On Wednesday, January 29, 2025 at 12:24:33 AM UTC-7 Jesse Mazer wrote:

On Wed, Jan 29, 2025 at 1:24 AM Alan Grayson <agrays...@gmail.com> wrote:



On Tuesday, January 28, 2025 at 9:01:14 PM UTC-7 Jesse Mazer wrote:

On Tue, Jan 28, 2025 at 8:54 PM Alan Grayson <agrays...@gmail.com> wrote:

On Tuesday, January 28, 2025 at 2:56:32 PM UTC-7 Brent Meeker wrote:

On 1/28/2025 6:49 AM, Alan Grayson wrote:

I figured you'd jump on my word "separation". You have no idea what I mean? 
Of course, events with different coordinates are separated in a physical 
sense. Otherwise they'd have the SAME coordinates! But separated wrt 
spacetime events means no causal connections; whereas timelike events DO 
have causal connections. Of course, you know this, so please stop splitting 
hairs to make an argument. As for relative velocity, if you don't know what 
I mean, then you don't know what the v means in the gamma function. Again, 
stop splitting hairs. Oh, about GPS, I will look up this issue, but I was 
informed of it from a Ph'D in physics from Brent's Ph'D alma mater, 
University of Texas at Austin. It's surely NOT a distraction if it 
establishes that results in SR are physically real, not just appearances. AG


There's an unfortunate but common confusion.  The un-intuitive aspects of 
special relativity are physically real, but not it the sense that they happen 
to the moving object.  If SR predicts length contraction, is the object is 
really shorter?  (1) It's really shorter in the reference frame where it's 
moving.  (2) It's not shorter in it's own frame.  And (3) it's a different 
degree of shorter in other reference frames where it is moving with 
different velocities.  Just looking at (2) people assume that it means (1) 
and (3) are just appearances.  What's true is that 

*the contraction, relative to things in some reference frame, with respect 
to which it's moving, is real. *Brent


*It's a baffling result. The LT doesn't tell us what will be MEASURED in a 
moving target frame being observed from a rest frame wrt length contraction 
and time dilation, so the result is just an APPEARANCE from the pov of the 
rest frame; and yet, from the pov of GPS clocks, these effects are real and 
measureable. This was the conclusion I argued, which is why I referenced 
the GPS clocks. *


Brent's comment wasn't saying there was any disagreement between what 
coordinates the LT predicts for a given frame and what is really true (or 
really measured) in that frame, just like I wasn't saying that (see my last 
response above). You're really deluding yourself by rushing to read every 
explanation people give you as confirmation of your pre-existing fixed 
opinions.

Jesse


IMO you're deluding yourself in one important respect; your insistence that 
the results of the LT from the pov of some rest frame predicting length 
contraction in a frame moving wrt to it, can be measured in that moving 
frame;


This statement is hard to follow because you ignore the distinction I made 
between frames and objects--


*I can't help you if you refuse to use your imagination. A rod or any 
object moving wrt a fixed source frame using the LT, or an object in moving 
frame at rest in that frame when the LT is applied from a fixed source 
frame, will be predicted as contracted. Period. AG*
 

if we have some object whose length we want to talk about, and we know the 
coordinates of the worldlines of the front and back of the object in the 
first (source) frame and then use the LT to predict its coordinates (giving 
us its length) in the second (target) frame, you can't make any general 
statement about whether the LT will be "predicting length contraction" of 
the object until you know the velocity of the object itself in each frame. 
If the object has a higher velocity v_rt in the target frame than its 
velocity v_rs in the source frame, the LT will predict the object will be 
contracted in the target frame; on the other hand, if the object has a 
lower velocity v_rt in the target frame (including the case I analyzed 
where v_rt = 0) than its velocity v_rs in the source frame, the LT will 
predict the object is EXPANDED in the target frame, not contracted, 
compared to its length in the source frame. In the past you disagreed with 
this, do you still disagree or have you changed your mind? 

Please give a clear answer on this, telling me whether you now AGREE or 
DISAGREE that when the rod has v_rt in the target frame lower than its v_rs 
in the source frame, the LT predicts the rod's length in the target frame 
is expanded, not contracted. And if you disagree, please address the 
questions I asked in my last reply to you (the one before my reply to your 
comment on Brent's post).


*The target frame is moving wrt the source frame. Objects in the target 
frame are at rest within that frame, and contracted according to 
relativity. One can also consider a moving rod as the frame AND the object 
under consideration.  This is how to model and analyze a shortened trip to 
Andromeda. If you have a better way to model it, I am all ears. AG*

 

So we're both correct from different points of view, but you were mistaken 
to ignore my comments about GPS. Also, to be candid, I don't appreciate 
your comment that I am rushing to accept an opinion that confirms my 
pre-existing fixed opinions. You like to focus on coordinates, but the fact 
is you were mistaken in claiming the LT makes a measurable prediction of 
what a source frame predicts. It does in the GPS case, but not in the case 
of what a target frame predicts internally. AG 


You never addressed my response to you about the GPS in my post at 
https://groups.google.com/g/everything-list/c/ykkIYDAL3mTg/m/ximYgKzKDAAJ 
<https://groups.google.com/g/everything-list/c/ykkIYDL3mTg/m/ximYgKzKDAAJ> 
-- any coordinate system covering a non-infinitesimal region of curved 
spacetime is non-inertial, and the LT isn't relevant to non-inertial 
coordinate systems. 


*An object in free fall is in inertial motion, called a geodesic in GR. The 
LT is probably applicable for infinitesmal motion notwithstanding that this 
is occurring in curved spacetime. But I'm NOT an expert on how or why SR is 
used in GPS to make clock corrections. What I do know is that it IS used, 
that consequently the LT is likely applied in some way, and I gave this 
example just to show that whereas the LT does NOT give predictions 
concerning what is predicted for objects moving wrt a fixed frame, one 
cannot categorically claim that it never does. IOW, for inertial motion, 
the LT sometimes gives APPEARANCES, and sometimes gives REALITY. AG*
 

But looking into this a little more, it seems based on p. 2-3 of 
http://math.bme.hu/~matolcsi/gpsmegjelentejp.pdf that at some point in the 
GPS calculations they do use an approximation that treats the spacetime 
around the Earth as flat so an inertial coordinate system can be used, and 
then they add higher-order corrections to account for the fact that the 
spacetime is actually curved and this is relevant to gravitational time 
dilation. 

But even if there were no gravity and we were just trying to define a 
GPS-like system to adjust clocks with various states of motion so they were 
all synchronized in a single inertial frame (as in the 'Suppose for a 
moment there were no gravitational fields' comment in the second to last 
paragraph in 'the realization of coordinate time' section of the GPS paper 
at https://pmc.ncbi.nlm.nih.gov/articles/PMC5253894/#Sec4 ), say the frame 
where the center of the Earth is at rest, I still don't understand why you 
think this would indicate any conflict between what the LT predicts and 
what is measured--the whole point of a GPS system is that the ticking rate 
of the clocks is being artificially adjusted so it no longer matches the 
"proper time" of an un-adjusted clock following the same trajectory, but 
instead matches the coordinate time in some preferred coordinate system 
you've programmed the clocks to keep pace with. If you have a system of 
adjustments like this for clocks in flat spacetime where inertial frames 
can be used, then if you know the adjusted ticking rate of a clock in some 
source frame (along with the coordinates of its worldline in this frame), 
you can use the LT to correctly predict the adjusted ticking rate of that 
same clock in a different target frame.

Jesse

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