Classical ElectrodynamicsProblems after each chapter |
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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 , according to Coulomb's law , is : 3 | F | = q2 a a2 ข - a2 y2 2 ( 2.6 ) For large separations the force is an inverse cube law , but close to the sphere it is proportional to the inverse square of the distance away from the ...
... force , according to Coulomb's law , is : 3 | F | = q2 a a2 ข - a2 y2 2 ( 2.6 ) For large separations the force is an inverse cube law , but close to the sphere it is proportional to the inverse square of the distance away from the ...
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 |
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