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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 : - 2 qe 2 = | F | = - a2 ( 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 surface of ...
... force , according to Coulomb's law , is : - 2 qe 2 = | F | = - a2 ( 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 surface of ...
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 angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer factor force equation frame frequency given Green's function impact parameter incident particle integral Kirchhoff Lagrangian Laplace's equation Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular plasma polarization power radiated problem radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ