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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 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 Lo = zą - z ' , where z , ' and z ' are the coordinates of the end points ...
... 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 Lo = zą - z ' , where z , ' and z ' are the coordinates of the end points ...
Page 454
... consider only the electromagnetic aspect . The charge distribution of the atomic nucleus can be crudely approximated by a uniform volume distribution inside a sphere of radius R , falling rapidly to zero outside R. This means that the ...
... consider only the electromagnetic aspect . The charge distribution of the atomic nucleus can be crudely approximated by a uniform volume distribution inside a sphere of radius R , falling rapidly to zero outside R. This means that the ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ