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 : • Tii ...
... 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 : • Tii ...
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 « 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 « 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 ...
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4-vector Ampère's law angle angular distribution approximation atomic axis boundary conditions calculate Chapter charge density charge q charged particle coefficients collisions component conductor consider coordinates cross section current density cylinder d³x delta function dielectric constant diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electron electrostatic energy loss expansion expression factor frequency given Green's function impact parameter incident particle inside integral inversion Laplace's equation linear Lorentz transformation macroscopic magnetic field magnetic induction magnetic moment magnitude Maxwell's equations meson modes molecules momentum motion multipole nonrelativistic normal obtain oscillations P₁ parallel plasma point charge Poisson's equation polarization problem radiation radius region relativistic result scalar scalar potential scattering shown in Fig shows solution spherical surface surface-charge density theorem transverse unit V₁ vanishes vector potential velocity volume wave equation wave number wavelength written zero ΦΩ