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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 ...
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... 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 |
Greens theorem | 14 |
BoundaryValue Problems in Electrostatics I | 26 |
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4-vector acceleration Ampère's law angular distribution antenna approximation atomic axis B₁ Babinet's principle behavior boundary conditions calculate Chapter charge q charged particle classical coefficients collisions component conducting conductor constant coordinate cross section cylinder d³x dielectric diffraction dimensions dipole direction discussed E₁ effects electric field electromagnetic fields electrons electrostatic energy loss energy transfer factor force equation formula frequency given Green's function impact parameter incident particle integral Kirchhoff Lorentz invariant Lorentz transformation magnetic field magnetic induction magnitude Maxwell's equations meson modes momentum motion multipole nonrelativistic obtain oscillations P₁ parallel perpendicular plane wave plasma plasma oscillations polarization power radiated Poynting's vector problem propagation quantum quantum-mechanical radius region relativistic result scalar scattering screen shown in Fig shows sin² solid angle solution sphere spherical surface transverse unit V₁ vanishes vector potential velocity wave number wavelength ΦΩ