## Classical ElectrodynamicsProblems after each chapter |

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Page 22

1.8 This expression for

high fields “ must ” contain considerable

thing about ( 1.55 ) . The

1.8 This expression for

**energy**density is intuitively reasonable , since regions ofhigh fields “ must ” contain considerable

**energy**. There is perhaps one puzzlingthing about ( 1.55 ) . The

**energy**density is positive definite . Consequently its ...Page 448

The corresponding relativistic expression without the density effect is , from (

13.36 ) , dE ( ze ) 0 ) , 1.123yc In ( 13.78 ) dx / b > a ca αω ) ( 1.1234c ) 1 We see

that the density effect produces a simplification in that the asymptotic

no ...

The corresponding relativistic expression without the density effect is , from (

13.36 ) , dE ( ze ) 0 ) , 1.123yc In ( 13.78 ) dx / b > a ca αω ) ( 1.1234c ) 1 We see

that the density effect produces a simplification in that the asymptotic

**energy**lossno ...

Page 537

( a ) Calculate the cross sections for

collisions ( write them as functions of Q / I as far as possible and in units of

2722e4 | mvora ) . Plot the two distributions for Qli > 1 for nonrelativistic motion of

the incident ...

( a ) Calculate the cross sections for

**energy**transfer Q for close and distantcollisions ( write them as functions of Q / I as far as possible and in units of

2722e4 | mvora ) . Plot the two distributions for Qli > 1 for nonrelativistic motion of

the incident ...

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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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