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Page 177
... this brilliant stroke in 1865 , the modified set of 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.
... this brilliant stroke in 1865 , the modified set of 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.
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 ...
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