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Page 25
... given by де = 1 123 -- ( 2 + 2 ) Е дп where R1 and R2 are the principal radii of curvature of the surface . 1.11 Prove Green's reciprocation theorem : If is the potential due to a volume- charge density p and a surface - charge density ...
... given by де = 1 123 -- ( 2 + 2 ) Е дп where R1 and R2 are the principal radii of curvature of the surface . 1.11 Prove Green's reciprocation theorem : If is the potential due to a volume- charge density p and a surface - charge density ...
Page 229
... given layer of the ionosphere , as shown in Fig . 7.12 , reaches a maximum , and then falls abruptly with further increase in height . A pulse of a given frequency o1 enters the layer without reflection because of the slow change in no ...
... given layer of the ionosphere , as shown in Fig . 7.12 , reaches a maximum , and then falls abruptly with further increase in height . A pulse of a given frequency o1 enters the layer without reflection because of the slow change in no ...
Page 305
... given by times equation ( 9.23 ) . ( b ) Show that the imaginary part of S has components in the r and directions given by sign ? Im S , Im So = = ck 8πу5 | p / 2 sin2 0 ck p2 4mr5 ( 1 + k22 ) sin cos 0 Make a sketch to show the ...
... given by times equation ( 9.23 ) . ( b ) Show that the imaginary part of S has components in the r and directions given by sign ? Im S , Im So = = ck 8πу5 | p / 2 sin2 0 ck p2 4mr5 ( 1 + k22 ) sin cos 0 Make a sketch to show the ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle coefficients collisions component conducting conductor consider 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave 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 number wavelength ΦΩ