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 ~ Pi COS α 4πT cos a + cos 0 2 cos a 2 ) 2 | 2J , ( ka ) ( 9.112 ) kaş where P , is given by ( 9.104 ) . If ...
... scalar equivalent of ( 9.102 ) . The power radiated per unit solid angle in the scalar Kirchhoff approximation is dP ΦΩ ( ka ) 2 ~ Pi COS α 4πT cos a + cos 0 2 cos a 2 ) 2 | 2J , ( ka ) ( 9.112 ) kaş where P , is given by ( 9.104 ) . If ...
Page 637
... scalar products , use in kinematics , 395 , 396 , 398 of phase of plane wave , 363 , 383 of products of fields , 389 ... Scalar , under Lorentz transformations , 374 Scalar potential , electrostatic , definition of , 8 for time - varying ...
... scalar products , use in kinematics , 395 , 396 , 398 of phase of plane wave , 363 , 383 of products of fields , 389 ... Scalar , under Lorentz transformations , 374 Scalar potential , electrostatic , definition of , 8 for time - varying ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charged particle coefficients collisions component conducting conductor consider constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ electric field electromagnetic fields electrons electrostatic energy loss factor force equation 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 parallel perpendicular phase velocity plane wave plasma polarization power radiated Poynting's vector problem propagation radius region relativistic result S₁ scalar scattering screen shown in Fig shows sin² solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave guide wave number wavelength ΦΩ