## Classical Electrodynamics |

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Page 12

This can be seen by letting the

double layer . The double layer is now imagined to consist of two parts , one

being a small disc directly under the

small ...

This can be seen by letting the

**observation**point come infinitesimally close to thedouble layer . The double layer is now imagined to consist of two parts , one

being a small disc directly under the

**observation**point . The disc is sufficientlysmall ...

Page 292

Historically , diffraction patterns were classed as Fresnel diffraction and

Fraunhofer diffraction , depending on the distance of the

the diffracting system . Generally the diffracting system ( e . g . , an aperture in an

opaque ...

Historically , diffraction patterns were classed as Fresnel diffraction and

Fraunhofer diffraction , depending on the distance of the

**observation**point fromthe diffracting system . Generally the diffracting system ( e . g . , an aperture in an

opaque ...

Page 531

81 ) where is the angle between u and the

semiclassical sense the electronic magnetic moment can be thought of as having

a magnitude u = V 3 ( eħ / 2mc ) , but being observed only through its projection

pz = E ...

81 ) where is the angle between u and the

**observation**direction n . In asemiclassical sense the electronic magnetic moment can be thought of as having

a magnitude u = V 3 ( eħ / 2mc ) , but being observed only through its projection

pz = E ...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

RelativisticParticle Kinematics and Dynamics | 391 |

Copyright | |

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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