Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 55
Page 549
... multipole fields contains the selection rules for multipole transitions between quantum states . A multipole transition of order ( l , m ) will connect an initial quantum state specified by total angular momentum J and z component M to ...
... multipole fields contains the selection rules for multipole transitions between quantum states . A multipole transition of order ( l , m ) will connect an initial quantum state specified by total angular momentum J and z component M to ...
Page 550
... multipole of order ( 1 , m ) the parity is ( −1 ) 11 . In this case the electric field Em is of the same form as Bim for electric multipoles . Hence the parities of the fields are just opposite to those of an electric multipole of the ...
... multipole of order ( 1 , m ) the parity is ( −1 ) 11 . In this case the electric field Em is of the same form as Bim for electric multipoles . Hence the parities of the fields are just opposite to those of an electric multipole of the ...
Page 557
... multipole moment qim ( 4.3 ) . The moment Qim ' is an induced electric multipole moment due to the magnetization . It is generally at least a factor kr smaller than the normal moment Qim For the magnetic multi- pole coefficient al , m ...
... multipole moment qim ( 4.3 ) . The moment Qim ' is an induced electric multipole moment due to the magnetization . It is generally at least a factor kr smaller than the normal moment Qim For the magnetic multi- pole coefficient al , m ...
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