Classical Theory of Electricity and Magnetism: (a Course of Lectures) |
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Page 33
... molecules of the medium we have positive charges ( protons in the nuclei ) as also electrons outside the nuclei ... molecule is an isosceles triangle with the hydrogen at the vertex and it possesses an intrinsic dipole moment . In ...
... molecules of the medium we have positive charges ( protons in the nuclei ) as also electrons outside the nuclei ... molecule is an isosceles triangle with the hydrogen at the vertex and it possesses an intrinsic dipole moment . In ...
Page 43
... molecule can ' sec ' the discrete molecular distribution and the continuous assumption must be given up . Hence to calculate the effective field on a particular molecule , we proceed as follows . ( a ) Consider a sphere of radius r ...
... molecule can ' sec ' the discrete molecular distribution and the continuous assumption must be given up . Hence to calculate the effective field on a particular molecule , we proceed as follows . ( a ) Consider a sphere of radius r ...
Page 44
... molecule as the dipole moment developed per molecule due to unit field strength . Thus if a be the polarizability of a molecule , the dipole moment per molecule will be μ = αε ' effective = α ( E + 4TP ) 3 The polarization P = nμ where ...
... molecule as the dipole moment developed per molecule due to unit field strength . Thus if a be the polarizability of a molecule , the dipole moment per molecule will be μ = αε ' effective = α ( E + 4TP ) 3 The polarization P = nμ where ...
Contents
The empirical basis of electrostatics | 1 |
Direct calculation of fields | 7 |
dipoles9 The Dirac 8function13 | 13 |
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angle angular axes axis B₁ boundary conditions calculate called charge density charged particle coil components conductor consider coordinates cos² cose dielectric constant dipole dipole moment direction distance E₁ electric field electromagnetic field electromotive force electron electrostatic equation 16 expression field due field point finite fluid formula frame frequency function gives Hence incident interaction Laplace's equation linear Lorentz Lorentz transformation magnetic field magnitude Maxwell's equations momentum motion normal obtain orthogonal P₁ permanent magnets perpendicular photon plane plasma point charge polarization Poynting vector R₁ radiation field radiation reaction radius refracted region scalar sin² solution spherical surface integral symmetry tensor term theorem theory of relativity transformation transverse uniform vanishes vector potential velocity wave length Απ дв дг ді дх