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Page 392
... sides with respect to time , then the left - hand side becomes the momentum or energy of the particle while the right - hand side is the four - dimensional integral of f . Since dx is a Lorentz invariant quantity , it follows that p1 ...
... sides with respect to time , then the left - hand side becomes the momentum or energy of the particle while the right - hand side is the four - dimensional integral of f . Since dx is a Lorentz invariant quantity , it follows that p1 ...
Page 555
... 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 ...
Page 567
... sides of ( 16.22 ) . Then we can put | x − x ' ~ r'nx 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 h1 ( kr ...
... sides of ( 16.22 ) . Then we can put | x − x ' ~ r'nx 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 h1 ( kr ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ 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 diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer 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 plasma polarization power radiated problem radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ