## Classical electrodynamics |

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Results 1-3 of 69

Page 63

If the point x is on the z

hand side becomes : 1 1 1 |x - x'| (r2 + r'2 - 2rr' cos y)" |r - r'| Expanding (3.43), we

find 1 _ 1 V (r<V - x'| r> £j \rj (3.43) (3.44) For points off the

If the point x is on the z

**axis**, the right-hand side reduces to (3.38), while the left-hand side becomes : 1 1 1 |x - x'| (r2 + r'2 - 2rr' cos y)" |r - r'| Expanding (3.43), we

find 1 _ 1 V (r<V - x'| r> £j \rj (3.43) (3.44) For points off the

**axis**it is only ...Page 166

(c) Show that at the end of a long solenoid the magnetic induction near the

has components 2WV7 WVY/p "z — i "a — — 5.3 A cylindrical conductor of radius

a has a hole of radius b bored parallel to, and centered a distance d from, the ...

(c) Show that at the end of a long solenoid the magnetic induction near the

**axis**has components 2WV7 WVY/p "z — i "a — — 5.3 A cylindrical conductor of radius

a has a hole of radius b bored parallel to, and centered a distance d from, the ...

Page 422

The speed of the particle is constant so that at any position along the z

* = v<? (12.126) where v0z = v^f + i;||02 is the square of the speed at z = 0. If we

assume that the flux linked is a constant of the motion, then (12.125) allows us to

...

The speed of the particle is constant so that at any position along the z

**axis**v* + v* = v<? (12.126) where v0z = v^f + i;||02 is the square of the speed at z = 0. If we

assume that the flux linked is a constant of the motion, then (12.125) allows us to

...

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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 Babinet's principle behavior 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 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 plane wave plasma point charge polarization power radiated problem quantum quantum-mechanical radiative radius region relativistic result scalar scattering screen shown in Fig shows solid angle solution spectrum spherical surface theorem transverse unit vanishes vector potential wave equation wave number wavelength written zero