Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 71
Page 297
... side of the sheet . The problem is to calculate the diffracted fields on the other side of the sheet . Since the sheet is assumed flat , the simple vector theorem ( 9.82 ) is appro- priate . Evidently the problem is solved if we can ...
... side of the sheet . The problem is to calculate the diffracted fields on the other side of the sheet . Since the sheet is assumed flat , the simple vector theorem ( 9.82 ) is appro- priate . Evidently the problem is solved if we can ...
Page 298
... side . But far away from the hole ( in terms of its dimensions ) , although still " near the conducting plane ... side of the perfectly conducting sheet which is an equipotential surface . Similarly for the magnetic induction , B must be ...
... side . But far away from the hole ( in terms of its dimensions ) , although still " near the conducting plane ... side of the perfectly conducting sheet which is an equipotential surface . Similarly for the magnetic induction , B must be ...
Page 567
... sides of ( 16.22 ) . Then we can put | x nx on the left - hand side , where n is a unit vector in the direction of x ' . On the right side r 、= r ' and r = r . Furthermore we can use the asymptotic form ( 16.13 ) for h ( kr ' ) . Then ...
... sides of ( 16.22 ) . Then we can put | x nx on the left - hand side , where n is a unit vector in the direction of x ' . On the right side r 、= r ' and r = r . Furthermore we can use the asymptotic form ( 16.13 ) for h ( kr ' ) . Then ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
21 other sections not shown
Other editions - View all
Common terms and phrases
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