Classical ElectrodynamicsProblems after each chapter |
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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 Jo ( x ) = 0. If the maximum value of ya is smaller than the first root ( x01 2.405 ) , there can be no ...
... modes , marked by the circles at the intersections of the two curves , exist . The vertical asymptotes are given by the roots of Jo ( x ) = 0. If the maximum value of ya is smaller than the first root ( x01 2.405 ) , there can be no ...
Page 576
... modes where xin = a 0 = ( 1 - 11 + 1 ) ) , 2πδ xin2 ( a / c ) win for TM modes . 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 where xin = a 0 = ( 1 - 11 + 1 ) ) , 2πδ xin2 ( a / c ) win for TM modes . 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 ...
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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ