## Classical Electrodynamics |

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Page 111

The surface may be taken as the plane z = 0, as

the appropriate solution to the equations: eIV - E = 4mp, z > 0 l e.V. E = 0, 2 < 0 (

4.47) and V x E = 0, everywhere subject to the boundary conditions at z = 0: | e1E

, ...

The surface may be taken as the plane z = 0, as

**shown in Fig**. 4.5. We must findthe appropriate solution to the equations: eIV - E = 4mp, z > 0 l e.V. E = 0, 2 < 0 (

4.47) and V x E = 0, everywhere subject to the boundary conditions at z = 0: | e1E

, ...

Page 117

It is customary to consider the two parts separately by imagining a spherical

surface of size large microscopically but small macroscopically surrounding a

molecule, as

...

It is customary to consider the two parts separately by imagining a spherical

surface of size large microscopically but small macroscopically surrounding a

molecule, as

**shown in Fig**. 4.11, and determining the field at the center due to the...

Page 155

pillbox is oriented so that its faces are in regions 1 and 2 and parallel to the

surface boundary, S, as

B = 0 to yield (B2 - B). n = 0 (5.88) where n is the unit normal to the surface

directed ...

pillbox is oriented so that its faces are in regions 1 and 2 and parallel to the

surface boundary, S, as

**shown in Fig**. 5.9, Gauss's theorem can be applied to V.B = 0 to yield (B2 - B). n = 0 (5.88) where n is the unit normal to the surface

directed ...

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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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