Classical ElectrodynamicsProblems after each chapter |
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Page 297
... side of the sheet . The problem is to calculate the diffracted fields on the other side of the sheet . Since the sheet is assumed flat , the simple vector theorem ( 9.82 ) is appro- priate . Evidently the problem is solved if we can ...
... side of the sheet . The problem is to calculate the diffracted fields on the other side of the sheet . Since the sheet is assumed flat , the simple vector theorem ( 9.82 ) is appro- priate . Evidently the problem is solved if we can ...
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 d'x 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 d'x is a Lorentz invariant quantity , it follows that P1 ...
Page 555
... sides with a typical Xm , 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 + k2 ...
... sides with a typical Xm , 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 + k2 ...
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Common terms and phrases
4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ