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Page 8
... scalar by the gradient operation . Since one function of position is easier to deal with . than three , it is worth while concentrating on the scalar function and giving it a name . Consequently we define the " scalar potential ...
... scalar by the gradient operation . Since one function of position is easier to deal with . than three , it is worth while concentrating on the scalar function and giving it a name . Consequently we define the " scalar potential ...
Page 296
... scalar equivalent of ( 9.102 ) . The power radiated per unit solid angle in the scalar Kirchhoff approximation is dP ΦΩ d Pi ( ka ) 2 4π COS a cos x + cos 0 2J1 ( kağ ) 2 cos x kağ 2 ( 9.112 ) where P , is given by ( 9.104 ) . If we ...
... scalar equivalent of ( 9.102 ) . The power radiated per unit solid angle in the scalar Kirchhoff approximation is dP ΦΩ d Pi ( ka ) 2 4π COS a cos x + cos 0 2J1 ( kağ ) 2 cos x kağ 2 ( 9.112 ) where P , is given by ( 9.104 ) . 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 angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle coefficients collisions component conducting conductor consider 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 momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular phase velocity plane wave 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 number wavelength ΦΩ