8 02 27

Lec 27 | MIT 8.02 Electricity and Magnetism, Spring 2002
$\lambda = \frac{2 \pi}{k}$
$T = \frac{2 \pi}{\omega}$
E & B propagation through vacuum
E & B are 'potentials'  $F = q E ; \vec{F} = q \vec{v}\times\vec{B}$