Proving Maxwell's Equations are Lorentz Invariant

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Discussion Overview

The discussion centers on proving that Maxwell's equations for the propagation of electromagnetic waves are Lorentz invariant. Participants explore various approaches to demonstrate this invariance, including transformations and covariant formulations.

Discussion Character

  • Exploratory
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • One participant seeks a method to prove the Lorentz invariance of Maxwell's equations.
  • Another suggests transforming the wave equation and observing that it remains unchanged, although they do not provide specific details.
  • A participant expresses appreciation for a resource that clarifies the relationship between Lorentz transformations and Maxwell's equations.
  • One participant proposes that reformulating Maxwell's equations in manifestly covariant form using four-vectors and four-tensors simplifies the proof of invariance.
  • Several participants request elaboration on the covariant formulation and its implications for invariance.
  • A later reply explains that when equations are written in tensor form, invariance under transformations is inherently included, citing specific tensor operations that remain unchanged under Lorentz transformations.

Areas of Agreement / Disagreement

Participants express differing views on the best approach to demonstrate Lorentz invariance, with some favoring direct transformations and others advocating for covariant formulations. No consensus is reached on a single method.

Contextual Notes

Some participants reference external resources for further clarification, indicating that there may be varying levels of familiarity with the mathematical concepts involved.

Who May Find This Useful

This discussion may be useful for students and researchers interested in the mathematical foundations of electromagnetism, particularly those exploring the relationship between Maxwell's equations and Lorentz transformations.

Bakali Thendo
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I want to know how can i prove that Maxwell's equations for the propagation of electromagnetic wave are Lorentz invariant.
 
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Yes, this give me a clear understanding on both the lorentz and maxwell. Thank you
 
Puh, that looks complicated ;-)). It's much easier to reformulate Maxwell's equations in manifestly covariant form with four-vectors and four-tensors. Then you immideately see, without to preform the pretty time-consuming Lorentz transformations, because then it's clear that the equations are covariant by construction!
 
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Can you elaborate on what you are talking about...
 
Bakali Thendo said:
Can you elaborate on what you are talking about...
Here is an introduction https://en.wikipedia.org/wiki/Covariant_formulation_of_classical_electromagnetism.

When equations are written in tensor form then invariance under certain transformations is 'built-in'.

Transformed tensor contractions eg ##v^a v_a \rightarrow \Lambda v^a {\Lambda}^{-1} v_a ## do not change because contravariant components transform with the inverse of the transformation of the covariant ones.

For instance ##f_{\alpha} = F_{\alpha\beta}J^{\beta}## is manifestly covariant because ##F## and ##J## are tensors. The contraction ##f^\alpha f_\alpha## is unaffected by a Lorentz transformation.
 
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