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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 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