Classical ElectrodynamicsProblems after each chapter |
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Page 193
... tensor of the second rank . While it is possible to deal with rectangular components of momentum , instead of the vectorial form ( 6.93 ) , the tensor can be handled within the framework of vector operations by introducing a ...
... tensor of the second rank . While it is possible to deal with rectangular components of momentum , instead of the vectorial form ( 6.93 ) , the tensor can be handled within the framework of vector operations by introducing a ...
Page 379
... tensor F : ДА ДА Εμν = Эхн дх ( 11.107 ) Explicitly , the field - strength tensor is 0 B3 -B2 - ¡ E - B3 0 B1 -iE2 ( 11.108 ) ( Fμv ) = B2 -B1 0 -iE3 iE1 ¡ E2 iE3 0 To complete the demonstration of the covariance of electrodynamics we ...
... tensor F : ДА ДА Εμν = Эхн дх ( 11.107 ) Explicitly , the field - strength tensor is 0 B3 -B2 - ¡ E - B3 0 B1 -iE2 ( 11.108 ) ( Fμv ) = B2 -B1 0 -iE3 iE1 ¡ E2 iE3 0 To complete the demonstration of the covariance of electrodynamics we ...
Page 385
... tensor of the second rank . We define the symmetric tensor T called the electromagnetic stress - energy - momentum tensor , Iμv = 1 4πT FuλFav + 18μvFÂœFठ( 11.132 ) It will be left to the problems ( Problem 11.12 ) to show that by ...
... tensor of the second rank . We define the symmetric tensor T called the electromagnetic stress - energy - momentum tensor , Iμv = 1 4πT FuλFav + 18μvFÂœFठ( 11.132 ) It will be left to the problems ( Problem 11.12 ) to show that by ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ 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