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Page 369
In Galilean relativity space and time coordinates are unconnected . Consequently
under Galilean transformations the infinitesimal elements of distance and time
are separately invariant . Thus ds2 = dx2 + dyż + dz2 = ds2 ( 11 . 59 ) dt ?
In Galilean relativity space and time coordinates are unconnected . Consequently
under Galilean transformations the infinitesimal elements of distance and time
are separately invariant . Thus ds2 = dx2 + dyż + dz2 = ds2 ( 11 . 59 ) dt ?
Page 370
63 ) 12 – 11 = J , T _ • * T ? where t , and t , are the corresponding times in K .
Another fruitful concept in special relativity is the idea of the light cone and "
space - like ” and “ time - like " separations between two events . Consider Fig .
11 .
63 ) 12 – 11 = J , T _ • * T ? where t , and t , are the corresponding times in K .
Another fruitful concept in special relativity is the idea of the light cone and "
space - like ” and “ time - like " separations between two events . Consider Fig .
11 .
Page 384
128 ) is evidently the space components of a 4 - vector . Hence f must be the
space part of a 4 - vector fu = ( 1 , 1 - 2 ) , where : fu = - Fundo ( 11 . 129 ) To see
the meaning of the fourth component of the force - density 4 - vector we write out
fo ...
128 ) is evidently the space components of a 4 - vector . Hence f must be the
space part of a 4 - vector fu = ( 1 , 1 - 2 ) , where : fu = - Fundo ( 11 . 129 ) To see
the meaning of the fourth component of the force - density 4 - vector we write out
fo ...
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Contents
Introduction to Electrostatics | 1 |
References and suggested reading | 23 |
Wave Guides and Resonant Cavities | 235 |
Copyright | |
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