19:27 PM UTC-5, jessem wrote:



 On Tue, Mar 4, 2014 at 8:37 AM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 I'm interested in finding the truth, not in assigning blame.

 The important thing is we both now agree that there IS ALWAYS A 
 CORRELATION OF ACTUAL AGES between any two observers.

 The difference is I think it's an EXACT correlation, and you think that 
 it's ALMOST EXACT except for cases of extreme separation or motion.

 I think we have to analyze the age correlation from a POV that preserves 
 the actual relationship of the accelerations that are the ONLY cause of age 
 rate differences. Whereas you think we have to consider all possible views 
 irrespective of whether they properly preserve the relationship of causes 
 of age rate differences. My method provides an EXACT correlation. Your 
 method provides an ALMOST EXACT correlation in all but extreme cases.


 Also now that I have pointed out the error in your Alice, Bob, Arlene, 
 Bart example do you agree my method does produce consistent, unambiguous 
 and transitive 1:1 correlations of proper ages among all observers?


 So you are just going to COMPLETELY IGNORE my response, which pointed out 
 that your supposed error relied on using the ambiguous phrase B's and 
 C's proper ages are 

Re: Block Universes

2014-03-04 Thread meekerdb

On 3/4/2014 11:19 AM, Jesse Mazer wrote:


On Tue, Mar 4, 2014 at 2:02 PM, Edgar L. Owen edgaro...@att.net 
mailto:edgaro...@att.net wrote:


Jesse,

You ask me to choose between 1. and 2.

1. If B's proper age at this point in spacetime is T, then C's proper age 
at this
point in spacetime must be T as well (i.e. their proper ages are 
simultaneous in
the sense that they must reach the same age simultaneously).

2. If B and C's worldlines both pass through a specific point in spacetime 
P, and
B's age is T1 when she passes through P, while C's age is T2 when she 
passes through
P, then B must be at age T1 simultaneously with C being at age T2 (i.e. 
whatever two
specific ages they have at P, they must reach those two ages 
simultaneously, even if
the two ages are different)


First I assume that by passing through the same point in spacetime you 
mean that
the worldlines cross at P simultaneously by the operational definition of 
no light
delay.

1. is true only in a SYMMETRIC case. In the symmetric case they would have 
the same
ages as they pass through the same point P, but in that case they have the 
same ages
during the WHOLE trip so no big surprise.



This isn't true.  In the inertial frame of a third party passing by, B and C age at 
different rates in different segments of their world lines even though those rates 
integrate to the same total aging between their two meetings.


Brent

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Re: Block Universes

2014-03-04 Thread Edgar L. Owen
Jesse,

BTW, in spite of your claim it can't be done, here is another simple way 
for any two observers at rest with respect to each other but separated by 
any arbitrary distance in space to determine their 1:1 age correlation.

If A and B are separated at any distance but at rest with respect to each 
other A sends B a light message telling B what A's current age is, and B 
immediately reflects that light message back to A with B's current age 
reading attached.

Because they are at rest A knows that the actual age difference is A's 
CURRENT age - B's REPORTED age + 1/2 delta c (half the light signal's round 
trip time). In this way A determines a unique 1:1 age correlation between 
his and B's age that will hold for as long as they are at rest. B can use 
the same method to determine his 1:1 age correlation with A. A and B do NOT 
have to synchronize the signals to do this.

This gives both A and B their single correct 1:1 age correlation at any 
distance which holds so long as they are at rest with respect to each 
other. 

Of course other observers may see this differently but IT'S NOT THEIR AGE 
CORRELATION, IT'S ONLY A'S AND B'S AGE CORRELATION and A and B can 
determine exactly what that correlation is. 

Do you agree?

I know you will claim it's not valid since other observers may view it 
differently, but frankly A and B's age correlation is NONE OF THEIR 
BUSINESS!


I'll respond to the rest of your post later when I have more time...

Edgar



On Tuesday, March 4, 2014 2:19:46 PM UTC-5, jessem wrote:


 On Tue, Mar 4, 2014 at 2:02 PM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 You ask me to choose between 1. and 2.

 1. If B's proper age at this point in spacetime is T, then C's proper age 
 at this point in spacetime must be T as well (i.e. their proper ages are 
 simultaneous in the sense that they must reach the same age 
 simultaneously).

 2. If B and C's worldlines both pass through a specific point in spacetime 
 P, and B's age is T1 when she passes through P, while C's age is T2 when 
 she passes through P, then B must be at age T1 simultaneously with C being 
 at age T2 (i.e. whatever two specific ages they have at P, they must reach 
 those two ages simultaneously, even if the two ages are different)


 First I assume that by passing through the same point in spacetime you 
 mean that the worldlines cross at P simultaneously by the operational 
 definition of no light delay.

 1. is true only in a SYMMETRIC case. In the symmetric case they would have 
 the same ages as they pass through the same point P, but in that case they 
 have the same ages during the WHOLE trip so no big surprise.

 2. is true in all cases. The actual ages T1 and T2 at which they 
 simultaneously cross will stand in a 1:1 correlation, but ONLY AT THAT 
 POINT P because their ages could be different due to acceleration 
 differences either before or after.



 Thanks for the clear answer. So now you hopefully see that you must 
 retract your claim that there's an error in my comments about the 
 scenario with the two pairs of twins A/B and C/D, since I never asserted 
 anything remotely resembling #1, my point about ages that occur at the same 
 point in spacetime being simultaneous in p-time referred SOLELY to #2.

 Now, can you please address the follow-up questions that I asked you to 
 address if you did agree with #2? I will requote them below:

 'On the other hand, if you would answer no, statement #2 is not in error, 
 I agree that in this case T1 and T2 are simultaneous in absolute terms, 
 then please have another look at the specific numbers I gave for x(t), 
 coordinate position as a function of coordinate time, and T(t), proper time 
 as a function of coordinate time, for each observer, and then tell me if 
 you agree or disagree with the following two statements:

 For A: x(t) = 25, T(t) = t
 For B: x(t) = 0, T(t) = t
 For C: x(t) = 0.8c * t, T(t) = 0.6*t
 For D: x(t) = [0.8c * t] + 9, T(t) = 0.6*t - 12

 --given the x(t) functions for B and C, we can see that they both pass 
 through the point in spacetime with coordinates x=0, t=0. Given their T(t) 
 functions, we can see that B has a proper time T=0 at those coordinates, 
 and C also has a proper time T=0 at those coordinates. Agree or disagree?

 --given the x(t) functions for A and D, we can see that they both pass 
 through the point in spacetime with coordinates x=25, t=20. Given their 
 T(t) functions, we can see that A has a proper time T=20 at those 
 coordinates, and D has a proper time T=0 at those coordinates. Agree or 
 disagree?'

 (if you don't understand the math of how to use x(t) to determine whether 
 someone passed through a given point in spacetime with known x and t 
 coordinates, or how to determine their proper time T at this point, then 
 just ask and I will elaborate)

  


 There are two equivalent ways they can confirm their actual 1:1 age 
 correlations in both (all cases) when they cross paths.

 

Re: Block Universes

2014-03-04 Thread Jesse Mazer
On Tue, Mar 4, 2014 at 4:04 PM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 BTW, in spite of your claim it can't be done, here is another simple way
 for any two observers at rest with respect to each other but separated by
 any arbitrary distance in space to determine their 1:1 age correlation.

 If A and B are separated at any distance but at rest with respect to each
 other A sends B a light message telling B what A's current age is, and B
 immediately reflects that light message back to A with B's current age
 reading attached.

 Because they are at rest A knows that the actual age difference is A's
 CURRENT age - B's REPORTED age + 1/2 delta c (half the light signal's round
 trip time). In this way A determines a unique 1:1 age correlation between
 his and B's age that will hold for as long as they are at rest. B can use
 the same method to determine his 1:1 age correlation with A. A and B do NOT
 have to synchronize the signals to do this.


This is a valid method for determining what ages are simultaneous in the
inertial frame where they are both at rest. But there is no basis in
relativity for judging this frame's views on simultaneity to be any more
valid than another frame's.



 This gives both A and B their single correct 1:1 age correlation at any
 distance which holds so long as they are at rest with respect to each
 other.


Again, you present no argument for why this is the single correct
correlation, you just assert it.




 Of course other observers may see this differently but IT'S NOT THEIR AGE
 CORRELATION, IT'S ONLY A'S AND B'S AGE CORRELATION and A and B can
 determine exactly what that correlation is.

 Do you agree?



No. You already agreed in an earlier post that for an inertial observer to
label the frame where they are at rest as their own frame is purely a
matter of HUMAN CONVENTION, not an objective reality that is forced on them
by nature. So even if we ignore these other observers, there is nothing
stopping A and B from using a different convention to define their own
frame, such as the inertial frame where they both have a velocity of 0.99c
along the x-axis.




 I know you will claim it's not valid since other observers may view it
 differently, but frankly A and B's age correlation is NONE OF THEIR
 BUSINESS!


Again, you are conflating observers with frames, even though you earlier
acknowledged that any link between particular observers and particular
frames is just a matter of convention.





 I'll respond to the rest of your post later when I have more time...


OK, thanks. Please prioritize my latest post discussing the scenario with
A/B and C/D and statement #1 vs. statement #2, since it seems that your
original argument for an error in my analysis was based on falsely
imagining I was asserting statement #1 rather than statement #2. Since the
analysis really only depends on #2 which you seem to agree with, I would
like to proceed with the analysis of this scenario to see if you can find
any other reason to object  to any other step in the reasoning--if you
can't, then presumably you will have no basis for denying the final
conclusion that two different ages of the same observer A would have to be
simultaneous in p-time, according to your own rules.

Jesse



 On Tuesday, March 4, 2014 2:19:46 PM UTC-5, jessem wrote:


 On Tue, Mar 4, 2014 at 2:02 PM, Edgar L. Owen edga...@att.net wrote:

 Jesse,

 You ask me to choose between 1. and 2.

 1. If B's proper age at this point in spacetime is T, then C's proper age
 at this point in spacetime must be T as well (i.e. their proper ages are
 simultaneous in the sense that they must reach the same age
 simultaneously).

 2. If B and C's worldlines both pass through a specific point in
 spacetime P, and B's age is T1 when she passes through P, while C's age is
 T2 when she passes through P, then B must be at age T1 simultaneously with
 C being at age T2 (i.e. whatever two specific ages they have at P, they
 must reach those two ages simultaneously, even if the two ages are
 different)


 First I assume that by passing through the same point in spacetime you
 mean that the worldlines cross at P simultaneously by the operational
 definition of no light delay.

 1. is true only in a SYMMETRIC case. In the symmetric case they would
 have the same ages as they pass through the same point P, but in that case
 they have the same ages during the WHOLE trip so no big surprise.

 2. is true in all cases. The actual ages T1 and T2 at which they
 simultaneously cross will stand in a 1:1 correlation, but ONLY AT THAT
 POINT P because their ages could be different due to acceleration
 differences either before or after.



 Thanks for the clear answer. So now you hopefully see that you must
 retract your claim that there's an error in my comments about the
 scenario with the two pairs of twins A/B and C/D, since I never asserted
 anything remotely resembling #1, my point about ages that occur at the same
 point in spacetime being 

Re: Block Universes

2014-03-04 Thread Edgar L. Owen
Brent,

First thanks for your comment. 

I think Jesse and I are both aware of that, but we are considering the age 
relationship JUST BETWEEN A and B and so must consider only how they see it 
in their OWN frames, not the view of a 3rd observer of that relationship. 
Though Jesse would probably disagree.

The current discussion is about choice of frames though. Check my latest 
post for a synopsis of one case..

Edgar



On Tuesday, March 4, 2014 2:56:49 PM UTC-5, Brent wrote:

  On 3/4/2014 11:19 AM, Jesse Mazer wrote:
  
  
 On Tue, Mar 4, 2014 at 2:02 PM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse, 

  You ask me to choose between 1. and 2.

  1. If B's proper age at this point in spacetime is T, then C's proper 
 age at this point in spacetime must be T as well (i.e. their proper ages 
 are simultaneous in the sense that they must reach the same age 
 simultaneously).

  2. If B and C's worldlines both pass through a specific point in 
 spacetime P, and B's age is T1 when she passes through P, while C's age is 
 T2 when she passes through P, then B must be at age T1 simultaneously with 
 C being at age T2 (i.e. whatever two specific ages they have at P, they 
 must reach those two ages simultaneously, even if the two ages are 
 different)

  
  First I assume that by passing through the same point in spacetime 
 you mean that the worldlines cross at P simultaneously by the operational 
 definition of no light delay.

  1. is true only in a SYMMETRIC case. In the symmetric case they would 
 have the same ages as they pass through the same point P, but in that case 
 they have the same ages during the WHOLE trip so no big surprise.
  
   
 This isn't true.  In the inertial frame of a third party passing by, B and 
 C age at different rates in different segments of their world lines even 
 though those rates integrate to the same total aging between their two 
 meetings.

 Brent

  

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Re: Block Universes

2014-03-04 Thread Edgar L. Owen
Jesse,

Good, we agree it's a valid method for determining 1:1 age correlations in 
a common inertial frame in which they are both at rest. I claim that frame 
is the correct one to determine the actual age correlation because it 
expresses the actual relation in a manner both A and B agree, is transitive 
among all observers, AND is the exact same method that gives the correct 
answer WHEN A AND B MEET and everyone, even you, agrees on the 1:1 age 
correlation.

Our disagreement over choice of frames is spinning its wheels and not 
getting anywhere. It's a matter of how to INTERPRET relativity, rather than 
relativity itself. And I have given very convincing reasons why a 
privileged frame that preserves the actual physical facts that affect age 
changes is appropriate. You just don't agree with them.

As to your example claiming to prove my method leads to a contradiction, 
just give me the bottom line, a simple synopsis. I don't have the time to 
wade through a detailed example only to find the only disagreement is over 
choice of frames again.

On the other hand if you ASSUME privileged frames the way I do and think my 
method of using them leads to a contradiction that isn't just another 
disagreement over choice of frames that were assumed, then give me a simple 
example, the simplest you can come up with.

Edgar


On Tuesday, March 4, 2014 4:37:32 PM UTC-5, jessem wrote:



 On Tue, Mar 4, 2014 at 4:04 PM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 BTW, in spite of your claim it can't be done, here is another simple way 
 for any two observers at rest with respect to each other but separated by 
 any arbitrary distance in space to determine their 1:1 age correlation.

 If A and B are separated at any distance but at rest with respect to each 
 other A sends B a light message telling B what A's current age is, and B 
 immediately reflects that light message back to A with B's current age 
 reading attached.

 Because they are at rest A knows that the actual age difference is A's 
 CURRENT age - B's REPORTED age + 1/2 delta c (half the light signal's round 
 trip time). In this way A determines a unique 1:1 age correlation between 
 his and B's age that will hold for as long as they are at rest. B can use 
 the same method to determine his 1:1 age correlation with A. A and B do NOT 
 have to synchronize the signals to do this.


 This is a valid method for determining what ages are simultaneous in the 
 inertial frame where they are both at rest. But there is no basis in 
 relativity for judging this frame's views on simultaneity to be any more 
 valid than another frame's.
  


 This gives both A and B their single correct 1:1 age correlation at any 
 distance which holds so long as they are at rest with respect to each 
 other. 


 Again, you present no argument for why this is the single correct 
 correlation, you just assert it.

  


 Of course other observers may see this differently but IT'S NOT THEIR AGE 
 CORRELATION, IT'S ONLY A'S AND B'S AGE CORRELATION and A and B can 
 determine exactly what that correlation is. 

 Do you agree?



 No. You already agreed in an earlier post that for an inertial observer to 
 label the frame where they are at rest as their own frame is purely a 
 matter of HUMAN CONVENTION, not an objective reality that is forced on them 
 by nature. So even if we ignore these other observers, there is nothing 
 stopping A and B from using a different convention to define their own 
 frame, such as the inertial frame where they both have a velocity of 0.99c 
 along the x-axis.

  


 I know you will claim it's not valid since other observers may view it 
 differently, but frankly A and B's age correlation is NONE OF THEIR 
 BUSINESS!


 Again, you are conflating observers with frames, even though you earlier 
 acknowledged that any link between particular observers and particular 
 frames is just a matter of convention.

  



 I'll respond to the rest of your post later when I have more time...


 OK, thanks. Please prioritize my latest post discussing the scenario with 
 A/B and C/D and statement #1 vs. statement #2, since it seems that your 
 original argument for an error in my analysis was based on falsely 
 imagining I was asserting statement #1 rather than statement #2. Since the 
 analysis really only depends on #2 which you seem to agree with, I would 
 like to proceed with the analysis of this scenario to see if you can find 
 any other reason to object  to any other step in the reasoning--if you 
 can't, then presumably you will have no basis for denying the final 
 conclusion that two different ages of the same observer A would have to be 
 simultaneous in p-time, according to your own rules.

 Jesse



 On Tuesday, March 4, 2014 2:19:46 PM UTC-5, jessem wrote:


 On Tue, Mar 4, 2014 at 2:02 PM, Edgar L. Owen edga...@att.net wrote:

 Jesse,

 You ask me to choose between 1. and 2.

 1. If B's proper age at this point in spacetime is T, then 

Re: Block Universes

2014-03-04 Thread Jesse Mazer
On Tue, Mar 4, 2014 at 4:57 PM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 Good, we agree it's a valid method for determining 1:1 age correlations in
 a common inertial frame in which they are both at rest. I claim that frame
 is the correct one to determine the actual age correlation because it
 expresses the actual relation in a manner both A and B agree


You are avoiding my question of whether identifying this frame with A and
B's view or perspective is just a matter of convention as you
previously seemed to agree, or whether it is tied to them in some more
fundamental way. If it's just a matter of convention, then A and B could
equally well agree to define any other frame as their own view of the
situation.




 is transitive among all observers, AND is the exact same method that gives
 the correct answer WHEN A AND B MEET and everyone, even you, agrees on the
 1:1 age correlation.

 Our disagreement over choice of frames is spinning its wheels and not
 getting anywhere. It's a matter of how to INTERPRET relativity, rather than
 relativity itself. And I have given very convincing reasons why a
 privileged frame that preserves the actual physical facts that affect age
 changes is appropriate. You just don't agree with them.


But you refuse to answer my very simple questions about your reasons,
like my question about whether you ASSUME FROM THE START that a particular
definition of simultaneity (the one you prefer) is the actual reality, or
whether you claim to have convincing reasons for this definition of
simultaneity representing reality that don't simply assume it from the
start.




 As to your example claiming to prove my method leads to a contradiction,
 just give me the bottom line, a simple synopsis. I don't have the time to
 wade through a detailed example only to find the only disagreement is over
 choice of frames again.


I promise you the example has nothing to do with any frames other than the
ones in which each pair is at rest. Again, the only assumptions about
p-time that I make in deriving the contradiction are:

ASSUMPTION 1. If two observers are at rest in the same inertial frame, then
events on their worldlines that are simultaneous in their rest frame are
also simultaneous in p-time

ASSUMPTION 2. If two observers cross paths at a single point in spacetime
P, and observer #1's proper time at P is T1 while observer #2's proper time
at P is T2, then the event of observer #1's clock showing T1 is
simultaneous in p-time with the event of observer #2's clock showing T2.

ASSUMPTION 3. p-time simultaneity is transitive

That's it! I make no other assumptions about p-time simultaneity. But if
you want to actually see how the contradiction is derived, there's really
no shortcut besides looking at the math. If you are willing to do that, can
we just start with the last 2 questions I asked about the scenario? Here's
what I asked again, with a few cosmetic modifications:

Please have another look at the specific numbers I gave for x(t),
coordinate position as a function of coordinate time, and T(t), proper time
as a function of coordinate time, for each observer (expressed using the
inertial frame where A and B are at rest, and C and D are moving at 0.8c),
and then tell me if you agree or disagree with the following two statements:

For A: x(t) = 25, T(t) = t
For B: x(t) = 0, T(t) = t
For C: x(t) = 0.8c * t, T(t) = 0.6*t
For D: x(t) = [0.8c * t] + 9, T(t) = 0.6*t - 12

--given the x(t) functions for B and C, we can see that they both pass
through the point in spacetime with coordinates x=0, t=0. Given their T(t)
functions, we can see that B has a proper time T=0 at those coordinates,
and C also has a proper time T=0 at those coordinates. Therefore, by
ASSUMPTION 1 above, the event of B's proper time clock reading T=0 is
simultaneous in p-time with the event of C's proper time clock reading T=0.
Agree or disagree?

--given the x(t) functions for A and D, we can see that they both pass
through the point in spacetime with coordinates x=25, t=20. Given their
T(t) functions, we can see that A has a proper time T=20 at those
coordinates, and D has a proper time T=0 at those coordinates. Therefore,
by ASSUMPTION 1 above, the event of A's proper time clock reading T=20 is
simultaneous in p-time with the event of D's proper time clock reading T=0.
Agree or disagree?

(if you don't understand the math of how to use x(t) to determine whether
someone passed through a given point in spacetime with known x and t
coordinates, or how to determine their proper time T at this point, then
just ask and I will elaborate)

If you agree with both of these, then I will proceed to the next few
agree/disagree statements that follow from the three assumptions, and if
you agree with them all you'll have no way to avoid the contradiction.





 On the other hand if you ASSUME privileged frames the way I do and think
 my method of using them leads to a contradiction that isn't just another
 disagreement over 

Re: Block Universes

2014-03-04 Thread Jesse Mazer
On Tue, Mar 4, 2014 at 5:45 PM, Jesse Mazer laserma...@gmail.com wrote:



 I promise you the example has nothing to do with any frames other than the
 ones in which each pair is at rest. Again, the only assumptions about
 p-time that I make in deriving the contradiction are:

 ASSUMPTION 1. If two observers are at rest in the same inertial frame,
 then events on their worldlines that are simultaneous in their rest frame
 are also simultaneous in p-time

 ASSUMPTION 2. If two observers cross paths at a single point in spacetime
 P, and observer #1's proper time at P is T1 while observer #2's proper time
 at P is T2, then the event of observer #1's clock showing T1 is
 simultaneous in p-time with the event of observer #2's clock showing T2.

 ASSUMPTION 3. p-time simultaneity is transitive

 That's it! I make no other assumptions about p-time simultaneity. But if
 you want to actually see how the contradiction is derived, there's really
 no shortcut besides looking at the math. If you are willing to do that, can
 we just start with the last 2 questions I asked about the scenario? Here's
 what I asked again, with a few cosmetic modifications:

 Please have another look at the specific numbers I gave for x(t),
 coordinate position as a function of coordinate time, and T(t), proper time
 as a function of coordinate time, for each observer (expressed using the
 inertial frame where A and B are at rest, and C and D are moving at 0.8c),
 and then tell me if you agree or disagree with the following two statements:

 For A: x(t) = 25, T(t) = t
 For B: x(t) = 0, T(t) = t
 For C: x(t) = 0.8c * t, T(t) = 0.6*t
 For D: x(t) = [0.8c * t] + 9, T(t) = 0.6*t - 12

 --given the x(t) functions for B and C, we can see that they both pass
 through the point in spacetime with coordinates x=0, t=0. Given their T(t)
 functions, we can see that B has a proper time T=0 at those coordinates,
 and C also has a proper time T=0 at those coordinates. Therefore, by
 ASSUMPTION 1 above, the event of B's proper time clock reading T=0 is
 simultaneous in p-time with the event of C's proper time clock reading T=0.
 Agree or disagree?

 --given the x(t) functions for A and D, we can see that they both pass
 through the point in spacetime with coordinates x=25, t=20. Given their
 T(t) functions, we can see that A has a proper time T=20 at those
 coordinates, and D has a proper time T=0 at those coordinates. Therefore,
 by ASSUMPTION 1 above, the event of A's proper time clock reading T=20 is
 simultaneous in p-time with the event of D's proper time clock reading T=0.
 Agree or disagree?


Another little correction--in the last two paragraphs there, where I said
Therefore, by ASSUMPTION 1 above, I should have written ASSUMPTION 2,
since in both cases I was deriving p-time simultaneity from the fact that
two clock readings happened at the same point in spacetime.

Jesse

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Re: Block Universes

2014-03-03 Thread Edgar L. Owen
Jesse,

Your position becomes more and more absurd.

You claim they DO have a unique 1:1 correlation of their ages when they are 
together but they DON'T when they separate.

So how far do they have to separate before this correlation is lost? 1 
meter? 1 kilometer, 1 light year?

And is the correlation lost all at once as they separate or gradually? And 
if all at once, what is the threshold distance where correlation is lost?

And if gradually what is the relativistic formula that determines how much 
the correlation falls off with distance?


The fact is that both twins DO HAVE AN ACTUAL AGE AT ALL TIMES. You've 
already agreed to this obvious fact. Thus there absolutely MUST be an 
actual correlation of those ages. That is pure logic, not relativity. All 
you are saying is that relativity does not give a unique answer for what 
that correlation is. Sure, I agree completely.

But my point is that if we choose the correct frame that preserves the 
relationship between ONLY the twins themselves we do get a unique 
unambiguous answer. And so that is the only correct answer. And it is 
consistent and transitive among all observers. Therefore it qualifies as an 
actual physical fact.

All you are saying is that relativity doesn't have a way to calculate an 
age correlation. But not having a way to calculate something DOES NOT MEAN 
it doesn't actually exist, it just means it can't be calculated. Do you 
agree with that?

So to falsify p-time you can't just say a correlation can't be calculated, 
you have to actually prove there is an actual CONTRADICTION between p-time 
and relativity. You haven't yet done that and I don't think you can...


Note also that the GPS system DOES establish actual 1:1 correlations of 
proper times between satellites and ground based receivers both moving 
relative to each other and at distance from each other. if it didn't, it 
couldn't work. So even relativity tells us this is possible.

Edgar



On Sunday, March 2, 2014 7:52:12 PM UTC-5, jessem wrote:



 On Sun, Mar 2, 2014 at 7:44 PM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 OK good, that's what I assumed you meant.

 BUT now take the two twins at rest standing on opposite sides of the 
 earth, and then they each start walking in different directions. By your 
 criterion you then have to say that suddenly and instantly there is NO more 
 1:1 correlation of their ages, that they COMPLETELY AND ABSOLUTELY lose 
 their 1:1 age correlation they had at rest even if they take a SINGLE STEP!


 You seem to have misunderstood me, although I thought I was pretty 
 clear--I said that they did NOT have a unique actual correlation in their 
 ages when they were at rest relative to each other but at different 
 positions in space, so nothing changes if they start walking, they still 
 don't have any unique actual correlation in their ages. Try reading what 
 I wrote again (with the correction I mentioned that 'any unique actual 
 truth about their ages' has been changed to 'any unique actual truth 
 about the correlation between their ages'):

 'No, of course I wouldn't agree that there is any unique actual truth 
 about the correlation between their ages in this case, nor would any 
 mainstream physicist. What part of all frames are equally valid don't you 
 understand? Or do you not get that if we use an inertial frame where the 
 twins are both moving with the same constant velocity, they do NOT have 
 identical ages at any given moment in this frame? (assuming they had 
 identical ages at any given moment in their rest frame)'

 Jesse

  

 On Sunday, March 2, 2014 7:13:31 PM UTC-5, jessem wrote:


 On Sun, Mar 2, 2014 at 7:01 PM, Jesse Mazer laser...@gmail.com wrote:

 

 ...

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Re: Block Universes

2014-03-03 Thread Jesse Mazer
On Mon, Mar 3, 2014 at 10:03 AM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 Your position becomes more and more absurd.


My position is simply that for any question on which different frames
give different answers, there is no physical basis for judging one frame's
judgments to be reality while others are not. I guarantee you that any
physicist would agree with this.



 You claim they DO have a unique 1:1 correlation of their ages when they
 are together but they DON'T when they separate.

 So how far do they have to separate before this correlation is lost? 1
 meter? 1 kilometer, 1 light year?


Any finite number--one trillionth of a nanometer, say. The theory says that
no matter how small the distance D you choose, if you have an inertial
frame where two clocks are at rest and synchronized a distance D apart,
then in another inertial frame where the two clocks are moving along the
axis between them at speed v, at any given moment in this new frame one
clock's time will be ahead of the other's by vD/c^2. There is a maximum to
how far their times can be out-of-sync since v must be smaller than c, this
implies that no inertial frame will see them as being out-of-sync by a time
greater than or equal to D/c (so if the two clocks are 1 light-second apart
in their rest frame, or 299792458 meters apart, any other frame will see
them out-of-sync by less than a second). And this means that if you are
rounding ages off at some point, in practice you may not have to worry
about disagreements in simultaneity between frames--if two people are
precisely the same age in their rest frame and are standing only a meter
apart in their inertial rest frame, all other frames will say their ages
differ by less than 1/299792458 of a second, so obviously if you're
rounding their ages to the nearest second you'll still say they're the
same age no matter what inertial frame you're using. But if you want to
talk about physical reality rather than mere practical approximations,
the fact remains that different frames will disagree somewhat on which ages
are simultaneous for ANY finite separation, and in relativity there can
NEVER be a physical basis for saying that one frame's judgments are a true
representation of physical reality while other's are not.





 And is the correlation lost all at once as they separate or gradually? And
 if all at once, what is the threshold distance where correlation is lost?

 And if gradually what is the relativistic formula that determines how much
 the correlation falls off with distance?


See above, if the clocks are at rest a distance D apart and synchronized in
their own rest frame, then in another frame moving at speed v along the
axis between the two clocks, at any given moment in this new frame the
clocks are out-of-sync by vD/c^2. This can be derived directly from the
Lorentz transformation which tells you the coordinates of any event in
frame #2 if you already have its coordinates in frame #1.






 The fact is that both twins DO HAVE AN ACTUAL AGE AT ALL TIMES. You've
 already agreed to this obvious fact. Thus there absolutely MUST be an
 actual correlation of those ages. That is pure logic, not relativity.



That isn't logical at all, in fact it's a complete non sequitur (note
that you make no attempt to actually explain the 'logic' that leads you
from the premise to the conclusion here).

Once again I would mention the geometric analogy:

--If you have two spatial paths between points A and B on a 2D plane, then
at any given point P on a specific path, there is an actual distance along
the path between point A and point P, which could be measured by a flexible
measuring tape laid along the path. This distance along the path from A to
P--call it the proper path distance from A to P--is totally
coordinate-independent, in the sense that if different Cartesian coordinate
systems have different coordinate descriptions of the same path, they can
each use their own coordinates to calculate this proper path distance
from A to P and they will all get the same answer. But if you use different
Cartesian coordinate systems to assign x,y coordinates to points on the
plane, two points P1 and P2 on *different* paths may have the same
y-coordinate in one coordinate system, but different y-coordinates in
another coordinate system. So the question do two points on different
paths share a common y-coordinate?, unlike the question what is the
proper path distance between two points on a single path?, is one that
different Cartesian coordinate systems answer differently. But I don't
think anyone would ever claim that one Cartesian coordinate system's answer
to the latter question would be physically correct while other coordinate
systems are objectively physically wrong--the notion of separated points
in space having the same y-coordinate is an INTRINSICALLY
coordinate-based idea, it HAS no physical reality independent of an
arbitrary choice of coordinate system.

All of this is exactly analogous 

Re: Block Universes

2014-03-03 Thread Edgar L. Owen
Jesse,

OK, this is some progress.

Now you've gone from saying there is NO correlation at all, to the ages ARE 
CORRELATED WITHIN SOME LIMIT. In other words we DO know that for any set of 
twins we can always say that their ages ARE the same within some limits. 
Correct?

This is a VERY BIG CHANGE in your stated position, from NO correlation at 
all to SOME correlation...

You though continue to claim that all frames are equally valid, even if 
they DO NOT preserve the actual age changing acceleration effects between 
the twins, while I claim that IF we properly choose a frame that DOES 
preserve the actual age changing acceleration effects that we narrow that 
limit to zero resulting in an EXACT 1:1 age correlation.

You, in fact, have previously agreed that IF we choose the frame in which 
the symmetric accelerations were preserved that we DO get an exact 1:1 
correlation, you just disagree that that frame is privileged because it 
preserves the actual age changing symmetric accelerations like I claim.

So I suggest that for the moment we ASSUME we should choose that frame, and 
then see if it can be consistently applied in a transitive manner to 
achieve a common age correlation between ALL observers.

If it can't my theory is falsified. If it can then we can still agree to 
disagree about how frames should be applied to analyze specific physical 
relationships.


Edgar


On Monday, March 3, 2014 11:39:10 AM UTC-5, jessem wrote:



 On Mon, Mar 3, 2014 at 10:03 AM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 Your position becomes more and more absurd.


 My position is simply that for any question on which different frames 
 give different answers, there is no physical basis for judging one frame's 
 judgments to be reality while others are not. I guarantee you that any 
 physicist would agree with this.
  


 You claim they DO have a unique 1:1 correlation of their ages when they 
 are together but they DON'T when they separate.

 So how far do they have to separate before this correlation is lost? 1 
 meter? 1 kilometer, 1 light year?


 Any finite number--one trillionth of a nanometer, say. The theory says 
 that no matter how small the distance D you choose, if you have an inertial 
 frame where two clocks are at rest and synchronized a distance D apart, 
 then in another inertial frame where the two clocks are moving along the 
 axis between them at speed v, at any given moment in this new frame one 
 clock's time will be ahead of the other's by vD/c^2. There is a maximum to 
 how far their times can be out-of-sync since v must be smaller than c, this 
 implies that no inertial frame will see them as being out-of-sync by a time 
 greater than or equal to D/c (so if the two clocks are 1 light-second apart 
 in their rest frame, or 299792458 meters apart, any other frame will see 
 them out-of-sync by less than a second). And this means that if you are 
 rounding ages off at some point, in practice you may not have to worry 
 about disagreements in simultaneity between frames--if two people are 
 precisely the same age in their rest frame and are standing only a meter 
 apart in their inertial rest frame, all other frames will say their ages 
 differ by less than 1/299792458 of a second, so obviously if you're 
 rounding their ages to the nearest second you'll still say they're the 
 same age no matter what inertial frame you're using. But if you want to 
 talk about physical reality rather than mere practical approximations, 
 the fact remains that different frames will disagree somewhat on which ages 
 are simultaneous for ANY finite separation, and in relativity there can 
 NEVER be a physical basis for saying that one frame's judgments are a true 
 representation of physical reality while other's are not.


  


 And is the correlation lost all at once as they separate or gradually? And 
 if all at once, what is the threshold distance where correlation is lost?

 And if gradually what is the relativistic formula that determines how much 
 the correlation falls off with distance?


 See above, if the clocks are at rest a distance D apart and synchronized 
 in their own rest frame, then in another frame moving at speed v along the 
 axis between the two clocks, at any given moment in this new frame the 
 clocks are out-of-sync by vD/c^2. This can be derived directly from the 
 Lorentz transformation which tells you the coordinates of any event in 
 frame #2 if you already have its coordinates in frame #1.


  



 The fact is that both twins DO HAVE AN ACTUAL AGE AT ALL TIMES. You've 
 already agreed to this obvious fact. Thus there absolutely MUST be an 
 actual correlation of those ages. That is pure logic, not relativity.



 That isn't logical at all, in fact it's a complete non sequitur (note 
 that you make no attempt to actually explain the 'logic' that leads you 
 from the premise to the conclusion here). 

 Once again I would mention the geometric analogy:

 --If you 

Re: Block Universes

2014-03-03 Thread LizR
By the way, a friend suggested how Edgar's p-time could be rescued from
relativity. If the universe is a simulation running on a game of life,
which is itself running in a Newtonian universe with separate space and
time dimensions (and assuming the simulation can handle relativity - we
weren't sure how easily it would manage QM) then it becomes at least
possible to envisage how it might exist.

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Re: Block Universes

2014-03-03 Thread Jesse Mazer
On Mon, Mar 3, 2014 at 12:36 PM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 OK, this is some progress.

 Now you've gone from saying there is NO correlation at all, to the ages
 ARE CORRELATED WITHIN SOME LIMIT. In other words we DO know that for any
 set of twins we can always say that their ages ARE the same within some
 limits. Correct?

 This is a VERY BIG CHANGE in your stated position, from NO correlation at
 all to SOME correlation...


Once again your argument turns on vague use of language. You were
consistently talking about a 1:1 correlation, so naturally I was using
correlation in this sense too. If we say all inertial frames agree that
my age T' is simultaneous with my twin's age having some value between T1
and T2, but they disagree on the precise value that is NOT a 1:1
correlation, period. So there's been no change in my position, it's you
whose changing the meaning of correlation in mid-argument in an attempt
to prove me wrong.




 You though continue to claim that all frames are equally valid, even if
 they DO NOT preserve the actual age changing acceleration effects between
 the twins,


What do you mean by actual age changing acceleration effect? If you're
talking about things that are directly measurable without use of a
particular frame--like each twin's proper age at any specific event on his
worldline (including their identical proper ages at the point in spacetime
where they reunite), or each twin's proper acceleration as a function of
proper age, then all frames DO preserve these effects. If instead you mean
the idea that identical ages of separated symmetrically-accelerating twins
are simultaneous in absolute, non-frame-dependent terms, then YOUR ARGUMENT
IS TOTALLY CIRCULAR--you are simply assuming from the start that
symmetrical acceleration implies that identical ages are simultaneous in
actual, absolute terms, WITHOUT DERIVING THIS IDEA FROM ANY MORE BASIC
PREMISES.




 while I claim that IF we properly choose a frame that DOES preserve the
 actual age changing acceleration effects that we narrow that limit to zero
 resulting in an EXACT 1:1 age correlation.


Yep, that sounds pretty circular all right. As near as I can tell, the
structure of your argument is this:

1. Assume without any prior argument that for symmetrically-accelerating
twins, the actual truth about simultaneity is that identical ages are
simultaneous.

2. Observe that there is only one frame that preserves this actual
truth.

3. Therefore, only this frame is valid, other frames are not.

4. If we use this valid frame we can find a unique 1:1 correlation in
their ages--and that is supposed to demonstrate the validity of premise #1
above!

Hopefully you can see that this argument would be completely circular. If
you think this isn't a fair representation of your own argument, then
perhaps you can lay your argument out in a step-by-step manner as above,
with each successive step being obviously derivable from only the previous
steps.





 You, in fact, have previously agreed that IF we choose the frame in which
 the symmetric accelerations were preserved


All frames agree the proper accelerations as a function of each twin's
proper time are symmetric. By the frame in which symmetric accelerations
were preserved do you mean that each twin's acceleration as a function of
COORDINATE time in that frame is symmetric?



 that we DO get an exact 1:1 correlation, you just disagree that that frame
 is privileged because it preserves the actual age changing symmetric
 accelerations like I claim.


Do you have any argument to DERIVE the conclusion that one frame's
acceleration and aging as a function of COORDINATE time is actual, or is
this just something you assume from the start and have no way to derive
from any more basic premises?





 So I suggest that for the moment we ASSUME we should choose that frame,
 and then see if it can be consistently applied in a transitive manner to
 achieve a common age correlation between ALL observers.

 If it can't my theory is falsified. If it can then we can still agree to
 disagree about how frames should be applied to analyze specific physical
 relationships.



Would you consider it a falsification of your theory to show that your
assumption about simultaneity for symmetrically-moving observers (combined
with transitivity and the idea that events at the same space and time
coordinates in some inertial frame are automatically simultaneous in
p-time) can lead in certain scenarios to a situation where we are forced to
conclude that two different proper times of the SAME observer (Bob's proper
time clock reading 0 and Bob's proper time clock reading 20, say) are
simultaneous in p-time? If so, this sort of falsification is exactly what I
have derived in my Alice/Bob/Arlene/Bart scenario from Feb. 9 at
https://groups.google.com/d/msg/everything-list/jFX-wTm_E_Q/pxg0VAAHJRQJwhich
you have CONSISTENTLY FAILED TO ADDRESS on all the myriad occasions I
have reminded you of 

Re: Block Universes

2014-03-03 Thread Edgar L. Owen
Liz,

Thanks but P-time doesn't need to be rescued from relativity since it's 
completely consistent with relativity, though apparently not with some 
people's interpretation of relativity.

Edgar

On Monday, March 3, 2014 1:42:48 PM UTC-5, Liz R wrote:

 By the way, a friend suggested how Edgar's p-time could be rescued from 
 relativity. If the universe is a simulation running on a game of life, 
 which is itself running in a Newtonian universe with separate space and 
 time dimensions (and assuming the simulation can 
 ...

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Re: Block Universes

2014-03-03 Thread Edgar L. Owen
Jesse,

No, it was you that said there was NO correlation. In any case that's 
irrelevant if we know you now accept that there is a very LARGE correlation 
in most situations, and a definable correlation in ALL situations. That 
there is always SOME correlation.

By actual age changing effect I mean proper accelerations and gravitations 
measurable by a comoving scale at specific clock tick events on his proper 
clock. There is no doubt these are real actual CAUSES with specific 
measurable values that thus must have real actual EFFECTS with specific 
actual values. So you are now saying that all frames DO preserve these 
effects?

Your 4 point representation of my method MAY BE circular, but my actual 
method is NOT circular.

Your statement 1. is an incorrect statement of my theory. What I assume 
FIRST in the symmetric case is NOT simultaneity of ages but simultaneity of 
the AGE CHANGING EFFECTS that relativity itself identifies, namely 
acceleration and gravitation. And in the general case the ages are NOT 
simultaneous nor are the age changing effects, yet my method still works. 
Would you claim that in the NON-symmetric case I start by assuming that 
NON-identical ages are NOT simultaneous. No, of course not, so your 
statement 1. does NOT represent an assumption my theory makes. 

I've defined this before but here it is again. The frame in which the 
accelerations are symmetric is a frame in which the same proper 
accelerations of BOTH twins occur at the same proper ages of both twins AND 
in which the proper ages of both twins have the same t value in that 
symmetry preserving frame. They have the same t value because the twins 
exchanged flight plans and agreed they would, and we know that their proper 
clocks MUST run at the same rates under the same accelerations at the same 
proper times. Therefore we must choose a frame that reflects that agreed 
upon symmetry.


To address your two pair moving relative to each other example if A's 
proper time comes out both 0 and 20 at the same point in spacetime that 
sounds like a falsification.

Let me paraphrase it for clarity in terms of a pair of observers A and B, 
and another pair C and D.

If I understand it correctly A and B have the same proper ages, are at rest 
with respect to each other but separated in space.

And C and D have the same proper ages, are at rest with respect to each 
other but also separated in space.

However B and C are initially at the SAME position in space as the pairs 
move past each other.

A's and B's proper ages are simultaneous in p-time because they are 
simultaneous in the A/B rest frame.

C's and D's proper ages are simultaneous in p-time because they are 
simultaneous in the C/D rest frame.

B's and C's proper ages are simultaneous in p-time because they are at the 
same place in spacetime.

NO. for that to be true we have to assume that B's and C's proper ages were 
INITIALLY THE SAME AND THERE WAS NO SUBSEQUENT PROPER ACCELERATION OR 
GRAVITATIONAL DIFFERENCES.

The simple fact that B and C are at the same point in spacetime DOES NOT 
require their proper ages to be the same. Obviously not since the twins in 
general are at DIFFERENT proper ages when they meet at the same point in 
spacetime. How could you believe differently?

So this is the ERROR in your example. Therefore it does NOT generate a 
result in which A's proper age is both 0 and 20 at the same point in 
spacetime.

Edgar







On Monday, March 3, 2014 1:50:40 PM UTC-5, jessem wrote:


 On Mon, Mar 3, 2014 at 12:36 PM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 OK, this is some progress.

 Now you've gone from saying there is NO correlation at all, to the ages 
 ARE CORRELATED WITHIN SOME LIMIT. In other words we DO know that for any 
 set of twins we can always say that their ages ARE the same within some 
 limits. Correct?

 This is a VERY BIG CHANGE in your stated position, from NO correlation at 
 all to SOME correlation...


 Once again your argument turns on vague use of language. You were 
 consistently talking about a 1:1 correlation, so naturally I was using 
 correlation in this sense too. If we say all inertial frames agree that 
 my age T' is simultaneous with my twin's age having some value between T1 
 and T2, but they disagree on the precise value that is NOT a 1:1 
 correlation, period. So there's been no change in my position, it's you 
 whose changing the meaning of correlation in mid-argument in an attempt 
 to prove me wrong.

  


 You though continue to claim that all frames are equally valid, even if 
 they DO NOT preserve the actual age changing acceleration effects between 
 the twins,


 What do you mean by actual age changing acceleration effect? If you're 
 talking about things that are directly measurable without use of a 
 particular frame--like each twin's proper age at any specific event on his 
 worldline (including their identical proper ages at the point in spacetime 
 where they reunite), or 

Re: Block Universes

2014-03-03 Thread Jesse Mazer
On Mon, Mar 3, 2014 at 3:45 PM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 No, it was you that said there was NO correlation.


Jeez Edgar, you really need to work on your reading comprehension. I just
got through AGREEING that I had said that there wasn't a correlation, but I
explained that this was because I was using correlation in the way YOU
had consistently been using it up until now, to refer to a 1:1 correlation
in which each proper age of a twin is matched up to one unique proper age
of the other twin. The archive at
http://www.mail-archive.com/everything-list@googlegroups.com/ has a better
search function than google's archive (returning individual posts rather
than threads), so I searched for posts from Edgar L. Owen with correlate
or correlation in them, results here:

http://www.mail-archive.com/search?a=1l=everything-list%40googlegroups.comhaswords=correlatefrom=Edgar+L.+Owennotwords=subject=datewithin=1ddate=order=datenewestsearch=Search


http://www.mail-archive.com/search?a=1l=everything-list%40googlegroups.comhaswords=correlationfrom=Edgar+L.+Owennotwords=subject=datewithin=1ddate=order=datenewestsearch=Search

Earliest posts on the block time thread I could find in these searches
(that were directed at me, and not some other poster) were these from Feb.
12 and 13 (shown in order below), where you can see from the quotes that
you were talking specifically about 1:1 correlations that map clock times
of one to specific clock times of the other:

http://www.mail-archive.com/everything-list%40googlegroups.com/msg48613.html

So all observers are always in the same p-time moment. Now it's just a
matter of correlating their clock times to see which clock times occurred
in any particular current moment of p-time.

http://www.mail-archive.com/everything-list%40googlegroups.com/msg48716.html

Do you see how this mutual agreed on understanding of how each's clock
time varies in the other's frame always allows each to correlate their own
comoving clock time with the comoving (own) clock time of the other? In
other words for A to always know what B's clock time was reading when A's
clock time was reading t, and for B to always know what A's clock time was
reading when B's clock time was reading t'?

http://www.mail-archive.com/everything-list%40googlegroups.com/msg48750.html

Do you understand that if we have equations for t' in terms of t in A's
frame, and t in terms of t' in B's frame, that we can always establish a 1:
1 correlation between t in A's frame and t' in B's frame?

And in subsequent posts I'm pretty sure you always used correlation in the
same manner, repeating the phrase 1:1 correlation many times (you may
have gotten this phrase from ghibbsa, who used it in a Feb. 6 post at
http://www.mail-archive.com/everything-list%40googlegroups.com/msg48264.htmlthat
you quoted in one of your posts that came up in the search results). A
similar search for posts by me that use correlate or correlation
doesn't show any posts of mine using these words on the thread prior to
your three posts to me above, and subsequently I always used correlation
in the same sense that YOU had been consistently using it, to refer to a
precise 1:1 correlation in ages/proper times.



 In any case that's irrelevant if we know you now accept that there is a
 very LARGE correlation in most situations, and a definable correlation in
 ALL situations. That there is always SOME correlation.

 By actual age changing effect I mean proper accelerations and gravitations
 measurable by a comoving scale at specific clock tick events on his proper
 clock. There is no doubt these are real actual CAUSES with specific
 measurable values that thus must have real actual EFFECTS with specific
 actual values. So you are now saying that all frames DO preserve these
 effects?


What EFFECTS do you think they cause? Can you name a SPECIFIC effect on a
SPECIFIC variable used in relativity? As I've told you before, if you are
talking about some notion of a change in clock rate, then in relativity
there is no frame-independent way to assign a specific actual value to
the concept of a clock rate, the clock rate can only be defined relative
to a particular coordinate system, so the clock rate at a particular
event on the clock's worldline can have DIFFERENT values depending on what
coordinate system you use. So, if this is in fact what you mean by
effects, then I would DENY that proper accelerations have real actual
EFFECTS with specific actual values. If you mean something else by real
actual EFFECTS, you'll have to name the specific effect or your argument
will be hopelessly vague.






 Your 4 point representation of my method MAY BE circular, but my actual
 method is NOT circular.

 Your statement 1. is an incorrect statement of my theory. What I assume
 FIRST in the symmetric case is NOT simultaneity of ages but simultaneity of
 the AGE CHANGING EFFECTS that relativity itself identifies, namely
 acceleration and gravitation.


Not 

Re: Block Universes

2014-03-03 Thread LizR
Jesse, much as I admire your attempt to engage with Edgar and his theory, I
suspect you will eventually have to accept that he isn't arguing rationally
- it looks to me as thought he will just pounce on some word you use, and
twist it around to try and make a case.

He is, in other words, a troll.


On 4 March 2014 11:51, Jesse Mazer laserma...@gmail.com wrote:



 On Mon, Mar 3, 2014 at 3:45 PM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 No, it was you that said there was NO correlation.


 Jeez Edgar, you really need to work on your reading comprehension. I just
 got through AGREEING that I had said that there wasn't a correlation, but I
 explained that this was because I was using correlation in the way YOU
 had consistently been using it up until now, to refer to a 1:1 correlation
 in which each proper age of a twin is matched up to one unique proper age
 of the other twin.


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Re: Block Universes

2014-03-03 Thread Bruno Marchal


On 04 Mar 2014, at 00:01, LizR wrote:

Jesse, much as I admire your attempt to engage with Edgar and his  
theory, I suspect you will eventually have to accept that he isn't  
arguing rationally - it looks to me as thought he will just pounce  
on some word you use, and twist it around to try and make a case.


He is, in other words, a troll.


He certainly behave like a troll. If only by the way he does not  
answer question. The list self-moderation principle is a bit sick  
those days.


Bruno





On 4 March 2014 11:51, Jesse Mazer laserma...@gmail.com wrote:


On Mon, Mar 3, 2014 at 3:45 PM, Edgar L. Owen edgaro...@att.net  
wrote:

Jesse,

No, it was you that said there was NO correlation.

Jeez Edgar, you really need to work on your reading comprehension. I  
just got through AGREEING that I had said that there wasn't a  
correlation, but I explained that this was because I was using  
correlation in the way YOU had consistently been using it up until  
now, to refer to a 1:1 correlation in which each proper age of a  
twin is matched up to one unique proper age of the other twin.



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http://iridia.ulb.ac.be/~marchal/



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Re: Block Universes

2014-03-02 Thread Edgar L. Owen
Jesse,

To answer your final question. If I understand your 3 points correctly then 
I agree with all 3. Though I suspect we understand them differently. When 
you spring your 'proof' we will find that out.

And to your first points. I agree completely that there is no objective or 
actual truth about VIEWS of simultaneity from different frames. That is 
standard relativity which I accept completely. But you still find it 
impossible to understand we can DEDUCE or calculate an ACTUAL physical 
simultaneity irrespective of VIEWS of it.

And just as proper time invariance is NOT ANY VIEW but a deduction or 
calculation, we CAN use deductions and calculations that DO NOT correspond 
to any particular view to determine relativistic truth That such a 
methodology is permissible?


Do you agree that the symmetric relationship defined by the twins executing 
the exact same proper accelerations at their exact same proper times is a 
meaningful physical concept? That we can speak meaningfully about a 
symmetric relationship? You've been referring to it as if you do. Note that 
the twins certainly consider it a meaningful physical scenario because they 
can exchange and execute specific flight plans on that basis.

If so you agree that some frames preserve that real physical relationship 
and some don't? 

If so please tell me why if we want to analyze that ACTUAL real physical 
relationship we should not choose a frame that preserves it?


And second, do you agree my method is consistently calculating something, 
and that something is transitive, even if you don't agree it's a physically 
meaningful concept? 

If not then please try to prove it's not unambiguous and transitive, using 
MY definitions of MY theory rather than your 3 points. In other words 
assume it and then try to disprove it works.

Edgar





On Saturday, March 1, 2014 5:51:37 PM UTC-5, jessem wrote:



 On Sat, Mar 1, 2014 at 5:35 PM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 Let me ask you one simple question.

 In the symmetric case where the twins part and then meet up again with the 
 exact same real actual ages isn't it completely logical to conclude they 
 must also have been the exact same real actual ages all during the trip?

 If, as you claim, the same exact proper accelerations do NOT result in the 
 exact same actual ages all during the trip then how in hell can the twins 
 actually have the exact same actual ages when they meet up?



 It's not that I'm claiming that there's an objective truth that they DON'T 
 have the same ages during the trip. I'm just saying that as far as physics 
 is concerned, there simply IS NO OBJECTIVE OR ACTUAL TRUTH ABOUT 
 SIMULTANEITY, and thus there is neither an actual truth that they are the 
 same age or an actual truth that they are different ages. These things 
 are purely a matter of human coordinate conventions, like the question of 
 which pairs of points on different measuring-tapes have the same y 
 coordinates in any given Cartesian coordinate system. Similarly, questions 
 of simultaneity reduce to questions about which pairs of points on 
 different worldlines have the same t coordinate in any given inertial 
 coordinate system, nothing more.

  


 What is the mysterious mechanism you propose that causes twins that do not 
 have the same actual ages during the trip to just happen to end up with the 
 exact same actual ages when they meet?


 Again, I do not say there is any objective truth that they do not have 
 the same actual ages, I simply say there is no objective truth about which 
 ages are actually simultaneous in some sense that is more than just an 
 arbitrary coordinate convention. But if you're just asking about how things 
 work in FRAMES where they don't have the same actual ages during the trip, 
 the answer is that in such a frame you always find that the answer to which 
 twin's clock is ticking faster changes at some point during the trip, so 
 the twin whose clock was formerly ticking faster is now ticking slower 
 after a certain time coordinate t, and it always balances out exactly 
 ...

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Re: Block Universes

2014-03-02 Thread Jesse Mazer
On Sat, Mar 1, 2014 at 7:09 PM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 To address your points in order:

 1. Yes, you said that proper ages are invariant. But note the important
 point that the proper age of A to himself is a direct observation (he looks
 at his age clock), but to anyone else is a computation and NOT an
 observation.


If he looks at his age clock, that's a direct measurement that is not
specifically tied to ANY frame, including his own comoving frame. And
there's nothing stopping an observer who is moving relative to him from
stealing a glance at his age clock too as she passes him nearby (or looks
at him through her telescope), so she can make a direct measurement of his
age just as easily.

A reference frame only needs to be used when you want to PREDICT some fact
you don't already know through direct measurement, given some other known
facts. For example, if you know that someone has a coordinate velocity v at
coordinate time t0 in some frame, and you know their proper age is T0 at
coordinate time t0, then as long as they move inertially, you can PREDICT
that at some later coordinate time t1, their proper age T1 will be equal to
T0 + (t1 - t0)*sqrt[1 - (v/c)^2]. Of course if you happen to be using the
person's inertial rest frame where v=0, this formula reduces to the simple
one T1 = T0 + (t1 - t0), but this still qualifies as a CALCULATION to
predict his proper age at a later coordinate time t1, not a direct
measurement.




 In fact from their native comoving frames they will observe A at some
 other age than their calculation. So the calculations trump the views.



Huh? You're not making any sense--you just got through agreeing proper
ages are invariant, how can you still maintain they'll observe A at some
other age than their calculation if you agree all frames will predict
exactly the same age for him at any event on his worldline, and this will
also be the age that he will be observed to have on his personal clock at
that event?

Do you just mean that the time coordinate they assign to that event may be
different than his proper age? That would be true, but no one familiar with
relativity would conflate a time coordinate with an age, and anyway it's
quite possible to have an inertial coordinate system where he's at rest but
his age still doesn't match the coordinate time, because his birth is
assigned some time coordinate different from t=0.





 Thus it is valid in relativity to CALCULATE things we CANNOT OBSERVE from
 our frame.


Actual physical measurements can be seen by any observer, like the example
of looking at the age clock of someone you're in motion relative to, so
there's nothing that one person can observe that someone else cannot
observe just because they're in a different rest frame, if by observe
you mean measure using a physical instrument. Of course, actual physical
measurements may be interpreted differently depending on what frame we
use--for example, if I see an object pass the x=10 meters mark on some
ruler when the clock there reads t=5 seconds, and later pass the x=20
meters mark on the same ruler when the clock there reads t=6 seconds, then
if I am using a frame that defines the ruler and clocks to be at rest and
the clocks to be synchronized, I'll say these measurements imply the object
had a velocity of 10 meters per second, but if I'm using a frame where the
ruler itself is moving and the clocks are out of sync, I can say that the
velocity of the object itself was larger or smaller.




 That's what I do to establish 1:1 correlations of actual ages. I use
 calculations that trump Views, that trump observations. We don't always
 have to use frame views to establish relativistic truth. Do you agree with
 that? You must if you accept proper age invariance.


Of course, you can determine relativistic truth by direct measurement, like
looking at someone's clock. But this only applies to quantities that are
frame-invariant, like proper time or proper acceleration. Other quantities
are DEFINED with respect to reference frames, there's absolutely no way to
determine them in a way that doesn't involve a frame. The x-coordinate of
an event would be an example of a quantity that's defined in terms of a
reference frame, you can't determine some object's x-coordinate except in
reference to a particular coordinate system that has a particular spatial
origin and its x-axis oriented in a particular direction. Likewise, the
t-coordinate of an event can only be defined relative to a particular
frame, and since simultaneity is DEFINED in relativity to mean nothing more
than events that have the same t-coordinate, simultaneity can only be
defined relative to a particular frame (talking specifically about physical
definitions of simultaneity in relativity--this doesn't preclude the
possibility of some metaphysical truth about simultaneity that's
impossible to demonstrate experimentally, and of course it's conceivable
that relativity will turn out to be 

Re: Block Universes

2014-03-02 Thread Jesse Mazer
On Sun, Mar 2, 2014 at 12:13 PM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 To answer your final question. If I understand your 3 points correctly
 then I agree with all 3. Though I suspect we understand them differently.
 When you spring your 'proof' we will find that out.


Thanks for addressing the question. As I mentioned in my previous comment
to you, the proof has already been sprung--it is the Alice/Bob/Arlene/Bart
example from Feb. 9 at
https://groups.google.com/d/msg/everything-list/jFX-wTm_E_Q/pxg0VAAHJRQJwhich
I have asked you to address in at least ten different posts since
then.





 And to your first points. I agree completely that there is no objective or
 actual truth about VIEWS of simultaneity from different frames. That is
 standard relativity which I accept completely. But you still find it
 impossible to understand we can DEDUCE or calculate an ACTUAL physical
 simultaneity irrespective of VIEWS of it.

 And just as proper time invariance is NOT ANY VIEW but a deduction or
 calculation, we CAN use deductions and calculations that DO NOT correspond
 to any particular view to determine relativistic truth That such a
 methodology is permissible?


 Do you agree that the symmetric relationship defined by the twins
 executing the exact same proper accelerations at their exact same proper
 times is a meaningful physical concept? That we can speak meaningfully
 about a symmetric relationship?


Only in terms of coordinate-invariant characterizations of their paths,
like the proper acceleration as a function of proper time, or the total
proper time elapsed between departing and reuniting. There is no logical
reason that this symmetry in coordinate-invariant aspects of their trips
somehow forces us to say that a coordinate system where
coordinate-dependent aspects of their trips are symmetrical too represents
actual physical reality where other coordinate systems do not.

Suppose we lay out two measuring tapes on different paths between two
intersection points A and B, and these paths are geometrically symmetrical
in the sense that each one looks like a mirror image of the other if your
mirror is laid out straight between points A and B. Both tapes have their 0
markings coincide with the first intersection point A, and obviously since
the two paths are symmetrical, both measuring tapes will have the same
marking coincide with the second intersection point B. Obviously we could
draw different spatial coordinate axes on the plane, and in some coordinate
systems their paths would be symmetrical in coordinate terms--for example,
a pair of identical markings on each tape would have the same
y-coordinates, and their slopes at these markings would have the same
absolute value--while in others they would not.

I can sketch out a diagram if you can't visualize what I'm talking about,
but assuming you can, do you think that coordinate-based statements based
on a symmetrical coordinate system, like the 4-centimeter marks on each
measuring tape have the same y-coordinate would represent actual
reality, whereas coordinate-based statements in other coordinate systems
would not?





 You've been referring to it as if you do. Note that the twins certainly
 consider it a meaningful physical scenario because they can exchange and
 execute specific flight plans on that basis.

 If so you agree that some frames preserve that real physical relationship
 and some don't?


No, I don't agree. ALL frames preserve the only symmetries I would
recognize as objective ones--same proper acceleration as a function of
proper time, same proper time when the twins reunite--while other
coordinate-depedent statements are not ones I would call a real physical
relationship. Note that they are perfectly free to agree to use a
coordinate system where the coordinate descriptions of their paths are not
symmetrical, and exchange and execute specific flight plans on that basis.




 If so please tell me why if we want to analyze that ACTUAL real physical
 relationship we should not choose a frame that preserves it?


 And second, do you agree my method is consistently calculating something,
 and that something is transitive, even if you don't agree it's a physically
 meaningful concept?



If you consider more than one pair of twins whose paths cross one another,
as I do in my Alice/Bob/Arlene/Bart scenario, then either your method leads
to a contradiction where two different ages of the same observer are judged
simultaneous, or else you'd have to drop one of the assumptions in your
method (meaning it'd no longer be quite the same method). One of those
assumptions was transitivity, so in principle you could drop that if you
wanted to avoid the contradiction I describe, but as I said in my previous
comment, it seems like a much more reasonable assumption to drop is the one
that says inertial clocks at rest relative to one another that are
synchronized in their rest frame must also be synchronized in p-time.
Though as I 

Re: Block Universes

2014-03-02 Thread Edgar L. Owen
Jesse,

I'll address your points in a later post, but first let me run this simple 
new case by you.

Imagine the symmetric trips of the twins continually criss cross each other 
at 1 second intervals (of their own proper clocks) for the duration of the 
entire trip.

At each 1 second meeting I'm sure you would agree their proper times are in 
a 1:1 correlation so their proper times are in a 1:1 correlation every 
second of the duration of the trip and both twins agree on that.

There is a 1:1 correlation of proper age clocks at the criss crosses 
because they are in the same point of space and time by your operational 
reflected light definition AND they both compute both their 1 second proper 
time intervals since the last criss cross as the same invariant number as 
each other, AND they BOTH HAVE AGREED TO CRISS CROSS WHEN EACH OF THEIR 
PROPER TIMES READS 1 SECOND INTERVALS which in itself ensures the 1:1 
correlation of proper times.

Now just take the limit of that and imagine a vanishingly small interval 
for the criss crosses. If we do that then clearly we can say the twins have 
a 1:1 correlation of their proper ages at EVERY MOMENT during the entire 
trip to any limit of accuracy we wish.

Since a criss cross symmetric trip is no different in principle than our 
previous symmetric trip (only a single meeting) it is clear that we have 
proven there is a 1:1 proper age correlation for any symmetric trip during 
EVERY MOMENT of the trip. 

Edgar



On Sunday, March 2, 2014 1:18:27 PM UTC-5, jessem wrote:



 On Sat, Mar 1, 2014 at 7:09 PM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 To address your points in order:

 1. Yes, you said that proper ages are invariant. But note the important 
 point that the proper age of A to himself is a direct observation (he looks 
 at his age clock), but to anyone else is a computation and NOT an 
 observation.


 If he looks at his age clock, that's a direct measurement that is not 
 specifically tied to ANY frame, including his own comoving frame. And 
 there's nothing stopping an observer who is moving relative to him from 
 stealing a glance at his age clock too as she passes him nearby (or looks 
 at him through her telescope), so she can make a direct measurement of his 
 age just as easily.

 A reference frame only needs to be used when you want to PREDICT some fact 
 you don't already know through direct measurement, given some other known 
 facts. For example, if you know that someone has a coordinate velocity v at 
 coordinate time t0 in some frame, and you know their proper age is T0 at 
 coordinate time t0, then as long as they move inertially, you can PREDICT 
 that at some later coordinate time t1, their proper age T1 will be equal to 
 T0 + (t1 - t0)*sqrt[1 - (v/c)^2]. Of course if you happen to be using the 
 person's inertial rest frame where v=0, this formula reduces to the simple 
 one T1 = T0 + (t1 - t0), but this still qualifies as a CALCULATION to 
 predict his proper age at a later coordinate time t1, not a direct 
 measurement.


  

 In fact from their native comoving frames they will observe A at some 
 other age than their calculation. So the calculations trump the views.



 Huh? You're not making any sense--you just got through agreeing proper 
 ages are invariant, how can you still maintain they'll observe A at some 
 other age than their calculation if you agree all frames will predict 
 exactly the same age for him at any event on his worldline, and this will 
 also be the age that he will be observed to have on his personal clock at 
 that event? 

 Do you just mean that the time coordinate they assign to that event may be 
 different than his proper age? That would be true, but no one familiar with 
 relativity would conflate a time coordinate with an age, and anyway it's 
 quite possible to have an inertial coordinate system where he's at rest but 
 his age still doesn't match the coordinate time, because his birth is 
 assigned some time coordinate different from t=0.


  


 Thus it is valid in relativity to CALCULATE things we CANNOT OBSERVE from 
 our frame.


 Actual physical measurements can be seen by any observer, like the example 
 of looking at the age clock of someone you're in motion relative to, so 
 there's nothing that one person can observe that someone else cannot 
 observe just because they're in a different rest frame, if by observe 
 you mean measure using a physical instrument. Of course, actual physical 
 measurements may be interpreted differently depending on what frame we 
 use--for example, if I see an object pass the x=10 meters mark on some 
 ruler when the clock there reads t=5 seconds, and later pass the x=20 
 meters mark on the same ruler when the clock there reads t=6 seconds, then 
 if I am using a frame that defines the ruler and clocks to be at rest and 
 the clocks to be synchronized, I'll say these measurements imply the object 
 had a velocity of 10 meters per second, but if 

Re: Block Universes

2014-03-02 Thread Jesse Mazer
On Sun, Mar 2, 2014 at 2:25 PM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 I'll address your points in a later post, but first let me run this simple
 new case by you.

 Imagine the symmetric trips of the twins continually criss cross each
 other at 1 second intervals (of their own proper clocks) for the duration
 of the entire trip.

 At each 1 second meeting I'm sure you would agree their proper times are
 in a 1:1 correlation so their proper times are in a 1:1 correlation every
 second of the duration of the trip and both twins agree on that.

 There is a 1:1 correlation of proper age clocks at the criss crosses
 because they are in the same point of space and time by your operational
 reflected light definition AND they both compute both their 1 second proper
 time intervals since the last criss cross as the same invariant number as
 each other, AND they BOTH HAVE AGREED TO CRISS CROSS WHEN EACH OF THEIR
 PROPER TIMES READS 1 SECOND INTERVALS which in itself ensures the 1:1
 correlation of proper times.


Sure, there is complete agreement about their respective ages at each
crossing-point.





 Now just take the limit of that and imagine a vanishingly small interval
 for the criss crosses. If we do that then clearly we can say the twins have
 a 1:1 correlation of their proper ages at EVERY MOMENT during the entire
 trip to any limit of accuracy we wish.



The problem is that in this limit, they also approach a state of simply
moving right alongside each other (since the spatial separation they can
achieve between crossings approaches zero), remaining at exactly the same
point in space at any given time, so their worldlines are identical. Of
course it is true in such a case that their ages will remain the same at
every moment in a frame-invariant sense, but this tell us anything about
simultaneity in a case where they have a finite spatial separation
throughout the trip.





 Since a criss cross symmetric trip is no different in principle than our
 previous symmetric trip (only a single meeting) it is clear that we have
 proven there is a 1:1 proper age correlation for any symmetric trip during
 EVERY MOMENT of the trip.

 Edgar



 On Sunday, March 2, 2014 1:18:27 PM UTC-5, jessem wrote:



 On Sat, Mar 1, 2014 at 7:09 PM, Edgar L. Owen edga...@att.net wrote:

 Jesse,

 To address your points in order:

 1. Yes, you said that proper ages are invariant. But note the important
 point that the proper age of A to himself is a direct observation (he looks
 at his age clock), but to anyone else is a computation and NOT an
 observation.


 If he looks at his age clock, that's a direct measurement that is not
 specifically tied to ANY frame, including his own comoving frame. And
 there's nothing stopping an observer who is moving relative to him from
 stealing a glance at his age clock too as she passes him nearby (or looks
 at him through her telescope), so she can make a direct measurement of his
 age just as easily.

 A reference frame only needs to be used when you want to PREDICT some
 fact you don't already know through direct measurement, given some other
 known facts. For example, if you know that someone has a coordinate
 velocity v at coordinate time t0 in some frame, and you know their proper
 age is T0 at coordinate time t0, then as long as they move inertially, you
 can PREDICT that at some later coordinate time t1, their proper age T1 will
 be equal to T0 + (t1 - t0)*sqrt[1 - (v/c)^2]. Of course if you happen to be
 using the person's inertial rest frame where v=0, this formula reduces to
 the simple one T1 = T0 + (t1 - t0), but this still qualifies as a
 CALCULATION to predict his proper age at a later coordinate time t1, not a
 direct measurement.




 In fact from their native comoving frames they will observe A at some
 other age than their calculation. So the calculations trump the views.



 Huh? You're not making any sense--you just got through agreeing proper
 ages are invariant, how can you still maintain they'll observe A at some
 other age than their calculation if you agree all frames will predict
 exactly the same age for him at any event on his worldline, and this will
 also be the age that he will be observed to have on his personal clock at
 that event?

 Do you just mean that the time coordinate they assign to that event may
 be different than his proper age? That would be true, but no one familiar
 with relativity would conflate a time coordinate with an age, and anyway
 it's quite possible to have an inertial coordinate system where he's at
 rest but his age still doesn't match the coordinate time, because his birth
 is assigned some time coordinate different from t=0.





 Thus it is valid in relativity to CALCULATE things we CANNOT OBSERVE from
 our frame.


 Actual physical measurements can be seen by any observer, like the
 example of looking at the age clock of someone you're in motion relative
 to, so there's nothing that one person can observe that someone 

Re: Block Universes

2014-03-02 Thread Edgar L. Owen
Jesse,

Glad we agree on the first point but, even if there is some minimum time 
limit to the criss crosses, you miss the real point of my example. Let me 
restate it:

Since a criss cross symmetric trip is NO DIFFERENT IN PRINCIPLE than our 
previous symmetric trip (only a single meeting) it is clear that we have 
proven there is a 1:1 proper age correlation for any symmetric trip during 
EVERY minimum time interval of the trip EVEN IF THERE ARE NO CRISS CROSSES.

We have confirmed there are proper age correlations (at every second) for 
the criss cross trip but it's exactly the same in principle as any non 
criss cross trip. Therefore there must also be proper age correlations (at 
every second) for ALL symmetric trips.

Edgar



On Sunday, March 2, 2014 2:37:13 PM UTC-5, jessem wrote:



 On Sun, Mar 2, 2014 at 2:25 PM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 I'll address your points in a later post, but first let me run this simple 
 new case by you.

 Imagine the symmetric trips of the twins continually criss cross each 
 other at 1 second intervals (of their own proper clocks) for the duration 
 of the entire trip.

 At each 1 second meeting I'm sure you would agree their proper times are 
 in a 1:1 correlation so their proper times are in a 1:1 correlation every 
 second of the duration of the trip and both twins agree on that.

 There is a 1:1 correlation of proper age clocks at the criss crosses 
 because they are in the same point of space and time by your operational 
 reflected light definition AND they both compute both their 1 second proper 
 time intervals since the last criss cross as the same invariant number as 
 each other, AND they BOTH HAVE AGREED TO CRISS CROSS WHEN EACH OF THEIR 
 PROPER TIMES READS 1 SECOND INTERVALS which in itself ensures the 1:1 
 correlation of proper times.


 Sure, there is complete agreement about their respective ages at each 
 crossing-point.


  


 Now just take the limit of that and imagine a vanishingly small interval 
 for the criss crosses. If we do that then clearly we can say the twins have 
 a 1:1 correlation of their proper ages at EVERY MOMENT during the entire 
 trip to any limit of accuracy we wish.



 The problem is that in this limit, they also approach a state of simply 
 moving right alongside each other (since the spatial separation they can 
 achieve between crossings approaches zero), remaining at exactly the same 
 point in space at any given time, so their worldlines are identical. Of 
 course it is true in such a case that their ages will remain the same at 
 every moment in a frame-invariant sense, but this tell us anything about 
 simultaneity in a case where they have a finite spatial separation 
 throughout the trip.


  


 Since a criss cross symmetric trip is no different in principle than our 
 previous symmetric trip (only a single meeting) it is clear that we have 
 proven there is a 1:1 proper age correlation for any symmetric trip during 
 EVERY MOMENT of the trip. 

 Edgar



 On Sunday, March 2, 2014 1:18:27 PM UTC-5, jessem wrote:



 On Sat, Mar 1, 2014 at 7:09 PM, Edgar L. Owen edga...@att.net wrote:

 Jesse,

 To address your points in order:

 1. Yes, you said that proper ages are invariant. But note the important 
 point that the proper age of A to himself is a direct observation (he looks 
 at his age clock), but to anyone else is a computation and NOT an 
 observation.


 If he looks at his age clock, that's a direct measurement that is not 
 specifically tied to ANY frame, including his own comoving frame. And 
 there's nothing stopping an observer who is moving relative to him from 
 stealing a glance at his age clock too as she passes him nearby (or looks 
 at him through her telescope), so she can make a direct measurement of his 
 age just as easily.

 A reference frame only needs to be used when you want to PREDICT some fact 
 you don't already know through direct measurement, given some other known 
 facts. For example, if you know that someone has a coordinate velocity v at 
 coordinate time t0 in some frame, and you know their proper age is T0 at 
 coordinate time t0, then as long as they move inertially, you can PREDICT 
 that at some later coordinate time t1, their proper age T1 will be equal to 
 T0 + (t1 - t0)*sqrt[1 - (v/c)^2]. Of course if you happen to be using the 
 person's inertial rest frame where v=0, this formula reduces to the simple 
 one T1 = T0 + (t1 - t0), but this still qualifies as a CALCULATION to 
 predict his proper age at a later coordinate time t1, not a direct 
 measurement.


  

 In fact from their native comoving frames they will observe A at some 
 other age than their calculation. So the calculations trump the views.



 Huh? You're not making any sense--you just got through agreeing proper 
 ages are invariant, how can you still maintain they'll observe A at some 
 other age than their calculation if you agree all frames will predict 
 exactly the 

Re: Block Universes

2014-03-02 Thread Edgar L. Owen
Jesse,

Just checking but I'm sure you would agree that twins AT REST with respect 
to each other are the same actual age (have a 1:1 proper age correlation) 
even if they are SEPARATED by distance? You just don't agree that if they 
are separated by distance AND in symmetric acceleration that there is any 
correlation of actual ages possible. Is that correct?

Edgar



On Sunday, March 2, 2014 2:37:13 PM UTC-5, jessem wrote:



 On Sun, Mar 2, 2014 at 2:25 PM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 I'll address your points in a later post, but first let me run this simple 
 new case by you.

 Imagine the symmetric trips of the twins continually criss cross each 
 other at 1 second intervals (of their own proper clocks) for the duration 
 of the entire trip.

 At each 1 second meeting I'm sure you would agree their proper times are 
 in a 1:1 correlation so their proper times are in a 1:1 correlation every 
 second of the duration of the trip and both twins agree on that.

 There is a 1:1 correlation of proper age clocks at the criss crosses 
 because they are in the same point of space and time by your operational 
 reflected light definition AND they both compute both their 1 second proper 
 time intervals since the last criss cross as the same invariant number as 
 each other, AND they BOTH HAVE AGREED TO CRISS CROSS WHEN EACH OF THEIR 
 PROPER TIMES READS 1 SECOND INTERVALS which in itself ensures the 1:1 
 correlation of proper times.


 Sure, there is complete agreement about their respective ages at each 
 crossing-point.


  


 Now just take the limit of that and imagine a vanishingly small interval 
 for the criss crosses. If we do that then clearly we can say the twins have 
 a 1:1 correlation of their proper ages at EVERY MOMENT during the entire 
 trip to any limit of accuracy we wish.



 The problem is that in this limit, they also approach a state of simply 
 moving right alongside each other (since the spatial separation they can 
 achieve between crossings approaches zero), remaining at exactly the same 
 point in space at any given time, so their worldlines are identical. Of 
 course it is true in such a case that their ages will remain the same at 
 every moment in a frame-invariant sense, but this tell us anything about 
 simultaneity in a case where they have a finite spatial separation 
 throughout the trip.


  


 Since a criss cross symmetric trip is no different in principle than our 
 previous symmetric trip (only a single meeting) it is clear that we have 
 proven there is a 1:1 proper age correlation for any symmetric trip during 
 EVERY MOMENT of the trip. 

 Edgar



 On Sunday, March 2, 2014 1:18:27 PM UTC-5, jessem wrote:



 On Sat, Mar 1, 2014 at 7:09 PM, Edgar L. Owen edga...@att.net wrote:

 Jesse,

 To address your points in order:

 1. Yes, you said that proper ages are invariant. But note the important 
 point that the proper age of A to himself is a direct observation (he looks 
 at his age clock), but to anyone else is a computation and NOT an 
 observation.


 If he looks at his age clock, that's a direct measurement that is not 
 specifically tied to ANY frame, including his own comoving frame. And 
 there's nothing stopping an observer who is moving relative to him from 
 stealing a glance at his age clock too as she passes him nearby (or looks 
 at him through her telescope), so she can make a direct measurement of his 
 age just as easily.

 A reference frame only needs to be used when you want to PREDICT some fact 
 you don't already know through direct measurement, given some other known 
 facts. For example, if you know that someone has a coordinate velocity v at 
 coordinate time t0 in some frame, and you know their proper age is T0 at 
 coordinate time t0, then as long as they move inertially, you can PREDICT 
 that at some later coordinate time t1, their proper age T1 will be equal to 
 T0 + (t1 - t0)*sqrt[1 - (v/c)^2]. Of course if you happen to be using the 
 person's inertial rest frame where v=0, this formula reduces to the simple 
 one T1 = T0 + (t1 - t0), but this still qualifies as a CALCULATION to 
 predict his proper age at a later coordinate time t1, not a direct 
 measurement.


  

 In fact from their native comoving frames they will observe A at some 
 other age than their calculation. So the calculations trump the views.



 Huh? You're not making any sense--you just got through agreeing proper 
 ages are invariant, how can you still maintain they'll observe A at some 
 other age than their calculation if you agree all frames will predict 
 exactly the same age for him at any event on his worldline, and this will 
 also be the age that he will be observed to have on his personal clock at 
 that event? 

 Do you just mean that the time coordinate they assign to that event may be 
 different than his proper age? That would be true, but no one familiar with 
 relativity would conflate a time coordinate with an age, and 

Re: Block Universes

2014-03-02 Thread Jesse Mazer
On Sun, Mar 2, 2014 at 6:49 PM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 Just checking but I'm sure you would agree that twins AT REST with respect
 to each other are the same actual age (have a 1:1 proper age correlation)
 even if they are SEPARATED by distance? You just don't agree that if they
 are separated by distance AND in symmetric acceleration that there is any
 correlation of actual ages possible. Is that correct?



No, of course I wouldn't agree that there is any unique actual truth
about their ages in this case, nor would any mainstream physicist. What
part of all frames are equally valid don't you understand? Or do you not
get that if we use an inertial frame where the twins are both moving with
the same constant velocity, they do NOT have identical ages at any given
moment in this frame? (assuming they had identical ages at any given moment
in their rest frame)

Jesse

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Re: Block Universes

2014-03-02 Thread Jesse Mazer
On Sun, Mar 2, 2014 at 6:40 PM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 Glad we agree on the first point but, even if there is some minimum time
 limit to the criss crosses, you miss the real point of my example. Let me
 restate it:

 Since a criss cross symmetric trip is NO DIFFERENT IN PRINCIPLE than our
 previous symmetric trip (only a single meeting) it is clear that we have
 proven there is a 1:1 proper age correlation for any symmetric trip during
 EVERY minimum time interval of the trip EVEN IF THERE ARE NO CRISS CROSSES.


Nonsense. We both agree that in case A where they are right next to each
other throughout the whole trip (same spatial position at every single
moment), there is an objective 1:1 correlation in their ages throughout the
trip. We disagree about whether there is a 1:1 correlation throughout the
trip in case B, where they do NOT occupy the same position through the
trip. So now you think you can prove your belief about CASE B by
considering a series of cases that IN THE LIMIT would have a 1:1
correlation throughout the trip, even though IN THE LIMIT this just reduces
to CASE A, which we already agreed on? Sorry, but this fails basic logic.

Jesse

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Re: Block Universes

2014-03-02 Thread Jesse Mazer
On Sun, Mar 2, 2014 at 7:01 PM, Jesse Mazer laserma...@gmail.com wrote:

 No, of course I wouldn't agree that there is any unique actual truth
 about their ages in this case, nor would any mainstream physicist.


Sorry, I wrote too quickly here--what I meant is that I don't agree there
is any unique actual truth about the CORRELATION between their ages, i.e.
whether or not they reach the same age simultaneously (of course there is
still a unique truth about each one's age at any specific event on his
worldline). They do reach the same age simultaneously in their comoving
inertial frame, but this frame's judgments can't be considered any more
valid than a different inertial frame.

Jesse

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Re: Block Universes

2014-03-02 Thread Edgar L. Owen
Jesse,

OK good, that's what I assumed you meant.

BUT now take the two twins at rest standing on opposite sides of the earth, 
and then they each start walking in different directions. By your criterion 
you then have to say that suddenly and instantly there is NO more 1:1 
correlation of their ages, that they COMPLETELY AND ABSOLUTELY lose their 
1:1 age correlation they had at rest even if they take a SINGLE STEP!

The way you state it this is EITHER OR. Either there is a 1:1 at rest, but 
if they are NOT at rest in the very slightest amount then they COMPLETELY 
AND ABSOLUTELY lose any 1:1 age correlation.

Now if you do NOT agree to that then you are forced to try to claim that 
it's a matter of degree then you have to come up with some mathematical 
function that tells us what VARYING AMOUNT of 1:1 age correlation holds 
with what amount of relative motion. What defines the degree of 1:1 age 
correlation or lack thereof? I certainly don't think relativity theory has 
any such function. For relativity it is absolutely either or. Is this not 
correct?

Or, on the other hand if you use simple logic from my many proofs you just 
admit that any two twins ALWAYS have a 1:1 actual real proper age 
correlation in all situations. And that is is always unambiguously 
calculable in a manner that all observers agree to, but that is not in 
general observable. And this problem and all the other problems simply go 
away

Which is it?

Edgar

On Sunday, March 2, 2014 7:13:31 PM UTC-5, jessem wrote:


 On Sun, Mar 2, 2014 at 7:01 PM, Jesse Mazer laser...@gmail.comjavascript:
  wrote:

 No, of course I wouldn't agree that there is any unique actual truth 
 about their ages in this case, nor would any mainstream physicist. 


 Sorry, I wrote too quickly here--what I meant is that I don't agree there 
 is any unique actual truth about the CORRELATION between their ages, i.e. 
 whether or not they reach the same age simultaneously (of course there is 
 still a unique truth about each one's age at any specific event on his 
 worldline). They do reach the same age simultaneously in their comoving 
 inertial frame, but this frame's judgments can't be considered any more 
 valid than a different inertial frame.

 Jesse



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Re: Block Universes

2014-03-02 Thread Jesse Mazer
On Sun, Mar 2, 2014 at 7:44 PM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 OK good, that's what I assumed you meant.

 BUT now take the two twins at rest standing on opposite sides of the
 earth, and then they each start walking in different directions. By your
 criterion you then have to say that suddenly and instantly there is NO more
 1:1 correlation of their ages, that they COMPLETELY AND ABSOLUTELY lose
 their 1:1 age correlation they had at rest even if they take a SINGLE STEP!


You seem to have misunderstood me, although I thought I was pretty clear--I
said that they did NOT have a unique actual correlation in their ages
when they were at rest relative to each other but at different positions in
space, so nothing changes if they start walking, they still don't have any
unique actual correlation in their ages. Try reading what I wrote again
(with the correction I mentioned that 'any unique actual truth about
their ages' has been changed to 'any unique actual truth about the
correlation between their ages'):

'No, of course I wouldn't agree that there is any unique actual truth
about the correlation between their ages in this case, nor would any
mainstream physicist. What part of all frames are equally valid don't you
understand? Or do you not get that if we use an inertial frame where the
twins are both moving with the same constant velocity, they do NOT have
identical ages at any given moment in this frame? (assuming they had
identical ages at any given moment in their rest frame)'

Jesse



 On Sunday, March 2, 2014 7:13:31 PM UTC-5, jessem wrote:


 On Sun, Mar 2, 2014 at 7:01 PM, Jesse Mazer laser...@gmail.com wrote:

 No, of course I wouldn't agree that there is any unique actual truth
 about their ages in this case, nor would any mainstream physicist.


 Sorry, I wrote too quickly here--what I meant is that I don't agree there
 is any unique actual truth about the CORRELATION between their ages, i.e.
 whether or not they reach the same age simultaneously (of course there is
 still a unique truth about each one's age at any specific event on his
 worldline). They do reach the same age simultaneously in their comoving
 inertial frame, but this frame's judgments can't be considered any more
 valid than a different inertial frame.

 Jesse

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Re: Block Universes

2014-03-02 Thread LizR
A little consideration of trains travelling at half lightspeed with photons
bouncing between parallel mirrors, and people observing lights being turned
on in the station should suffice to demonstrate that there is no objective
truth about the order of spatially separated events. This margin is too
narrow to contain the exact proof, but maybe Brent can oblige?

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Re: Block Universes

2014-03-01 Thread Bruno Marchal


On 01 Mar 2014, at 02:18, Russell Standish wrote:


On Fri, Feb 28, 2014 at 04:14:29PM +0100, Bruno Marchal wrote:


Isn't it crazy to reject what there is enormous evidence for and
accept what there is NO evidence for?


That is what you do. There are no evidence for any universe, and
indeed, as you assume comp, you could understand that there is no
universe. The notion is close to inconsistent, and explanatively
empty.
Physicists measure numbers, and infer relation among numbers. Then
even cosmological theories usually avoid metaphysical commitment.
This is done by physicalist philosophers, and can make sense, but
then not together with the assumption that the brain functions
mechanically at some level.



Sorry to be pernicketty, but if you are working in a theory that makes
no ontologicical commitment (or metaphysical, which I assume is the
same thing), then how does that contradict your reversal result?


Because it is theology, but done scientifically, and so can assume  
an ontology with the only goal to refute it by absurdo, although here,  
as in any applied theory, we need Occam razor.





It is
only a theory _about_ phenomena, not about what's ontologically real.


Theology is concerned with ontology, but does not commit itself on any  
of them, except for refuting them by absurdo. But that is not a  
commitment, only a temporary assumption.


bruno





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Re: Block Universes

2014-03-01 Thread Edgar L. Owen
Jesse,

Of course there is a rational justification for selecting one frame over 
another in many cases. All frames are NOT equal when it comes to 
representing ACTUAL physical facts.

E.g. we can choose various frames to make someone's age pretty much any 
number we like but nevertheless they are still actually the age they think 
they are. If Alice is really 30 we can choose a frame in which she is all 
sorts of different ages but she is still actually 30. Different VIEWS of 
her age don't change her actual age. Isn't that obvious, and don't you 
agree with this?

Your expertise in relativity is clear but you don't seem to understand that 
all frames are NOT equal when it comes to representing actual physical 
fact. You don't understand the fundamental notion in relativity that some 
frames represent actual physical fact, but others represent only HOW OTHER 
OBSERVERS VIEW those physical facts. 

This is quite obvious from the age example above, but it also applies to 
the actual relationship BETWEEN TWINS in my examples. The relationship 
between twins is exactly that, it is a RELATIONSHIP BETWEEN ONLY THOSE 
TWINS. Of course you can come up with frames in which that relationship is 
VIEWED differently, but that DOES NOT CHANGE the actual relationship 
between the twins TO THEMSELVES which is what my theory is based on because 
that is the ACTUAL REALITY of that physical situation. It is not just some 
arbitrary VIEW of that reality, it is the REALITY ITSELF. My theory 
recognizes the need to concentrate on actual physical fact as opposed to 
VIEWS of physical facts.

There is a simple CRITERION to determine whether we are talking about 
PHYSICAL FACT or a VIEW of a physical fact. If the parties TO THE FACT 
AGREE on their views of the fact then that agreed view probably represents 
the actual physical fact. If they DO NOT agree then this disagreement 
represents VIEWS of physical facts rather than the FACTS THEMSELVES. I can 
perhaps think of a few explainable exceptions but this is the generally 
applicable criterion.

For example the different ages of the twins when they meet is AGREED by 
both twins. Thus it is a physical fact. But the different ages of twins in 
relative motion is NOT AGREED by both twins. Thus those are VIEWS OF FACTS, 
RATHER THAN THE FACTS THEMSELVES. An absolutely crucial distinction in 
understanding what relativity is all about.

If we can agree on this obvious point, and that we CAN establish a 1:1 
proper time correlation on this basis, then I look forward to considering 
your example which you claim PROVES this 1:1 proper time correlation is not 
transitive. I'm pretty sure it is transitive when properly understood but 
am certainly willing to consider your 'proof'.

Edgar


On Friday, February 28, 2014 11:55:40 AM UTC-5, jessem wrote:


 On Fri, Feb 28, 2014 at 11:18 AM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 You point out that from the POV of all arbitrary frames they won't be, BUT 
 the point is we MUST use a frame that MAINTAINS the real and actual 
 symmetry to determine the ACTUAL REALITY of this situation.


 Why? You give no rational justification for why reality should coincide 
 with the frame where the coordinates assigned to their paths are 
 symmetrical as opposed to any other frame which makes the same physical 
 predictions, this just seems like a quasi-aesthetic intuition on your part. 
 But I also have a more definitive argument against identifying 
 simultaneity in the frame where their paths look symmetrical with any 
 sort of absolute simultaneity--because, as I have said over and over, it 
 leads directly to contradictions when we consider multiple symmetrical 
 pairs of observers, and the transitive nature of absolute 
 simultaneity/p-time. If you will just respond to my Feb 24 post at 
 https://groups.google.com/d/msg/everything-list/jFX-wTm_E_Q/dM2tcGYspfMJas 
 you promised to do earlier, then as soon as we are completely settled on 
 the matter of whether events that have the same space and time coordinates 
 in an inertial frame must have happened at the same p-time, we can go back 
 and look at the Alice/Bob/Arlene/Bart example at 
 https://groups.google.com/d/msg/everything-list/jFX-wTm_E_Q/pxg0VAAHJRQJwhich 
 PROVES that a contradiction follows fr
 ...

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Re: Block Universes

2014-03-01 Thread Edgar L. Owen
Jesse,

To address your questions:

1. Yes, of course the choice of their own frame is a matter of 
convention. But that does NOT mean that all frames are equal when it comes 
to accurately representing some particular physical fact or relationship.

2. The their experience in my symmetric example is the actual physical 
fact that they know their accelerations are symmetric because they 
exchanged flight plans to ensure that. And because their ACTUAL EXPERIENCE 
is the fact that they both can feel their proper accelerations AND time 
them by their own proper clocks to ensure they are in accordance with the 
flight plans they exchanged. By simple logic they then KNOW BEYOND DOUBT 
that their proper times are always in synch. AND they confirm this by 
meeting with the exact same clock readings that they AGREE upon.

It is true their OBSERVATIONAL experiences of each other do not reflect 
this 1:1 proper time correlation but they are SMART ENOUGH TO UNDERSTAND 
that these are NON agreed VIEWS which do NOT reflect the actual physical 
FACTS of the relationship on which they DO AGREE and thus which is an 
actual physical fact rather than just views of facts.

3. I DO want to address your 'proof of non-transitivity. But for the sake 
of clarity and saving time can you please just restate it in the simplest 
possible terms? I'll make it easier by restating my thesis concisely.

I claim:

a. That any two observers can always establish an agreed 1:1 correlation of 
their proper times BETWEEN THEMSELVES.
(This does NOT MEAN that A's t is always = B's t'. It means there is a 
1:1 correlation that both A and B agree upon.)
b. That this 1:1 relationship will be transitive in the sense that if A's t 
:: B's t', and B's t' :: C's t'', then C's t'' :: A's t.

Assuming my method of establishing the 1:1 correlation what's your proof 
this is incorrect?

Edgar



On Friday, February 28, 2014 1:28:01 PM UTC-5, jessem wrote:


 On Fri, Feb 28, 2014 at 12:38 PM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 First I would appreciate it if you didn't snip my proximate post that you 
 are replying to... 

 Anyway we MUST choose a frame that preserves the symmetry because remember 
 we are trying to establish a 1:1 proper time correlation BETWEEN THE TWINS 
 THEMSELVES (not them and anyone else), and it is only a symmetric frame 
 that preserves the facts as EXPERIENCED BY THE TWINS THEMSELVES. ALL we 
 need to do in my p-time theory is demonstrate that each twin can correlate 
 his OWN proper time with that of the other twin.


 But you agreed earlier (in your post at 
 https://groups.google.com/d/msg/everything-list/jFX-wTm_E_Q/PYrVLII1ClYJ) 
 that the idea of calling the comoving inertial frame of an observer 
 their own frame is purely a matter of CONVENTION, not anything imposed on 
 them by reality. So, we could easily choose a different convention--one 
 in which each twin defines their own frame, or what they experience 
 themselves, as the inertial frame in which they have a velocity of 0.99c 
 along the x-axis. If they both agreed to define the facts as experienced 
 by the twins themselves in this way, by convention, they could also agree 
 on a 1:1 correlation between their proper times, one that would be 
 different from the 1:1 correlation they'd get if they used the comoving 
 frame.

 Do you wish to take back your earlier agreement that phrases like their 
 own frame, their view, what they observe/experience are only by 
 CONVENTION understood to refer to the comoving inertial frame, that this 
 isn't something forced on us by reality? If you still agree this is a 
 matter of convention, then it seems to me that trying to use something 
 that's merely a matter of human linguistic convention to prove something 
 absolute about reality is obviously silly, like trying to prove something 
 about the essential nature of God by noting that according to the spelling 
 conventions of English, God is dog spelled backwards.
  


 All the other frames are the views of OTHER observers, not the views of 
 the twins themselves which is all that we need to consider to establish 
 whether the TWINS THEMSELVES can establish a 1:1.

 Obviously if all observers agreed on an invariant 1:1 correlation we never 
 would have to establish the 1:1 on a successive observer pair basis and 
 then try to prove it transitive as I've consistently worked on doing. 

 MY theory establishes this 1:1 correlation BETWEEN THE ACTUAL TWINS 
 THEMSELVES on a pairwise basis, not on the basis of any invariance. 
 Therefore it obviously uses a symmetric frame that is consistent with how 
 those two twins experience their own and each other's realities and doesn't 
 require input from any other frames to do that.


 That isn't obvious at all--I don't see how the symmetric frame reflects 
 their experience in any way that isn't purely a matter of convention, 
 they certainly don't experience their proper times and velocities being 
 equal 

Re: Block Universes

2014-03-01 Thread Jesse Mazer
On Sat, Mar 1, 2014 at 9:55 AM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 Of course there is a rational justification for selecting one frame over
 another in many cases. All frames are NOT equal when it comes to
 representing ACTUAL physical facts.

 E.g. we can choose various frames to make someone's age pretty much any
 number we like but nevertheless they are still actually the age they think
 they are. If Alice is really 30 we can choose a frame in which she is all
 sorts of different ages


I've already told you that proper time at an event on Alice's worldline is
frame-independent, did you forget already? If one frame says Alice is 30 at
a particular event in her worldline, like the event of her passing a
particular object or observer (or her age when she reunites with her twin),
then ALL frames say this, there is no need to use her comoving frame to get
the correct answer. Different frames may disagree about simultaneity--what
Alice's age is at the same moment that Bob turns 40, at a distant spatial
location--but this is precisely why physicists don't believe there is any
actual physical fact about simultaneity in relativity (this doesn't rule
out presentism since there could still be a metaphysical fact about
simultaneity, but no physical experiment would be able to determine it if
there was, unless relativity turns out to be incorrect in its physical
predictions).




 but she is still actually 30. Different VIEWS of her age don't change her
 actual age. Isn't that obvious, and don't you agree with this?


Don't change her actual age WHEN? Doesn't change her age at some specific
event on her worldline, or doesn't change what her age is now at the same
moment that some distant observer like Bob reaches a particular age, say
40? If the first I agree that she has an actual age at any given event on
her wrodline, but there ARE no different views of this since all frames
agree on her proper age at any specific event on her worldline. If the
latter I don't agree there is any physical basis for saying she has a
unique actual age when Bob is 40, since relativity doesn't give any
physical basis for a preferred definition of simultaneity.



 Your expertise in relativity is clear but you don't seem to understand
 that all frames are NOT equal when it comes to representing actual physical
 fact. You don't understand the fundamental notion in relativity that some
 frames represent actual physical fact, but others represent only HOW OTHER
 OBSERVERS VIEW those physical facts.


Not a physicist in the world would agree with you that there is a
fundamental notion in relativity that some frames represent actual
physical facts, you appear to be completely confused about the difference
between your own p-time views and mainstream relativity. In special
relativity there can NEVER be a basis for considering one inertial frame
more correct than any other. There are only two kinds of facts in
relativity:

1. Facts about frame-independent matters like the proper time of an
observer at a particular event on their worldline; all frames agree in
their predictions about these, so they don't give any reason to prefer one
frame over another.

2. Facts about frame-dependent matters like the coordinate velocity of an
object at a particular event on its worldline, or the question of which
point on worldline B is simultaneous with a particular point on worldline
A; different frames disagree on these matters, and in relativity NO FRAME'S
STATEMENTS ABOUT FRAME-DEPENDENT MATTERS ARE CONSIDERED MORE VALID THAN ANY
OTHER FRAME'S.

If you don't believe me that it's a basic principle of relativity that all
frames are considered equally valid and none are preferred over others,
here are some quotes from books written by physicists that I found on
google books:

If one reference frame moves uniformly relative to another, then the two
are equally good frames for observing nature, and two identical experiments
performed in the two frames will give identical results.

--From Relativity for the Questioning Mind by Daniel Styer, at
http://books.google.com/books?id=Ebr7YhJcUd0Clpg=PP1pg=PA13

The descriptions of the two sets of observers are equally real and equally
valid, each within their own frame of reference. Since no preferred frame
exists, there is no objective basis for ascribing any more reality to one
description than the other.

--From Understanding Relativity: A Simplified Approach to Einstein's
Theories by Leo Sartori, at
http://books.google.com/books?id=gV6kgxrZjL8Clpg=PP1pg=PA173

If Albert and Betty clap nearly simultaneously, one observer may report
that Albert clapped first, whereas a second observer, in motion with
respect to the first, may report that Betty clapped first. It makes no
sense to ask, 'Who really clapped first?' The question assumes that one
viewpoint, one reference frame, is valid or 'real' and the other is not.
But time is not absolute; it is a property of a particular frame of
reference. Both 

Re: Block Universes

2014-03-01 Thread LizR
On 2 March 2014 05:42, Jesse Mazer laserma...@gmail.com wrote:

 On Sat, Mar 1, 2014 at 9:55 AM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 Of course there is a rational justification for selecting one frame over
 another in many cases. All frames are NOT equal when it comes to
 representing ACTUAL physical facts.

 E.g. we can choose various frames to make someone's age pretty much any
 number we like but nevertheless they are still actually the age they think
 they are. If Alice is really 30 we can choose a frame in which she is all
 sorts of different ages


Edgar

I'm sorry, but this sort of comment shows that your grasp of relativity
theory is about as good as your understanding of block universes - which is
to say that yet again, you're completely missing the point. All frames are
equal when it comes to representing physical facts, some are just more
convenient than others for doing the maths (hence relativity). And you
can't make Alice's age whatever you like, you can only obtain different
values by measuring it from frames moving at different velocities, because
the planes of simultaneity attached to those frames intersect Alice's
worldline at different points in space-time.

Why not go away and read up on the subject before you pontificate about it?

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Re: Block Universes

2014-03-01 Thread Edgar L. Owen
Liz,

Hmmm, that's exactly what I said. So why are you disagreeing with yourself 
again? Looks like you are out of touch both with reality and English 
comprehension...

Edgar

On Saturday, March 1, 2014 3:51:18 PM UTC-5, Liz R wrote:

 On 2 March 2014 05:42, Jesse Mazer laser...@gmail.com javascript:wrote:

 On Sat, Mar 1, 2014 at 9:55 AM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 Of course there is a rational justification for selecting one frame over 
 another in many cases. All frames are NOT equal when it comes to 
 representing ACTUAL physical facts.

 E.g. we can choose various frames to make someone's age pretty much any 
 number we like but nevertheless they are still actually the age they think 
 they are. If Alice is really 30 we can choose a frame in which she is all 
 sorts of different ages


 Edgar

 div class=gmail_e
 ...

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Re: Block Universes

2014-03-01 Thread Jesse Mazer
On Sat, Mar 1, 2014 at 5:35 PM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 Let me ask you one simple question.

 In the symmetric case where the twins part and then meet up again with the
 exact same real actual ages isn't it completely logical to conclude they
 must also have been the exact same real actual ages all during the trip?

 If, as you claim, the same exact proper accelerations do NOT result in the
 exact same actual ages all during the trip then how in hell can the twins
 actually have the exact same actual ages when they meet up?



It's not that I'm claiming that there's an objective truth that they DON'T
have the same ages during the trip. I'm just saying that as far as physics
is concerned, there simply IS NO OBJECTIVE OR ACTUAL TRUTH ABOUT
SIMULTANEITY, and thus there is neither an actual truth that they are the
same age or an actual truth that they are different ages. These things
are purely a matter of human coordinate conventions, like the question of
which pairs of points on different measuring-tapes have the same y
coordinates in any given Cartesian coordinate system. Similarly, questions
of simultaneity reduce to questions about which pairs of points on
different worldlines have the same t coordinate in any given inertial
coordinate system, nothing more.




 What is the mysterious mechanism you propose that causes twins that do not
 have the same actual ages during the trip to just happen to end up with the
 exact same actual ages when they meet?


Again, I do not say there is any objective truth that they do not have the
same actual ages, I simply say there is no objective truth about which
ages are actually simultaneous in some sense that is more than just an
arbitrary coordinate convention. But if you're just asking about how things
work in FRAMES where they don't have the same actual ages during the trip,
the answer is that in such a frame you always find that the answer to which
twin's clock is ticking faster changes at some point during the trip, so
the twin whose clock was formerly ticking faster is now ticking slower
after a certain time coordinate t, and it always balances out exactly so
that their clocks have elapsed the same total time when they reunite. If
you like I could give you a simple numerical example where I analyze a
symmetric trip both from the frame where their velocities are symmetrical,
and a different frame where their velocities are non-symmetrical, and show
that it does work out that the second frame predicts their ages will be the
same when they reunite despite them aging at different rates during
different phases of the trip in this frame.

Meanwhile, are you going to address the question about whether you agree
with the 3 premises that I claim together lead to a contradiction? I'll
repost the question from my last post:

'Again, the 3 premises are:

1. If a pair of inertial observers are at rest relative to one another,
then events (like clock readings) that are simultaneous in their comoving
frame are also simultaneous in p-time

2. Any two events that happen at precisely the same position and time
coordinate in a particular inertial frame must be simultaneous in p-time

3. p-time simultaneity is transitive

So to start with, please just tell me if you do agree with all these
premises, or if there is one or more you disagree with or aren't sure about
and require clarification on. And if you disagree with or are not sure
about #2, this is the same point in spacetime issue we had been
discussing earlier before you stopped responding, so in this case please go
back to my last post on the subject at
https://groups.google.com/d/msg/everything-list/jFX-wTm_E_Q/dM2tcGYspfMJand
respond to that.'

Jesse

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Re: Block Universes

2014-03-01 Thread LizR
On 2 March 2014 11:51, Jesse Mazer laserma...@gmail.com wrote:

 On Sat, Mar 1, 2014 at 5:35 PM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 Let me ask you one simple question.

 In the symmetric case where the twins part and then meet up again with
 the exact same real actual ages isn't it completely logical to conclude
 they must also have been the exact same real actual ages all during the
 trip?

 If, as you claim, the same exact proper accelerations do NOT result in
 the exact same actual ages all during the trip then how in hell can the
 twins actually have the exact same actual ages when they meet up?


The same answer as usual. Because the lengths of their worldlines through
space-time between the start and end points are the same.

Do pay attention, 007.

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Re: Block Universes

2014-03-01 Thread ghibbsa

On Monday, February 24, 2014 10:57:14 PM UTC, Edgar L. Owen wrote:

 Ghibbsa,

 I apologize, but I'm a little unsure as to what you are actually asking of 
 me here, but I'll try to answer.

 First P-time and relativity are NOT causally isolated. A proper 
 interpretation of relativity actually implies the necessity of P-time. i've 
 demonstrated why. Please read to my proximate reply to Quentin for an 
 explanation of some of it.

 So because they are causally connected, there could be an inconsistency, 
 which would be fatal, but there isn't any such consistency that has arisen 
 even after many have tried to find one.

 Edgar

 
 
They actually are not causally connected Edgar. 
 
p-time doesn't infer from within itself the layer above will be 
relativistic. And Relativity calculates everything and 
theoretically carries its own weight too without ever once depending on a 
p-time. 
 
What you do is, propose a common shared moment at the point of a handshake 
in a local space. Relativity explains how they got there independently of 
that, but because your proposition is inherently not causal, in that, it's 
an encapsulating dimension. Which it would be possible to propose a 
further encapsulation of that too, without changing anything. Because 
that's the nature of your proposition, there is no definitive, resolvable 
inconsistency.
 
By the way that's the right way to do it IMHO. It's correct to introduce a 
theory that way. It's super robust. No one can refuse it. 
 
However the approach method is that of the tautology. It's the very best 
way to begin. But the introduction is then worth nothing in and of 
itself. Everything hangs on what you construct from that tautological 
foundation.
 
The two problems I've pointed out in your efforts, have been, this one. 
 
And the one where you argue you can correlate moment for moment between 
twins, and that as a proof for p-time. Unfortunately it's not legitimate, 
what you say, because - remembering you are doing this correlating from 
absolute time, it's always going to be possible to 1:1 correlate, moment 
for moment, literally any two objects in the universe, if you are allowed 
to stretch or contract one of them in the dimension of measurement. Which 
is what you allow yourself to do to handle relativistic effects.  

  


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Re: Block Universes

2014-03-01 Thread Edgar L. Owen
Jesse,

To address your points in order:

1. Yes, you said that proper ages are invariant. But note the important 
point that the proper age of A to himself is a direct observation (he looks 
at his age clock), but to anyone else is a computation and NOT an 
observation. In fact from their native comoving frames they will observe A 
at some other age than their calculation. So the calculations trump the 
views.

Thus it is valid in relativity to CALCULATE things we CANNOT OBSERVE from 
our frame. That's what I do to establish 1:1 correlations of actual ages. I 
use calculations that trump Views, that trump observations. We don't always 
have to use frame views to establish relativistic truth. Do you agree with 
that? You must if you accept proper age invariance.

Also note that the ticks of the symmetric twins' own comoving clocks serve 
as event markers. So if the proper ages of the twins are invariant to all 
observers, then all observers can simply observe their clock tick markers 
reading exactly the same for the same proper ages of both twins. That 
PROVES the 1:1 correlation that the real actual ages of the symmetric twins 
always occur at the same clock tick markers and thus they are the same 
proper ages at the same times.

Thus all observers agree that the proper ages of both twins occur at the 
same clock tick marker readings of the twins own proper clocks.

This is one more proof the actual ages of the symmetric twins are equal 
during the trip, and EVERY OBSERVER AGREES ON THIS. Thus it is a real 
physical fact.


2. What all these quotes mean in saying that all frames are equally valid 
is that all observer VIEWS are real actual VIEWS of reality. That they are 
what the observer actually observes. I certainly agree with that. However 
as I've pointed out they don't all preserve the actual physical reality of 
SPECIFIC facts. I just pointed out how they don't with respect to the 
invariance of proper times which are not observable views but calculations. 
Proper age invariance is a physical fact at odds with the notion that all 
frames are equally valid as anything else than VIEWS.

3. No. By the different ages of twins in relative motion are not agreed 
and thus are views rather than actual physical facts I mean just that, and 
just what I've always said. The 1:1 correlation is NOT the VIEW of one twin 
of the other's clock. It is a logical calculation and not a view that 
establishes that 1:1.

4. **You now say you DON'T CLAIM YOU PROVE P-TIME SIMULTANEITY IS NOT 
TRANSITIVE!. OK, great. Wonderful! That's progress, and a complete change 
from what you said previously. You then are apparently trying to prove 
something else. But please, respectfully, you are trying to disprove MY 
theory, so please let ME state MY theory and then try to disprove that 
rather than trying to disprove something that isn't my actual theory.

I just gave a concise statement of my theory earlier today. Can you 
disprove it or can't you?

Edgar







On Saturday, March 1, 2014 11:42:18 AM UTC-5, jessem wrote:



 On Sat, Mar 1, 2014 at 9:55 AM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 Of course there is a rational justification for selecting one frame over 
 another in many cases. All frames are NOT equal when it comes to 
 representing ACTUAL physical facts.

 E.g. we can choose various frames to make someone's age pretty much any 
 number we like but nevertheless they are still actually the age they think 
 they are. If Alice is really 30 we can choose a frame in which she is all 
 sorts of different ages


 I've already told you that proper time at an event on Alice's worldline is 
 frame-independent, did you forget already? If one frame says Alice is 30 at 
 a particular event in her worldline, like the event of her passing a 
 particular object or observer (or her age when she reunites with her twin), 
 then ALL frames say this, there is no need to use her comoving frame to get 
 the correct answer. Different frames may disagree about simultaneity--what 
 Alice's age is at the same moment that Bob turns 40, at a distant spatial 
 location--but this is precisely why physicists don't believe there is any 
 actual physical fact about simultaneity in relativity (this doesn't rule 
 out presentism since there could still be a metaphysical fact about 
 simultaneity, but no physical experiment would be able to determine it if 
 there was, unless relativity turns out to be incorrect in its physical 
 predictions).


  

  but she is still actually 30. Different VIEWS of her age don't change her 
 actual age. Isn't that obvious, and don't you agree with this?


 Don't change her actual age WHEN? Doesn't change her age at some 
 specific event on her worldline, or doesn't change what her age is now at 
 the same moment that some distant observer like Bob reaches a particular 
 age, say 40? If the first I agree that she has an actual age at any given 
 event on her wrodline, but there ARE no 

Re: Block Universes

2014-03-01 Thread Edgar L. Owen
Jesse,

Yes, but what you are saying here is just that it is impossible to 
unambiguously OBSERVE that the proper ages are the same. I agree. But it is 
possible to unambiguously DEDUCE and CALCULATE that they MUST be the same, 
which is all my theory says.

If we can use calculation and deduction with respect to an invariant notion 
of proper ages that we CANNOT unambiguously observe, why can't we use 
calculation and deduction with proper age simultaneity as well?

Edgar



On Saturday, March 1, 2014 5:51:37 PM UTC-5, jessem wrote:



 On Sat, Mar 1, 2014 at 5:35 PM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 Let me ask you one simple question.

 In the symmetric case where the twins part and then meet up again with the 
 exact same real actual ages isn't it completely logical to conclude they 
 must also have been the exact same real actual ages all during the trip?

 If, as you claim, the same exact proper accelerations do NOT result in the 
 exact same actual ages all during the trip then how in hell can the twins 
 actually have the exact same actual ages when they meet up?



 It's not that I'm claiming that there's an objective truth that they DON'T 
 have the same ages during the trip. I'm just saying that as far as physics 
 is concerned, there simply IS NO OBJECTIVE OR ACTUAL TRUTH ABOUT 
 SIMULTANEITY, and thus there is neither an actual truth that they are the 
 same age or an actual truth that they are different ages. These things 
 are purely a matter of human coordinate conventions, like the question of 
 which pairs of points on different measuring-tapes have the same y 
 coordinates in any given Cartesian coordinate system. Similarly, questions 
 of simultaneity reduce to questions about which pairs of points on 
 different worldlines have the same t coordinate in any given inertial 
 coordinate system, nothing more.

  


 What is the mysterious mechanism you propose that causes twins that do not 
 have the same actual ages during the trip to just happen to end up with the 
 exact same actual ages when they meet?


 Again, I do not say there is any objective truth that they do not have 
 the same actual ages, I simply say there is no objective truth about which 
 ages are actually simultaneous in some sense that is more than just an 
 arbitrary coordinate convention. But if you're just asking about how things 
 work in FRAMES where they don't have the same actual ages during the trip, 
 the answer is that in such a frame you always find that the answer to which 
 twin's clock is ticking faster changes at some point during the trip, so 
 the twin whose clock was formerly ticking faster is now ticking slower 
 after a certain time coordinate t, and it always balances out exactly 
 ...

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Re: Block Universes

2014-02-28 Thread Bruno Marchal


On 26 Feb 2014, at 15:32, Edgar L. Owen wrote:


Stathis,

At least we AGREE there is NO empirical evidence for a block universe.


There is no evidence for a universe. (in the usual aristotelian sense  
of the word).





But there is OVERWHELMING evidence for flowing time and a present  
moment.


Not 3p evidences, and the relativity theory makes it senseless (as  
Jesse made rather clear here).

Your p-time seems transitive, and this implies p-time is block-time.



The experience of our existence in a present moment is the most  
fundamental empirical observation of our existence.


It is a 1p evidence. It is not sharable. Using that type of evidence  
is not allow in polite conversation.






And all science, all knowledge, is based on empirical observation.


OK. But consciousness and flowing time are not empirical evidence.  
They are complex data top explain, but cannot be taken for granted, or  
even well defined.





So, in the face of this obvious weight of evidence, why do you  
insist on a block universe instead of a universe in which time flows?


Isn't it crazy to reject what there is enormous evidence for and  
accept what there is NO evidence for?


That is what you do. There are no evidence for any universe, and  
indeed, as you assume comp, you could understand that there is no  
universe. The notion is close to inconsistent, and explanatively empty.
Physicists measure numbers, and infer relation among numbers. Then  
even cosmological theories usually avoid metaphysical commitment. This  
is done by physicalist philosophers, and can make sense, but then not  
together with the assumption that the brain functions mechanically at  
some level.


If you doubt this, then you must find a flaw in the UD Argument.

Bruno




Edgar

On Tuesday, February 25, 2014 5:39:21 PM UTC-5, stathisp wrote:
On 26 February 2014 08:07, Edgar L. Owen edga...@att.net wrote:
 Stathis,

 I know that's your point. You are just restating it once again,  
but you are
 completely UNABLE TO DEMONSTRATE IT without using some example in  
which time

 is already FLOWING.

 Since you can't demonstrate it, there is no reason to believe it.  
Belief in
 a block universe becomes a matter of blind faith, rather than a  
logical
 consequence of anything, and it is certainly NOT based on any  
empirical

 evidence whatsoever.

I'm not arguing that there is empirical evidence for a block universe,
just that a block universe is consistent with our experience.


--
Stathis Papaioannou

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http://iridia.ulb.ac.be/~marchal/



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Re: Block Universes

2014-02-28 Thread Edgar L. Owen
Bruno,

Your contention that there is no evidence for a universe is simply 
delusional. The very fact you can make any statement absolutely PROVES a 
universe of some kind.

Your contention is so absurd it's laughable..

Edgar



On Friday, February 28, 2014 10:14:29 AM UTC-5, Bruno Marchal wrote:


 On 26 Feb 2014, at 15:32, Edgar L. Owen wrote:

 Stathis,

 At least we AGREE there is NO empirical evidence for a block universe.


 There is no evidence for a universe. (in the usual aristotelian sense of 
 the word). 



 But there is OVERWHELMING evidence for flowing time and a present moment. 


 Not 3p evidences, and the relativity theory makes it senseless (as Jesse 
 made rather clear here).
 Your p-time seems transitive, and this implies p-time is block-time.



 The experience of our existence in a present moment is the most 
 fundamental empirical observation of our existence. 


 It is a 1p evidence. It is not sharable. Using that type of evidence is 
 not allow in polite conversation.




 And all science, all knowledge, is based on empirical observation.


 OK. But consciousness and flowing time are not empirical evidence. They 
 are complex data top explain, but cannot be taken for granted, or even well 
 defined.



 So, in the face of this obvious weight of evidence, why do you insist on a 
 block universe instead of a universe in which time flows?

 Isn't it crazy to reject what there is enormous evidence for and accept 
 what there is NO evidence for?


 That is what you do. There are no evidence for any universe, and indeed, 
 as you assume comp, you could understand that there is no universe. The 
 notion is close to inconsistent, and explanatively empty.
 Physicists measure numbers, and infer relation among numbers. Then even 
 cosmological theories usually avoid metaphysical commitment. This is done 
 by physicalist philosophers, and can make sense, but then not together with 
 the assumption that the brain functions mechanically at some level.

 If you doubt this, then you must find a flaw in the UD Argument.

 Bruno



 Edgar

 On Tuesday, February 25, 2014 5:39:21 PM UTC-5, stathisp wrote:

 On 26 February 2014 08:07, Edgar L. Owen edga...@att.net wrote: 
  Stathis, 
  
  I know that's your point. You are just restating it once again, but you 
 are 
  completely UNABLE TO DEMONSTRATE IT without using some example in which 
 time 
  is already FLOWING. 
  
  Since you can't demonstrate it, there is no reason to believe it. Belief 
 in 
  a block universe becomes a matter of blind faith, rather t

 ...

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Re: Block Universes

2014-02-28 Thread Edgar L. Owen
Jesse,

With regards to your contention in your first paragraph below it may 
express the correct view of frame DEPENDENT simultaneity, but that is NOT 
the point I'm making. I'll try to explain more clearly. This example is 
revised to attempt to conform with your previous objections so please bear 
with me. I'll keep it short...

Take twins who start and finish a trip with the same proper ages.

Define their trips as symmetric in the sense they both experience exactly 
equivalent proper accelerations at the exact same moments by their own 
proper clocks. (This is a new definition of symmetric.) This is why their 
ages must be the same when they meet.

Now first I still maintain that in this case it is simple logic to conclude 
that there is a 1:1 correlation of their proper times during the trip, but 
I think we can now do better than that.

Take the beginnings and ends of every phase of their acceleration changes, 
beginning with the start of the trip, as event markers. Now you, yourself, 
tell us that the proper times between every one of these markers is 
invariant. 

Now the question is whether these two invariant proper time sequences are 
synchronized or not. Whether there is a 1:1 correlation of proper times as 
each twin passes through these event markers that are defined identically 
in terms of each twin's proper acceleration? 

You point out that from the POV of all arbitrary frames they won't be, BUT 
the point is we MUST use a frame that MAINTAINS the real and actual 
symmetry to determine the ACTUAL REALITY of this situation. In any frame 
that PRESERVES that symmetry the observer WILL conclude that the proper 
times of both twins between all markers will be exactly the same, and thus 
the proper times of the twins at every one of these symmetric markers will 
be equal. Thus we do have a natural 1:1 correlation between the proper 
times of the twins that is also consistent with the direct observational 
agreement of proper times at start and finish, which we must account for in 
any accurate analysis.

So my point is that there is a REAL AND ACTUAL SYMMETRY between the trips 
of the twins, and thus to get an accurate view of that real symmetry we 
must analyze it in a frame that preserves that symmetry. And when we do 
this we DO achieve a 1:1 correlation of proper ages during the trip, which 
must obviously be correct if they are to meet with the same ages.

My whole approach depends on recognizing the difference between what is 
REALLY HAPPENING to someone as opposed to how any other observer may VIEW 
what is happening to that OTHER person. It is always what is actually 
happening to someone that is the reality irrespective of other's VIEWS of 
that reality.

You consistently present the correct relativistic analysis of relativistic 
VIEWS without recognizing there is an ACTUAL REALITY involved that can be 
properly analyzed only by frames that recognize and preserve that reality.


Do you agree that if we choose a frame that preserves the real and actual 
symmetry of the trip that we do get EQUAL proper times between all markers 
on the twins respective trips? And thus that we CAN establish a 1:1 
correlation of proper times in this case?

Edgar




On Thursday, February 27, 2014 7:11:08 PM UTC-5, jessem wrote:



 On Thu, Feb 27, 2014 at 6:43 PM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 My understanding of the first part of your reply is though proper time is 
 ONLY one's reading of one's own clock (as I stated) it IS possible for 
 any other observer to calculate that proper time and always come up with 
 the same answer. Is that correct?


 For a given clock C, it is possible for any observer to calculate the 
 proper time between events ON C'S OWN WORLDLINE, and everyone will get the 
 same answer (it is frame-invariant). But what is NOT frame-invariant is the 
 answer to a question like what is the proper time on that distant clock 
 RIGHT NOW, at the same moment that my own clock shows some specific time 
 T--in that case you aren't talking about a specific event on C's 
 worldline, you're talking about a specific event on your worldline (the 
 event of your clock showing time T), and asking which event on C's 
 worldline is simultaneous with that. Since simultaneity is frame-dependent 
 in relativity, there is no frame-invariant answer to this second type of 
 question.

  


 If so that's precisely what I've been claiming all along! That it's always 
 possible for any observer to calculate any other observer's PROPER TIME. 
 Why did I get the strong impression you were claiming that wasn't so from 
 your previous replies? That is precisely the whole crux of my case, and 
 precisely what I've been claiming

 In my view that is exactly what is necessary to establish a 1:1 
 correlation between proper times. If everyone can always calculate 
 everyone's proper times including their own in an UNAMBIGUOUS INVARIANT WAY 
 then why isn't it possible to 

Re: Block Universes

2014-02-28 Thread Jesse Mazer
On Fri, Feb 28, 2014 at 11:18 AM, Edgar L. Owen edgaro...@att.net wrote:

 You point out that from the POV of all arbitrary frames they won't be, BUT
 the point is we MUST use a frame that MAINTAINS the real and actual
 symmetry to determine the ACTUAL REALITY of this situation.


Why? You give no rational justification for why reality should coincide
with the frame where the coordinates assigned to their paths are
symmetrical as opposed to any other frame which makes the same physical
predictions, this just seems like a quasi-aesthetic intuition on your part.
But I also have a more definitive argument against identifying
simultaneity in the frame where their paths look symmetrical with any
sort of absolute simultaneity--because, as I have said over and over, it
leads directly to contradictions when we consider multiple symmetrical
pairs of observers, and the transitive nature of absolute
simultaneity/p-time. If you will just respond to my Feb 24 post at
https://groups.google.com/d/msg/everything-list/jFX-wTm_E_Q/dM2tcGYspfMJ as
you promised to do earlier, then as soon as we are completely settled on
the matter of whether events that have the same space and time coordinates
in an inertial frame must have happened at the same p-time, we can go back
and look at the Alice/Bob/Arlene/Bart example at
https://groups.google.com/d/msg/everything-list/jFX-wTm_E_Q/pxg0VAAHJRQJwhich
PROVES that a contradiction follows from your assumptions, given the
premise that events with the same space and time coordinates in an inertial
frame happened at the same p-time.



 Do you agree that if we choose a frame that preserves the real and actual
 symmetry of the trip that we do get EQUAL proper times between all markers
 on the twins respective trips? And thus that we CAN establish a 1:1
 correlation of proper times in this case?



The real and actual symmetry is that they have symmetrical proper
accelerations as a function of proper time, but ALL frames preserve this
symmetry. I agree that we are free to use a frame where their coordinate
velocities and proper time as a function of coordinate time are ALSO
symmetrical, but these are simply statements about coordinates, I see no
reason to consider them any more real and actual than the coordinates
assigned to their paths in any other frame.

Jesse

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Re: Block Universes

2014-02-28 Thread Edgar L. Owen
Jesse,

First I would appreciate it if you didn't snip my proximate post that you 
are replying to... 

Anyway we MUST choose a frame that preserves the symmetry because remember 
we are trying to establish a 1:1 proper time correlation BETWEEN THE TWINS 
THEMSELVES (not them and anyone else), and it is only a symmetric frame 
that preserves the facts as EXPERIENCED BY THE TWINS THEMSELVES. ALL we 
need to do in my p-time theory is demonstrate that each twin can correlate 
his OWN proper time with that of the other twin.

All the other frames are the views of OTHER observers, not the views of the 
twins themselves which is all that we need to consider to establish whether 
the TWINS THEMSELVES can establish a 1:1.

Obviously if all observers agreed on an invariant 1:1 correlation we never 
would have to establish the 1:1 on a successive observer pair basis and 
then try to prove it transitive as I've consistently worked on doing. 

MY theory establishes this 1:1 correlation BETWEEN THE ACTUAL TWINS 
THEMSELVES on a pairwise basis, not on the basis of any invariance. 
Therefore it obviously uses a symmetric frame that is consistent with how 
those two twins experience their own and each other's realities and doesn't 
require input from any other frames to do that.

MY theory then attempts to prove these correlations are transitive on a 
pair by pair basis, not by considering all irrelevant frames and trying to 
establish some invariance that I agree is impossible.

Does this make it clear what my theory is trying to do? The theory is based 
on pair wise correlations, not invariance

Edgar



On Friday, February 28, 2014 11:55:40 AM UTC-5, jessem wrote:


 On Fri, Feb 28, 2014 at 11:18 AM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 You point out that from the POV of all arbitrary frames they won't be, BUT 
 the point is we MUST use a frame that MAINTAINS the real and actual 
 symmetry to determine the ACTUAL REALITY of this situation.


 Why? You give no rational justification for why reality should coincide 
 with the frame where the coordinates assigned to their paths are 
 symmetrical as opposed to any other frame which makes the same physical 
 predictions, this just seems like a quasi-aesthetic intuition on your part. 
 But I also have a more definitive argument against identifying 
 simultaneity in the frame where their paths look symmetrical with any 
 sort of absolute simultaneity--because, as I have said over and over, it 
 leads directly to contradictions when we consider multiple symmetrical 
 pairs of observers, and the transitive nature of absolute 
 simultaneity/p-time. If you will just respond to my Feb 24 post at 
 https://groups.google.com/d/msg/everything-list/jFX-wTm_E_Q/dM2tcGYspfMJas 
 you promised to do earlier, then as soon as we are completely settled on 
 the matter of whether events that have the same space and time coordinates 
 in an inertial frame must have happened at the same p-time, we can go back 
 and look at the Alice/Bob/Arlene/Bart example at 
 https://groups.google.com/d/msg/everything-list/jFX-wTm_E_Q/pxg0VAAHJRQJwhich 
 PROVES that a contradiction follows from your assumptions, given
 ...

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Re: Block Universes

2014-02-28 Thread Bruno Marchal


On 27 Feb 2014, at 04:45, Jesse Mazer wrote:



On Wed, Feb 26, 2014 at 8:52 PM, Edgar L. Owen edgaro...@att.net  
wrote:


Can you agree to this at least?

To repeat what I said in my second-to-last post:

'If you continue to ask me Do you agree? type questions while  
ignoring the similar questions I ask you, I guess I'll have to take  
that as a sign of contempt, in which case as I said I won't be  
responding to further posts of yours. Any response is better than  
just completely ignoring questions, even if it's something like I  
find your questions ambiguous or you've asked too many questions  
and I don't have time for them all right now, please narrow it down  
to one per post.'


If you decide to treat me with the same basic level of respect I  
have treated you, rather than making a show of asking me questions  
while you contemptuously ignore my requests that you address mine,  
then I will keep going with this. If not, I have better things to do.


I think some people does not argue, they fake it only. Edgar does not  
answer the question asked.


Bruno





Jesse

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Re: Block Universes

2014-02-28 Thread Bruno Marchal


On 28 Feb 2014, at 00:10, LizR wrote:

Any attempt to separate out time from space-time and remain within  
the context of special relativity is bound to fail, because SR is  
the unification of space and time. In Newtonian theory there was  
absolute space and absolute time. In SR there is only absolute space- 
time (in the sense of invariant distances through space-time). In  
SR, time is relative, and lunch time doubly so.


:)


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Re: Block Universes

2014-02-28 Thread Jesse Mazer
On Fri, Feb 28, 2014 at 12:38 PM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 First I would appreciate it if you didn't snip my proximate post that you
 are replying to...

 Anyway we MUST choose a frame that preserves the symmetry because remember
 we are trying to establish a 1:1 proper time correlation BETWEEN THE TWINS
 THEMSELVES (not them and anyone else), and it is only a symmetric frame
 that preserves the facts as EXPERIENCED BY THE TWINS THEMSELVES. ALL we
 need to do in my p-time theory is demonstrate that each twin can correlate
 his OWN proper time with that of the other twin.


But you agreed earlier (in your post at
https://groups.google.com/d/msg/everything-list/jFX-wTm_E_Q/PYrVLII1ClYJ )
that the idea of calling the comoving inertial frame of an observer their
own frame is purely a matter of CONVENTION, not anything imposed on them
by reality. So, we could easily choose a different convention--one in
which each twin defines their own frame, or what they experience
themselves, as the inertial frame in which they have a velocity of 0.99c
along the x-axis. If they both agreed to define the facts as experienced
by the twins themselves in this way, by convention, they could also agree
on a 1:1 correlation between their proper times, one that would be
different from the 1:1 correlation they'd get if they used the comoving
frame.

Do you wish to take back your earlier agreement that phrases like their
own frame, their view, what they observe/experience are only by
CONVENTION understood to refer to the comoving inertial frame, that this
isn't something forced on us by reality? If you still agree this is a
matter of convention, then it seems to me that trying to use something
that's merely a matter of human linguistic convention to prove something
absolute about reality is obviously silly, like trying to prove something
about the essential nature of God by noting that according to the spelling
conventions of English, God is dog spelled backwards.



 All the other frames are the views of OTHER observers, not the views of
 the twins themselves which is all that we need to consider to establish
 whether the TWINS THEMSELVES can establish a 1:1.

 Obviously if all observers agreed on an invariant 1:1 correlation we never
 would have to establish the 1:1 on a successive observer pair basis and
 then try to prove it transitive as I've consistently worked on doing.

 MY theory establishes this 1:1 correlation BETWEEN THE ACTUAL TWINS
 THEMSELVES on a pairwise basis, not on the basis of any invariance.
 Therefore it obviously uses a symmetric frame that is consistent with how
 those two twins experience their own and each other's realities and doesn't
 require input from any other frames to do that.


That isn't obvious at all--I don't see how the symmetric frame reflects
their experience in any way that isn't purely a matter of convention,
they certainly don't experience their proper times and velocities being
equal at each coordinate time if they don't CHOOSE to use a particular
coordinate system. All that they directly experience in a way that
doesn't depend on coordinate systems is the way that their proper
acceleration varied as a function of their proper time.



 MY theory then attempts to prove these correlations are transitive on a
 pair by pair basis, not by considering all irrelevant frames and trying to
 establish some invariance that I agree is impossible.

 Does this make it clear what my theory is trying to do? The theory is
 based on pair wise correlations, not invariance



My proof of a contradiction in your ideas about p-time doesn't consider the
other frames you consider irrelevant either, it is based SOLELY on the
following premises:

1. If a pair of inertial observers are at rest relative to one another,
then events (like clock readings) that are simultaneous in their comoving
frame are also simultaneous in p-time

2. Any two events that happen at precisely the same position and time
coordinate in a particular inertial frame must be simultaneous in p-time

3. p-time simultaneity is transitive

Your only response was to dispute premise #2, but subsequent discussion
suggested you were originally misunderstanding what I meant by same
position and time coordinate and that properly understood, you would most
like agree with premise #2 after all. That's why I want you to address my
last few questions about the same position and time coordinate issue at
https://groups.google.com/d/msg/everything-list/jFX-wTm_E_Q/dM2tcGYspfMJwhich
you promised to address earlier, but have subsequently ignored all my
requests to get back to. Once again, if you continue to just ignore the
requests, that indicates a lack of respect for me and for the two-way
nature of discussions. Here, I'll even repost those questions to save you
the time of going back through your inbox to find the original post to
reply to:

On Mon, Feb 24, 2014 at 6:53 PM, Edgar L. Owen edgaro...@att.netwrote:

 Jesse,

 Well, I 

Re: Block Universes

2014-02-28 Thread Bruno Marchal


On 28 Feb 2014, at 16:20, Edgar L. Owen wrote:


Bruno,

Your contention that there is no evidence for a universe is simply  
delusional.


I meant the Aristotelian universe, where physics is supposed to  
describe the fundamental ontology, or what is.
Of course I believe in something, and I take very seriously the  
appearance of some physical reality into account.




The very fact you can make any statement absolutely PROVES a  
universe of some kind.


I agree. And I tend to believe in the arithmetical reality.


The computable is a part of the arithmetical reality, which is larger.  
It happens that the arithmetical computable part can infer and even  
mirror larger and larger part of the non computable.


See the book by Matiyasevich to see how diophantine relations can  
simulate Turing machines.



Bruno




Your contention is so absurd it's laughable..








Edgar



On Friday, February 28, 2014 10:14:29 AM UTC-5, Bruno Marchal wrote:

On 26 Feb 2014, at 15:32, Edgar L. Owen wrote:

Stathis,

At least we AGREE there is NO empirical evidence for a block universe.

There is no evidence for a universe. (in the usual aristotelian  
sense of the word).




But there is OVERWHELMING evidence for flowing time and a present  
moment.


Not 3p evidences, and the relativity theory makes it senseless (as  
Jesse made rather clear here).

Your p-time seems transitive, and this implies p-time is block-time.



The experience of our existence in a present moment is the most  
fundamental empirical observation of our existence.


It is a 1p evidence. It is not sharable. Using that type of evidence  
is not allow in polite conversation.





And all science, all knowledge, is based on empirical observation.

OK. But consciousness and flowing time are not empirical evidence.  
They are complex data top explain, but cannot be taken for granted,  
or even well defined.




So, in the face of this obvious weight of evidence, why do you  
insist on a block universe instead of a universe in which time flows?


Isn't it crazy to reject what there is enormous evidence for and  
accept what there is NO evidence for?


That is what you do. There are no evidence for any universe, and  
indeed, as you assume comp, you could understand that there is no  
universe. The notion is close to inconsistent, and explanatively  
empty.
Physicists measure numbers, and infer relation among numbers. Then  
even cosmological theories usually avoid metaphysical commitment.  
This is done by physicalist philosophers, and can make sense, but  
then not together with the assumption that the brain functions  
mechanically at some level.


If you doubt this, then you must find a flaw in the UD Argument.

Bruno



Edgar

On Tuesday, February 25, 2014 5:39:21 PM UTC-5, stathisp wrote:
On 26 February 2014 08:07, Edgar L. Owen edga...@att.net wrote:
 Stathis,

 I know that's your point. You are just restating it once again,  
but you are
 completely UNABLE TO DEMONSTRATE IT without using some example in  
which time

 is already FLOWING.

 Since you can't demonstrate it, there is no reason to believe it.  
Belief in

 a block universe becomes a matter of blind faith, rather t
...

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Re: Block Universes

2014-02-28 Thread Edgar L. Owen
Bruno,

Nonsense. You continually ask the exact same questions which I answered 
several times but just ignore my answers and keep asking the same 
questions, and when you rarely do respond to my answers you do so 
incoherently and only in terms of your own very rigid worldview.

Well perhaps that's the way that 1p zombies 1p clones operate?

Anyway I do answer all serious questions...

Edgar



On Friday, February 28, 2014 12:42:26 PM UTC-5, Bruno Marchal wrote:


 On 27 Feb 2014, at 04:45, Jesse Mazer wrote:


 On Wed, Feb 26, 2014 at 8:52 PM, Edgar L. Owen edga...@att.netjavascript:
  wrote:


 Can you agree to this at least?


 To repeat what I said in my second-to-last post:

 'If you continue to ask me Do you agree? type questions while ignoring 
 the similar questions I ask you, I guess I'll have to take that as a sign 
 of contempt, in which case as I said I won't be responding to further posts 
 of yours. Any response is better than just completely ignoring questions, 
 even if it's something like I find your questions ambiguous or you've 
 asked too many questions and I don't have time for them all right now, 
 please narrow it down to one per post.'

 If you decide to treat me with the same basic level of respect I have 
 treated you, rather than making a show of asking me questions while you 
 contemptuously ignore my requests that you address mine, then I will keep 
 going with this. If not, I have better things to do.


 I think some people does not argue, they fake it only. Edgar does not 
 answer the question asked. 

 Bruno




 Jesse

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Re: Block Universes

2014-02-28 Thread LizR
On 1 March 2014 04:14, Bruno Marchal marc...@ulb.ac.be wrote:

 On 26 Feb 2014, at 15:32, Edgar L. Owen wrote:

 Stathis,

 At least we AGREE there is NO empirical evidence for a block universe.

 There is no evidence for a universe. (in the usual Aristotelian sense of
 the word).


True. If only because evidence isn't for things.

But in any case, Edgar doesn't appear to grasp what a block universe is, as
he proves by his continual meaningless comments about it. He has some weird
idea that has nothing to do with the scientific concept expounded in
relativity, and that's what he's arguing against. So, rather like the
discussion Jesse has been having with him about p-time,  this is a
pointless discussion. As I mentioned (it must have been some weeks ago now)
with regard to Edgar-ism, you can't argue with a religious fanatic who
refuses to consider any opposing viewpoint, and who sees everything you say
through the lens of his own fantasy.

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Re: Block Universes

2014-02-28 Thread LizR
On 1 March 2014 06:42, Bruno Marchal marc...@ulb.ac.be wrote:

 On 27 Feb 2014, at 04:45, Jesse Mazer wrote:

 On Wed, Feb 26, 2014 at 8:52 PM, Edgar L. Owen edgaro...@att.net wrote:


 Can you agree to this at least?


 To repeat what I said in my second-to-last post:

 'If you continue to ask me Do you agree? type questions while ignoring
 the similar questions I ask you, I guess I'll have to take that as a sign
 of contempt, in which case as I said I won't be responding to further posts
 of yours. Any response is better than just completely ignoring questions,
 even if it's something like I find your questions ambiguous or you've
 asked too many questions and I don't have time for them all right now,
 please narrow it down to one per post.'

 If you decide to treat me with the same basic level of respect I have
 treated you, rather than making a show of asking me questions while you
 contemptuously ignore my requests that you address mine, then I will keep
 going with this. If not, I have better things to do.


 I think some people does not argue, they fake it only. Edgar does not
 answer the question asked.


On most forums he would have been banned as a troll, because either (a) he
is too stupid to grasp the arguments of his opponents and give a rational
response or (b) he is deliberately refusing to do so. The polite assumption
is (b), which makes him a troll - someone who deliberately tries to provoke
arguments for their own malicious amusement. If this forum wasn't full of
saints, everyone would by now have given up talking to him. Instead,
because we tend to believe that everyone is rational and can be educated if
we try hard enough, we keep trying (I did for quite a while). But of course
a troll is, in game-theoretic terms, a defector in what is mostly a
community of co-operators. Hence they flourish for a while, until everyone
gets tired of hitting their head against a brick wall.

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Re: Block Universes

2014-02-28 Thread Russell Standish
On Fri, Feb 28, 2014 at 04:14:29PM +0100, Bruno Marchal wrote:
 
 Isn't it crazy to reject what there is enormous evidence for and
 accept what there is NO evidence for?
 
 That is what you do. There are no evidence for any universe, and
 indeed, as you assume comp, you could understand that there is no
 universe. The notion is close to inconsistent, and explanatively
 empty.
 Physicists measure numbers, and infer relation among numbers. Then
 even cosmological theories usually avoid metaphysical commitment.
 This is done by physicalist philosophers, and can make sense, but
 then not together with the assumption that the brain functions
 mechanically at some level.
 

Sorry to be pernicketty, but if you are working in a theory that makes
no ontologicical commitment (or metaphysical, which I assume is the
same thing), then how does that contradict your reversal result? It is
only a theory _about_ phenomena, not about what's ontologically real.


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Principal, High Performance Coders
Visiting Professor of Mathematics  hpco...@hpcoders.com.au
University of New South Wales  http://www.hpcoders.com.au


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Re: Block Universes

2014-02-28 Thread Bruno Marchal


On 28 Feb 2014, at 21:05, Edgar L. Owen wrote:


Bruno,

Nonsense. You continually ask the exact same questions which I  
answered several times but just ignore my answers and keep asking  
the same questions, and when you rarely do respond to my answers you  
do so incoherently and only in terms of your own very rigid worldview.


Define what you mean by computation. you did not answer this, or  
give me the link. What you did is to repeat things like reality  
computes, which add more mystery to the notion.

You never answered if you are OK with Church thesis.

Bruno






Well perhaps that's the way that 1p zombies 1p clones operate?

Anyway I do answer all serious questions...

Edgar



On Friday, February 28, 2014 12:42:26 PM UTC-5, Bruno Marchal wrote:

On 27 Feb 2014, at 04:45, Jesse Mazer wrote:


On Wed, Feb 26, 2014 at 8:52 PM, Edgar L. Owen edga...@att.net  
wrote:


Can you agree to this at least?

To repeat what I said in my second-to-last post:

'If you continue to ask me Do you agree? type questions while  
ignoring the similar questions I ask you, I guess I'll have to take  
that as a sign of contempt, in which case as I said I won't be  
responding to further posts of yours. Any response is better than  
just completely ignoring questions, even if it's something like I  
find your questions ambiguous or you've asked too many questions  
and I don't have time for them all right now, please narrow it down  
to one per post.'


If you decide to treat me with the same basic level of respect I  
have treated you, rather than making a show of asking me questions  
while you contemptuously ignore my requests that you address mine,  
then I will keep going with this. If not, I have better things to do.


I think some people does not argue, they fake it only. Edgar does  
not answer the question asked.


Bruno




Jesse

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Re: Block Universes

2014-02-27 Thread Edgar L. Owen
Jesse,

I haven't answered those questions out of any disrespect or rudeness but 
because I was working on a new explanation which I think does specifically 
address and answer all of them which I present in this post. I will be 
happy to answer any of your questions if you think they are still relevant 
after reading this post which I think solves the 1:1 age correlation to 
your satisfaction.


If you find any of the terminology confusing please let me know what you 
think it SHOULD be rather than just saying it's wrong.

Twins A and B start at the same location in deep space. No acceleration, no 
gravitation. Their ages are obviously the same, and their age clocks are 
running at the same rate.

They exchange flight plans and embark on their separate trips according to 
those flight plans.

Now the only effects that will alter the rates of their age clocks are 
acceleration or gravitation. But each twin can continually measure the 
amount of acceleration or gravitation he experiences with a scale.

So each twin can always calculate how much his age has slowed relative to 
what his age WOULD HAVE BEEN had he NOT experienced any gravitation or 
acceleration. Let's call that his 'inertial age', the age he WOULD have 
been had he NOT experienced any acceleration or gravitation.

So each twin always knows what inertial age corresponds to his actual age. 

And because each twin has the exact flight plan of the other twin, he also 
can calculate what inertial age corresponds to the actual age of the other 
twin at any point on his trip because the flight plan tells him what all 
accelerations and gravitational effects will be.

Thus it is a simple, frame independent matter for both twins to get a 1:1 
correspondence between their respective actual ages in terms of their 
inertial ages since their inertial ages will always be the same.

If A is age a' when his inertial age is I', and B is age a'' when his 
inertial age is I', then A will be actual age a' when B is actual age a'', 
and we can always establish such a 1:1 correspondence of actual ages for 
any actual age of either.

And both twins will always AGREE on this 1:1 correlation of their actual 
ages.


Note it is not even necessary to exchange flight plans. Each twin can just 
continually transmit a light signal to the other giving his current actual 
age in terms of his inertial age. That again allows both twins to correlate 
their actual ages.

So this gives us a frame independent way for any two observers who 
initially synchronize their inertial ages to the same arbitrary value to 
always establish an UN-ambiguous, AGREED 1:1 correlation of their actual 
ages.

Do you agree?


Edgar


On Wednesday, February 26, 2014 10:45:51 PM UTC-5, jessem wrote:


 On Wed, Feb 26, 2014 at 8:52 PM, Edgar L. Owen edga...@att.netjavascript:
  wrote:


 Can you agree to this at least?


 To repeat what I said in my second-to-last post:

 'If you continue to ask me Do you agree? type questions while ignoring 
 the similar questions I ask you, I guess I'll have to take that as a sign 
 of contempt, in which case as I said I won't be responding to further posts 
 of yours. Any response is better than just completely ignoring questions, 
 even if it's something like I find your questions ambiguous or you've 
 asked too many questions and I don't have time for them all right now, 
 please narrow it down to one per post.'

 If you decide to treat me with the same basic level of respect I have 
 treated you, rather than making a show of asking me questions while you 
 contemptuously ignore my requests that you address mine, then I will keep 
 going with this. If not, I have better things to do.

 Jesse


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Everything List group.
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to everything-list+unsubscr...@googlegroups.com.
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Re: Block Universes

2014-02-27 Thread Jesse Mazer
On Thu, Feb 27, 2014 at 9:25 AM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 I haven't answered those questions out of any disrespect or rudeness but
 because I was working on a new explanation which I think does specifically
 address and answer all of them which I present in this post. I will be
 happy to answer any of your questions if you think they are still relevant
 after reading this post which I think solves the 1:1 age correlation to
 your satisfaction.


That's the problem, you continually come up with new arguments and
explanations that you think resolve the questions I asked and therefore
mean you don't need to address them, but inevitably I disagree. Please just
respect my judgment about what's relevant TO ME, and answer the questions
that I ask ALONGSIDE any new arguments or explanations you might want to
supply. You say above I will be happy to answer any of your questions if
you think they are still relevant after reading this post, so I will hold
you to that by repeating a question I'd like you to answer at the end of
this post.





 If you find any of the terminology confusing please let me know what you
 think it SHOULD be rather than just saying it's wrong.

 Twins A and B start at the same location in deep space. No acceleration,
 no gravitation. Their ages are obviously the same, and their age clocks are
 running at the same rate.

 They exchange flight plans and embark on their separate trips according to
 those flight plans.

 Now the only effects that will alter the rates of their age clocks are
 acceleration or gravitation. But each twin can continually measure the
 amount of acceleration or gravitation he experiences with a scale.



Let's consider just the issue of accelerations in flat SR spacetime for
now, since it's simpler. The problem with this statement is that although
it's true each twin can measure their proper acceleration, there is no
FRAME-INDEPENDENT equation in relativity for how a given acceleration
affects the rates of their age clocks, the only equations dealing with
clock rates and acceleration in SR deal with how changes in coordinate
velocity (determined by acceleration) affect the rate a clock is ticking
relative to coordinate time in some specific coordinate system.



 So each twin can always calculate how much his age has slowed relative to
 what his age WOULD HAVE BEEN had he NOT experienced any gravitation or
 acceleration. Let's call that his 'inertial age', the age he WOULD have
 been had he NOT experienced any acceleration or gravitation.



I see no way to define this in any frame-independent way. The only version
of this that relativity would allow you to calculate is what your age would
have been at a PARTICULAR COORDINATE TIME if you had remained inertial, and
you can compare that to what your age is at that SAME COORDINATE TIME given
your acceleration history. But this comparison obviously gives different
results in different coordinate systems. So, I don't agree with your
subsequent conclusion that this allows two twins to define a 1:1
correlation in their ages in a frame-independent way.

There are a number of questions I asked in the last few posts that none of
your answers have addressed, but I'll restrict myself to repeating one for
now:

'Also, do you understand that even for inertial observers, the idea that an
observer's own rest frame can be labeled his view or taken to describe
his observations is PURELY A MATTER OF CONVENTION, not something that is
forced on us by the laws of nature? Physicists just don't want to have to
write out in the observer's comoving inertial frame all the time, so they
just adopt a linguistic convention that lets them write simpler things like
from this observer's perspective or in his frame as a shorthand for the
observer's comoving inertial frame. Physically there is no reason an
observer can't assign coordinates to events using rulers and clocks that
are moving relative to himself though, lots of real-world experiments
involve measuring-instruments that move relative to the people carrying out
the experiment.'

Do you agree with the above paragraph?

Jesse




 On Wednesday, February 26, 2014 10:45:51 PM UTC-5, jessem wrote:


 On Wed, Feb 26, 2014 at 8:52 PM, Edgar L. Owen edga...@att.net wrote:


 Can you agree to this at least?


 To repeat what I said in my second-to-last post:

 'If you continue to ask me Do you agree? type questions while ignoring
 the similar questions I ask you, I guess I'll have to take that as a sign
 of contempt, in which case as I said I won't be responding to further posts
 of yours. Any response is better than just completely ignoring questions,
 even if it's something like I find your questions ambiguous or you've
 asked too many questions and I don't have time for them all right now,
 please narrow it down to one per post.'

 If you decide to treat me with the same basic level of respect I have
 treated you, rather than making a show of asking me questions while you
 

Re: Block Universes

2014-02-27 Thread Edgar L. Owen
Jesse,

First the answer to your question at the end of your post.

Yes, of course I agree. Again that's just standard relativity theory. 
However as you point out by CONVENTION it means the observer's comoving 
inertial frame which is the way I was using it.



Now to your replies to my post beginning with your first paragraph.

Certainly there are equations that do what you say they do, but I don't see 
why what I say isn't correct based on that. Why do you claim it is 
impossible to just take proper acceleration and calculate what my age would 
have been if there was not any proper acceleration? An observer knows what 
his proper acceleration is, and he knows how much various accelerations are 
slowing his proper time relative to what it would be if those accelerations 
didn't happen. He has a frame independent measure of acceleration. He knows 
that particular acceleration will slow his proper time by 1/2 so he can 
define and calculate an 'inertial time' whose rate is 2x his proper rate.

You seem to think it would be necessary to MEASURE THIS FROM SOME FRAME for 
the concept to be true. It's not an observable measure, it's the 
CALCULATION of a useful variable. Therefore there is NO requirement that 
it's measurable in any frame because it's a frame independent concept, a 
calculation rather than an observable.

Therefore I don't see any reason to accept your criticism in this 
paragraph. If you disagree, which I'm sure you will, then explain why this 
concept of inertial time is not frame independent and valid. Perhaps a 
clear example would help?

Another way to approach this is do you deny that if we drop a coordinate 
grid on an area of EMPTY space that the coordinate clocks at the grid 
intersections all run at the same rate? And if not, why? 

And don't start making up other frames on me here. Just compare the proper 
times of those coordinate clocks. Do they all run at the same rate or not?

Edgar






On Thursday, February 27, 2014 11:56:08 AM UTC-5, jessem wrote:



 On Thu, Feb 27, 2014 at 9:25 AM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 I haven't answered those questions out of any disrespect or rudeness but 
 because I was working on a new explanation which I think does specifically 
 address and answer all of them which I present in this post. I will be 
 happy to answer any of your questions if you think they are still relevant 
 after reading this post which I think solves the 1:1 age correlation to 
 your satisfaction.


 That's the problem, you continually come up with new arguments and 
 explanations that you think resolve the questions I asked and therefore 
 mean you don't need to address them, but inevitably I disagree. Please just 
 respect my judgment about what's relevant TO ME, and answer the questions 
 that I ask ALONGSIDE any new arguments or explanations you might want to 
 supply. You say above I will be happy to answer any of your questions if 
 you think they are still relevant after reading this post, so I will hold 
 you to that by repeating a question I'd like you to answer at the end of 
 this post.

  



 If you find any of the terminology confusing please let me know what you 
 think it SHOULD be rather than just saying it's wrong.

 Twins A and B start at the same location in deep space. No acceleration, 
 no gravitation. Their ages are obviously the same, and their age clocks are 
 running at the same rate.

 They exchange flight plans and embark on their separate trips according to 
 those flight plans.

 Now the only effects that will alter the rates of their age clocks are 
 acceleration or gravitation. But each twin can continually measure the 
 amount of acceleration or gravitation he experiences with a scale.



 Let's consider just the issue of accelerations in flat SR spacetime for 
 now, since it's simpler. The problem with this statement is that although 
 it's true each twin can measure their proper acceleration, there is no 
 FRAME-INDEPENDENT equation in relativity for how a given acceleration 
 affects the rates of their age clocks, the only equations dealing with 
 clock rates and acceleration in SR deal with how changes in coordinate 
 velocity (determined by acceleration) affect the rate a clock is ticking 
 relative to coordinate time in some specific coordinate system.
  


 So each twin can always calculate how much his age has slowed relative to 
 what his age WOULD HAVE BEEN had he NOT experienced any gravitation or 
 acceleration. Let's call that his 'inertial age', the age he WOULD have 
 been had he NOT experienced any acceleration or gravitation.



 I see no way to define this in any frame-independent way. The only version 
 of this that relativity would allow you to calculate is what your age would 
 have been at a PARTICULAR COORDINATE TIME if you had remained inertial, and 
 you can compare that to what your age is at that SAME COORDINATE TIME given 
 your acceleration history. But this comparison obviously 

Re: Block Universes

2014-02-27 Thread Jesse Mazer
On Thu, Feb 27, 2014 at 2:38 PM, Edgar L. Owen edgaro...@att.net wrote:

 Jesse,

 First the answer to your question at the end of your post.

 Yes, of course I agree. Again that's just standard relativity theory.
 However as you point out by CONVENTION it means the observer's comoving
 inertial frame which is the way I was using it.


Thanks, it seemed like you might have been suggesting there was some
natural truth to calculations done in the comoving frame of two
obserervers at rest relative to each other, even though they could equally
well agree to calculate things from the perspective of a totally different
frame.


 Now to your replies to my post beginning with your first paragraph.

 Certainly there are equations that do what you say they do, but I don't
 see why what I say isn't correct based on that. Why do you claim it is
 impossible to just take proper acceleration and calculate what my age would
 have been if there was not any proper acceleration?


I don't claim it's impossible, just that it can only be done relative to a
particular frame. I can make statements like I am now 30, but in frame A,
if I hadn't accelerated I would now be 20 and I am now 30, but in frame
B, if I hadn't accelerated I would now be 25.



 An observer knows what his proper acceleration is, and he knows how much
 various accelerations are slowing his proper time relative to what it would
 be if those accelerations didn't happen.


Slowing his proper time only has meaning relative to a particular frame,
there is no frame-independent sense in which clocks slow down (or speed up)
due to acceleration in relativity.



 He has a frame independent measure of acceleration. He knows that
 particular acceleration will slow his proper time by 1/2 so he can define
 and calculate an 'inertial time' whose rate is 2x his proper rate.


Given the exact same proper acceleration, there may be one frame A where at
the end of the acceleration his clock has slowed by 1/2 (relative to the
time coordinate of that frame), and another frame B where it has slowed by
1/3, and even another frame where it has *sped up* by a factor of 10. Do
you disagree?



 You seem to think it would be necessary to MEASURE THIS FROM SOME FRAME
 for the concept to be true. It's not an observable measure, it's the
 CALCULATION of a useful variable. Therefore there is NO requirement that
 it's measurable in any frame because it's a frame independent concept, a
 calculation rather than an observable.


Calculations are always calculations of the values of particular numerical
quantities, like the rate a clock is ticking. So, what matters is whether
the quantity in question is frame-dependent (like velocity, or rate of
clock ticking) or frame-independent (like proper time at a specific event
on someone's worldine), there is nothing inherent in the notion of
calculations that make them frame-independent.

Also, *all* calculated quantities in relativity can also be
observables--it's straightforward to observe frame-independent quantities
like proper time (just look at the clock the observer carries), and
frame-dependent ones can also be observed if you have a physical grid of
rulers and coordinate clocks as I have described before (for example, to
find the rate a clock is ticking relative to a coordinate system, you
look at the time T1 it reads as it passes next to a coordinate clock that
reads t1, and the time T2 it reads as it passes next to another coordinate
clock that reads t2, and then you can just define the average rate over
that interval as [T2 - T1]/[t2 - t1], and if the difference between T2 and
T1 approaches 0 this approaches the *instantaneous* rate at T1).




 Therefore I don't see any reason to accept your criticism in this
 paragraph. If you disagree, which I'm sure you will, then explain why this
 concept of inertial time is not frame independent and valid. Perhaps a
 clear example would help?



If you disagree with my statement above that different frames can disagree
on the amount that a clock slowed down (or sped up) after a given proper
acceleration, I can give you a numerical example.




 Another way to approach this is do you deny that if we drop a coordinate
 grid on an area of EMPTY space that the coordinate clocks at the grid
 intersections all run at the same rate? And if not, why?


Are you talking about an inertial coordinate grid of rigid rulers, or an
arbitrary non-inertial coordinate grid where we can imagine different grid
points connected by rubbery rulers that can stretch and compress over time?
In the simpler case of an inertial grid, obviously all inertial coordinate
clocks tick at the same rate relative to any other inertial coordinate
system, though not necessarily relative to an arbitrary non-inertial
system. And the clocks of an arbitrary non-inertial coordinate system need
not tick at a constant rate relative to inertial systems.


 And don't start making up other frames on me here. Just compare the proper
 times of those 

Re: Block Universes

2014-02-27 Thread Edgar L. Owen
Jesse,

Remember we are talking ONLY about PROPER TIMES, or actual ages. These DO 
NOT HAVE any MEANING IN OTHER FRAMES than that of the actual frame of the 
observer in question. So your comments that an observer's age will be 
measured differently in other frames, while obviously true, is NOT the 
observer's PROPER AGE or PROPER TIME. Every observer has one and only one 
proper age, that is his proper age to himself, NOT to anyone else, not in 
any other frame.

That holds for all your comments about age effects of acceleration being 
different in different frames. Of course they can be but that is NOT PROPER 
ACTUAL AGE.

So I have to disregard all those comments because they don't apply to 
PROPER TIMES OR ACTUAL AGES. Proper time is ONLY one's reading of one's own 
clock, NOT one's own clock viewed from some other frame.

Correct?


Now a very basic question. Do you agree or disagree that all PROPER TIMES 
run at the same rate unless some effect causes them to run at different 
rates? Again this is NOT how clocks appear to run in any other frames but 
their OWN.

If you do not agree then please explain why not and please PROVE to me that 
PROPER TIMES do not run at the same rate unless there is some actual effect 
that causes them to run at different rates.

Edgar





On Thursday, February 27, 2014 3:07:41 PM UTC-5, jessem wrote:



 On Thu, Feb 27, 2014 at 2:38 PM, Edgar L. Owen edga...@att.netjavascript:
  wrote:

 Jesse,

 First the answer to your question at the end of your post.

 Yes, of course I agree. Again that's just standard relativity theory. 
 However as you point out by CONVENTION it means the observer's comoving 
 inertial frame which is the way I was using it.


 Thanks, it seemed like you might have been suggesting there was some 
 natural truth to calculations done in the comoving frame of two 
 obserervers at rest relative to each other, even though they could equally 
 well agree to calculate things from the perspective of a totally different 
 frame.


 Now to your replies to my post beginning with your first paragraph.

 Certainly there are equations that do what you say they do, but I don't 
 see why what I say isn't correct based on that. Why do you claim it is 
 impossible to just take proper acceleration and calculate what my age would 
 have been if there was not any proper acceleration?


 I don't claim it's impossible, just that it can only be done relative to a 
 particular frame. I can make statements like I am now 30, but in frame A, 
 if I hadn't accelerated I would now be 20 and I am now 30, but in frame 
 B, if I hadn't accelerated I would now be 25. 

  

 An observer knows what his proper acceleration is, and he knows how much 
 various accelerations are slowing his proper time relative to what it would 
 be if those accelerations didn't happen.


 Slowing his proper time only has meaning relative to a particular frame, 
 there is no frame-independent sense in which clocks slow down (or speed up) 
 due to acceleration in relativity.

  

 He has a frame independent measure of acceleration. He knows that 
 particular acceleration will slow his proper time by 1/2 so he can define 
 and calculate an 'inertial time' whose rate is 2x his proper rate.


 Given the exact same proper acceleration, there may be one frame A where 
 at the end of the acceleration his clock has slowed by 1/2 (relative to the 
 time coordinate of that frame), and another frame B where it has slowed by 
 1/3, and even another frame where it has *sped up* by a factor of 10. Do 
 you disagree? 



 You seem to think it would be necessary to MEASURE THIS FROM SOME FRAME 
 for the concept to be true. It's not an observable measure, it's the 
 CALCULATION of a useful variable. Therefore there is NO requirement that 
 it's measurable in any frame because it's a frame independent concept, a 
 calculation rather than an observable.


 Calculations are always calculations of the values of particular numerical 
 quantities, like the rate a clock is ticking. So, what matters is whether 
 the quantity in question is frame-dependent (like velocity, or rate of 
 clock ticking) or frame-independent (like proper time at a specific event 
 on someone's worldine), there is nothing inherent in the notion of 
 calculations that make them frame-independent. 

 Also, *all* calculated quantities in relativity can also be 
 observables--it's straightforward to observe frame-independent quantities 
 like proper time (just look at the clock the observer carries), and 
 frame-dependent ones can also be observed if you have a physical grid of 
 rulers and coordinate clocks as I have described before (for example, to 
 find the rate a clock is ticking relative to a coordinate system, you 
 look at the time T1 it reads as it passes next to a coordinate clock that 
 reads t1, and the time T2 it reads as it passes next to another coordinate 
 clock that reads t2, and then you can just define the average rate over 
 that 

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