Relativistic Vectors: Opposite Direction Assumption

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Discussion Overview

The discussion centers on the nature of position and velocity vectors in the context of special relativity (SR), particularly focusing on the assumption that the relative velocity of one object with respect to another is equal in magnitude and opposite in direction. Participants explore the implications of this assumption and question how it relates to the frame-specific nature of vectors.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant questions the assumption that position vectors in different frames can be considered equal in magnitude and opposite in direction, suggesting this may not hold true in special relativity.
  • Another participant points out the importance of the relativity of simultaneity, indicating that position vectors cannot be directly compared at the same moment across different frames as they could in classical physics.
  • There is a repeated inquiry about the relationship v(ba) = -v(ab), with a participant expressing confusion over how this relationship can be justified in the context of frame-specific vectors.
  • A later reply mentions that the symmetry of velocities in SR applies to inertial objects that do not accelerate, implying that their velocities remain consistent across time in a given frame, unlike position vectors.
  • Another participant notes that the relationship v(ba) = -v(ab) can be derived from the Lorentz transformation, which is based on the fundamental postulates of special relativity, and requests an illustration of this derivation.

Areas of Agreement / Disagreement

Participants express uncertainty and differing views regarding the treatment of position and velocity vectors in special relativity. There is no consensus on the implications of these vectors being frame-specific or how to reconcile the assumptions made in special relativity with classical mechanics.

Contextual Notes

The discussion highlights limitations in understanding the comparison of position vectors across different frames due to the relativity of simultaneity and the dynamic nature of position in contrast to the static nature of velocity in inertial frames.

anantchowdhary
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In special relativity we assume relative velocity of B wrt A is the same in magnitude and opposite in direction as of velocity of A wrt B. Now doesn't this demand that the position vectors in both frames(A's and B's) are the just opposite in direction...?

I mean to ask...how can we take for granted that the position vectors will just be the same in magnitude and opposite in direction ?? O_o

Thanks!
 
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Position vectors at what moment in each frame? Because of the relativity of simultaneity, you can't just compare the position vector of B in A's frame with the position vector of A in B's frame "at the same moment" as you could in classical physics.
 
What i meant to ask is that how is v(ba)=-v(ab) ??

In Newtonian mechanics we do this simply as we consider space to be absolute,so the vector as seen from A's origin to B's origin will be just the opposite of what it is from B's origin to A's origin(we take that for granted i guess)

So isn;t a vector frame specific??

According to SR it should be,shouldn't it?

So as you said,we ca't compare position vectors in both frames just like that,how can we say that the relative velocitues are same in magnitude ??

Thanks
 
Last edited:
anantchowdhary said:
What i meant to ask is that how is v(ba)=-v(ab) ??

In Newtonian mechanics we do this simply as we consider space to be absolute,so the vector as seen from A's origin to B's origin will be just the opposite of what it is from B's origin to A's origin(we take that for granted i guess)

So isn;t a vector frame specific??

According to SR it should be,shouldn't it?

So as you said,we ca't compare position vectors in both frames just like that,how can we say that the relative velocitues are same in magnitude ??
Well, when you talk about the symmetry of velocities in SR you're talking about the velocities of inertial objects which never accelerate, so whatever the value of their velocity is at one moment in a given frame, it should be the same at every other moment in that frame (unlike with position vectors which are constantly changing). The fact that v(ba) = -v(ab) can be derived from the Lorentz transformation, which itself is derived from the two basic postulates of SR.
 
JesseM said:
The fact that v(ba) = -v(ab) can be derived from the Lorentz transformation, which itself is derived from the two basic postulates of SR.

Could you please illustrate this

Thanks!
 

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