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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 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 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 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 p → m . Thus we find eikr B = k2 ( n x m ) x n − + [ 3n ( n · m ) ...
Contents
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Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
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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 classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result 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