Classical Electrodynamics |
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Page 365
The Thomas precession , as it is called , also gives a qualitative explanation for a
spinorbit interaction in atomic nuclei and shows why the doublets are “ inverted ”
in nuclei . The Uhlenbeck - Goudsmit hypothesis was that an electron ...
The Thomas precession , as it is called , also gives a qualitative explanation for a
spinorbit interaction in atomic nuclei and shows why the doublets are “ inverted ”
in nuclei . The Uhlenbeck - Goudsmit hypothesis was that an electron ...
Page 369
21 ) it is easy to show that the invariant " length " element is ds2 = dx2 + dy2 +
d22 – c2 dt2 ( 11 . 60 ) This leads ... 62 ) shows that the time t , called the proper
time of the particle , is a Lorentz invariant quantity . This is of considerable ...
21 ) it is easy to show that the invariant " length " element is ds2 = dx2 + dy2 +
d22 – c2 dt2 ( 11 . 60 ) This leads ... 62 ) shows that the time t , called the proper
time of the particle , is a Lorentz invariant quantity . This is of considerable ...
Page 373
70 ) it is elementary to show that ( 11 . 75 ) yields exactly the ... 11 shows a
rotation of the axes through an angle y . The coordinates of the ... 75 ) shows that
the angle y is a complex angle whose tangent tan y = iß ( 11 . 78 ) This result can
be ...
70 ) it is elementary to show that ( 11 . 75 ) yields exactly the ... 11 shows a
rotation of the axes through an angle y . The coordinates of the ... 75 ) shows that
the angle y is a complex angle whose tangent tan y = iß ( 11 . 78 ) This result can
be ...
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Contents
Introduction to Electrostatics | 1 |
BoundaryValue Problems in Electrostatics I | 26 |
RelativisticParticle Kinematics and Dynamics | 391 |
Copyright | |
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