## Classical electrodynamics |

### From inside the book

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Page 16

We want to show the uniqueness of the solution of Poisson's equation, V2<1> =

— 4np,

conditions on the closed bounding surface S. We suppose, to the contrary, that

there ...

We want to show the uniqueness of the solution of Poisson's equation, V2<1> =

— 4np,

**inside**a volume V subject to either Dirichlet or Neumann boundaryconditions on the closed bounding surface S. We suppose, to the contrary, that

there ...

Page 236

Then, just as in the static case, there is no electric field

charges

instantly in response to changes in the fields, no matter how rapid, and always ...

Then, just as in the static case, there is no electric field

**inside**the conductors. Thecharges

**inside**a perfect conductor are assumed to be so mobile that they moveinstantly in response to changes in the fields, no matter how rapid, and always ...

Page 370

Consequently as time goes on it would trace out a path, called its world line,

the ...

Consequently as time goes on it would trace out a path, called its world line,

**inside**the upper half- cone, e.g., the curve OB. Since the path of the system lies**inside**the upper half-cone for times / > 0, that region is called the future. Similarlythe ...

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### Contents

Introduction to Electrostatics | 1 |

Scalar potential | 7 |

Greens theorem | 14 |

Copyright | |

17 other sections not shown

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### Common terms and phrases

4-vector acceleration angular distribution approximation assumed atomic average 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 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 photon 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