## Classical ElectrodynamicsProblems after each chapter |

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Page 377

This correspondence will sometimes be

This correspondence will sometimes be

**written**A = ( A , A ) ( 11.95 ) Sometimes the subscript on the 4 - vector will be omitted , e.g. f ( x ) means f ( x , t ) . 4. Scalar products of 4 - vectors will be denoted by ( AB ) = A · B - AB ...Page 385

( 11.129 ) , the force density becomes 1 F # 471 дах , OF va fu ( 11.131 ) HV The right - hand side of ( 11.131 ) can be

( 11.129 ) , the force density becomes 1 F # 471 дах , OF va fu ( 11.131 ) HV The right - hand side of ( 11.131 ) can be

**written**as the divergence of a tensor of the second rank . We define the symmetric tensor TH called the ...Page 395

Since the initial system had zero momentum , the two particles must have equal and opposite momenta , P. = -P2 = p . From ( 12.11 ) the conservation of energy can be

Since the initial system had zero momentum , the two particles must have equal and opposite momenta , P. = -P2 = p . From ( 12.11 ) the conservation of energy can be

**written**V p2 + m1 ? + V pa + m2 ( 12.16 ) From this equation it is a ...### 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 | |

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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