I'm literally crying having only you to read... why ????

Le mer. 1 janv. 2025, 01:55, Alan Grayson <[email protected]> a écrit :

>
>
> On Tuesday, December 31, 2024 at 6:44:17 PM UTC-7 Alan Grayson wrote:
>
> 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.
>
>
> *All I want is to make some rhetorical points. What else could possibly
> matter? And NO, I am definitely NOT making any effort to understand. Why
> should I? After all, I am just a troll and this is what trolls do. AG*
>
> *This problem arose as an apparent paradox because two frames give
> diametrically opposite conclusions in a particular situation. My result
> using length contraction showed the same opposite conclusions. So, in an
> effort to resolve the paradox, I consulted many sources, and it seems they
> all reached the same conclusion as I did, but through different routes.
> That's why Brent posted there's no objective result. Moreover, the videos
> do not prove, despite what some of them claim, that the car fits in the
> garage from the pov of the car frame. If the foregoing is correct, I don't
> believe these various path resolve the paradox. Rather, they're just
> re-stating it under different conditions. Correct me if I am wrong. AG *
>
>
> *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.
>
> Jesse
>
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