## Classical Electrodynamics |

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Page 13

called Poisson ' s

, the ...

**Equations**( 1 . 13 ) and ( 1 . 16 ) can be combined into one partial differential**equation**for the single function Q ( x ) : V20 = - 477p ( 1 . 28 ) This**equation**iscalled Poisson ' s

**equation**. In regions of space where there is no charge density, the ...

Page 337

an independent

magnetic field , we suspect that there exist solutions of a purely electrostatic

nature , with ...

an independent

**equation**, but may be derived by combining the last two**equations**in ( 10 . 91 ) . Since the force**equation**in ( 10 . 91 ) is independent ofmagnetic field , we suspect that there exist solutions of a purely electrostatic

nature , with ...

Page 582

8 ) 3 c3 The modified

It can be considered as an

8 ) 3 c3 The modified

**equation**of motion then reads mlı – TÜ ) = Fext ( 17 . 9 )**Equation**( 17 . 9 ) is sometimes called the Abraham - Lorentz**equation**of motion .It can be considered as an

**equation**which includes in some approximate and ...### What people are saying - Write a review

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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