## Classical Electrodynamics |

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Page 18

1.10 Formal Solution of Electrostatic Boundary-Value Problem with Green's

either Dirichlet or Neumann boundary conditions on the bounding surface S can

be ...

1.10 Formal Solution of Electrostatic Boundary-Value Problem with Green's

**Function**The solution of Poisson's or Laplace's equation in a finite volume V witheither Dirichlet or Neumann boundary conditions on the bounding surface S can

be ...

Page 78

Then it is convenient to express the Green's

expansion involved by considering spherical coordinates. For the case of no ...

Then it is convenient to express the Green's

**function**as a series of products of the**functions**appropriate to the coordinates in question. We first illustrate the type ofexpansion involved by considering spherical coordinates. For the case of no ...

Page 183

The fields are given by E - – 12* c 0t (6.53) B = V × A 6.6 Green's

Time-Dependent Wave Equation The wave equations (6.37), (6.38), and (6.52)

all have the basic structure, W*p — co as: = —4trf(x, t) (6.54) where f(x, t) is a ...

The fields are given by E - – 12* c 0t (6.53) B = V × A 6.6 Green's

**Function**for theTime-Dependent Wave Equation The wave equations (6.37), (6.38), and (6.52)

all have the basic structure, W*p — co as: = —4trf(x, t) (6.54) where f(x, t) is a ...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

References and suggested reading | 50 |

Copyright | |

16 other sections not shown

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