Classical Theory of Electricity and Magnetism: (a Course of Lectures) |
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Page 2
... exponential term of the form e where Το is related with the mass of the exchanged particle . Such a term makes the interaction fall off sharply with distance , being effectively negligible for r » ro . Now if the interaction is really ...
... exponential term of the form e where Το is related with the mass of the exchanged particle . Such a term makes the interaction fall off sharply with distance , being effectively negligible for r » ro . Now if the interaction is really ...
Page 179
... exponential part merely makes the variables oscillate while the falling off is as 1 / r ) we have from equations ( 27 ) and ( 29 ) of the last chapter and equation ( 2 ) above Eoo ( r ) = iw ¿ ® [ ( n · A ̧ ) n – A ... ]。 ίω = f ( r ) ...
... exponential part merely makes the variables oscillate while the falling off is as 1 / r ) we have from equations ( 27 ) and ( 29 ) of the last chapter and equation ( 2 ) above Eoo ( r ) = iw ¿ ® [ ( n · A ̧ ) n – A ... ]。 ίω = f ( r ) ...
Page 199
... exponential e should not be confused . ) ( The sine term being an odd function of vanishes on integration . ) Now ao + cos ( w § ) . d b2 [ 52 + ( 1 - B3 ) ] 12 cos ndn = 2 1/2 ( η = ω ξ ) w282 1/2 n2 + u2 ( 1 - B2 ) The infinite ...
... exponential e should not be confused . ) ( The sine term being an odd function of vanishes on integration . ) Now ao + cos ( w § ) . d b2 [ 52 + ( 1 - B3 ) ] 12 cos ndn = 2 1/2 ( η = ω ξ ) w282 1/2 n2 + u2 ( 1 - B2 ) The infinite ...
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