Classical Electrodynamics |
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Page 4
... function has as argument a function f ( x ) of the independent variable x , it can be transformed according to the rule , 1 ( 5 ) 8 ( f ( x ) ) = d ( x · xo ) , where f ( x ) = 0 . df dx This can be proved by noting that d ( ƒ ) df = d ...
... function has as argument a function f ( x ) of the independent variable x , it can be transformed according to the rule , 1 ( 5 ) 8 ( f ( x ) ) = d ( x · xo ) , where f ( x ) = 0 . df dx This can be proved by noting that d ( ƒ ) df = d ...
Page 18
... functions . " In obtaining result ( 1.36 ) —not a solution - we chose the function y to be 1 / xx ' , it being the potential of a unit point charge , satisfying the equation : - V / 2 - 1 · x'l = −4πÔ ( x − x ' ) - ( 1.31 ) The function ...
... functions . " In obtaining result ( 1.36 ) —not a solution - we chose the function y to be 1 / xx ' , it being the potential of a unit point charge , satisfying the equation : - V / 2 - 1 · x'l = −4πÔ ( x − x ' ) - ( 1.31 ) The function ...
Page 78
... function as a series of products of the functions appropriate to the coordi- nates in question . We first illustrate the type of expansion involved by considering spherical coordinates . For the case of no boundary surfaces , except at ...
... function as a series of products of the functions appropriate to the coordi- nates in question . We first illustrate the type of expansion involved by considering spherical coordinates . For the case of no boundary surfaces , except at ...
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss 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 modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result 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