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 ΦΩ ~ ( ka ) 2 cos α + cos 0 2 Pi COS α 2 cos α 2J1 ( ka§ ) kaž ( 9.112 ) 4πT where P , is given by ( 9.104 ) . i If we ...
... scalar equivalent of ( 9.102 ) . The power radiated per unit solid angle in the scalar Kirchhoff approximation is dP ΦΩ ~ ( ka ) 2 cos α + cos 0 2 Pi COS α 2 cos α 2J1 ( ka§ ) kaž ( 9.112 ) 4πT where P , is given by ( 9.104 ) . i 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 ...
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