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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 Lo 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 = zą ' — z1 , where z , ' and z ' are the coordinates of the end points ...
... Consider a rod of length Lo 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 = zą ' — z1 , where z , ' and z ' are the coordinates of the end points ...
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