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Page ix
... example of the covariance of physical laws under Lorentz transformations . The special theory of relativity is discussed in Chapter 11 , where all the necessary formal apparatus is developed , various kinematic consequences are explored ...
... example of the covariance of physical laws under Lorentz transformations . The special theory of relativity is discussed in Chapter 11 , where all the necessary formal apparatus is developed , various kinematic consequences are explored ...
Page 93
... example , Smythe , pp . 111 , 156 , or Jeans , p . 244 . REFERENCES AND SUGGESTED READING The mathematical apparatus ... examples and problems , can be found in Hildebrand , Chapters 4 , 5 , and 8 . A somewhat old - fashioned source of ...
... example , Smythe , pp . 111 , 156 , or Jeans , p . 244 . REFERENCES AND SUGGESTED READING The mathematical apparatus ... examples and problems , can be found in Hildebrand , Chapters 4 , 5 , and 8 . A somewhat old - fashioned source of ...
Page 400
... example we find a factor - of - 3 increase over the actual mass difference , whereas in the photoproduction example the increase was only 7.2 per cent . Other threshold calculations are left to Problem 12.1 . 12.4 Transformation of ...
... example we find a factor - of - 3 increase over the actual mass difference , whereas in the photoproduction example the increase was only 7.2 per cent . Other threshold calculations are left to Problem 12.1 . 12.4 Transformation of ...
Contents
1 | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
Dielectrics | 98 |
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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