Twin Paradox (by acceleration)

In summary, the twin paradox states that if two twins start off at the same age and one travels near the speed of light while the other stays stationary, the traveling twin will age slower due to time dilation. However, this time dilation must have occurred during the acceleration of the traveling twin, as each twin would see the other moving at near the speed of light during any other time. This time dilation is a function of both acceleration and distance, and can be explained by the analogy of distance in 2D geometry. The standard twin paradox also depends on the spacetime path of the twins, with the inertial twin accumulating the most proper time. If the traveling twin is never inertial, the key factor becomes the path length and not the
  • #36
Demystifier said:
Now you will probably ask: But if I accelerate, then I accelerate with respect to what? In Newtonian mechanics it was not completely clear. For example, Mach thought that acceleration is defined with respect to (all) distant stars in the Universe. But in the relativity theory, this question can be answered: You accelerate with respect to the metric field (metric tensor).
Isn't this equivalent to Mach's principle, if the metric field is determined by distant masses?
 
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  • #37
But in the relativity theory, this question can be answered: You accelerate with respect to the metric field (metric tensor).
WHAT!?

Why haven't I been told this before!?

Thank you very much Demistyfier, I really really need to learn general relativity.
I am still a bit confused, (because I have not learned about Mach's principle or general theory of relativity.) For instance, another question I have is, why isn't the metric field considered an 'absolute reference frame'?
 
  • #38
Jonnyb42 said:
WHAT!?

Why haven't I been told this before!?

Thank you very much Demistyfier, I really really need to learn general relativity.
I am still a bit confused, (because I have not learned about Mach's principle or general theory of relativity.) For instance, another question I have is, why isn't the metric field considered an 'absolute reference frame'?
It's like an electromagnetic field, defined at every point in spacetime, but it doesn't have a rest frame (maybe Demystifier could clarify what it means to 'accelerate with respect to' something that has no rest frame?)
 
  • #39
Al68 said:
Isn't this equivalent to Mach's principle, if the metric field is determined by distant masses?
GR does not obey the Mach principle because the metric field is not determined ONLY by distant masses. Instead, when the matter is fixed, you still have a freedom to choose initial conditions for the metric field. In particular, even if there is no matter at all, there is still a metric field with respect to which acceleration is defined.
 
  • #40
Jonnyb42 said:
For instance, another question I have is, why isn't the metric field considered an 'absolute reference frame'?
Because the velocity is still relative. Only acceleration is absolute. In other words, you cannot talk about velocity of the metric field, but in a sense you can talk about acceleration of the metric field. This is related to the fact that metric field is not a first-rank tensor (i.e., a vector), but a second-rank tensor. This is just a rough, hopefully intuitive explanation, while a proper explanation requires more math.
 
  • #41
JesseM said:
It's like an electromagnetic field, defined at every point in spacetime, but it doesn't have a rest frame (maybe Demystifier could clarify what it means to 'accelerate with respect to' something that has no rest frame?)
Note that a photon moving with the velocity of light does have a rest frame, but that this frame is not a Lorentz frame. Instead, it is a light-cone frame.
Note also that the velocity of photon is related to the Poynting vector of the EM field. Finally, note that not all EM fields have a non-zero Poynting vectors.
 
  • #42
Demystifier said:
Note that a photon moving with the velocity of light does have a rest frame, but that this frame is not a Lorentz frame. Instead, it is a light-cone frame.
Note also that the velocity of photon is related to the Poynting vector of the EM field. Finally, note that not all EM fields have a non-zero Poynting vectors.
OK, but what about my question about how you define acceleration "relative to" a tensor field that has no rest frame of its own? I suppose by the equivalence principle, in the local neighborhood of any point in curved spacetime we can define locally inertial frames, so can we say that any worldline that passes through that point must have either zero or nonzero instantaneous acceleration relative to these local inertial frames?
 
  • #43
Demystifier said:
Al68 said:
Isn't this equivalent to Mach's principle, if the metric field is determined by distant masses?
GR does not obey the Mach principle because the metric field is not determined ONLY by distant masses. Instead, when the matter is fixed, you still have a freedom to choose initial conditions for the metric field. In particular, even if there is no matter at all, there is still a metric field with respect to which acceleration is defined.
Fair enough, but to my knowledge, Mach's Principle was never specific enough to say that GR doesn't "obey" it.

GR certainly seems very "Machian" to me, at least compared to Newtonian physics, even if it doesn't actually explain the source of inertia.
 
  • #44
kev said:
The slightly surpising result, if I have worked it out correctly (and I might not of, because I am a bit tired) is that A (who has a spent a year lazing around while B hurtles off at 0.99c relative to him) has aged less than B. It seems that the twin that ages the most, is the one that does the short final burst of acceleration to come to rest in the other twin's rest frame.
Mike_Fontenot said:
No, it's the opposite. The twin who does the accelerating, WHEN THEIR SEPARATION IS NON-ZERO, will be the younger, after they are again stationary with respect to one another.

Yep, your right. I made a typo in the final sentence. Thanks for picking it up and have now edited the original post. The second sentence obviously contradicts the sentence immediately preceding it. Knew I shouldn't have been posting stuff when I was tired. Good to see someone is paying attention :wink:
 
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  • #45
Al68 said:
Fair enough, but to my knowledge, Mach's Principle was never specific enough to say that GR doesn't "obey" it.

GR certainly seems very "Machian" to me, at least compared to Newtonian physics, even if it doesn't actually explain the source of inertia.
Fair enough. But there are even theories of gravity which are more Machian than GR. The Brans-Dicke theory for example.
 
  • #46
JesseM said:
OK, but what about my question about how you define acceleration "relative to" a tensor field that has no rest frame of its own? I suppose by the equivalence principle, in the local neighborhood of any point in curved spacetime we can define locally inertial frames, so can we say that any worldline that passes through that point must have either zero or nonzero instantaneous acceleration relative to these local inertial frames?
Yes.
 
  • #47
This is related to the fact that metric field is not a first-rank tensor (i.e., a vector), but a second-rank tensor. This is just a rough, hopefully intuitive explanation, while a proper explanation requires more math.
Daaang. Just guessing, but would an acceleration be relative in a third-rank tensor??
I am ashamed to not know what tensors are and what these things mean. I want to know enough math. I have to finish up some projects for the end of the year (I am a senior right now.) and when summer starts I am going to study vector calculus and general relativity like mad.

Thanks for all the help.
This stuff is crazy.
 
  • #48
Jonnyb42 said:
I am ashamed to not know what tensors are and what these things mean. I want to know enough math. I have to finish up some projects for the end of the year (I am a senior right now.) and when summer starts I am going to study vector calculus and general relativity like mad.

Thanks for all the help.
This stuff is crazy.
There are many excellent textbooks on this stuff, but if you need a recommendation, I suggest
http://xxx.lanl.gov/abs/gr-qc/9712019
 
  • #49
Thank you very much, I will definitely read that, whenever I do!

I have another question that comes to my mind,

Is the theory of General Relativity being expanded on/updated, or has it been the same since Einstein published it?
I wonder the same with quantum mechanics.
 
  • #50
GR hasn't really been modified since 1915, but people are still working on ways to find new interesting solutions to the main equation of the theory. That equation (Einstein's equation) describes the relationship between how things are distributed in the universe and how things move. It's so hard to solve that it took 48 years to find the solution that describes a universe that's completely empty except for a single rotating star.

QM hasn't really changed since the early 1930's, but a lot of work has been done on theories of matter and interactions in the framework of QM (mostly quantum field theories), and people are still working on them.

The big thing right now is of course to figure out how these two fit together.
 
  • #51
Mike_Fontenot said:
and who happened to be momentarily adjacent at the instant they are both born,

Does this make sense as they are moving relative to each other? I don't think you can say this and then continue to calculate with accelerating frames assuming they started with a certain simultaneity.
 
  • #52
Aaron_Shaw said:
Does this make sense as they are moving relative to each other? I don't think you can say this and then continue to calculate with accelerating frames assuming they started with a certain simultaneity.
Why would it make a difference? Any physical situation can be analyzed using any frame you like, a frame is just a coordinate system for analyzing events in spacetime. And all frames agree about local events, so if it's true in one frame that their mothers were passing right next to each other at the moment each baby was born, then this is true in all frames.
 

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