Invariance of Acceleration in Inertial Reference Frames

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Discussion Overview

The discussion revolves around the invariance of acceleration in inertial reference frames, exploring whether acceleration (both direction and magnitude) remains the same across different inertial frames. The conversation touches on concepts from classical mechanics and special relativity, examining the implications of proper and coordinate acceleration.

Discussion Character

  • Debate/contested
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • Some participants claim that acceleration is invariant in all inertial frames, while others suggest this may not hold true under relativistic conditions.
  • One participant points out that the statement may be valid if velocities are much less than the speed of light, referencing special relativity.
  • Another participant emphasizes the distinction between proper acceleration and coordinate acceleration, noting historical disagreements stemming from this lack of qualification.
  • Several participants present mathematical equations related to acceleration transformations, with some expressing uncertainty about the correctness of their calculations.
  • There is a question regarding whether the discussed equations apply to all components of acceleration or just the x-component.
  • Some participants express a need for references to better understand the topic and validate their claims.

Areas of Agreement / Disagreement

Participants do not reach a consensus on the invariance of acceleration across inertial frames, with multiple competing views and interpretations of the equations presented. The discussion remains unresolved regarding the applicability of the equations and the definitions of acceleration being used.

Contextual Notes

The discussion highlights the importance of distinguishing between proper and coordinate acceleration, as well as the potential impact of relativistic effects on the validity of claims about acceleration invariance. Some mathematical steps and assumptions remain unresolved, contributing to the ongoing debate.

0pt618
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Claim: The acceleration (both direction and magnitude) for any object is the same in any inertial reference frame.

Is this claim true? I think it is, but someone mentioned to me that time may be an issue as it's not agreed upon in all inertial reference frames.

I'd appreciate any references, if available.
 
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Why don't you look up the equations in special relativity and calculate it yourself? My calculation suggests that this statement is wrong, but don't take my words for it, my math is rusted.
$$a{\rm{'}} = \sqrt {1 - {{{v^2}} \over {{c^2}}}} {(1 - {{vu} \over {{c^2}}})^{ - 3}}a$$
 
Thanks Xu Shuang for your reply. It's been a long time ago since I studied special relativity. But from your equation, it seems if the velocities are all much less than the velocity of light, then the statement would be valid, correct?
 
0pt618 said:
Is this claim true? I

It is true for proper acceleration but not true for coordinate acceleration.
Wars have been fought and cities razed to the ground because someone made a statement about acceleration without qualifying whether they meant coordinate or proper acceleration, so it's not surprising that you're finding some disagreement.

The concept of proper acceleration is usually introduced when you first study special relativity, so this thread maybe belongs in the relativity forum.
 
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Since this thread was originally not in the relativity forum, I think it is worth pointing out that the acceleration is the same in all inertial frames in classical mechanics. It is only when relativistic effects become important when this is no longer true. But as Xu said, you should not take anyone's word for this either, you can simply derive the relation yourself based on the Galilei transformations.
 
Xu Shuang said:
My calculation suggests that this statement is wrong, but don't take my words for it, my math is rusted.
$$a{\rm{'}} = \sqrt {1 - {{{v^2}} \over {{c^2}}}} {(1 - {{vu} \over {{c^2}}})^{ - 3}}a$$

Is this only for the x-component or for all 3 components?

Does this mean that the direction of the acceleration vector doesn't change?
 
greswd said:
Is this only for the x-component or for all 3 components?

Does this mean that the direction of the acceleration vector doesn't change?
This is just x component. 4-dimensional space-time is too much for my math.
 
Xu Shuang said:
This is just x component. 4-dimensional space-time is too much for my math.

I think it should be

$$a{\rm{'}} = (\sqrt {1 - {{{v^2}} \over {{c^2}}}})^{3} {(1 - {{vu} \over {{c^2}}})^{ - 3}}a$$
 
greswd said:
I think it should be

$$a{\rm{'}} = (\sqrt {1 - {{{v^2}} \over {{c^2}}}})^{3} {(1 - {{vu} \over {{c^2}}})^{ - 3}}a$$
Are you sure? It was a full paper of calculation.
 
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Xu Shuang said:
Are you sure? It was a full paper of calculation.

Quite sure.
 
  • #11
0pt618 said:
I'd appreciate any references, if available.
I've been meaning to take a closer look at this for a while, it seems to be fairly exhaustive and correct (I went through it once without taking it in properly).
 
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  • #12
greswd said:
I think it should be

$$a{\rm{'}} = (\sqrt {1 - {{{v^2}} \over {{c^2}}}})^{3} {(1 - {{vu} \over {{c^2}}})^{ - 3}}a$$
I did it again, yours is right.
 
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