## Classical Electrodynamics |

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Page 9

Then application of Stokes's theorem [if A(x) is a vector field, S is an open surface

, and C is the closed curve bounding S, # A-1 -s v x A) • n da where d1 is a line

element of C, n is the

Then application of Stokes's theorem [if A(x) is a vector field, S is an open surface

, and C is the closed curve bounding S, # A-1 -s v x A) • n da where d1 is a line

element of C, n is the

**normal**to S, and the path C is traversed in a right-hand ...Page 155

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

the subscripts refer to values at the surface in the two media. If we now consider a

...

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 from region 1 into region 2, andthe subscripts refer to values at the surface in the two media. If we now consider a

...

Page 238

If n is the unit

inward into the conductor, then the gradient operator can be written V c —n 3. 05

neglecting the other derivatives when operating on the fields within the ...

If n is the unit

**normal**outward from the conductor and 5 is the**normal**coordinateinward into the conductor, then the gradient operator can be written V c —n 3. 05

neglecting the other derivatives when operating on the fields within the ...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

BoundaryValue Problems in Electrostatics II | 54 |

Copyright | |

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acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge 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 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 shows side solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written