## 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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angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge classical collisions compared component conducting conductor Consequently consider constant coordinates cross section cylinder defined density depends derivative determine dielectric dimensions dipole direction discussed distance distribution effects electric field electromagnetic electron electrostatic energy equal equation example expansion expression factor force frame frequency function given gives incident inside integral involved limit Lorentz loss magnetic magnetic field magnetic induction magnitude mass means momentum motion moving multipole normal observation obtain origin parallel particle physical plane plasma polarization position potential problem properties radiation radius region relation relative result satisfy scalar scattering shows side simple solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written