Classical Electrodynamics |
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Page 7
... scalar rather than vector functions of position , and then to derive the vector quantities at the end if necessary ( see below ) . 1.5 Another Equation of Electrostatics and the Scalar Potential The single equation ( 1.13 ) is not ...
... scalar rather than vector functions of position , and then to derive the vector quantities at the end if necessary ( see below ) . 1.5 Another Equation of Electrostatics and the Scalar Potential The single equation ( 1.13 ) is not ...
Page 296
... scalar equivalent of ( 9.102 ) . The power radiated per unit solid angle in the scalar Kirchhoff approximation is dP ( ka ) 2 ~ Pi COS α ΦΩ 4π i where P is given by ( 9.104 ) . cos x + cos 02 2J1 ( ka§ ) a 2 cos a ( 9.112 ) kaž If we ...
... scalar equivalent of ( 9.102 ) . The power radiated per unit solid angle in the scalar Kirchhoff approximation is dP ( ka ) 2 ~ Pi COS α ΦΩ 4π i where P is given by ( 9.104 ) . cos x + cos 02 2J1 ( ka§ ) a 2 cos a ( 9.112 ) kaž If we ...
Page 538
... scalar potential was used extensively for problems possessing some symmetry property with respect to an origin of coordinates . Not only was it useful in handling boundary - value problems in spherical coordinates , but with a source ...
... scalar potential was used extensively for problems possessing some symmetry property with respect to an origin of coordinates . Not only was it useful in handling boundary - value problems in spherical coordinates , but with a source ...
Common terms and phrases
4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis 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 dielectric constant diffraction dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss 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 phase velocity plane wave plasma polarization power radiated problem propagation radius region relativistic result 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