## Classical ElectrodynamicsProblems after each chapter |

### From inside the book

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Page 297

The dimensions of the hole are

wavelength of the electromagnetic fields which are

of the sheet . The problem is to calculate the diffracted fields on the other side of

the ...

The dimensions of the hole are

**assumed**to be very small compared to awavelength of the electromagnetic fields which are

**assumed**to exist on one sideof the sheet . The problem is to calculate the diffracted fields on the other side of

the ...

Page 301

... evidently the diffraction contribution , while the integral from the illuminated

region is the reflected wave . To proceed much further we must specify the shape

of the obstacle . We will

.

... evidently the diffraction contribution , while the integral from the illuminated

region is the reflected wave . To proceed much further we must specify the shape

of the obstacle . We will

**assume**that it is a perfectly conducting sphere of radius a.

Page 351

с The difference between the two transit times is 2 ୮ d2 dy At = tz - ti ( 11.6 ) U2

v2 1 c2 If we

ΔΙΑ ) + ( 11.7 ) 2 If the apparatus is now rotated through 90 ° , the transit times ...

с The difference between the two transit times is 2 ୮ d2 dy At = tz - ti ( 11.6 ) U2

v2 1 c2 If we

**assume**that v < c , we can expand the denominators , obtaining d1ΔΙΑ ) + ( 11.7 ) 2 If the apparatus is now rotated through 90 ° , the transit times ...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

Wave Guides and Resonant Cavities | 235 |

Copyright | |

5 other sections not shown

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### Common terms and phrases

acceleration angle angular applied approximation assumed atomic average axis becomes boundary conditions calculate called Chapter charge charged particle classical coefficients collisions compared component conducting Consequently consider constant coordinates cross section cylinder defined density dependence derivative determine dielectric dimensions dipole direction discussed distance distribution effects electric field electromagnetic electron electrostatic energy equal equation example expansion expression factor force frame frequency function given gives incident inside integral involved light limit Lorentz loss magnetic magnetic field magnetic induction magnitude mass means momentum motion moving multipole normal observation obtain origin parallel particle physical plane plasma polarization position potential problem properties radiation radius region relation relative relativistic result satisfy scalar scattering shows side solution space sphere spherical surface transformation unit vanishes vector velocity volume wave written