## Classical ElectrodynamicsProblems after each chapter |

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Page 13

Poisson's

scalar ...

**Equations**( 1.13 ) and ( 1.16 ) can be combined into one partial differential**equation**for the single function P ( x ) : V20 = -47p ( 1.28 ) This**equation**is calledPoisson's

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

Page 337

we ܗܽܘܢ 1 ( ap ) van = 0 m an independent

combining the last two

) is independent of magnetic field , suspect that there exist solutions of a purely ...

we ܗܽܘܢ 1 ( ap ) van = 0 m an independent

**equation**, but may be derived bycombining the last two

**equations**in ( 10.91 ) . Since the force**equation**in ( 10.91) is independent of magnetic field , suspect that there exist solutions of a purely ...

Page 582

v dt = 0 Then it is permissible to identify the radiative reaction force as 2 e Frad =

MTÜ ( 17.8 ) 3 c3 The modified

17.9 )

v dt = 0 Then it is permissible to identify the radiative reaction force as 2 e Frad =

MTÜ ( 17.8 ) 3 c3 The modified

**equation**of motion then reads mlý – TÜ ) = Fext (17.9 )

**Equation**( 17.9 ) is sometimes called the Abraham - Lorentz**equation**of ...### What people are saying - Write a review

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### Contents

Introduction to Electrostatics | 1 |

References and suggested reading | 23 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

6 other sections not shown

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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 shows side solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written