Classical ElectrodynamicsProblems after each chapter |
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Page 193
... vector on the left can form scalar or vector products from the left , and correspondingly for the unit vector on the right . Given the dyadic , we can determine the tensor elements by taking the appropriate scalar products : T1 ...
... vector on the left can form scalar or vector products from the left , and correspondingly for the unit vector on the right . Given the dyadic , we can determine the tensor elements by taking the appropriate scalar products : T1 ...
Page 283
... vector fields , we expect that a considerable improvement can be made by developing vector equivalents to the Kirchhoff integral ( 9.65 ) . 9.6 Vector Equivalents of Kirchhoff Integral To obtain vector equivalents to the Kirchhoff ...
... vector fields , we expect that a considerable improvement can be made by developing vector equivalents to the Kirchhoff integral ( 9.65 ) . 9.6 Vector Equivalents of Kirchhoff Integral To obtain vector equivalents to the Kirchhoff ...
Page 307
... vector makes an angle a with the normal to the screen . The polarization vector is perpendicular to the plane of incidence . ( a ) Calculate the diffracted fields and the power per unit solid angle transmitted through the opening ...
... vector makes an angle a with the normal to the screen . The polarization vector is perpendicular to the plane of incidence . ( a ) Calculate the diffracted fields and the power per unit solid angle transmitted through the opening ...
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