## Classical Electrodynamics |

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Page 16

This is called a Dirichlet problem , or Dirichlet boundary conditions . Similarly it is

plausible that specification of the electric field ( normal

everywhere on the surface ( corresponding to a given surface - charge density ) ...

This is called a Dirichlet problem , or Dirichlet boundary conditions . Similarly it is

plausible that specification of the electric field ( normal

**derivative**of the potential )everywhere on the surface ( corresponding to a given surface - charge density ) ...

Page 172

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 .

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 .

Page 188

70 ) is the so - called Kirchhoff representation of the field inside the volume V in

terms of the values of y and its

assume that there are no sources within V and that the initial values of y and əylət

...

70 ) is the so - called Kirchhoff representation of the field inside the volume V in

terms of the values of y and its

**derivatives**on the boundary surface S . We thusassume that there are no sources within V and that the initial values of y and əylət

...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

RelativisticParticle Kinematics and Dynamics | 391 |

Copyright | |

8 other sections not shown

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acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge charged particle classical collisions compared component conducting Consequently consider constant coordinates cross section cylinder defined density dependence 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 light limit Lorentz loss magnetic magnetic field magnetic induction magnitude mass means modes momentum motion moving multipole normal observation obtain origin parallel particle physical plane plasma polarization position potential problem properties radiation radius region relation relative relativistic result satisfy scalar scattering shown in Fig shows side solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written