2014/1/4 Edgar L. Owen <[email protected]>

> Jason,
>
> If you don't agree with my theory of the Present moment, then what is your
> theory of this present moment we all experience our existence and all our
> actions within?
>
> It clearly is not a clock time simultaneity since Pam and Sam shake hands
> and compare watches in the same present moment and their clock times are
> not simultaneous.
>
> When they do they are in the same reference frame... that's all there is
to it... the rest is crackpotery.

Quentin


> This question is the key to the whole issue. Be interested to hear your
> answer...
>
> Edgar
>
> On Friday, January 3, 2014 11:51:53 AM UTC-5, Jason wrote:
>
>>
>>
>>
>> On Fri, Jan 3, 2014 at 11:10 AM, Edgar L. Owen <[email protected]> wrote:
>>
>> Jason,
>>
>> Thanks for your several posts and charts. You really made me think and I
>> like that!
>>
>>
>> Thanks, I am glad to hear it. :-)
>>
>>
>> I'm combining my responses to your multiple recent posts here.
>>
>> First though there are two ways to analyze it, GR acceleration, as
>> opposed to SR world lines, is the most useful because it makes the
>> following argument re present time easier to understand.
>>
>>
>> In my example, acceleration effects can account for no more than 4
>> minutes worth of age difference, since they spend no more than 4 minutes
>> accelerating.  How do we explain the other 3 years, 355 days, 23 hours and
>> 56 minutes that are missing from Pam's memory?
>>
>>
>>
>> Imagine a new experiment in which Pam is completely still relative to Sam
>> but somewhere way off in the universe and in a gravitational field of
>> exactly the same strength. In this case both Pam's and Sam's clock times
>> run at exactly the same rates and both agree to this. Therefore it is clear
>> they inhabit the exact same present moment even by your arguments, and
>> their identical clock times correlate to this.
>>
>> Now assume Pam's gravitational field increases to the point where her
>> clock time runs half as fast as Sam's. Again there is no relative motion so
>> again both agree that Pam's clock time is running half as fast as Sam's.
>> And again both exist in the exact same present moment, it's just that Sam's
>> clock time is running twice as fast through that common present moment.
>> Again clock time correlates with present moment time...
>>
>>
>> I think we should resolve the apparent problems P-time has with SR before
>> trying to tackle GR...
>>
>>
>> This gravitational time slowing is a GR, not SR effect, and GR effects
>> are absolute in the sense that they are permanent real effects that all
>> observers agree upon. They must be distinguished from SR effects which make
>> the situation more difficult to understand in terms of a present moment.
>>
>>
>> You may be right that P-time has no difficulties with GR, but it seems to
>> have some with SR so let us focus on solving that.
>>
>>
>> An acceleration equivalent to the gravitational field would produce the
>> exact same GR effect, but also introduces an SR relative velocity effect.
>>
>> Now consider an pure SR effect in which Pam and Sam are traveling past
>> each other at relativistic speeds but there is no acceleration. Velocity is
>> relative, as opposed to acceleration which is absolute, therefore both
>> observers think the other is moving relative to them, and both views are
>> equally true. Now because of this relativity of velocity both observers see
>> the clock of the other observer slow and by equal amounts. But the
>> absolutely crucial thing to understand here is that this SR form of time
>> dilation is not permanent and absolute like GR time dilation is. It
>> vanishes as soon as the relative motion stops,
>>
>>
>> That is not true, the the effects of dilation in SR remain as well. Let's
>> say James was born on a space ship at Proxima Cenauri travelling at 80% c
>> toward Earth. It takes 5 years to get to Earth at this speed, but when we
>> see baby James on board as he whizzes by he is only 3 years old.  If the
>> ship stops (or not), James is still 3 years old. GR never was a factor in
>> James's reduced age.
>>
>>
>> whereas GR time differences are absolute and persist even after the
>> acceleration stops.
>>
>> This is why the SR versus GR model is more useful in understanding what
>> is going on particularly with respect to the common present moment.
>>
>>
>> SR and GR are not two ways of looking at the same phenomenon, but two
>> ways of explaining two different phenomena.
>>
>>
>>
>> So during relative motion between Pam and Sam there most certainly is a
>> common present moment, but trying to figure out what clock times of Pam and
>> Sam correspond to that present moment leads to a contradiction (as you
>> quite rightly pointed out with your diagrams) because Pam and Sam see clock
>> time differently and do not agree on it. They did agree on their GR
>> relativistic time differences and thus knowing which of their clock times
>> corresponded to the same present moment was easy. With SR, equal and
>> opposite, time dilation it is impossible to correlate both observers' clock
>> times to the same present moment. Nevertheless that's just an artifact of
>> SR clock time which doesn't falsify a common present moment. A common
>> present moment exists, it just isn't correlated with clock times the same
>> way by both observers.
>>
>>
>> Gabriel offered a clear example that I think falsifies the notion of a
>> single consistent present moment, and his point has not yet been adequately
>> addressed.
>>
>>
>>
>> All the nice chart examples you took the time to produce demonstrate
>> this. They are trying to assign an agreed upon clock time to the common
>> present moment time during SR relative velocities and thus they correctly
>> lead to the contradiction you pointed out.
>>
>> However once you understand how this works
>>
>>
>> Do you currently understand how this works or are you also still trying
>> to figure it out?
>>
>>
>> you understand that fact doesn't falsify a common present moment as you
>> implied.
>>
>>
>> Why doesn't it? I am not seeing it or you haven't explained it clearly
>> enough for me to get it.
>>
>>
>> Now consider the twins from the original example. In this case there is
>> both lots of relative velocity SR effects between both twins, and there is
>> the absolute GR acceleration effect on Pam only.
>>
>> Now the SR effects persist only during relative motion and when the twins
>> meet up again that leaves ONLY the GR acceleration effect which is the only
>> cause of the twins' clock time difference.
>>
>>
>> If Pam were under acceleration for just a few minutes it could not
>> explain an age difference of years.  If you put Pam under the gravity of a
>> black hole for 4 minutes, she would not age much during those 4 minutes,
>> and so when you took the black hole away you would find her 4 minutes
>> younger.  In the experiment I described, the acceleration, which you
>> compare to gravity, only lasts a few minutes.  It is the time dilation of
>> special relativity that accumulates over the years, and remains to explain
>> the bulk of their age difference.
>>
>>
>> All SR relative velocity effects must vanish when the relative velocities
>> cease. Otherwise we would have Pam and Sam meeting up again with each
>> claiming the other's clock time was going slower than theirs. That is
>> impossible.
>>
>>
>> It is possible when you consider the geometry of the situation, as
>> Brent's nice charts further clarify. (What software did you use to make
>> them Brent?)
>>
>>
>>  At rest in the same present moment all observers must be able to agree
>> on their clock time differences. Both agree Pam's clock time passed more
>> slowly than Sam's and both agree as to the amount, based ONLY on GR
>> (acceleration) effects.
>>
>>
>> Not true.
>>
>>
>> Assume again the twins passing each other at a constant (no acceleration)
>> velocity. Both see the other's time passing slower than theirs and thus
>> both see each other at an earlier clock time date than themselves. This is
>> contradictory
>>
>>
>> It is not contradictory, it is because their paths are at an angle to
>> each other through space time. If both of our paths are at 22.5 degrees
>> toward each other, either of us can consistently say "the other is at a 45
>> degree angle toward me." This is not inconsistency, only relativity.
>>
>>
>> and cannot last when they meet. It is the acceleration that brings the
>> relative velocities to zero that produces the only absolute persistent time
>> effect and when, and only when, that happens will the twins agree as to
>> their time differences, as always in a shared universal present moment.
>>
>>
>> In my "James example", there is no acceleration on James but he ages only
>> 3 years in his 5 year journey.
>>
>>
>> This is why is is possible to correlated clock times to present moment
>> time for GR acceleration time dilation, but NOT for SR relative velocity
>> time dilation.
>>
>> Hope this is clear. It may be a little difficult...
>>
>>
>>
>> I don't think we've yet addressed the core issues between SR and P-time.
>>  Also, you have not said what use P-time has beyond SR. What can it explain
>> that SR cannot? In other words, when would it make a prediction that
>> differs from SR?
>>
>> Jason
>>
>>
>>
>>
>> On Thursday, January 2, 2014 9:52:54 PM UTC-5, Jason wrote:
>>
>>
>>
>>
>> On Thu, Jan 2, 2014 at 9:31 PM, LizR <[email protected]> wrote:
>>
>> Jason,
>>
>> You may be missing the fact that the acceleration of the space traveller
>> is what causes the twin paradox.
>>
>>
>> I would say it is not so much the acceleration that explains the paradox,
>> but the fact that no matter how you rotate the paths, you always see a kink
>> in the path Pam takes.  So even if we start in Pam's reference frame where
>> she is still, she has to stop (putting her back in the reference frame
>> where Sam is 5 (not 1.8), then accelerate to 0.8 c back toward Earth, which
>> she will see as length contracted to 2.4 ly again, and she will experience
>> as taking 3 years, but in this frame, of heading back toward Earth at 0.8
>> c, Sam is not 5, but 7, so when she gets there after 3 years, Sam is (as
>> she expects) 10 years old.
>>
>> It isn't the acceleration which causes her age to suddenly change, but
>> rather, her changing frames of reference (present moments), that causes her
>> perspective of Sam to radically change, depending on her velocity.
>>
>>
>> As Edgar pointed out, time dilation is mutual, but only while velocities
>> are constant.
>>
>>
>> Their relative velocity in relation to each other, and therefore their
>> relative time dilations and length contractions, are always the same.
>>
>>
>> Your diagram demonstrated that the straight line parts of Pam's movement
>> could be mapped either way onto Sam's (just tilt the diagram. But you can't
>> may the entire trajectory onto Earth time by tilting the diagram.
>>
>>
>> I'm not sure what you mean by this..
>>
>>
>>
>> Apologies if I'm teaching my gradnmother to suck eggs.
>>
>>
>> No worries. Let me know if my example or explanation still does not make
>> sense. :-)
>>
>> Jason
>>
>>
>>
>>
>> On 3 January 2014 15:25, Jason Resch <[email protected]> wrote:
>>
>>
>>
>>
>> On Thu, Jan 2, 2014 at 8:57 PM, Edgar L. Owen <[email protected]> wrote:
>>
>> Jason,
>>
>> An excellent question. First of all let's stick with the actual example
>> of only Sam and Pam. Now how do you know all this stuff about who is doing
>> what when?
>>
>>
>> I calculate it from the parameters of the experiment as I described it.
>> The different answers depend on different reference frames, which you can
>> consider as straight lines dividing the past and future (but at different
>> angles depending on one's velocity through space).
>>
>> [image: Inline image 1]
>>
>> If you consider the gold and purple stars as two different events, the
>> person moving to the right sees the present as all events on the blue line,
>> and so they see the purple star happen before the yellow star, and vice
>> versa for the observer moving to the left, whose present is represented by
>> the red line. They see the yellow star come before the purple star.
>>
>>
>> How are you measuring it to know it's true?
>>
>>
>> 4 light years away, at 80% the speed of light.  It is no different than
>> figuring out how long it takes to travel 4 miles at 0.8 miles per year.
>> However, when travelling at these speeds, you have to contend with length
>> contraction and time dilation (which are two aspects of the same phenomenon
>> seen from two different perspectives).
>>
>> See: http://faraday.physics.utoronto.ca/PVB/Harrison/SpecRel
>> /Flash/LengthContract.html for a good explanation.
>>
>>
>> And again the important point to understand is that you MUST disregard SR
>> relative velocity effects which are illusory and non-permanent and vanish
>> when the relative velocities cease when they meet again.
>>
>>
>> You cannot disregard them. Otherwise you cannot explain why Pam is 6 when
>> she meets with Sam at 10.
>>
>>
>>  SR effects are not 'real' in the sense of being absolute. They are
>> transient and relative and equal and opposite for both observers. Both see
>> the other's time slow but that is just measurements, their time is not
>> actually slowing in any absolute permanent sense. By that I mean they are
>> illusions of measurement that exist only during relative motion. So they
>> are not relevant when trying to analyze what is happening in the present
>> moment.
>>
>>
>> They aren't illusions, from each one's own reference frame, the other is
>> going more slowly through time.
>>
>>
>>
>> GR acceleration affects on the other hand are real and absolute and
>> experienced the same by both observers as the slowing of only the
>> accelerating twin's clock relative to the non-accelerating twin's clock.
>>
>>
>> Relativity explains clock desynchronization. GR only comes into play when
>> gravity is concerned. Pam would still be 6 and Sam 10, even if they
>> accelerated instantly, or if Pam was already in motion when they were both
>> born.
>>
>>
>>
>> I think when temporary SR effects are eliminated this problem is resolved
>> and your question is answered...
>>
>>
>> It's the SR effects that explain the age differences, and Pam doesn't age
>> 4 years when she decelerates.
>>
>> Jason
>>
>>
>>
>> On Thursday, January 2, 2014 8:39:08 PM UTC-5, Jason wrote:
>>
>>
>>
>>
>> On Thu, Jan 2, 2014 at 8:07 PM, Edgar L. Owen <[email protected]> wrote:
>>
>> Jason,
>>
>> That's very simple P-time allows us to explain how there is a present
>> moment in which we experience our mutual existence, are able to converse
>> together, shake hands, and compare our (different) clock times.
>>
>> If there weren't such a common present moment distinct from our different
>> clock times we could do none of those things because we would be in
>> different moments of existence. We wouldn't even inhabit the same reality.
>>
>> Obviously that's not a function of being in the same clock time, because
>> it happens when we are in different clock times as well....
>>
>>
>> I think it does lead to a problem.  Pam and Sam start at the same time,
>> they are both zero and at Earth. They kiss each other good bye and Pam goes
>> off into space. The present moment advances and both Pam and Sam experience
>> something, they are now slightly older and both doing and experiencing
>> something at this time.
>>
>> A little time later, they are both slightly older, and they are both
>> experiencing something. and so on, and this keeps happening, each of them
>> experiences one moment after the other. Now, eventually, the event happens
>> where Pam gets to her destination, Pam is now 3.
>>
>> You agreed in an earlier e-mail that Sam is definitely doing something in
>> this common present P-time when Pam arrives.
>>
>> Then a little time later, both are slightly older, and both are
>> experiencing something. Then Sam turns 2 years old. A little time later,
>> they are both slightly older, and they are both experiencing something. and
>> so on, and this keeps happening, each of them experiences one moment after
>> the other.
>>
>> Finally, Pam arrives back on Earth, Sam is 10 and Pam is 6. They shake
>> hands and hug.
>>
>> Notice though that from one P-time to the next, and so on, continuously,
>> in one P-time Pam was at her destination, and Sam was definitely doing
>> something, and he was definitely less than 2 years old, because in a later
>> P-time Sam had his 2nd birthday at the same time Pam was already on her way
>> back to Earth.
>>
>> Yet, in an equally valid perspective (according to relativity) Sam's 2nd
>> birthday happens before Pam reaches her destination. So if there is a
>> single P-time, how can the event, Sam's 2nd birthday, happen when Pam is on
>> her way back AND happen before Pam reaches her destination.  If every
>> P-time is ordered and sequential, this simply isn't possible.  You have to
>> accept that there is more than one consistent way to order the succession
>> of present moments, which means there is no common present moment everyone
>> shares.
>>
>> You are right that without "some principle X" we wouldn't inhabit the
>> same reality, but relativity shows that "some principle X" is not, and
>> cannot be a global, shared, agreed upon succession of present moments.  The
>> "some principle X" is instead, a four-dimensional existence, space-time,
>> and consistent presents are just "slices" through this space time. If you
>> envision it in this way, you can perfectly account for all the consistent
>> views and orderings either Sam, Pam, or Bob might have about which events
>> happen when, and where, and in what order.
>>
>> Jason
>>
>>
>>
>> On Thursday, January 2, 2014 6:05:36 PM UTC-5, Jason wrote:
>>
>>
>>
>>
>> On Thu, Jan 2, 2014 at 5:56 PM, Edgar L. Owen <[email protected]> wrote:
>>
>> Jason,
>>
>> I said I don't know because SR doesn't know. What's wrong with that? It's
>> consistent with SR.
>>
>>
>> Nothing is wrong with that position, I just thought P-time might offer an
>> answer to this problem which exists in SR.
>>
>>
>>
>> I don't know WHAT Sam is doing at any particular moment in the shared
>> present moment, but I know he exists and is doing something. What's wrong
>> with that? If I had a mathematical way to determine that I'd certainly let
>> you know but as far as I know there isn't any. We just have to accept the
>> fact that everything isn't mathematical. Consciousness and the present
>> moment are examples. Clocks don't measure P-time. There is no P-time clock
>> that reads P-time. We know we are in the same present moment P-time not but
>> having synchronized clocks but by shaking hands and comparing clocks, and
>> by just living our lives and communicating like we always did whether our
>> clocks are the same or not.
>>
>> There is no clock that displays P-time. However everything is logical,
>> and I've given the logical reasoning...
>>
>>
>> What does P-time predict or allow us to explain that special relativity
>> does not or cannot?
>>
>> Thanks for your answers.
>>
>> Jason
>>
>>
>>
>> On Thursday, January 2, 2014 4:30:37 PM UTC-5, Jason wrote:
>>
>>
>>
>>
>> On Thu, Jan 2, 2014 at 4:17 PM, Edgar L. Owen <[email protected]> wrote:
>>
>> Liz,
>>
>> We'll let Jason judge whether I answered him or not.
>>
>>
>> You did answer, but your answer is that you did not know (you said it
>> what was whatever relativity predicts, but relativity also has no answer
>> without a defined reference frame).
>>
>> However according to P-time, Sam must be doing *something *at the exact
>> moment Pam arrives
>>
>>  ...
>
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-- 
All those moments will be lost in time, like tears in rain. (Roy
Batty/Rutger Hauer)

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