Classical Theory of Electricity and Magnetism: (a Course of Lectures) |
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Page 113
... dissipation of energy due to induced currents is Zπ2r w2 B2 / R . 5. Two circuits having inductors L1 , L2 and resistance R1 , R2 respectively are so placed that their mutual inductance is M. A sinusoidal electromotive force is ...
... dissipation of energy due to induced currents is Zπ2r w2 B2 / R . 5. Two circuits having inductors L1 , L2 and resistance R1 , R2 respectively are so placed that their mutual inductance is M. A sinusoidal electromotive force is ...
Page 148
... dissipation of electromagnetic energy into heat . This dissipation may be evaluated by calculating the flux of electromagnetic energy into the body of the conductor in case of infinite conductivity this flux vanishes as E has no ...
... dissipation of electromagnetic energy into heat . This dissipation may be evaluated by calculating the flux of electromagnetic energy into the body of the conductor in case of infinite conductivity this flux vanishes as E has no ...
Page 149
... dissipated as heat during one cycle of the mode energy of the mode energy dissipated in time1 / w where w is the angular frequency of the mode . ( 33 ) There is an intimate connection between Q and the sharpness of response of the ...
... dissipated as heat during one cycle of the mode energy of the mode energy dissipated in time1 / w where w is the angular frequency of the mode . ( 33 ) There is an intimate connection between Q and the sharpness of response of the ...
Contents
The empirical basis of electrostatics | 1 |
Direct calculation of fields | 7 |
dipoles9 The Dirac 8function13 | 13 |
Copyright | |
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angle angular axes axis B₁ boundary conditions calculate called charge density charged particle coil components conductor consider coordinates cos² cose dielectric constant dipole dipole moment direction distance E₁ electric field electromagnetic field electromotive force electron electrostatic equation 16 expression field due field point finite fluid formula frame frequency function gives Hence incident interaction Laplace's equation linear Lorentz Lorentz transformation magnetic field magnitude Maxwell's equations momentum motion normal obtain orthogonal P₁ permanent magnets perpendicular photon plane plasma point charge polarization Poynting vector R₁ radiation field radiation reaction radius refracted region scalar sin² solution spherical surface integral symmetry tensor term theorem theory of relativity transformation transverse uniform vanishes vector potential velocity wave length Απ дв дг ді дх