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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 o ( 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 o ( x ) on it , and another surface S ' , lying close to S , have an equal and opposite ...
Page 132
... dipole . In the presence of magnetic materials the dipole tends to align itself in a certain direction . That direction is by definition the direction of the magnetic - flux density , denoted by B , provided the dipole is sufficiently ...
... dipole . In the presence of magnetic materials the dipole tends to align itself in a certain direction . That direction is by definition the direction of the magnetic - flux density , denoted by B , provided the dipole is sufficiently ...
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 → m . Thus we find P eikr B = = k2 ( n × m ) × n + [ 3n ( n⚫ 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 → m . Thus we find P eikr B = = k2 ( n × m ) × n + [ 3n ( n⚫ m ) ...
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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ