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Page 243
... TRANSVERSE MAGNETIC ( TM ) The boundary condition is B1 = 0 everywhere E , s = 0 TRANSVERSE ELECTRIC ( TE ) E. = 0 everywhere The boundary condition is дв = = 0 an is The designations " Electric ( or E ) Waves " and " Magnetic ( or H ) ...
... TRANSVERSE MAGNETIC ( TM ) The boundary condition is B1 = 0 everywhere E , s = 0 TRANSVERSE ELECTRIC ( TE ) E. = 0 everywhere The boundary condition is дв = = 0 an is The designations " Electric ( or E ) Waves " and " Magnetic ( or H ) ...
Page 382
... transverse electric field E1 as B → 1. Even at nonrelativistic velocities where y 1 , this magnetic induction is equivalent to ~ B ~ qvx r 7.3 ( 11.119 ) which is just the Ampère - Biot - Savart expression for the magnetic field of a ...
... transverse electric field E1 as B → 1. Even at nonrelativistic velocities where y 1 , this magnetic induction is equivalent to ~ B ~ qvx r 7.3 ( 11.119 ) which is just the Ampère - Biot - Savart expression for the magnetic field of a ...
Page 639
... Transverse magnetic ( TM ) waves , at- tenuation of , in wave guides , 251 connection of , with multipole mo- ments , 553 f . cylindrical , 243 in cylindrical cavity , 254 in dielectric wave guide , 263 spherical , 545 Transverse waves ...
... Transverse magnetic ( TM ) waves , at- tenuation of , in wave guides , 251 connection of , with multipole mo- ments , 553 f . cylindrical , 243 in cylindrical cavity , 254 in dielectric wave guide , 263 spherical , 545 Transverse waves ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer factor force equation frame 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 P₂ parallel perpendicular plasma polarization power radiated problem radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ