## Classical ElectrodynamicsProblems after each chapter |

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Page 400

Since the photon has no rest

Mev, while the target

Tth = 135.o| 1 + 135'° 1 = 135.0(1.072) = 144.7 Mev 2(938.5)J As another

example ...

Since the photon has no rest

**mass**, the**mass**difference is AM = /»„<> = 135.0Mev, while the target

**mass**is m2 = mv = 938.5 Mev. Then the threshold energy isTth = 135.o| 1 + 135'° 1 = 135.0(1.072) = 144.7 Mev 2(938.5)J As another

example ...

Page 590

... field.f Nonelectromagnetic forces imply a contribution m0 to the

particle from such forces. Within the framework of the Abraham-Lorentz model as

discussed so far, this additional

... field.f Nonelectromagnetic forces imply a contribution m0 to the

**mass**of aparticle from such forces. Within the framework of the Abraham-Lorentz model as

discussed so far, this additional

**mass**merely appears as an added coefficient ...Page 623

Glasstone, S., and R. H. Lovberg, Controlled Thermonuclear Reactions, Van

Nostrand, Princeton, N.J. (1960). Goldstein, H., Classical Mechanics, Addison-

Wesley, Reading,

Yale ...

Glasstone, S., and R. H. Lovberg, Controlled Thermonuclear Reactions, Van

Nostrand, Princeton, N.J. (1960). Goldstein, H., Classical Mechanics, Addison-

Wesley, Reading,

**Mass**. (1950). Hadamard, J., Lectures on Cauchy's Problem,Yale ...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

Multipoles Electrostatics of Macroscopic Media | 98 |

Copyright | |

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