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Page 174
... consider these contributions . Suppose for a moment that we have only a single circuit with a constant current I flowing in it . If the flux through the circuit changes , an electro- motive force & is induced around it . In order to ...
... consider these contributions . Suppose for a moment that we have only a single circuit with a constant current I flowing in it . If the flux through the circuit changes , an electro- motive force & is induced around it . In order to ...
Page 208
... considers making a linear superposition . Initially we will find it most convenient to use k as an independent variable . To allow for the possibility of dispersion we will consider w as a general function of k : @ = w ( k ) ( 7.25 ) ...
... considers making a linear superposition . Initially we will find it most convenient to use k as an independent variable . To allow for the possibility of dispersion we will consider w as a general function of k : @ = w ( k ) ( 7.25 ) ...
Page 358
... Consider a rod of length L at rest parallel to the z ' axis in the system K ' of the previous section , as indicated schematically in Fig . 11.6 . By definition L1 = z2z , where z , ' and z ' are the coordinates of the end points of the ...
... Consider a rod of length L at rest parallel to the z ' axis in the system K ' of the previous section , as indicated schematically in Fig . 11.6 . By definition L1 = z2z , where z , ' and z ' are the coordinates of the end points of the ...
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