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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 514
... frame for our calculation and then transform to the laboratory at the end . Thus we will find that all but the final ... frame K ' , where the incident particle is at rest initially and the nucleus moves by with velocity vc , the ...
... frame for our calculation and then transform to the laboratory at the end . Thus we will find that all but the final ... frame K ' , where the incident particle is at rest initially and the nucleus moves by with velocity vc , the ...
Page 591
... frame of the particle ; U is the electrostatic self - energy ( 17.30 ) . ― From these values of energy and momentum in the rest frame we wish to obtain the corresponding values in a different Lorentz frame and so exhibit the ...
... frame of the particle ; U is the electrostatic self - energy ( 17.30 ) . ― From these values of energy and momentum in the rest frame we wish to obtain the corresponding values in a different Lorentz frame and so exhibit the ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
Copyright | |
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4-vector acceleration Ampère's law angle angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate cavity Chapter charge q charged particle coefficients collisions component conducting conductor 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 modes momentum multipole nonrelativistic obtain oscillations P₁ P₂ parallel perpendicular 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 guide wave number wavelength ΦΩ