## Classical electrodynamics |

### From inside the book

Results 1-3 of 99

Page 9

If the path is closed, the line integral is zero, r E-dl = Q (1.21) a result that can also

be obtained directly from Coulomb's law. Then application of Stokes's theorem [if

A(x) is a vector field, S is an open

If the path is closed, the line integral is zero, r E-dl = Q (1.21) a result that can also

be obtained directly from Coulomb's law. Then application of Stokes's theorem [if

A(x) is a vector field, S is an open

**surface**, and C is the closed curve bounding ...Page 10

The tangential component of electric field can be shown to be continuous across

a boundary

It is only necessary to take a rectangular path with negligible ends and one side ...

The tangential component of electric field can be shown to be continuous across

a boundary

**surface**by using (1.21) for the line integral of E around a closed path.It is only necessary to take a rectangular path with negligible ends and one side ...

Page 240

According to Ohm's law, there exists a current density J near the

conductor: J = aEc = (1 - 0(n x H^-W-<W (8.13) V 6TT The time-average rate of

dissipation of energy per unit volume in ohmic losses is £J • E* = (l/2<r) |J|2, so

that ...

According to Ohm's law, there exists a current density J near the

**surface**of theconductor: J = aEc = (1 - 0(n x H^-W-<W (8.13) V 6TT The time-average rate of

dissipation of energy per unit volume in ohmic losses is £J • E* = (l/2<r) |J|2, so

that ...

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### Contents

Introduction to Electrostatics | 1 |

Scalar potential | 7 |

Greens theorem | 14 |

Copyright | |

19 other sections not shown

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### Common terms and phrases

4-vector acceleration angular distribution approximation assumed atomic axis behavior Bessel functions boundary conditions bremsstrahlung calculate Chapter charge density charge q charged particle classical coefficients collisions component conductor Consequently consider coordinates cross section current density cylinder defined delta function dielectric constant diffraction dimensions dipole direction discussed effects electric field electromagnetic fields electron electrostatic emitted energy loss expansion expression factor force equation frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation limit linear Lorentz invariant Lorentz transformation macroscopic magnetic field magnetic induction magnitude Maxwell's equations meson molecules momentum multipole multipole expansion nonrelativistic obtain orbit oscillations parallel perpendicular plane wave plasma point charge polarization power radiated problem quantum quantum-mechanical radiative radius region relativistic result scalar scattering shown in Fig shows solid angle solution spectrum spherical surface theorem transverse vanishes vector potential wave equation wave number wavelength written zero