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Page 10
... dipole - layer distribution on a surface S. A dipole layer can be imagined as being formed by letting the surface S have a surface - charge density σ ( x ) on it , and another surface S ' , lying close to S , have an equal and opposite ...
... dipole - layer distribution on a surface S. A dipole layer can be imagined as being formed by letting the surface S have a surface - charge density σ ( x ) on it , and another surface S ' , lying close to S , have an equal and opposite ...
Page 150
... dipole shows that the dipole tends to orient itself parallel to the field in the position of lowest potential energy . We remark in passing that ( 5.73 ) is not the total energy of the magnetic moment in the external field . In bringing ...
... dipole shows that the dipole tends to orient itself parallel to the field in the position of lowest potential energy . We remark in passing that ( 5.73 ) is not the total energy of the magnetic moment in the external field . In bringing ...
Page 274
... dipole . This means that the magnetic induction for the present magnetic dipole source will be equal to the electric field for the electric dipole , with the substitution pm . Thus we find B = k2 ( n x m ) eikr r + [ 3n ( n · m ) – m ] ...
... dipole . This means that the magnetic induction for the present magnetic dipole source will be equal to the electric field for the electric dipole , with the substitution pm . Thus we find B = k2 ( n x m ) eikr r + [ 3n ( n · m ) – m ] ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ