## Classical ElectrodynamicsProblems after each chapter |

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Page 16

This is called a Dirichlet problem , or Dirichlet

This is called a Dirichlet problem , or Dirichlet

**boundary conditions**. ... of the normal derivative is known as the Neumann**boundary condition**.Page 19

The freedom available in the definition of G ( 1.40 ) means that we can make the surface integral depend only on the chosen type of

The freedom available in the definition of G ( 1.40 ) means that we can make the surface integral depend only on the chosen type of

**boundary conditions**.Page 90

3.11 solutions of Laplace's or Poisson's equation ( Section 1.9 ) it was pointed out , however , that mixed

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 ...### What people are saying - Write a review

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### Contents

Introduction to Electrostatics | 1 |

Greens theorem | 14 |

BoundaryValue Problems in Electrostatics I | 26 |

Copyright | |

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### Common terms and phrases

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 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 relativistic result satisfy scalar scattering shown in Fig shows side solution sphere spherical surface transformation unit vanishes vector velocity volume wave written