Classical ElectrodynamicsProblems after each chapter |
From inside the book
Results 1-3 of 39
Page 388
... frame ( this makes the occupants feel at home ) . It accelerates in a straight - line path for 5 years ( by its own clocks ) , decelerates at the same rate for 5 more years , turns around , accelerates for 5 years , decelerates for 5 ...
... frame ( this makes the occupants feel at home ) . It accelerates in a straight - line path for 5 years ( by its own clocks ) , decelerates at the same rate for 5 more years , turns around , accelerates for 5 years , decelerates for 5 ...
Page 393
... frame of the particle ( p ' = 0 ) the scalar product ( 12.5 ) gives the energy of the particle at rest : E ' = λ ( 12.6 ) To determine λ we consider the Lorentz transformation ( 12.4 ) of p1 from the rest frame of the particle to the frame ...
... frame of the particle ( p ' = 0 ) the scalar product ( 12.5 ) gives the energy of the particle at rest : E ' = λ ( 12.6 ) To determine λ we consider the Lorentz transformation ( 12.4 ) of p1 from the rest frame of the particle to the frame ...
Page 414
... frame where E = 0 if | B | > | E | , or B = 0 if | E | > | B | . In those coordinate frames the motion was relatively simple . If E B 0 , electric and magnetic fields will exist simultaneously in all Lorentz frames , the angle between ...
... frame where E = 0 if | B | > | E | , or B = 0 if | E | > | B | . In those coordinate frames the motion was relatively simple . If E B 0 , electric and magnetic fields will exist simultaneously in all Lorentz frames , the angle between ...
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