Difference between revisions of "Maxwell's Equations"
Jump to navigation
Jump to search
| Line 19: | Line 19: | ||
<math>\boldsymbol{\nabla \times B} - \mu_0\epsilon_0\frac{\partial \boldsymbol{E}}{\partial t}= 0 </math> | <math>\boldsymbol{\nabla \times B} - \mu_0\epsilon_0\frac{\partial \boldsymbol{E}}{\partial t}= 0 </math> | ||
| − | <font color="red">Need to add possibly derivation of wave equation and definitely Maxwell's equation in presence</font> | + | <font color="red">Need to add possibly derivation of wave equation and definitely Maxwell's equation in presence. Need also to introduce D and H and relate them to E and B.</font> |
Gauss' Law: | Gauss' Law: | ||
Revision as of 15:40, 21 March 2007
In Free Space
These are the Maxwell's Equations we will be using to solve for regions "I" and "II" in our approximation of the Michelson interferometer.
Gauss' Law:
Gauss' Law for Magnetism:
Faradays's Law:
Ampere's Law:
Need to add possibly derivation of wave equation and definitely Maxwell's equation in presence. Need also to introduce D and H and relate them to E and B.
Gauss' Law:
Gauss' Law for Magnetism:
Faradays's Law:
Ampere's Law: