Classical Electrodynamics |
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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 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 → m . Thus we find P ik eikr B = k2 ( n x m ) x 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 ik eikr B = k2 ( n x m ) x n + [ 3n ( n⚫ m ) ...
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss factor force equation frame frequency given Green's function impact parameter incident particle integral Kirchhoff Lagrangian Laplace's equation Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ