Classical Theory of Electricity and Magnetism: (a Course of Lectures) |
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Page 144
... transverse waves in pipes similar to those in free unbounded space . Transverse electromagnetic waves ( TEM waves ) By TEM waves we mean Eo ̧ = Bo , = 0. We have then from equations ( 10 ) and ( 7 ) E ° VY ( x , y ) V2 Ψ = 0 ( 21 ) ( 22 ) ...
... transverse waves in pipes similar to those in free unbounded space . Transverse electromagnetic waves ( TEM waves ) By TEM waves we mean Eo ̧ = Bo , = 0. We have then from equations ( 10 ) and ( 7 ) E ° VY ( x , y ) V2 Ψ = 0 ( 21 ) ( 22 ) ...
Page 145
... transverse ( called TM modes ) and the other in which the electric field alone is transverse ( called TE modes ) . TM and TE modes ( a ) In TM modes B2 = 0 , E2 = 0 . ( b ) In TE modes E2 = 0 , B2 0 . In case ( a ) we have from ...
... transverse ( called TM modes ) and the other in which the electric field alone is transverse ( called TE modes ) . TM and TE modes ( a ) In TM modes B2 = 0 , E2 = 0 . ( b ) In TE modes E2 = 0 , B2 0 . In case ( a ) we have from ...
Page 146
... transverse , the Poynting vector will have a transverse component . As however from equation ( 15 ) we find that the transverse com- ponents have a phase difference of π / 2 with the longitudinal components , the time average of the ...
... transverse , the Poynting vector will have a transverse component . As however from equation ( 15 ) we find that the transverse com- ponents have a phase difference of π / 2 with the longitudinal components , the time average of the ...
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