Classical ElectrodynamicsProblems after each chapter |
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Page 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 bodies . At the moment ...
... 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 bodies . At the moment ...
Page 298
... fields will be the same as if the hole were not there , namely , normal E , and tangential Bo . The electric field lines might appear as shown in Fig . 9.12 . Since the departures of the fields E and B from their unperturbed values E ...
... fields will be the same as if the hole were not there , namely , normal E , and tangential Bo . The electric field lines might appear as shown in Fig . 9.12 . Since the departures of the fields E and B from their unperturbed values E ...
Page 614
... electric field is dimensionally different from force per unit charge , There is , however , nothing to be gained by this extra freedom in the definition of E , since E is the first derived field quantity to be defined . Only when we ...
... electric field is dimensionally different from force per unit charge , There is , however , nothing to be gained by this extra freedom in the definition of E , since E is the first derived field quantity to be defined . Only when we ...
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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ