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Page 25
... given by 1 де = 1 噐一(元 + 元) Е дп where R1 and R , 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 1 де = 1 噐一(元 + 元) Е дп where R1 and R , 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 w , enters the layer without reflection because of the slow change in n ...
... 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 w , enters the layer without reflection because of the slow change in n ...
Page 305
... given by r - 2 times equation ( 9.23 ) . ( b ) Show that the imaginary part of S has components in the r and directions given by Im Sr Im So = = ck 8π - 5 | p | 2 sin2 0 ck p2 4π5 ( 1 + k22 ) sin 0 cos 0 Make a sketch to show the ...
... given by r - 2 times equation ( 9.23 ) . ( b ) Show that the imaginary part of S has components in the r and directions given by Im Sr Im So = = ck 8π - 5 | p | 2 sin2 0 ck p2 4π5 ( 1 + k22 ) sin 0 cos 0 Make a sketch to show the ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
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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 classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result 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