## Classical Electrodynamics |

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Page 31

3 Point Charge in the Presence of a Charged , Insulated , Conducting

the previous section we considered the problem of a point charge 9 near a

grounded

3 Point Charge in the Presence of a Charged , Insulated , Conducting

**Sphere**Inthe previous section we considered the problem of a point charge 9 near a

grounded

**sphere**and saw that a surface - charge density was induced on the**sphere**.Page 33

4 Point Charge near a Conducting

which can be discussed easily is that of a point charge near a conducting

held at a fixed potential V . The potential is the same as for the charged

4 Point Charge near a Conducting

**Sphere**at Fixed Potential Another problemwhich can be discussed easily is that of a point charge near a conducting

**sphere**held at a fixed potential V . The potential is the same as for the charged

**sphere**...Page 39

As a very simple example of the solution of a potential problem by inversion we

consider an isolated conducting

The potential has the constant value Q / R inside the

...

As a very simple example of the solution of a potential problem by inversion we

consider an isolated conducting

**sphere**of radius R with a total charge Q on it .The potential has the constant value Q / R inside the

**sphere**and falls off inversely...

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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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### Common terms and phrases

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