## Classical Electrodynamics |

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Page 357

Consequently three successive

components of the velocity v in three mutually ... But a more general

this Lorentz ...

Consequently three successive

**transformations**corresponding to thecomponents of the velocity v in three mutually ... But a more general

**transformation**would allow the axes in K' to be rotated relative to those in K. Eventhis Lorentz ...

Page 372

This is then exactly the requirement that Lorentz

four-dimensional Euclidean space or, ... Q.: pu = 1, 2, 3, 4 (11.70) pivovw 3.

where the coefficients a, are constants characteristic of the particular

This is then exactly the requirement that Lorentz

**transformations**are rotations in afour-dimensional Euclidean space or, ... Q.: pu = 1, 2, 3, 4 (11.70) pivovw 3.

where the coefficients a, are constants characteristic of the particular

**transformation**.Page 380

0 (11.112) w 11.10

E and B are elements of the field-strength tensor F., their

properties can be found from Fiv = a,zav, Fa, (11.113) With

from a ...

0 (11.112) w 11.10

**Transformation**of the Electromagnetic Fields Since the fieldsE and B are elements of the field-strength tensor F., their

**transformation**properties can be found from Fiv = a,zav, Fa, (11.113) With

**transformation**(11.75)from a ...

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### Contents

Introduction to Electrostatics | 1 |

BoundaryValue Problems in Electrostatics I | 26 |

References and suggested reading | 50 |

Copyright | |

16 other sections not shown

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