Classical ElectrodynamicsProblems after each chapter |
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Page 368
... orbit coupling by a factor of ( sometimes called the Thomas factor ) , yielding U = — e S.B + mc 1 2m2c2 1 dv S.L r dr ( 11.56 ) as the correct spin - orbit interaction energy for an atomic electron . In atomic nuclei the nucleons ...
... orbit coupling by a factor of ( sometimes called the Thomas factor ) , yielding U = — e S.B + mc 1 2m2c2 1 dv S.L r dr ( 11.56 ) as the correct spin - orbit interaction energy for an atomic electron . In atomic nuclei the nucleons ...
Page 421
... orbit subtracts from the first term . This gives e J = = γεωπα ( Βπα ” ) ( 12.124 ) с making use of B particle's orbit . = eBlymc . The quantity Bra2 is the flux through the If the particle moves through regions where the magnetic field ...
... orbit subtracts from the first term . This gives e J = = γεωπα ( Βπα ” ) ( 12.124 ) с making use of B particle's orbit . = eBlymc . The quantity Bra2 is the flux through the If the particle moves through regions where the magnetic field ...
Page 608
... orbits in a Bohr atom the orbit radius and the principal quantum number n are related by r = nao / Z . If the transition probability for transitions from n → ( n - 1 ) is defined as -dn / dt , show that the result of ( a ) agrees with ...
... orbits in a Bohr atom the orbit radius and the principal quantum number n are related by r = nao / Z . If the transition probability for transitions from n → ( n - 1 ) is defined as -dn / dt , show that the result of ( a ) agrees with ...
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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