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Page 172
... derivative in ( 6.4 ) must take into account this motion . The flux through the circuit may change because ( a ) the flux changes with time at a point , or ( b ) the translation of the circuit changes the location of the boundary . It ...
... derivative in ( 6.4 ) must take into account this motion . The flux through the circuit may change because ( a ) the flux changes with time at a point , or ( b ) the translation of the circuit changes the location of the boundary . It ...
Page 188
... derivatives on the boundary surface S. We thus assume that there are no sources within V and that the initial values of y ... derivative of the delta function can be integrated by parts with respect to the time t ' . Then the Kirchhoff ...
... derivatives on the boundary surface S. We thus assume that there are no sources within V and that the initial values of y ... derivative of the delta function can be integrated by parts with respect to the time t ' . Then the Kirchhoff ...
Page 311
... derivative of the velocity on the left side of ( 10.2 ) is the convective derivative , d dt д = — + v . V ді ( 10.4 ) which gives the total time rate of change of a quantity moving instanta- neously with the velocity v . With the ...
... derivative of the velocity on the left side of ( 10.2 ) is the convective derivative , d dt д = — + v . V ді ( 10.4 ) which gives the total time rate of change of a quantity moving instanta- neously with the velocity v . With the ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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 coefficients collisions component conducting conductor consider 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave 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 number wavelength ΦΩ