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... side of the figure is a constant , uniform magnetic induction Bo , parallel to the x axis . A particle spirals around the field lines with a gyration radius a and a velocity pa , while moving with a uniform velocity v , along the lines ...
... side of the figure is a constant , uniform magnetic induction Bo , parallel to the x axis . A particle spirals around the field lines with a gyration radius a and a velocity pa , while moving with a uniform velocity v , along the lines ...
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... sides with a typical X , and integrate over all angles . All the terms on the left - hand side of the equation involving gim ( r ) vanish because of orthogonality , and only one term involving an fim ( r ) survives : ď2 2 d + Ldr2 r dr ...
... sides with a typical X , and integrate over all angles . All the terms on the left - hand side of the equation involving gim ( r ) vanish because of orthogonality , and only one term involving an fim ( r ) survives : ď2 2 d + Ldr2 r dr ...
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... sides of ( 16.22 ) . Then we can put | x − x ' ~ r ' — n⚫x on the left - hand side , where n is a unit vector in the direction of x ' . On the right side r 、= r ' and r = r . Furthermore we can use the asymptotic form ( 16.13 ) for h ...
... sides of ( 16.22 ) . Then we can put | x − x ' ~ r ' — n⚫x on the left - hand side , where n is a unit vector in the direction of x ' . On the right side r 、= r ' and r = r . Furthermore we can use the asymptotic form ( 16.13 ) for h ...
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