## 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

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

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 fluxthrough 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

'.

... 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 | |

30 other sections not shown

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