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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 a = + v . V Ət ( 10.4 ) which gives the total time rate of change of a quantity moving instanta- neously with the velocity v . With the neglect ...
... derivative of the velocity on the left side of ( 10.2 ) is the convective derivative , d dt a = + v . V Ət ( 10.4 ) which gives the total time rate of change of a quantity moving instanta- neously with the velocity v . With the neglect ...
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