## Classical Electrodynamics |

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Page 367

Using the general formula (11.21) twice, it is a straightforward matter to

the time variables in K" and K" are related ... U2 T = | -- correct to first order in Öv.

This

Using the general formula (11.21) twice, it is a straightforward matter to

**show**thatthe time variables in K" and K" are related ... U2 T = | -- correct to first order in Öv.

This

**shows**that the direct transformation from K' to K" involves an infinitesimal ...Page 371

O £3 With definitions (11.68) and (11.70) it is elementary to

yields exactly the Lorentz transformation ... -H cos y ar, Comparison of the

coefficients in (11.77) with the transformation coefficients in (11.75)

the angle p ...

O £3 With definitions (11.68) and (11.70) it is elementary to

**show**that (11.75)yields exactly the Lorentz transformation ... -H cos y ar, Comparison of the

coefficients in (11.77) with the transformation coefficients in (11.75)

**shows**thatthe angle p ...

Page

Why? Make quantitative statements if you can. As in Problem 14.2a a charge e

moves in simple harmonic motion along the z axis, z(t') = a cos (opot'). (a)

that the instantaneous power radiated per unit solid angle is: dP(t) e°cB' sin” 0

cos” ...

Why? Make quantitative statements if you can. As in Problem 14.2a a charge e

moves in simple harmonic motion along the z axis, z(t') = a cos (opot'). (a)

**Show**that the instantaneous power radiated per unit solid angle is: dP(t) e°cB' sin” 0

cos” ...

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### Contents

Introduction to Electrostatics | 1 |

Nº 3 | 3 |

Greens theorem | 14 |

Copyright | |

30 other sections not shown

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