## Classical Electrodynamics |

### From inside the book

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Page 29

We note that , as the

grows in magnitude and moves out from the center of the sphere . When q is just

outside the surface of the sphere , the image charge is equal and opposite in ...

We note that , as the

**charge q**is brought closer to the sphere , the image chargegrows in magnitude and moves out from the center of the sphere . When q is just

outside the surface of the sphere , the image charge is equal and opposite in ...

Page 31

This charge was of total amount q ' = - ag / y , and was distributed over the

surface in such a way as to be in equilibrium under all forces acting If we wish to

consider the problem of an insulated conducting sphere with total

...

This charge was of total amount q ' = - ag / y , and was distributed over the

surface in such a way as to be in equilibrium under all forces acting If we wish to

consider the problem of an insulated conducting sphere with total

**charge Q**in the...

Page 51

2 A point

plane conductor held at zero potential . Using the method of images , find : ( a )

the surface - charge density induced on the plane , and plot it ; ( b ) the force

between ...

2 A point

**charge q**is brought to a position a distance d away from an infiniteplane conductor held at zero potential . Using the method of images , find : ( a )

the surface - charge density induced on the plane , and plot it ; ( b ) the force

between ...

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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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### 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