- #1
tylerscott
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Homework Statement
A gauge transformation is defined so as to leave the fields invariant. The gauge transformations are such that [itex]\vec{A}=\vec{A'}+\nabla\Lambda[/itex] and [itex]\Phi=\Phi'-\frac{\partial\Lambda}{\partial t}[/itex]. Consider the Coulomb Gauge [itex]\nabla\cdot\vec{A}=0[/itex]. Find out what properties the function [itex]\Lambda[/itex] must satisfy in order for the Coulomb Gauge to be satisfied.
Homework Equations
Lorentz Gauge Condition
[itex]\nabla\vec{A}+\frac{1}{c^{2}}\frac{\partial\Phi}{\partial t}=0[/itex]
The Attempt at a Solution
[itex]\nabla\cdot\vec{A}=\nabla\left(\vec{A'}+\nabla\Lambda\right)=0[/itex]
[itex]\nabla\cdot\vec{A'}+\nabla^{2}\Lambda=0[/itex]
so
[itex]\nabla\cdot\vec{A'}+\nabla^{2}\Lambda+\frac{1}{c^{2}}\frac{\partial }{\partial t}(\Phi'-\frac{\partial\Lambda}{\partial t})=0[/itex]
and
[itex]\nabla\cdot\vec{A'}+\frac{1}{c^{2}}\frac{\partial\Phi'}{\partial t}=\frac{1}{c^{2}}\frac{\partial^{2}\Lambda}{\partial t^{2}}-\nabla^{2}\Lambda[/itex]
So in order for these to be invariant, [itex]\frac{1}{c^{2}}\frac{\partial^{2}\Lambda}{\partial t^{2}}-\nabla^{2}\Lambda=0[/itex]
So [itex]\Lambda[/itex] must satisfy wave equation.
Now, I feel like I'm missing some of the properties of the gauge, so any help into more insight into [itex]\Lambda[/itex] would be appreciated.