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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 and a = - 2 = ( 1 - 1 + 1 ) ) . for TM modes where xin = 2πδ Xinz 2 ( 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 and a = - 2 = ( 1 - 1 + 1 ) ) . for TM modes where xin = 2πδ Xinz 2 ( 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 |
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4-vector acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ