Classical Electrodynamics |
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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 ' is a Lorentz invariant quantity , it follows that p ...
... 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 ' is a Lorentz invariant quantity , it follows that p ...
Page 567
... sides of ( 16.22 ) . Then we can put 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 h ( kr ' ) . Then we ...
... sides of ( 16.22 ) . Then we can put 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 h ( kr ' ) . Then we ...
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