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Page 247
... mode is the only propagating mode . Beyond that frequency other modes rapidly begin to enter . The field configurations of the TE10 mode and other modes are shown in many books , e.g. , American Institute of Physics Handbook , McGraw ...
... mode is the only propagating mode . Beyond that frequency other modes rapidly begin to enter . The field configurations of the TE10 mode and other modes are shown in many books , e.g. , American Institute of Physics Handbook , McGraw ...
Page 263
... modes , marked by the circles at the intersections of the two curves , exist . The vertical asymptotes are given by the roots of = 0. If the maximum value of ya is smaller than the first root 2.405 ) , there can be no intersection of ...
... modes , marked by the circles at the intersections of the two curves , exist . The vertical asymptotes are given by the roots of = 0. If the maximum value of ya is smaller than the first root 2.405 ) , there can be no intersection of ...
Page 576
... modes 2πδ ' and a 1 ( 1 + 1 ) е = for TM modes 2пб 2 xin where xin = ( a / c ) win for TM modes . 16.10 Discuss the normal modes of oscillation of a perfectly conducting solid sphere of radius a in free space . ( a ) Determine the ...
... modes 2πδ ' and a 1 ( 1 + 1 ) е = for TM modes 2пб 2 xin where xin = ( a / c ) win for TM modes . 16.10 Discuss the normal modes of oscillation of a perfectly conducting solid sphere of radius a in free space . ( a ) Determine the ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation frequency given Green's function impact parameter incident particle integral Kirchhoff Lagrangian Laplace's equation Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain oscillations P₁ parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ