## Classical ElectrodynamicsProblems after each chapter |

### From inside the book

Results 1-3 of 74

Page 63

If the point x is on the z

left - hand side becomes : 1 1 | x – X'l 1 ir – p ' ! ( 3.43 ) ( r2 + p 2 2rr ' cos y )

Expanding ( 3.43 ) , we find 1 | x – X ' ! 1Σ ( ες ) ( 3.44 ) I = 0 For points off the

it is ...

If the point x is on the z

**axis**, the right - hand side reduces to ( 3.38 ) , while theleft - hand side becomes : 1 1 | x – X'l 1 ir – p ' ! ( 3.43 ) ( r2 + p 2 2rr ' cos y )

Expanding ( 3.43 ) , we find 1 | x – X ' ! 1Σ ( ες ) ( 3.44 ) I = 0 For points off the

**axis**it is ...

Page 166

( c ) Show that at the end of a long solenoid the magnetic induction near the

has components 20NI πΝΙ B , - B ... conductor of radius a has a hole of radius b

bored parallel to , and centered a distance d from , the cylinder

( c ) Show that at the end of a long solenoid the magnetic induction near the

**axis**has components 20NI πΝΙ B , - B ... conductor of radius a has a hole of radius b

bored parallel to , and centered a distance d from , the cylinder

**axis**( d + b < a ) .Page 422

The speed of the particle is constant so that at any position along the z

v2 = 0 v 2 ( 12.126 ) where v.2 = 0.02 + 0,10 % 2 is the square of the speed at z =

0. If we assume that the flux linked is a constant of the motion , then ( 12.125 ) ...

The speed of the particle is constant so that at any position along the z

**axis**v ,? +v2 = 0 v 2 ( 12.126 ) where v.2 = 0.02 + 0,10 % 2 is the square of the speed at z =

0. If we assume that the flux linked is a constant of the motion , then ( 12.125 ) ...

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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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