Classical ElectrodynamicsProblems after each chapter |
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Page 189
... electromagnetic energy into mechanical or thermal energy . It must be balanced by a corresponding rate of decrease of energy in the electromagnetic field within the volume V. In order to exhibit this conservation law explicitly , we ...
... electromagnetic energy into mechanical or thermal energy . It must be balanced by a corresponding rate of decrease of energy in the electromagnetic field within the volume V. In order to exhibit this conservation law explicitly , we ...
Page 595
... electromagnetic contributions to the self - energy and momentum can be defined to have the proper Lorentz transformation properties . This not only would be esthetically pleasing , but also would have the added virtue of separating , at ...
... electromagnetic contributions to the self - energy and momentum can be defined to have the proper Lorentz transformation properties . This not only would be esthetically pleasing , but also would have the added virtue of separating , at ...
Page 616
... Electromagnetic Units ( A.11 ) The various systems of electromagnetic units differ in their choices of the magnitudes and dimensions of the various constants above . Because of relations ( A.5 ) and ( A.11 ) there are only two constants ...
... Electromagnetic Units ( A.11 ) The various systems of electromagnetic units differ in their choices of the magnitudes and dimensions of the various constants above . Because of relations ( A.5 ) and ( A.11 ) there are only two constants ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution approximation atomic axis behavior boundary conditions bremsstrahlung calculation Chapter charge q charged particle Cherenkov radiation classical coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic emitted energy loss energy transfer equation of motion factor force equation frame frequency given Green's function impact parameter incident particle integral Lagrangian limit Lorentz force Lorentz invariant Lorentz transformation m₁ magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum multipole nonrelativistic obtain orbit oscillations P₁ P₂ parallel perpendicular photon plane plasma polarization power radiated problem quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution spectrum sphere spherical surface transverse V₁ vanishes vector potential wave number wavelength ΦΩ