SR, electromagnetic waves in moving reference frames.

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SUMMARY

The discussion focuses on the propagation of electromagnetic waves in a moving reference frame, specifically frame S' moving at a constant velocity relative to inertial frame S. The participant seeks to derive the second-order partial derivatives for the Laplacian and time in the context of special relativity. Key insights reveal that the electromagnetic wave equation is not invariant under Galilean transformations, but is invariant under Lorentz transformations, indicating that there is no preferential reference frame for electromagnetic waves.

PREREQUISITES
  • Understanding of special relativity concepts, particularly Lorentz transformations.
  • Familiarity with electromagnetic wave equations and their properties.
  • Knowledge of partial derivatives and their applications in physics.
  • Basic mathematical skills in calculus, specifically second-order derivatives.
NEXT STEPS
  • Study the derivation of the Lorentz transformation equations in detail.
  • Explore the implications of electromagnetic wave invariance under Lorentz transformations.
  • Learn about the mathematical formulation of the electromagnetic wave equation.
  • Investigate the differences between Galilean and Lorentz transformations in various physical contexts.
USEFUL FOR

Students of physics, particularly those studying electromagnetism and special relativity, as well as educators and researchers seeking to clarify the behavior of electromagnetic waves in different reference frames.

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Homework Statement


Not really a homework/coursework problem, I'm just trying to make sense of some class notes from our chapter on special relativity. I'm trying to find the expression for electromagnetic wave propagation in a reference frame S' that is moving at a constant velocity with respect to an inertial reference frame S.
[PLAIN]http://img193.imageshack.us/img193/4058/p1000897f.jpg
Where capital phi is either the B or E vector (see relevant equations).

Homework Equations


[URL]http://upload.wikimedia.org/math/4/5/a/45adde5635abaf78b4b9174bf210f504.png[/URL]
[URL]http://upload.wikimedia.org/math/d/a/4/da48cd00768a325141e38f519b4ca55e.png[/URL]
or more generally:
[URL]http://upload.wikimedia.org/math/6/7/0/670fa614a400a15236d39ece735e6f14.png[/URL]

Just need to find the 2nd order partials with respect to x, y, z for the Laplacian and the 2nd order partial with respect to t.

The Attempt at a Solution



I have no trouble finding the first order partial derivatives of phi with respect to all 4 variables (note the red checkmark), nor the 2nd order partial derivatives with respect to x, y and z. But I don't know what happened with the 2nd derivative with respect to time, I don't know where the two middle terms came from. (see arrows)

2nd question: What does the solution imply? I didn't understand/am missing the bit of theory that came afterwards (I'm not studying in my native language and my lecturer speaks blazingly fast lol), supposedly the solution for this equation in a moving reference frame gives an answer of 0, which implies that their is no preferential reference frame.

Sorry for posing a question so convoluted but I'd appreciate any help.
 
Last edited by a moderator:
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The transformation you've written down there [tex]x^\prime = x - vt[/tex] is a Galilean transformation. The relativistic transformation is known as the Lorentz transformation.

I haven't looked over your maths in detail, but if my memory serves me right, the EM wave equation is not invariant under a Galilean transformation but it is under a Lorentz transformation. You've basically shown there that the Galilean transformation doesn't work for EM waves.
 

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