## Classical Electrodynamics |

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Page 166

(b) Show that an alternative

kp) 0 (c) Write down integral

induction, using the

components of B ...

(b) Show that an alternative

**expression**for A4 is oo A4(p, z) = *. dke-ko J1(ka).J1(kp) 0 (c) Write down integral

**expressions**for the components of magneticinduction, using the

**expressions**of (a) and (b). Evaluate explicitly thecomponents of B ...

Page 295

For ka > 1, the second form in (9.109) can be used to obtain an asymptotic

ka, but are not ...

For ka > 1, the second form in (9.109) can be used to obtain an asymptotic

**expression**, 1 1 - ( #) Tcz 1 — — — — —iz sin 2ka ... These approximate**expressions**(9.109) and (9.110) for T give the general behavior as a function ofka, but are not ...

Page 447

where we have used the dipole moment

second term is small, the imaginary part of 1/e(0) can be readily calculated and

substituted into (13.70). Then the integral over do can be performed in the same ...

where we have used the dipole moment

**expression**(13.19). Assuming that thesecond term is small, the imaginary part of 1/e(0) can be readily calculated and

substituted into (13.70). Then the integral over do can be performed in the same ...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

References and suggested reading | 50 |

Copyright | |

16 other sections not shown

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