Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 82
Page 25
... given by 1 де = Е дп 1 · - ( + ) R1 R2 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 within a volume V and a ...
... given by 1 де = Е дп 1 · - ( + ) R1 R2 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 within a volume V and a ...
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 w1 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 w1 enters the layer without reflection because of the slow change in no ...
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 S , = ck 8πу5 | p | 2 sin2 0 Im So = ck pl2 4прб 12 ( 1 + k2r2 ) sin 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 S , = ck 8πу5 | p | 2 sin2 0 Im So = ck pl2 4прб 12 ( 1 + k2r2 ) sin cos 0 Make a sketch to show the ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
18 other sections not shown
Other editions - View all
Common terms and phrases
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