Classical Electrodynamics |
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Page 90
3.11 solutions of Laplace's or Poisson's equation (Section 1.9) it was pointed out,
however, that mixed boundary conditions, where the potential is specified over
part of the boundary and its normal derivative is specified over the remainder, ...
3.11 solutions of Laplace's or Poisson's equation (Section 1.9) it was pointed out,
however, that mixed boundary conditions, where the potential is specified over
part of the boundary and its normal derivative is specified over the remainder, ...
Page 172
6.2, the total time derivative in (6.4) must take into account this motion. The flux
through the circuit may change because (a) the flux changes with time at a point,
or (b) the translation of the circuit changes the location of the boundary. It is easy
...
6.2, the total time derivative in (6.4) must take into account this motion. The flux
through the circuit may change because (a) the flux changes with time at a point,
or (b) the translation of the circuit changes the location of the boundary. It is easy
...
Page 188
... representation of the field inside the volume V in terms of the values of p and its
derivatives on the boundary surface S. ... R R” + CR ( ) The term involving the
derivative of the delta function can be integrated by parts with respect to the time t
'.
... representation of the field inside the volume V in terms of the values of p and its
derivatives on the boundary surface S. ... R R” + CR ( ) The term involving the
derivative of the delta function can be integrated by parts with respect to the time t
'.
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Contents
Introduction to Electrostatics | 1 |
Nš 3 | 3 |
Greens theorem | 14 |
Copyright | |
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