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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 , ( 5 ) 8 ( f ( x ) ) = 1 df dx - d ( x − xo ) , where f ( x ) = 0 . This can be proved by noting that 8 ( ƒ ) df ...
... function has as argument a function f ( x ) of the independent variable x , it can be transformed according to the rule , ( 5 ) 8 ( f ( x ) ) = 1 df dx - d ( x − xo ) , where f ( x ) = 0 . This can be proved by noting that 8 ( ƒ ) df ...
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 : 1 V / 2 | x − x ' ] - = -4πd ( x − x ' ) - ( 1.31 ) The ...
... 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 : 1 V / 2 | x − x ' ] - = -4πd ( x − x ' ) - ( 1.31 ) The ...
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 ...
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