Classical Electrodynamics |
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Page ix
And even after almost 60 years, classical electrodynamics still impresses and
delights as a beautiful example of the covariance of physical laws under Lorentz
transformations. The special theory of relativity is discussed in Chapter 11, where
...
And even after almost 60 years, classical electrodynamics still impresses and
delights as a beautiful example of the covariance of physical laws under Lorentz
transformations. The special theory of relativity is discussed in Chapter 11, where
...
Page 93
See, for example, Smythe, pp. 111, 156, or Jeans, p. 244. REFERENCES AND
SUGGESTED READING The mathematical apparatus and special functions
needed for the solution of potential problems in spherical, cylindrical, spheroidal,
and ...
See, for example, Smythe, pp. 111, 156, or Jeans, p. 244. REFERENCES AND
SUGGESTED READING The mathematical apparatus and special functions
needed for the solution of potential problems in spherical, cylindrical, spheroidal,
and ...
Page 400
135.0(1.072) = 144.7 Mev As another example consider the production of a
proton-antiproton pair in proton-proton collisions: p + p → p + p + p + p The mass
difference is AM = 2m, = 1.877 Bev. From (12.41) we find Ton = 2m ...
135.0(1.072) = 144.7 Mev As another example consider the production of a
proton-antiproton pair in proton-proton collisions: p + p → p + p + p + p The mass
difference is AM = 2m, = 1.877 Bev. From (12.41) we find Ton = 2m ...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
References and suggested reading | 50 |
Copyright | |
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