On Tuesday, December 31, 2024 at 3:31:33 PM UTC-7 Jesse Mazer wrote:

On Tue, Dec 31, 2024 at 12:57 AM Alan Grayson <[email protected]> wrote:

On Monday, December 30, 2024 at 1:03:20 PM UTC-7 Jesse Mazer wrote:

On Sat, Dec 28, 2024 at 1:51 AM Alan Grayson <[email protected]> wrote:

On Friday, December 27, 2024 at 10:05:51 PM UTC-7 Jesse Mazer wrote:

On Friday, December 27, 2024, Alan Grayson <[email protected]> wrote:

On Friday, December 27, 2024 at 6:48:56 PM UTC-7 Jesse Mazer wrote:

On Fri, Dec 27, 2024 at 4:58 PM Alan Grayson <[email protected]> wrote:

On Friday, December 27, 2024 at 9:16:39 AM UTC-7 Jesse Mazer wrote:

On Friday, December 27, 2024, Alan Grayson <[email protected]> wrote:

On Thursday, December 26, 2024 at 9:39:41 PM UTC-7 Jesse Mazer wrote:

On Thursday, December 26, 2024, Alan Grayson <[email protected]> wrote:

On Thursday, December 26, 2024 at 2:56:04 PM UTC-7 Jesse Mazer wrote:

On Thursday, December 26, 2024, Alan Grayson <[email protected]> wrote:

On Thursday, December 26, 2024 at 3:26:41 AM UTC-7 Alan Grayson wrote:

On Thursday, December 26, 2024 at 12:12:43 AM UTC-7 Jesse Mazer wrote:

On Wednesday, December 25, 2024, Alan Grayson <[email protected]> wrote:

       On Wednesday, December 25, 2024 at 5:14:21 PM UTC-7 Jesse Mazer 
wrote:

On Wednesday, December 25, 2024, Alan Grayson <[email protected]> wrote:

*Why do refer to transformations that don't preserve time ordering? IIUC, 
such transformations only occur when assuming motion faster than light. *


No, that’s not correct. Motion faster than light would be required if there 
was a claim of causal influence between events with a spacelike separation; 
but there’s no such claim here; in both Brent’s example and mine, if we 
consider the event A of the back of the car passing the front of the garage 
and the event B of the front of the car reaching the back of the garage, 
there is a spacelike separation between those events, and neither event has 
a causal influence on the other.


*I'm asking a general question. Why do you refer to failure of time 
ordering? What was the point you thought you were making? AG*


Because as you previously agreed, the question of whether the car fits 
reduces to the question of whether the event A = back of car passes front 
of garage happens before, after, or simultaneously with the event B = front 
of car reaches back of garage. Since these events have a spacelike 
separation in both Brent’s and my numerical examples, in relativity 
different frames can disagree on their order, that’s the whole reason we 
say frames disagree on whether the car fits.


*As I recall, you were writing about the failure of TIME ordering, and this 
would mean violation of causality, not what we're discussing on this 
thread. AG * 


You either recall incorrectly or misunderstood at the time, but 
disagreement about the time ordering of two events A and B does NOT imply 
any violation of causality; it just implies the spacetime interval between 
A and B is spacelike, but normally this is combined with the assumption 
that there are no causal influences between events with a spacelike 
separation. 

Do you understand what the spacetime interval is? If I gave you the 
difference in time coordinates T = tB - tA for the two events along with 
the difference in position coordinates X = xB - xA, would you know how to 
calculate the spacetime interval and judge whether it is timelike, 
spacelike or lightlike? 

 


*But if so, you're not within the postulates of SR, which is what this 
discussion is about. So what point do you think you're making? AG*

*Re: paradox: Assume there's an observer located in the garage. This 
observer is in the garage frame. This observer sees the car easily fit in 
the garage. Imagine another observer riding in the car. This observer is in 
the car frame and observes being in the garage but never fitting in the 
garage. What are the observations when the two observers pass each other, 
in juxtaposed positions?*


I’ve asked this before, but by “see” do you mean in terms of when the light 
from different events reaches their eyes, or something more abstract like a 
computer animation they create of when events occur in their frame, once 
they have measured the time and position coordinates of all events using 
local readings on rulers and clocks at rest relative to themselves?


*Nothing more abstract. One observer sees the car sticking outside the back 
of garage, the other sees it inside, when both are juxtaposed. *


You didn’t quite answer my question—you are just talking about what they 
see with their eyes, right?


*I used the word "see". Is this not clear enough? AG*

 

Not entirely, since it’s routine in relativity problems to use words 
differently from everyday speech, for example in ordinary speech when you 
talk about “observing” some event we are usually talking about visual 
sight, but in relativity talking about what someone “observes” always 
refers to how things happen in the coordinates of their frame, not to 
visual sight. 

 

If so, there is no disagreement between observers passing through the same 
point in spacetime about whether the car fits in a visual sense.


*Really? So if the garage is 10' long in rest frame, *


Do you mean 10’ in the garage’s rest frame? As I said before, just using 
“rest frame” without specifying a particular object is unclear.


*I appreciate your thoroughness but here I just left out "its", as in "... 
10' long in its rest frame", and I think you should have easily inferred my 
meaning. AG *


Given that you had recently objected to my use of the phrases “car’s rest 
frame” and “garage’s rest frame” and hadn’t acknowledged my response about 
how this is a standard way of speaking in relativity, I didn’t think it was 
safe to assume that. It would help if you would acknowledge when something 
I’ve said has led you to revise a view, even on something minor like 
terminology, otherwise I don’t know when a given point needs to be 
re-litigated. The recent discussion about how we can talk about events that 
are spacelike separated without implying any faster than light causal 
influence is another example; do I need to keep arguing that or does the 
fact that you dropped that discussion mean you concede the point?


Could you please address my comment above so I know if we’re in 
disagreement on these points?


*I don't object to your terminology. As I stated, if I had included "its" 
in my statement, there would have been no ambiguity about terminology. And 
as far as I can recall, I never objected to the use of your quoted 
statements about rest frames. AG* 


You objected multiple times in the last few days to my terminology where 
"car's rest frame" refers to the frame where the car is at rest (i.e. it 
has position coordinates that don't change with time) and the garage is 
moving (so the garage is Lorentz-contracted in the car's rest frame), while 
"garage's rest frame" symmetrically refers to the frame where the garage is 
at rest and the car is moving (so the car is Lorentz-contracted in the 
garage's rest frame). For example in the post at 
https://groups.google.com/g/everything-list/c/vcrAzg4HSSc/m/XZrHB-IdAwAJ I 
said:

"In garage rest frame, garage has length 20 and car has length 25/1.25 = 
20. In the car rest frame, the garage has length 20/1.25 = 16 and the car 
has length 25.”

And you responded:

"OK, assuming car is moving, but I wouldn't call that "in the car rest 
frame" since you have garage length as contracted. AG"

Then at 
https://groups.google.com/g/everything-list/c/vcrAzg4HSSc/m/mFVsDGUtAwAJ 
you responded by imagining “the rest frame” referred to some imaginary 
initial conditions that were never part of the problem I described, 
conditions where both the car and garage were at rest relative to each 
other:

“IMO, the rest frame is defined as the initial conditions in this problem 
when the car isn't moving, and is longer than the garage. When the car is 
moving, we have been calling the other two frames, simply the car frame and 
the garage frame.”

Then at 
https://groups.google.com/g/everything-list/c/vcrAzg4HSSc/m/1AWAOHA4AwAJ 
you again objected to the standard terminology in which “car’s rest frame” 
just refers to the frame where the car is at rest in the sense of having a 
fixed position coordinate, even if it is moving relative to the garage:

“No one uses "rest frame" when describing the results in either frame when 
the car is moving. You introduced that terminology recently, claiming it is 
standard. AG”

Then just yesterday at 
https://groups.google.com/g/everything-list/c/vcrAzg4HSSc/m/O12FCXvmAwAJ 
you again objected to this standard terminology:

“What could be the meaning of "rest frame" associated with "garage"? I 
don't have a clue. Shall we consult Webster's Dictionary?”


*I was being sarcastic. Not to be taken at face value. AG *


The Webster’s dictionary comment was sarcastic, but ‘What could be the 
meaning of “rest frame” associated with “garage”?’ didn’t seem to be a 
sarcastic question, especially since it echoed your confusion in the other 
comments I quoted.


 


So it would be helpful to know if you're willing to accept that my use of 
"car's rest frame" and "garage's rest frame" is the standard way of talking 
among physicists, or if you still object. 


*Instead of haggling over this issue, and possibly taking some of my 
comments out of context, we agree that when using the LT from either frame, 
the car or garage length in that frame has not changed from its initial 
condition, 12' or 10', respectively.*


I don’t know what you mean by “its initial condition.” Do you just mean its 
length its own rest frame? Or do you think it’s essential to the problem 
that we imagine some initial condition where both are at rest relative to 
each other, and then the car is accelerated? If so I would definitely 
object to that, the term “car’s rest frame” has no such implications, it 
would have exactly the same meaning if we assumed the car and garage have 
had a fixed relative velocity for an infinite time prior to the car passing 
through the garage.


* At that point it was agreed that car cannot fit in garage because of 
length considerations. Consequently, following that agreement, I calculated 
using the LT, that the car fits or not -- fits in garage frame, doesn't fit 
in **car frame -- based solely on length considerations. **If the car can't 
fit from its frame when v = 0, it can't fit for any v > 0, since the garage 
gets even shorter. I think you and Brent believe it can't fit in car frame 
due to disagreement about simultaneity, whereas I use length contraction to 
reach the same conclusion. *


I didn’t use any word like “because” or talk about the best conceptual 
explanation, I just said that the question of whether the car fits in some 
frame is *equivalent* to the question of the order of the events A and B in 
that frame. It is of course also equivalent to the question of whether the 
length of the car is shorter, greater, or equal to the length of the garage 
in that frame. Equivalent here just means logical equivalence, ie the truth 
value of the statement “the car doesn’t fit in this frame” is guaranteed to 
be the same as the truth-value of “B happens before A in this frame” and 
*also* the same as the truth-value of “the car is longer than the garage in 
this frame”; it’s impossible in either relativity or classical physics for 
one of these statements to be true while another one is false, or vice 
versa. Do you agree they are equivalent in that sense?


Could you address my question here about whether you agree that, given the 
clarification that I am talking about logical equivalence in the sense I 
discussed above, the question of whether the car fits is completely 
equivalent to question of the order of the events A="back of car passes 
front of garage" and B="front of car reaches back of garage"?


*I apologize for being so dumb, but whereas I'm comfortable using relative 
lengths of car and garage to determine fitting or not, I don't really 
understand that the reversal of time order, of event B preceding event A, 
is equivalent to car not fitting in garage.*


 OK, but are you making an effort to understand? In general do you actually 
want to understand what relativity says about these matters, or do you just 
want to score a rhetorical "win" for your own arguments? If you're 
interested in understanding rather than winning then you can't just stick 
by whatever way of thinking is most comfortable for you, or most conducive 
to your argument.

*Concerning those videos, two which were reviewed on this MB, one by Brent 
and one by you, they falsely claim to show that from the car frame, the car 
really does fit in the garage.*


I watched the video and I never saw him make the false claim that the pole 
(which takes the place of a car in that video) fits in the garage in the 
pole's own frame. If you disagree, can you point to a time index in the 
video where he says this, or a time index in the first video where he says 
the car fits in the garage in the car's frame?

 

* This is what one expect to show if the disagreement of the frames is the 
cause of the paradox, but apparently it isn't, and the disagreement about 
simultaneity alone is sufficient to resolve the paradox. This is what I am 
trying now to understand. AG*


*And we agree it can fit from the pov of the garage frame, since the car's 
length contracts. So what are we arguing about is this; does the 
disagreement about fit constitute an objective fact and thus a paradox? AG*

 

 


*What could be the meaning of "rest frame" associated with "garage"? I 
don't have a clue. Shall we consult Webster's Dictionary? As for my 
numerical example, I suggest you do the arithmetic, and if you don't get my 
prediction, I will concede the argument. AG *


*Yeah, use 12' and 10' for the lengths of the car and garage respectively 
when at rest (which means no motion of car). Then using the LT determine 
how fast the car must be moving to contract the car's rest length to 
.000001' from the pov of the garage frame. Then place the car in the center 
of garage, and recognize how easily it fits (by any method of your choice). 
Now, from the pov of the car frame, and the speed of the car previously 
calculated, calculate the contracted length of the garage, and place the 
car at the center of the garage. Does the front of the car extend beyond 
the rear of the garage, whereas previously it did not? No need to worry 
about what "seeing" means in this comparison.*


It’s critical that you specify if by “see” you are talking about what light 
signals are reaching their eyes at that point, or if you are talking about 
the coordinates they assign to front and back of car and garage at 
simultaneous moments in their own frames; the answer will be completely 
different depending on what you mean. If you are just talking about visual 
seeing, I can do that, but just be aware that most of the usual textbook 
equations of relativity including length contraction are *not* intended to 
address visual appearances.

Jesse 


*Let's forget about "seeing" in these scenarios since I agree it 
unnecessarily complicates the analyses. I will go back to your post with my 
question marks and try to resolve as much as possible. However, I don't 
think we can resolve anything in these discussions, for this reasonaaaaa. I 
proposed a scenario where from the garage frame the car fits with ease, 
whereas from the car frame it fails to fit and in fact easily extends 
beyond the rear end of garage. I conjecture that your response will be that 
different frames give different measurements, so there's nothing 
particularly noteworthy about this situation, and it certainly doesn't 
amount to a paradox. This result concerning fitting or not can easily be 
concluded without any arithmetic. Is my conjecture about your response 
correct? AG*


Sure, if we are talking about local measurements in each frame rather than 
visual seeing, I see no paradox in the fact that they disagree on the time 
order of the spacelike separated events A=“back of car passes front of 
garage” and B=“front of car passes back of garage” and therefore disagree 
on fitting.


*In the example I posted, the frames disagree on fitting, and AFAICT 
there's nothing to suggest a disagreement on the time order of events. In 
fact, what you claim doesn't seem physically impossible in either frame. 
Can you show me EXACTLY how you reached this conclusion, without referring 
to one of your other posts? It seems that you pulled that conclusion out of 
the preverbial hat. AG*


You can easily just look at the times of events in either Brent’s numerical 
example or mine to see the two frames disagree on the order of the two 
events I keep bringing up, A=“back of car passes front of garage” and 
B=“front of car reaches back of garage”. In my example, A and B happen 
simultaneously at t = 0 in the garage frame, while in the car frame B 
happens at t’ = -15, which is before the time when A happens in the car 
frame at t’ = 0.

And isn’t it obvious that if some frame says that B happens before A, 
meaning the front of the car reaches the back of the garage before the back 
of the car has yet entered the front of the garage, then that’s equivalent 
to the statement that in that frame the car doesn’t fit, whereas in a frame 
where A happens before B or simultaneously with it, the car does fit in 
that frame?

This is one of the most basic aspects of analyzing the problem that we’ve 
talked about over and over, and you’ve previously agreed to, I don’t 
understand why there’s be any confusion here.


*Your memory is in error. I never agreed to that. *


Yes you did! See our discussion at 
https://groups.google.com/g/everything-list/c/gbOE5B-7a6g/m/B15IG50SAQAJ 
where I was responding to your previous comment at "I haven't thought about 
ordering", and I said the following:

"You haven't thought about it?? Disagreement about the ordering of these 
two specific events (due to differences in simultaneity) is what Brent and 
I have both been emphasizing as the fundamental resolution of the paradox, 
have you not even understood that this is central to what we are arguing, 
and considered in an open-minded way whether or not it makes sense?


*As I think I posted, I don't understand the argument that disagreement 
about simultaneity resolves the paradox. This is surely the standard 
alleged solution, but using the LT and length contraction, I seem to get a 
paradox if we assume disagreement about fitting is the cause of the 
paradox. You claim time-ordering shows the car can't fit. This is my 
conclusion using length contraction, whiich seems simpler. So, our 
disagreement of the resolution apparently has nothing to do with whether 
the car fits from its frame, since we're in agreement that it does not. AG *


No, I wasn’t talking about the best way to understand or explain why the 
car doesn’t fit, I was just talking about logical equivalence. But as I 
have said elsewhere, an analysis of relativity of simultaneity is needed 
conceptually if you want to answer the *separate* question “given that 
different frames disagree about whether the car fits, how can we avoid the 
conclusion that they must disagree in their predictions about local 
physical facts?” 


If you don't see why the ordering of these two events is considered 
equivalent to the question of fitting, consider a simpler classical 
scenario where everyone agrees about simultaneity and length. A car is 
passing through a covered bridge, and we are observing it in a side view 
with the car driving from left to right, so the front of the car begins to 
disappear from view under the bridge as soon as it passes the left end of 
the bridge, and begins to re-emerge into view as soon as it passes the 
right end of the bridge. Would you agree in *this* scenario, if the back of 
the car disappears from view on the left end before the front of the car 
emerges into view on the right end, that means for some time the car was 
fully hidden under the covered bridge, meaning it "fit" inside? And would 
you likewise agree that if the front of the car starts to emerge from view 
on the right end before the back of the car has disappeared from view on 
the left end (say it's a very short covered bridge and the car is a stretch 
limo), so there was never a time when the car was fully obscured from view 
by the covered bridge, that means the car did *not* fit inside?"


*I'm not sure. I have to think about this some more. Why can't we just 
stick to lengths? AG *


You could at least ask some questions about whatever is puzzling you rather 
than just avoiding the subject by switching to exclusive talk about length. 
Remember, this is a purely classical scenario, no tricky issues of length 
contraction or simultaneity. Classically, if we have an 18-foot long 
limousine driving through a covered bridge that's only 6 feet wide, and 
you're watching from the side with the limousine moving left to right, are 
you genuinely unsure about whether you'll see the front of the limousine 
poke out of the right side of the covered bridge BEFORE or AFTER the back 
of the limousine first disappears behind the left side of the covered 
bridge?

 

If the front didn't poke out from behind the right side of the covered 
bridge until AFTER the back disappeared behind the left side, that would 
mean there was some period of time where the 18-foot limousine was wholly 
obscured from view behind the 6-foot covered bridge, which doesn't make a 
lot of sense geometrically.


*I see front of car emerging from right side of bridge first, BEFORE back 
of car crosses entry of bridge on left side, so the car never completely 
fits. I can't account for your interpretation and I didn't think it 
worthwhile to argue about it. Mine seems simple enough and correct. AG*

*As for the videos, some of them CLAIM in their subject line, to provide a 
resolution of the paradox, but fail to do so. This initial claim is what I 
was referring to as false. And Brent posted the numbers the author 
calculated and IIUC they contradicted that the car could fit, even that's 
what was alleged. AG*

*Didn't Brent's plots establish the car doesn't fit from the pov of the car 
frame? If so, wasn't this the origin of the paradox? If so, I fail to see 
how this resolves the issue. It just seems to repeat the situation which 
caused the idea of a paradox to arise in the first place. TY, AG* 


Jesse

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