Negative Velocities in Lorentz Transformations

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Discussion Overview

The discussion centers on the implications of negative velocities in Lorentz transformations within the context of special relativity. Participants explore how relativistic effects, such as length contraction and time dilation, are affected when considering velocities in the negative direction, particularly in relation to proper lengths and frame of reference. The scope includes conceptual clarifications and technical reasoning.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • An undergraduate student questions whether Lorentz elongation exists when considering a frame moving in the -x direction and how this relates to the measurement of lengths in different frames.
  • Some participants assert that a negative velocity simply represents an inverse Lorentz boost, suggesting that the mathematical framework remains valid regardless of direction.
  • One participant notes that the equations for length contraction and time dilation depend on the square of the velocity, implying that the sign of the velocity does not affect the outcomes of these effects.
  • Another participant raises a hypothetical scenario about directional choices for length expansion and contraction, suggesting that this could complicate the understanding of relativistic effects in different directions.
  • A participant expresses concern that the textbook's treatment of velocities may be overly simplistic, arguing that it does not adequately account for vector treatment of velocities.

Areas of Agreement / Disagreement

Participants express differing views on the implications of negative velocities in Lorentz transformations. While some agree on the mathematical validity of the transformations regardless of direction, others raise questions about the conceptual understanding of length measurements and directional effects, indicating that the discussion remains unresolved.

Contextual Notes

There are limitations in the discussion regarding the assumptions made about the treatment of velocities as scalars versus vectors, and the implications of directional choices on relativistic effects are not fully explored.

TheConfusedOne
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Undergrad studying engineering here, and my physics class has been doing a unit about intro to special relativity. Essentially, all of our problems and studies concern themselves with velocities which are in the +x direction relative to a "home frame" (I think physicists call this standard orientation). However, I'm curious as to how relativistic effects occur when velocities are allowed to be negative.

To begin I'll summarize an issue:

For example, does a Lorentz Elongation exist? For example, letting Frame A move in the -x direction relative to Frame B is the same as letting Frame B move in the +x direction relative to Frame A. Therefore isn't it equally valid to say that Frame A measures lengths in Frame B along x to be LONGER than they are as resting in B? Of course, one could note that any length has a "proper length", which is measured in a frame which is not moving relative to this length (I suppose by length I mean the distance between two independent "events". In this notation the "rest frame" is defined for which the events occur at the simultaneously). Here is where my troubles begin, however. Suppose there is a defined proper length L. Thus, in a frame with +x velocity, this L is measured as L' which is shorter than L. But, in a frame with -x velocity, according to L'=Lsqrt(1-v^2/c^2) this L' is still shorter, even though I have this weird gut feeling it might be longer. I am concurrently in multivariable calculus and I suspect the equation my textbook gave me fails for -x direction velocities because it has neglected to treat the matter as vectors and instead has opted for simpler scalar equations.
 
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Nope. ##\vec{v} \rightarrow -\vec{v}## just represents an inverse Lorentz boost.
 
(v)2=(-v)2

Event ordering depends on the direction of motion, but length contraction and time dilation both depend on the square of the velocity, which is independent of the sign.
 
How would you choose between East and West to determine which is the length expansion direction?

Lets say you choose East and between North and South you choose North as the length expansion direction. This means that an object going North West or South East relative to you, would have no length contraction, an object going North East would have length expansion squared and an object going or South West would have length contraction squared. Since time dilation is intimately connected to length contraction, we would have to have directional time dilation and relative time speeding up in some directions.
 
TheConfusedOne said:
I suspect the equation my textbook gave me fails for -x direction velocities because it has neglected to treat the matter as vectors and instead has opted for simpler scalar equations.

Note that a scalar is a 1-dimensional vector. The "V" in the standard Lorentz tranformations is a scalar, but can be +ve or -ve. Although the equations may have been derived using diagrams that show the S' frame moving to the right (+ve), they are valid for the S' frame moving to the left (where V is -ve).

It might be a useful exercise to check this out for yourself.

(I'm just learning this stuff myself, so apologies to the experts!)
 

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