Lorenz Gauge

#Physics

Topics

• Canonical Momentum

$\displaystyle \nabla \cdot \vec{A}=-{\mu}{0}{\varepsilon}{0}\partial_{t}V$

• Choosing this gauge makes it easier to solve for $\displaystyle \vec{A}$

$\displaystyle \Box ^{2}V=-\frac{1}{{\varepsilon}_{0}}\rho$

• $\displaystyle \Box$ is the d'Alembert operator

$\displaystyle \Box ^{2}\vec{A}=-{\mu}_{0}\vec{J}$