Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 86
Page 447
... limits ( 3.103 ) . Then in the relativistic limit the Fermi expression ( 13.70 ) is dE ~ dx / b > a 2 ( ze ) 2 π c2 • Re ( " i ( -1 ) S ίω X In ( 1.123c ) – In ( 1 − e ( ) ) ] do ( 13.75 ) ωα - - It is worth while right here to point ...
... limits ( 3.103 ) . Then in the relativistic limit the Fermi expression ( 13.70 ) is dE ~ dx / b > a 2 ( ze ) 2 π c2 • Re ( " i ( -1 ) S ίω X In ( 1.123c ) – In ( 1 − e ( ) ) ] do ( 13.75 ) ωα - - It is worth while right here to point ...
Page 493
... limit qa < 1 holds , and a region of wider angles where the limit qa > 1 applies . For qa 1 , the arguments of exponents in ( 14.111 ) are all so small that the exponential factors can be approximated by unity . Then the differential ...
... limit qa < 1 holds , and a region of wider angles where the limit qa > 1 applies . For qa 1 , the arguments of exponents in ( 14.111 ) are all so small that the exponential factors can be approximated by unity . Then the differential ...
Page 518
... limit . The constant value is the semi- classical result . The curve marked " Bethe - Heitler " is the quantum- mechanical Born approximation . For extremely relativistic particles the screening can be " complete . " Complete screening ...
... limit . The constant value is the semi- classical result . The curve marked " Bethe - Heitler " is the quantum- mechanical Born approximation . For extremely relativistic particles the screening can be " complete . " Complete screening ...
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