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Page 2
... forces of Coulomb . 1.2 Electric Field Although the thing that eventually gets measured is a force , it is useful to introduce a concept one step removed from the forces , the concept of an electric field due to some array of charged ...
... forces of Coulomb . 1.2 Electric Field Although the thing that eventually gets measured is a force , it is useful to introduce a concept one step removed from the forces , the concept of an electric field due to some array of charged ...
Page 30
... force between the charge q and the image charge q ' . The distance between them is y — y ' y ( 1 a2 / y2 ) . Hence the attractive force , according to Coulomb's law , is : - = | F | = · 2 ( 9 ) ( 1 – y2 2 ( 2.6 ) For large separations ...
... force between the charge q and the image charge q ' . The distance between them is y — y ' y ( 1 a2 / y2 ) . Hence the attractive force , according to Coulomb's law , is : - = | F | = · 2 ( 9 ) ( 1 – y2 2 ( 2.6 ) For large separations ...
Page 32
... force on a point charge q due to an insulated , conducting sphere of radius a carrying a total charge Q. Positive values mean a repulsion , negative an attraction . The asymptotic dependence of the force has been divided out . Fy2 / q2 ...
... force on a point charge q due to an insulated , conducting sphere of radius a carrying a total charge Q. Positive values mean a repulsion , negative an attraction . The asymptotic dependence of the force has been divided out . Fy2 / q2 ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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