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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 370
... derivative will behave in the same way because of the invariance of dr . But its ordinary time derivative will not have the same transformation properties . From ( 11.62 ) we see that a certain proper time interval ( 7271 ) will be seen ...
... derivative will behave in the same way because of the invariance of dr . But its ordinary time derivative will not have the same transformation properties . From ( 11.62 ) we see that a certain proper time interval ( 7271 ) will be seen ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ