gallieo1985
5h ago
According to standard electromagnetic theory, if the charge A is stationary and the charge B is moving along arbitrary trajectory then the electromagnetic force on charge A is: $$\vec{F}_A = q_A \left(-\nabla\phi - \frac{\partial}{\partial t}\vec{A}\right)$$ where $\phi$ and $\vec{A}$ are velocity dependent scalar and vector potentials (Lienard-Wiechert potentials), i.e. $$\phi = \frac{1}{4\pi\ep…









