Proving Maxwell's Equations are Lorentz Invariant

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SUMMARY

This discussion focuses on proving that Maxwell's equations for electromagnetic wave propagation are Lorentz invariant. Participants emphasize the importance of reformulating these equations in manifestly covariant form using four-vectors and four-tensors, which inherently demonstrates their invariance without the need for extensive Lorentz transformations. Key insights include the role of tensor contractions, such as ##f_{\alpha} = F_{\alpha\beta}J^{\beta}##, which remain unchanged under Lorentz transformations, confirming the covariant nature of the equations.

PREREQUISITES
  • Understanding of Maxwell's equations
  • Familiarity with Lorentz transformations
  • Knowledge of tensor calculus
  • Basic concepts of four-vectors and four-tensors
NEXT STEPS
  • Study the covariant formulation of classical electromagnetism
  • Learn about tensor contractions and their properties
  • Explore the implications of Lorentz invariance in physics
  • Review the mathematical foundations of four-vectors and four-tensors
USEFUL FOR

This discussion is beneficial for physicists, students of electromagnetism, and anyone interested in the mathematical foundations of relativity and field theory.

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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