Classical Theory of Electricity and Magnetism: (a Course of Lectures) |
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Page 10
... physical situation , so the intensity should not change . ) We next consider the case of a distribution of dipoles . One may imagine opposite charges of equal density distributed over two parallel surfaces separated by a short distance ...
... physical situation , so the intensity should not change . ) We next consider the case of a distribution of dipoles . One may imagine opposite charges of equal density distributed over two parallel surfaces separated by a short distance ...
Page 23
... field and the charge distribution if π.χ пу ΠΖ C Ø = sin sin sin [ for 0≤x≤a , 0 ≤ y ≤b , 0 ≤ z < cl a and give a physical picture of the situation . multipole moments We suppose that the charges are contained in GAUSS'S THEOREM 23.
... field and the charge distribution if π.χ пу ΠΖ C Ø = sin sin sin [ for 0≤x≤a , 0 ≤ y ≤b , 0 ≤ z < cl a and give a physical picture of the situation . multipole moments We suppose that the charges are contained in GAUSS'S THEOREM 23.
Page 61
... physical situation , you have a solution of a physically relevant problem . If y be the imaginary ( real ) part corresponding to ø , then the y - constant lines are everywhere orthogonal to the ø - constant lines . Thus while Ø ...
... physical situation , you have a solution of a physically relevant problem . If y be the imaginary ( real ) part corresponding to ø , then the y - constant lines are everywhere orthogonal to the ø - constant lines . Thus while Ø ...
Contents
The empirical basis of electrostatics | 1 |
Direct calculation of fields | 7 |
dipoles9 The Dirac 8function13 | 13 |
Copyright | |
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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