## Classical Electrodynamics |

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Page 129

4.3 4.4 4.5 (c) Nuclear-charge distributions can be approximated by a

charge density throughout a spheroidal volume of semimajor axis a and

semiminor axis b. Calculate the quadrupole moment of such a nucleus, assuming

that the ...

4.3 4.4 4.5 (c) Nuclear-charge distributions can be approximated by a

**constant**charge density throughout a spheroidal volume of semimajor axis a and

semiminor axis b. Calculate the quadrupole moment of such a nucleus, assuming

that the ...

Page 130

4.6 Two concentric conducting spheres of inner and outer radii a and b,

respectively, carry charges +Q. The empty space between the spheres is half-

filled by a hemispherical shell of dielectric (of dielectric

the figure.

4.6 Two concentric conducting spheres of inner and outer radii a and b,

respectively, carry charges +Q. The empty space between the spheres is half-

filled by a hemispherical shell of dielectric (of dielectric

**constant**e), as shown inthe figure.

Page 614

Only when we define other field quantities may it be convenient to insert

dimensional proportionality

dimensions ... II" dl 2ks d (A.4) The

ki in (A.2).

Only when we define other field quantities may it be convenient to insert

dimensional proportionality

**constants**in the definitions in order to adjust thedimensions ... II" dl 2ks d (A.4) The

**constant**k, is a proportionality**constant**akin toki in (A.2).

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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