Revisiting the Flaws of the Light Clock in Special and General Relativity

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The discussion critiques the use of the light clock thought experiment in explaining time dilation in special relativity (SR) and its application to the Twin Paradox. It argues that acceleration plays a crucial role in resolving the paradox, as the twins do not remain in identical inertial frames due to one twin's acceleration. The conversation highlights that while SR can handle acceleration, the light clock's functionality is compromised under significant acceleration, leading to bending of the light beam. Additionally, it emphasizes that the proper time experienced by each twin can be calculated based on their unique paths through spacetime, illustrating that the traveling twin will always have aged less upon reunion. Ultimately, the resolution of the Twin Paradox requires a careful consideration of both SR and general relativity (GR) principles.
  • #121


JesseM said:
it plays a conceptual role in understanding why the inertial twin is always the one who ages more than the one who turns around).
Indeed, that is why it very important in STR education to stress that fact!
 
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  • #122


Passionflower said:
Sorry but this is just absurd, you cannot ignore acceleration, great or small, in the twin experiment. Without acceleration there is no absolute time dilation.

The proper time of the traveling twin can be calculated using

d \tau=\frac{T_c}{\gamma}+\frac{c}{a} \, \, asinh(a T_a / c)

Where T_c and Ta are total cruise and acceleration times, then when a is very large and Ta is necessarily brief because the terminal velocity v is reached very quickly, the second term goes to zero and this is why some textbooks assume instantaneous acceleration and the error due to ignoring the the time dilation during the acceleration phase is negligible. The equation can not be reversed to consider the point of view of the accelerating twin, because it is only valid for an inertial observer.
 
  • #123


kev said:
I was talking about a different scenario where the acceleration phase was much more extreme and took place in seconds.

I know, I pointed out to you that doing so is incorrect.
Not only that your math was incorrect but your physics was unrealistic. Calculate the acceleration that woulg get your rocket to your 0.8c in 1s . What do you get?



With very extreme acceleration with the acceleration phase period tending to zero, the time dilation due to acceleration becomes negligable.


You can't get high speeds in short time (see the exercise above)



The greater the acceleration is, the more you can ignore it.

Err, this one is in the category "not even wrong".
 
  • #124


kev said:
The proper time of the traveling twin can be calculated using

d \tau=\frac{T_c}{\gamma}+\frac{c}{a} \, \, asinh(a T_a / c)

Where T_c and Ta are total cruise and acceleration times, then when a is very large and Ta is necessarily brief because the terminal velocity v is reached very quickly, the second term goes to zero [/color]

No, it doesn't. Do the exercise I gave you and you'll find how false it is.
As a simple alternative, use a=10g (a huge number) and evaluate the second term. What did you get?




The equation can not be reversed to consider the point of view of the accelerating twin, because it is only valid for an inertial observer.

This is false as well. There are papers on this subject. Try to get your facts straight.
 
  • #125


Passionflower said:
Indeed, that is why it very important in STR education to stress that fact!
If you're talking about the conceptual explanation for why one twin ages less than the other, of course. But from the context of kev's comments it was clear he was just saying the acceleration phase didn't always need to be considered in actual calculations of elapsed proper time. Also, when you originally objected to "acceleration is not relevant" type arguments in post #89, it followed on the heels of a discussion I was having with starthaus where we were talking about the clock hypothesis, and there it is important to emphasize the reverse, that acceleration is indeed completely irrelevant if you want to know the instantaneous rate of a clock at a single instant, the rate is solely a function of its instantaneous velocity.
 
  • #126


starthaus said:
I know, I pointed out to you that doing so is incorrect.
Not only that your math was incorrect but your physics was unrealistic. Calculate the acceleration that woulg get your rocket to your 0.8c in 1s . What do you get?
Virtually all textbook calculations involve simplifications, and instantaneous accelerations (which imply infinite proper acceleration) are routinely assumed in textbooks on SR. Anyway this sort of simplification would be a reasonable approximation if the acceleration phase only lasted a few days or weeks while the inertial legs lasted for years, which might be realistic for an interstellar journey.
starthaus said:
The equation can not be reversed to consider the point of view of the accelerating twin, because it is only valid for an inertial observer.
This is false as well. There are papers on this subject. Try to get your facts straight.
I assume kev meant that the equation you posted wouldn't accurately calculate elapsed proper time if we were using the time coordinate of a non-inertial frame, which is correct.
 
  • #127


JesseM said:
the instantaneous rate of a clock at a single instant, the rate is solely a function of its instantaneous velocity.
Velocity with respect to what?

If your answer is with the prior instant, than it is the acceleration between the two instants that changed the rate! So what causes clock rates to change? Acceleration!

If the answer is different I am happy to await your further explanation.
 
  • #128


JesseM said:
I was having with starthaus where we were talking about the clock hypothesis, and there it is important to emphasize the reverse, that acceleration is indeed completely irrelevant if you want to know the instantaneous rate of a clock at a single instant, the rate is solely a function of its instantaneous velocity.

No one is disputing the "clock hypothesis". What I and passionflower are disputing is the incorrect statements made by kev.
 
  • #129


JesseM said:
Virtually all textbook calculations involve simplifications, and instantaneous accelerations (which imply infinite proper acceleration) are routinely assumed in textbooks on SR. Anyway this sort of simplification would be a reasonable approximation if the acceleration phase only lasted a few days or weeks while the inertial legs lasted for years, which might be realistic for an interstellar journey.


It would be good if you stopped defending kev's hacks for a while and you let him answer,. By stepping in for him every time you preclude him from learning.

I assume kev meant that the equation you posted wouldn't accurately calculate elapsed proper time if we were using the time coordinate of a non-inertial frame, which is correct.

This is not what he claimed.
 
  • #130


Passionflower said:
Velocity with respect to what?
An inertial coordinate system.
Passionflower said:
If your answer is with the prior instant
How could you talk about a "velocity" with respect to an "instant"? I'm guessing you meant to ask "rate of a clock with respect to what"? If so, the answer would again be relative to the time coordinate of an inertial frame (i.e. d\tau /dt). The clock hypothesis says that this only depends on the instantaneous velocity in that frame (it's always true that d\tau /dt = \sqrt{1 - v^2/c^2}), it doesn't depend on instantaneous acceleration or instantaneous position or anything else.
 
  • #131


JesseM said:
Virtually all textbook calculations involve simplifications, and instantaneous accelerations (which imply infinite proper acceleration) are routinely assumed in textbooks on SR. Anyway this sort of simplification would be a reasonable approximation if the acceleration phase only lasted a few days or weeks while the inertial legs lasted for years, which might be realistic for an interstellar journey.
starthaus said:
It would be good if you stopped defending kev's hacks for a while and you let him answer,. By stepping in for him every time you preclude him from learning.
Well, perhaps I object to your silly arguments because you use a lot of the same type of silly arguments on me, like how the irrelevant practical concerns you raise about realistic accelerations here resemble the irrelevant practical concerns about the size of real gaps in train tracks in the train-on-a-bridge thread. If you cracked open a real physics textbook once in a while instead of thinking you can learn everything about physics from from wikipedia, you might see that it's universal to include all sorts of simplifications in order to illustrate the basic physical concepts involved.

Irrelevant practical concerns aside, can you point to a single error in math or physics kev has made in this discussion?
starthaus said:
I assume kev meant that the equation you posted wouldn't accurately calculate elapsed proper time if we were using the time coordinate of a non-inertial frame, which is correct.
This is not what he claimed.
It isn't? What do you think he meant by "the point of view of the accelerating twin", if not a non-inertial rest frame for the accelerating twin?
 
  • #132


JesseM said:
An inertial coordinate system.
A change in velocity in an inertial coordinate system is equivalent with acceleration. Do you actually agree with me that a change in velocity in an inertial coordinate system causes a change in clock rate?
 
  • #133


Passionflower said:
A change in velocity in an inertial coordinate system is equivalent with acceleration. Do you actually agree with me that a change in velocity in an inertial coordinate system causes a change in clock rate?
Sure, why wouldn't I? The clock hypothesis says the instantaneous clock rate depends on the instantaneous velocity (so the instantaneous acceleration is irrelevant), which means if you're considering some extended interval of time where the clock is accelerating, the instantaneous velocity will be different at the beginning of the interval than the end, so the clock rate will be different too.
 
  • #134


JesseM said:
Well, perhaps I object to your silly arguments because you use a lot of the same type of silly arguments on me,

Perhaps this is because the two of you share the same misconceptions and , occasionally, the same errors in computations.

like how the irrelevant practical concerns you raise about realistic accelerations here resemble the irrelevant practical concerns about the size of real gaps in train tracks in the train-on-a-bridge thread.

...and the same penchant for dragging out past discussions where we disagreed.. This shows a severe smallness of character.

If you cracked open a real physics textbook once in a while instead of thinking you can learn everything about physics from from wikipedia, you might see that it's universal to include all sorts of simplifications in order to illustrate the basic physical concepts involved.

I happen to have a lot of books and I have cited them repeatedly, so your remark is both insulting and unwarranted. I have cited Rindler repeatedly on GR. My favorite book that I cite from is Moller precisely because he doesn't resort to any of the hacks that you and kev seem to favor.
Irrelevant practical concerns aside, can you point to a single error in math or physics kev has made in this discussion?

Read the thread, I pointed them out as he made them.
It isn't? What do you think he meant by "the point of view of the accelerating twin", if not a non-inertial rest frame for the accelerating twin?

It means that the calculation , in kev's incorrect opinion, cannot be made from the perspective of the accelerated twin. This is false.
 
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  • #135


JesseM said:
Sure, why wouldn't I? The clock hypothesis says the instantaneous clock rate depends on the instantaneous velocity (so the instantaneous acceleration is irrelevant), which means if you're considering some extended interval of time where the clock is accelerating, the instantaneous velocity will be different at the beginning of the interval than the end, so the clock rate will be different too.

...meaning that the elapsed proper time is a function of proper acceleration, as demonstrated by the formula I've posted. To make matters even more interesting, when one does the calculations from the perspective of the accelerating twin, the elapsed time definitely depends on acceleration. There is an excellent paper by H.Nikolic (who happens to be the excellent physics forums science advisor called Demystifier) on this subject on this subject. There is another one by Minguzzi and one by Iorio, I suggest that you read them, they would go a long way in correcting your misconceptions about the acceleration role on the elapsed proper time. Here, start with the Nikolic one. I am attaching it such that you don't continue to claim that I do my learning from wiki.
 

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  • #136


JesseM said:
Sure, why wouldn't I?
First of all I do not know why you constantly raise the clock hypothesis, as far as I see nobody is contesting this here.

Ok, good, so let me ask you this: Would you then agree that \gamma in this case directly depends on the rate and duration of the acceleration? And if so, do you readily see that since \gamma is a factor in the formula to calculate the absolute time dilation that effectively the rate and duration of acceleration is a factor, not the only factor, but nevertheless a factor, of the absolute time dilation?
 
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  • #137


starthaus said:
Perhaps this is because the two of you share the same misconceptions and , occasionally, the same errors in computations.
Point to any "misconceptions" or "errors" I have made. The only reason for the initial difference between your equation and mind (and kev's) is that we made different physical assumptions, I assumed the only acceleration was at the turnaround while you assumed (or copied your equation from a wikipedia page which assumed) an initial and final acceleration as well. If you think I have made any physical or mathematical errors aside given my physical assumptions, please point them out instead of just making vague accusations.
starthaus said:
...and the same penchant for dragging out past discussions where we disagreed.. This shows a severe smallness of character.
I just like to point out how you use the same irritating tactics in thread after thread.
starthaus said:
I happen to have a lot of books and I have cited them repeatedly, so your remark is both insulting and unwarranted. I have cited Rindler repeatedly on GR.
And do you think that's a book that avoids simplifying assumptions, of the kind you call "hacks"?
starthaus said:
My favorite book that I cite from is Moller precisely because he doesn't resort to any of the hacks that you and kev favor.
I don't know which book you're referring to, what's the title?
starthaus said:
Read the thread, I pointed them out as he made them.
I only saw you object on the basis that he made different physical assumptions than you, or that he used "hacks" (simplifications of the type that are routinely used in textbook discussions), or that you interpreted an English statement by him in a silly uncharitable way (like the one below). Again, show me a single clear error in his actual calculations.
starthaus said:
It means that the calculation , in kev's incorrect opinion, cannot be made from the perspective of the accelerated twin. This is false.
No, he didn't say a calculation of elapsed time couldn't be made, he just said you couldn't use the same equation ('The equation can not be reversed') to calculate the elapsed time from the point of view of the accelerated twin, where I presume by "point of view" he meant a non-inertial frame (especially since he went on to say that the equation can't be reversed 'because it is only valid for an inertial observer').
 
  • #138


JesseM said:
And do you think that's a book that avoids simplifying assumptions, of the kind you call "hacks"?

Most of the time.

I don't know which book you're referring to, what's the title?

C.Moller "The Theory of Relativity"
I only saw you object on the basis that he made different physical assumptions than you, or that he used "hacks" (simplifications of the type that are routinely used in textbook discussions), or that you interpreted an English statement by him in a silly uncharitable way (like the one below). Again, show me a single clear error in his actual calculations.

Look thru the thread, there are plenty. You can look for the "Err,no".
No, he didn't say a calculation of elapsed time couldn't be made, he just said you couldn't use the same equation ('The equation can not be reversed') to calculate the elapsed time from the point of view of the accelerated twin, where I presume by "point of view" he meant a non-inertial frame (especially since he went on to say that the equation can't be reversed 'because it is only valid for an inertial observer').

You tend to "presume" a lot.
 
  • #139


Passionflower said:
First of all I do not know why you constantly raise the clock hypothesis, as far as I see nobody is contesting this here.
I didn't say anyone was contesting it. But starthaus brought it up in post #80, and I was just making the point in the next few posts after that that it could be misleading to both bring up the clock hypothesis and at the same time make statements like the one that the elapsed time will "depend on the acceleration a". See my summary of the point I was making in post #92
Passionflower said:
Ok, good, so let me ask you this: Would you then agree that \gamma in this case directly depends on the rate and duration of the acceleration?
Gamma in what case? Gamma at any given instant of course is just a function of the velocity at that instant, so presumably you mean "depends on" in some other way, like that the velocity at a given instant itself depends on the clock's history of past accelerations (in that sense one could even say that gamma for a man in a rocket 'depends on' his decision 20 years earlier to enter the space academy and become an astronaut)
Passionflower said:
And if so, do you readily see that since \gamma is a factor in the formula to calculate the absolute time dilation that effectively the rate and duration of acceleration is a factor, not the only factor, but nevertheless a factor, of the absolute time dilation?
What does "absolute time dilation" mean? Are you talking about elapsed proper time rather than instantaneous clock rates? And by "factor", do you just mean some sort of causal factor, or do you mean something more specific like that we must include a variable representing acceleration in our calculations?
 
  • #140


If a formula is wrong it should be called out without fear of personal retribution, if it is called incorrectly wrong it should be called out as well again without fear of personal retribution.

Could we please get back on track and leave personal remarks out?
 
  • #141


JesseM said:
Gamma at any given instant of course is just a function of the velocity at that instant, so presumably you mean "depends on" in some other way, like that the velocity at a given instant itself depends on the clock's history of past accelerations (in that sense one could even say that gamma for a man in a rocket 'depends on' his decision 20 years earlier to enter the space academy and become an astronaut)
If a person undergoes constant proper acceleration in an inertial frame of reference his gamma increases. You in all honesty do not see any connection of the increase in gamma with acceleration?

Does the formula:

\Delta \gamma = \Delta xa_p

Mean anything to you?

Another interesting relation between gamma and acceleration is:

\gamma = (a_pa_c)^{1/3}

Where ap is proper acceleration and ac is coordinate acceleration.
 
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  • #142


starthaus said:
Most of the time.
So for example, would you complain about the lack of realism in the scenario of a man running towards a barn at 0.866c in the barn-pole paradox on p. 63? Is a rocket that takes a very brief time to accelerate from relativistic velocity in one direction to a relativistic velocity in the opposite direction significantly more unrealistic than a man running towards a barn at 0.866c?
starthaus said:
C.Moller "The Theory of Relativity"
Conveniently this book is available online in pdf form. Looking at the section where he discusses what he calls the "clock paradox", note that on p. 260 of the book (p. 278 of the pdf file), he considers the limit as the acceleration goes to infinity and "the velocity v is attained nearly instantaneously", and derives some equations for this case. He again talks more about infinite acceleration on pp. 261-262 (279-280 of the pdf). I suppose you would lecture Moller that this is a pointless exercise, since "realistically" no ship could withstand such great accelerations?
starthaus said:
Look thru the thread, there are plenty. You can look for the "Err,no".
I looked back over all the posts from p. 6 on (starting with post #81), the only "err, no"'s you wrote in response to actual equations or quantitative statements kev made were when kev posted your equation and said it was wrong, but he thought it was wrong because he misunderstood the scenario you were considering (which you never spelled out), not realizing you were supposing an initial and final acceleration as well as a turnaround. So, looks like no actual physical/mathematical errors, just a misunderstanding of what scenario was being analyzed. And I note you also didn't respond to my request to back up your claim that I had made errors.
JesseM said:
No, he didn't say a calculation of elapsed time couldn't be made, he just said you couldn't use the same equation ('The equation can not be reversed') to calculate the elapsed time from the point of view of the accelerated twin, where I presume by "point of view" he meant a non-inertial frame (especially since he went on to say that the equation can't be reversed 'because it is only valid for an inertial observer').
starthaus said:
You tend to "presume" a lot.
So you weren't "presuming" when you interpreted him to be saying "the calculation ... cannot be made from the perspective of the accelerated twin"? Do you have some infallible mind-reading powers I don't know about? If not, hopefully now you can see that you were jumping to conclusions, and that my alternate interpretation above is consistent with the words he used. But perhaps kev himself can settle the matter and tell us which interpretation is closer to what he meant.
 
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  • #143


Passionflower said:
If a person undergoes constant proper acceleration in an inertial frame of reference his gamma increases. You in all honesty do not see any connection of the increase in gamma with acceleration?
You didn't say anything about "increase in gamma" or any other change in gamma with time, you just said "gamma in this case [which I took to mean the value of gamma at some instant] directly depends on the rate and duration of the acceleration". Your reading of my statements is really pretty uncharitable if you think I don't know perfectly well that a continuous acceleration will produce an increase in speed over time which will produce an increase in gamma over time. I think I was pretty clear on the fact that I was talking about the value of gamma at any particular moment, which is just a function of the velocity at that moment and doesn't depend on acceleration or past history (i.e. two clocks that have the same instantaneous velocity at some time also, I'm sure you'd agree, have the same value for gamma and the same instantaneous rate of ticking at that time, even if their histories are different and they are accelerating differently)
Passionflower said:
Does the formula:

\Delta \gamma = \Delta xa_p

Mean anything to you?
I haven't seen that one before, no. If a rocket is undergoing constant proper acceleration in the +x direction, and it started at x=0 at time t=0 when its velocity was also zero, then one of the http://math.ucr.edu/home/baez/physics/Relativity/SR/rocket.html says that its position at time t will be:

x = (c2/a) (sqrt[1 + (at/c)2] - 1) = (c2/a)*sqrt[1 + (at/c)2] - (c2/a)

And also

gamma = sqrt[1 + (at/c)2]

So, it doesn't seem to me that your equation is correct, at least not if we are considering the change in x and gamma from t=0 to some later time. It would rather be true in this case that:

\Delta \gamma = (a/c^2) * (\Delta x + (c^2 / a))

But even this equation might not continue to be true if we considered the change in gamma and x between two times where the first time wasn't t=0 when the rocket had an initial velocity of 0.
Passionflower said:
Another interesting relation between gamma and acceleration is:

\gamma = (a_pa_c)^{1/3}

Where ap is proper acceleration and ac is coordinate acceleration.
Hmm, the coordinate acceleration at time t would be the derivative with respect to t of the coordinate velocity, which is given by v = at * (1 + (at/c)2)-1/2. By the product rule, the derivative of this is equal to:

a * (1 + (at/c)2)-1/2 + at * d/dt (1 + (at/c)2)-1/2

And by the chain rule, d/dt (1 + (at/c)2)-1/2 = (-1/2)*(1 + (at/c)2)-3/2 * 2(a/c)2t = -t*(a/c)2*(1 + (at/c)2)-3/2

So plugging that back in, the coordinate acceleration looks to be:

a*(1 + (at/c)2)-1/2 - a*t2*(a/c)2*(1 + (at/c)2)-3/2

= a*(1 + (at/c)2)-1/2*[1 - (at/c)2*(1 + (at/c)2)-1]

= a*(1 + (at/c)2)-1/2*[(1 + (at/c)2) - (at/c)2]/(1 + (at/c)2)

= a*(1 + (at/c)2)-1/2/(1 + (at/c)2)

= a*(1 + (at/c)2)-3/2

So to get back gamma I think you would have to take the coordinate acceleration, divide by the proper acceleration, and then put the result to the -1/3 power, i.e.

\gamma (t) = (a_c (t) / a_p)^{-1/3}

Note that this equation would only hold under the specialized conditions of constant proper acceleration and a velocity of 0 at t=0, though. Two clocks with the same coordinate acceleration and proper acceleration at a given instant might have different values for gamma if they hadn't both had the same constant proper acceleration since t=0 and/or hadn't started from a velocity of 0 at t=0.
 
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  • #144


starthaus said:
C.Moller "The Theory of Relativity"

The book of that title and author that I have, dated 1953, although very good, treats the basics of SR pretty much the same as most of the other texts, and I have at least 25 of them to compare it with. One little complaint I have about it is that it is one of the few texts that claims that the twin paradox cannot be resolved within SR. Perhaps that is due to the era in which the book was written, but if this is the only text a beginner read, although unlikely in the present day, he or she would be misled in this respect.

Matheinste.
 
  • #145


JesseM said:
And I note you also didn't respond to my request to back up your claim that I had made errors.

Sure I did, read post 135. If, after reading the paper, you will continue to maintain that the elapsed time differential is not dependent on acceleration, I will provide you with more papers published in peer reviewed journals that contradict your misconception. Read the paper by Nikolic first, he's one of the best science advisors in this forum (next to DrGreg).
 
  • #146


JesseM said:
So to get back gamma I think you would have to take the coordinate acceleration, divide by the proper acceleration, and then put the result to the -1/3 power, i.e.

\gamma (t) = (a_c (t) / a_p)^{-1/3}
Yes you are correct, I missed the division operator in the latex.
 
  • #147


JesseM said:
I looked back over all the posts from p. 6 on (starting with post #81), the only "err, no"'s you wrote in response to actual equations or quantitative statements kev made were when kev posted your equation and said it was wrong, but he thought it was wrong because he misunderstood the scenario you were considering (which you never spelled out), not realizing you were supposing an initial and final acceleration as well as a turnaround. So, looks like no actual physical/mathematical errors, just a misunderstanding of what scenario was being analyzed.

This is not true, look again at posts 97 (last entry) and 124.
 
  • #148


JesseM said:
Conveniently this book is available online in pdf form. Looking at the section where he discusses what he calls the "clock paradox", note that on p. 260 of the book (p. 278 of the pdf file), he considers the limit as the acceleration goes to infinity and "the velocity v is attained nearly instantaneously", and derives some equations for this case. He again talks more about infinite acceleration on pp. 261-262 (279-280 of the pdf). I suppose you would lecture Moller that this is a pointless exercise, since "realistically" no ship could withstand such great accelerations?

Conveniently, you left out the fact that Moller, before taking the limit, calculates the exact formula of elapsed proper time:

\tau'_2=\frac{c}{g} sinh^{-1}(\frac{g \Delta T}{c}) (eq 158)

where g represents ... acceleration. So, Moller doesn't cut any corners, he derived the exact formula. Selective quoting makes for very bad science, or no science at all.
I have no objection when a true scientist derives an exact formula only to take it to the limit afterwards. I have very strong objections when someone uses the truncated formula as a starting point. This is why I disagree with you and kev.
 
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  • #149


matheinste said:
One little complaint I have about it is that it is one of the few texts that claims that the twin paradox cannot be resolved within SR.

I looked on page 260 and he uses the hyperbolic motion treatment, consistent with SR.He doesn't claim that the paradox can be treated using GR only I like his book very much, he's a model of rigor.
 
  • #150


starthaus said:
I looked on page 260 and he uses the hyperbolic motion treatment, consistent with SR.He doesn't claim that the paradox can be treated using GR only I like his book very much, he's a model of rigor.

Look at page 49. It is not a simple "we cannot" statement so perhaps I have misinterpreted it. What do you think of it?

Matheinste.
 

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