## Classical ElectrodynamicsProblems after each chapter |

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Page 61

This uniqueness provides a

from a knowledge of the potential in a limited domain , namely on the symmetry

axis . On the symmetry axis ( 3.33 ) becomes ( with 2 = r ) : O 0 ( z = r ) = { [ Aįr ...

This uniqueness provides a

**means**of obtaining the solution of potential problemsfrom a knowledge of the potential in a limited domain , namely on the symmetry

axis . On the symmetry axis ( 3.33 ) becomes ( with 2 = r ) : O 0 ( z = r ) = { [ Aįr ...

Page 559

Tell ) The presence of the factor ( ka ) 2 in the transition probability ( 16.104 )

rapidly with increasing multipole order , for a fixed frequency . Consequently in

an atomic ...

Tell ) The presence of the factor ( ka ) 2 in the transition probability ( 16.104 )

**means**that in the long - wavelength limit ( ka < 1 ) the transition rate falls offrapidly with increasing multipole order , for a fixed frequency . Consequently in

an atomic ...

Page 587

This

reads an + 1 - n ! cn + 2 деп + 1 n = 0 др dp ( -1 ) " dox d®x'p ( x , t ) R -1 { } dt

where ( 17.25 ) VR * + 1 { } = J ( x ' , 1 ) + ( x ' , t ) at ( n + 1 ) ( n + 2 ) R " -1 With the

...

This

**means**that we can change the summation indices so that the sum nowreads an + 1 - n ! cn + 2 деп + 1 n = 0 др dp ( -1 ) " dox d®x'p ( x , t ) R -1 { } dt

where ( 17.25 ) VR * + 1 { } = J ( x ' , 1 ) + ( x ' , t ) at ( n + 1 ) ( n + 2 ) R " -1 With the

...

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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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