- #1
Sammy268
- 7
- 0
At the moment we are working through problems in Griffiths' Electrodynamics textbook and it got me thinking...
In magnetostatics we have the magnetic vector potential A and in the use of dielectrics problems we have the vector D. Why is it advantageous to use these vectors and not just stick to using B and E?
In magnetostatics we have the magnetic vector potential A and in the use of dielectrics problems we have the vector D. Why is it advantageous to use these vectors and not just stick to using B and E?