Absolute motion's point of reference

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Discussion Overview

The discussion centers on the concept of absolute motion and reference frames in the context of special relativity. Participants explore the implications of acceleration, the nature of rest, and how different observers perceive motion and forces in various coordinate systems.

Discussion Character

  • Debate/contested
  • Conceptual clarification
  • Exploratory
  • Mathematical reasoning

Main Points Raised

  • Some participants assert that acceleration is an absolute motion, while others clarify that proper acceleration is Lorentz invariant but does not equate to absolute motion.
  • It is suggested that an observer can consider themselves at rest depending on the chosen spacetime coordinate system, with non-inertial observers having multiple possible coordinate systems.
  • Questions arise regarding the implications of acceleration on the laws of physics, particularly whether an accelerating observer can throw a ball and have it return to them.
  • Some participants propose that an observer who accelerates might claim to be at rest, but they acknowledge that this is not an inertial frame and that standard equations of special relativity may not apply.
  • There is a discussion about how to define rest and motion, particularly in scenarios where multiple observers are involved, leading to questions about the validity of claiming one observer is at rest while others are in motion.
  • Concerns are raised about the applicability of physical laws in non-inertial frames, with references to Galileo's ship and the effects of gravity.
  • Participants explore hypothetical scenarios involving multiple observers (A, B, and C) to illustrate the complexities of defining rest and motion in different frames.

Areas of Agreement / Disagreement

Participants express differing views on the nature of absolute motion, the definition of rest, and the implications of acceleration. There is no consensus on these issues, and the discussion remains unresolved.

Contextual Notes

Limitations include the dependence on the definitions of rest and motion, the complexity of non-inertial frames, and unresolved questions about the application of physical laws in various scenarios.

yoelhalb
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According to special relativity acceleration is an absolute motion, so according to what is it moving?
 
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Its velocity is changing relative to all inertial frames (frames where light always has a coordinate speed of c and the equations expressing the laws of physics take a certain special form), although different frames disagree on the value of the velocity at any given instant on the object's worldline.
 
yoelhalb said:
According to special relativity acceleration is an absolute motion
Better state: According to relativity, the magnitude of proper acceleration is Lorentz invariant. That doesn't mean the same as saying acceleration is absolute motion.
 
My question is what does he think? what is by him considered rest and according to what is he moving?
 
yoelhalb said:
My question is what does he think? what is by him considered rest and according to what is he moving?
That depends on what spacetime coordinate system he chooses to use--there is no physical reason that any given observer must use one coordinate system or another, although the usual convention is that each observer uses a coordinate where his coordinate position doesn't change with coordinate time (a coordinate system where he is 'at rest'). For a non-inertial observer there would be many different possible non-inertial coordinate systems where this could be true, which would have different judgments about the velocities of distant objects. And while his own coordinate acceleration would be zero in such a coordinate system, that wouldn't change the fact that he feels G-forces, which would be explained in terms of some sort of "pseudo-gravitational force" in this system (similar to a fictitious force in Newtonian physics), see the equivalence principle analysis from the twin paradox FAQ for details on this.
 
So in other words one who accelerates might claim that he is at rest
 
But if this is true then why does not all physics laws hold true for him?
For example if he throws a ball will it fall right back to him?
 
yoelhalb said:
So in other words one who accelerates might claim that he is at rest
Yes, but he would know the coordinate system where he remains at rest is not an inertial frame, so the usual equations of SR such as the time dilation equation won't apply in this frame (though at any single instant on his worldline there will be some inertial frame where he is instantaneously at rest).
 
Do you have a good source that explains special relativity in such a level of detail?
 
  • #10
Until someone, anyone, accelerates, they can consider themselves to be at rest. When they accelerate for some period of time, they end up with an absolute velocity with respect to their initial rest state before they started to accelerate. The answer to your question is: the absolute motion after acceleration is according to the rest state before acceleration.
 
  • #11
so if he was never at rest?
 
  • #12
Anyone who is not accelerating can consider himself to be at rest. That was the brilliance of Einstein which nobody else was able to consider.
 
  • #13
If he is accelerating and was never to rest according to what is he accelerating?
 
  • #14
JesseM said:
That depends on what spacetime coordinate system he chooses to use--there is no physical reason that any given observer must use one coordinate system or another, although the usual convention is that each observer uses a coordinate where his coordinate position doesn't change with coordinate time (a coordinate system where he is 'at rest'). For a non-inertial observer there would be many different possible non-inertial coordinate systems where this could be true, which would have different judgments about the velocities of distant objects. And while his own coordinate acceleration would be zero in such a coordinate system, that wouldn't change the fact that he feels G-forces, which would be explained in terms of some sort of "pseudo-gravitational force" in this system (similar to a fictitious force in Newtonian physics), see the equivalence principle analysis from the twin paradox FAQ for details on this.

If so then why does Galileo's ship which is clearly on Earth and feels gravity, how can all physics law's apply to him?
 
  • #15
The question that I was answering for you was concerning special relativity. Nobody has been accelerating forever. But if you want to pretend, then you can pick a time that you can call his rest state and consider my answer to apply after that time.
 
  • #16
yoelhalb said:
If so then why does Galileo's ship which is clearly on Earth and feels gravity, how can all physics law's apply to him?
You are now asking about General Relativity instead of your original question which was limited to Special Relativity and which I tried to answer for you in a way I thought you could and would understand. Do you understand my answer to your original question?
 
  • #17
Here is a similar question.
Imagine A,B,C are at one position, then A and B starts to move away with uniform motion.
C moves with acceleration starting with a lower speed and eventually catching up with A.
How can we claim that A was at rest?
 
  • #18
yoelhalb said:
Do you have a good source that explains special relativity in such a level of detail?
I don't think any of my introductory SR texts goes into much detail on the issue of accelerating frames, but I often find one can find interesting-looking textbooks by entering keywords into google books...with keywords "relativity" + "accelerating" + "frame" I found http://books.google.com/books?id=LyVxtGv1RwEC&lpg=PA83&dq=relativity%20accelerating%20frame&pg=PA81#v=onepage&q=relativity%20accelerating%20frame&f=false , Dynamics and Relativity, and Explorations in mathematical physics: the concepts behind an elegant language (which has a very nice discussion of the derivation of Rindler coordinates, the most common type of accelerated frame, on p. 240), for example.
 
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  • #19
No.
A person has to move according to something but now there is n o point of reference.
 
  • #20
yoelhalb said:
Here is a similar question.
Imagine A,B,C are at one position, then A and B starts to move away with uniform motion.
C moves with acceleration starting with a lower speed and eventually catching up with A.
How can we claim that A was at rest?
Just by analyzing things from the perspective of the inertial frame where A was at rest as B and C moved away. If you choose to use a non-inertial frame where C is at rest, then in this frame A was not at rest.
 
  • #21
JesseM said:
Just by analyzing things from the perspective of the inertial frame where A was at rest as B and C moved away. If you choose to use a non-inertial frame where C is at rest, then in this frame A was not at rest.

Let's put it differently.
the same example again but n ow together with all of them also started D in the direction of B with the same acceleration of C in A's direction will he catch up with B?
 
  • #22
JesseM said:
Just by analyzing things from the perspective of the inertial frame where A was at rest as B and C moved away. If you choose to use a non-inertial frame where C is at rest, then in this frame A was not at rest.
So how will C ever meet him if he moved away?
 
  • #23
yoelhalb said:
Here is a similar question.
Imagine A,B,C are at one position, then A and B starts to move away with uniform motion.
C moves with acceleration starting with a lower speed and eventually catching up with A.
How can we claim that A was at rest?

Your "similar question" can be interpreted many ways. I will try to interpret it the way I think you meant which is:

A, B and C are at rest with respect to each other. A and B accelerate together for awhile and then stop accelerating so that they are moving at a constant speed with respect to their initial rest condition and to C's current rest condition. Then C accelerates at a lower acceleration and as he approaches A (why is B in this?) he decelerates in such a way that he ends up at the same speed and in the same location as A. Now A, B and C are moving together with respect to their initial, at rest, condition.

If you didn't mean it this way, you will have to explain what you did mean in more detail.

Also, I don't know why you feel the need to ask "How can we claim that A was at rest?" As I said earlier, anyone who is not accelerating can claim to be at rest. This was the brilliance of Einstein. Don't feel bad if it doesn't seem clear to you, it didn't seem clear to anyone else except Einstein when he said it.
 
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  • #24
yoelhalb said:
So how will C ever meet him if he moved away?
Because in a non-inertial frame of C, A would move away but then move back towards C.
 
  • #25
yoelhalb said:
Let's put it differently.
the same example again but n ow together with all of them also started D in the direction of B with the same acceleration of C in A's direction will he catch up with B?
Are you assuming B and A both go in opposite directions at the same speed in the frame where all four were originally at rest next to each other? Then C accelerates in the direction of A, D accelerates in the same way but in the direction of B? In this case, yes, B should catch up with B and C should catch up with A.
 
  • #26
yoelhalb said:
Let's put it differently.
the same example again but n ow together with all of them also started D in the direction of B with the same acceleration of C in A's direction will he catch up with B?

I'm afraid you're going to have to be much more precise in order to get a reasonable answer. You have now introduced D doing something like what B was doing and I don't even know why you had B in the first example.

You also stated in your first example that you were asking a similar question but I don't see what it is similar to or why you think it is similar. Please provide more details.
 
  • #27
JesseM said:
Because in a non-inertial frame of C, A would move away but then move back towards C.

Let m e explain the whole question again.
ABC are at the same position one next to the other.
Now A and B are moving apart with a constant speed of 100 mph (imagine ships in the water).
Also according to C in the same second A and B took apart, he started accelrating with a speed of 1 mph in the direction of A's travel.
(actually the question starts here will he be a mile close to A or to B?).
A initially sees this as C moving away from him with 99 mph.
The next hour C speeds up with another 1 mph to a total of 2 mph, and so on till he meets A.
According to A how can this happen? C initially moved away form him and never moved back.
(As you can see there are actually 2 questions)
 
  • #28
Sorry the second question can be answered because he needs to accelrate with a speed higher then 100 mph.
But what about the first question?
 
  • #29
yoelhalb said:
Let m e explain the whole question again.
ABC are at the same position one next to the other.
Now A and B are moving apart with a constant speed of 100 mph (imagine ships in the water).
Do you mean each is moving at 100 mph in the other's rest frame, or do you mean that in the frame where both were originally at rest (the frame of the ocean) they are both moving at 100 mph in opposite directions? It doesn't really matter since it will only affect the specific numbers and not the overall analysis, so I'll assume the second one for now...
yoelhalb said:
Also according to C in the same second A and B took apart, he started accelrating with a speed of 1 mph in the direction of A's travel.
(actually the question starts here will he be a mile close to A or to B?).
If C accelerates in the direction of A, he'll be closer to A than to B, although the distance from A to C is still increasing rather than decreasing (it's just not as increasing as fast as the distance from B to C)
yoelhalb said:
A initially sees this as C moving away from him with 99 mph.
The next hour C speeds up with another 1 mph to a total of 2 mph, and so on till he meets A.
According to A how can this happen? C initially moved away form him and never moved back.
(As you can see there are actually 2 questions)
If C keeps accelerating by 1 mph every hour in the ocean frame, then eventually C's speed will exceed A's speed of 100 mph in this frame. At that point, in A's inertial rest frame, C should start moving back towards A.
 
  • #30
JesseM said:
If C accelerates in the direction of A, he'll be closer to A than to B, although the distance from A to C is still increasing rather than decreasing (it's just not as increasing as fast as the distance from B to C)
Again ABC are togheter.

then A <-----------> B are moving apart with 100 mph.
C also starts accelerating to the left.
because he claims that he is accarating will he be to the left of A or B?
 

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