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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 [ 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 [ 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 acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss energy transfer factor force equation frame 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 P₂ parallel perpendicular plasma polarization power radiated problem radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ