Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 80
Page 270
... compared to a wavelength it is appropriate to expand the integral in ( 9.8 ) in powers of k : lim A ( x ) kr → ∞ ikr e == cr Σ ( — ik ) " f ' J ( x ' ) ( n • x ' ) " d ° x ' n ! n The magnitude of the nth term is given by ( 9.9 ) n ...
... compared to a wavelength it is appropriate to expand the integral in ( 9.8 ) in powers of k : lim A ( x ) kr → ∞ ikr e == cr Σ ( — ik ) " f ' J ( x ' ) ( n • x ' ) " d ° x ' n ! n The magnitude of the nth term is given by ( 9.9 ) n ...
Page 297
... compared in Fig . 9.11 for the angle of incidence equal to 45 ° and for an aperture one wave- length in diameter ... compared to a wavelength , an entirely different approach is necessary . We will consider a thin , flat , perfectly ...
... compared in Fig . 9.11 for the angle of incidence equal to 45 ° and for an aperture one wave- length in diameter ... compared to a wavelength , an entirely different approach is necessary . We will consider a thin , flat , perfectly ...
Page 432
... compared to the orbital period of motion , it may be expected that the collision will be sudden enough that the electron may be treated as free . If , on the other hand , the collision time ( 11.120 ) is very long compared to the ...
... compared to the orbital period of motion , it may be expected that the collision will be sudden enough that the electron may be treated as free . If , on the other hand , the collision time ( 11.120 ) is very long compared to the ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
24 other sections not shown
Other editions - View all
Common terms and phrases
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