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Page 121
... dipole moments . This orientation polari- zation is important in " polar ” substances such as HCl and H2O and was first discussed by Debye ( 1912 ) . All molecules are assumed to possess a permanent dipole moment po which can be ...
... dipole moments . This orientation polari- zation is important in " polar ” substances such as HCl and H2O and was first discussed by Debye ( 1912 ) . All molecules are assumed to possess a permanent dipole moment po which can be ...
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 p → m . Thus we find ik B = eikr 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 p → m . Thus we find ik B = eikr k2 ( n x m ) x n + [ 3n ( n⚫ m ) ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ