Using the Lorentz transformation of the four-vector potential (A^{mu}) and the wave equations from the previous problem,

Question:

Using the Lorentz transformation of the four-vector potential \(A^{\mu}\) and the wave equations from the previous problem, deduce the Lorentz transformations of charge density \(ho_{Q}\) and current density \(\mathbf{J}\).

Data from previous problem

Show that Maxwell's equations given by 8.16 imply the wave equations

\[abla^{2} \phi-\frac{1}{c^{2}} \frac{\partial^{2} \phi}{\partial t^{2}}=-4 \pi ho_{Q}\]

and

\[abla^{2} \mathbf{A}-\frac{1}{c^{2}} \frac{\partial^{2} \mathbf{A}}{\partial t^{2}}=-\frac{4 \pi}{c} \mathbf{J}\]

To do this, you will need the vector identity \(\boldsymbol{abla} \times \boldsymbol{abla} \times \mathbf{A}=\boldsymbol{abla}(\boldsymbol{abla} \cdot \mathbf{A})-abla^{2} \mathbf{A}\). You will also need to fix the gauge freedom using 

image text in transcribed

The latter is allowed due to the gauge symmetry.

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Modern Classical Mechanics

ISBN: 9781108834971

1st Edition

Authors: T. M. Helliwell, V. V. Sahakian

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