Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 89
Page 24
... magnitude 47σ , where σ is the charge density per unit area on the surface . 1.2 Two infinite , conducting , plane sheets of uniform thicknesses t1 and tą , respectively , are placed parallel to one another with their adjacent faces ...
... magnitude 47σ , where σ is the charge density per unit area on the surface . 1.2 Two infinite , conducting , plane sheets of uniform thicknesses t1 and tą , respectively , are placed parallel to one another with their adjacent faces ...
Page 475
... magnitude of applied force . For circular motion , the magnitude of the rate of change of momentum ( which is equal to the applied force ) is ymv . Consequently , ( 14.46 ) can be written 2 Peircular ( t ' ) = e2 3 m2c3 22 dt ( 14.47 ) ...
... magnitude of applied force . For circular motion , the magnitude of the rate of change of momentum ( which is equal to the applied force ) is ymv . Consequently , ( 14.46 ) can be written 2 Peircular ( t ' ) = e2 3 m2c3 22 dt ( 14.47 ) ...
Page 614
... magnitude of the two mechanical forces ( A.2 ) and ( A.4 ) for known charges and currents , the magnitude of the ratio k1 / k , in free space can be found . The numerical value is closely given by the square of the velocity of light in ...
... magnitude of the two mechanical forces ( A.2 ) and ( A.4 ) for known charges and currents , the magnitude of the ratio k1 / k , in free space can be found . The numerical value is closely given by the square of the velocity of light in ...
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