Classical ElectrodynamicsProblems after each chapter |
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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 4πT cos x + cos 0 ) 22J1 ( ka§ ) ( 9.112 ) kağ dQ where P is given by ( 9.104 ) . i 2 cos α 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 4πT cos x + cos 0 ) 22J1 ( ka§ ) ( 9.112 ) kağ dQ where P is given by ( 9.104 ) . i 2 cos α If we ...
Page
... 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 ...
Contents
1 | 1 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
Copyright | |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ