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 9
... E = 0 . 1.6 Surface Distributions of Charges and Dipoles and Discontinuities in the Electric Field and Potential One of the common problems in electrostatics is the determination of electric field or potential due to a given surface ...
... E = 0 . 1.6 Surface Distributions of Charges and Dipoles and Discontinuities in the Electric Field and Potential One of the common problems in electrostatics is the determination of electric field or potential due to a given surface ...
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 ...
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