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Page 177
... equations is justly known as Maxwell's equations . The faulty equation is Ampère's law . It was derived [ Sect . 6.3 ] Time - Varying Fields , Maxwell's Equations , Conservation Laws 177 Maxwell's displacement current, Maxwell's equations,
... equations is justly known as Maxwell's equations . The faulty equation is Ampère's law . It was derived [ Sect . 6.3 ] Time - Varying Fields , Maxwell's Equations , Conservation Laws 177 Maxwell's displacement current, Maxwell's equations,
Page 179
John David Jackson. known as Maxwell's equations , forms the basis of all electromagnetic phenomena . When combined with the Lorentz force equation and Newton's second law of motion , these equations provide a complete description of the ...
John David Jackson. known as Maxwell's equations , forms the basis of all electromagnetic phenomena . When combined with the Lorentz force equation and Newton's second law of motion , these equations provide a complete description of the ...
Page 180
... Maxwell's equations . The dynamic behavior of A and will be determined by the two inhomogeneous equations in ( 6.28 ) . At this stage it is convenient to restrict our considerations to the microscopic form of Maxwell's equations . Then ...
... Maxwell's equations . The dynamic behavior of A and will be determined by the two inhomogeneous equations in ( 6.28 ) . At this stage it is convenient to restrict our considerations to the microscopic form of Maxwell's equations . Then ...
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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