## Classical Electrodynamics |

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Page 116

0 ( ) 4.6 Molecular Polarizability and Electric Susceptibility In this section and the

next we will consider the relation between molecular

macroscopically defined parameter, the electric susceptibility X. Our discussion

will be in ...

0 ( ) 4.6 Molecular Polarizability and Electric Susceptibility In this section and the

next we will consider the relation between molecular

**properties**and themacroscopically defined parameter, the electric susceptibility X. Our discussion

will be in ...

Page 126

If , however , the dielectric

) the contributions in ( 4 . 99 ) are not necessarily the same . In fact , we have just

calculated the change in energy brought about by introducing a dielectric body ...

If , however , the dielectric

**properties**are altered , € ( x ) = f ( x ) + de ( x ) ( 4 . 100) the contributions in ( 4 . 99 ) are not necessarily the same . In fact , we have just

calculated the change in energy brought about by introducing a dielectric body ...

Page 216

5 Reflection and Refraction of Electromagnetic Waves at a Plane Interface

between Dielectrics The reflection and refraction of light at a plane surface

between two media of different dielectric

various ...

5 Reflection and Refraction of Electromagnetic Waves at a Plane Interface

between Dielectrics The reflection and refraction of light at a plane surface

between two media of different dielectric

**properties**are familiar phenomena . Thevarious ...

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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