## Classical electrodynamics |

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Page 10

The

infinitesimally close to S while the surface-charge density <r(x) becomes infinite

in such a manner that the product of CT(X) and the local separation d(\) of S and

...

The

**dipole**-layer distribution of strength D(x) is formed by letting S' approachinfinitesimally close to S while the surface-charge density <r(x) becomes infinite

in such a manner that the product of CT(X) and the local separation d(\) of S and

...

Page 132

The basic entity in magnetic studies was what we now know as a magnetic

. In the presence of magnetic materials the

direction. That direction is by definition the direction of the magnetic-flux density,

...

The basic entity in magnetic studies was what we now know as a magnetic

**dipole**. In the presence of magnetic materials the

**dipole**tends to align itself in a certaindirection. That direction is by definition the direction of the magnetic-flux density,

...

Page 274

Considering only the magnetization term, we have the vector potential, eikr/ 1 \ A(

x) = ik(u x m) — 1 - — (9.33) r \ ikrl where m is the magnetic

M <Px = — | (x x J) <Px (9.34) J 2cJ The fields can be determined by noting that ...

Considering only the magnetization term, we have the vector potential, eikr/ 1 \ A(

x) = ik(u x m) — 1 - — (9.33) r \ ikrl where m is the magnetic

**dipole**moment, m = I,M <Px = — | (x x J) <Px (9.34) J 2cJ The fields can be determined by noting that ...

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### Contents

Introduction to Electrostatics | 1 |

Scalar potential | 7 |

Greens theorem | 14 |

Copyright | |

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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