## Classical Electrodynamics |

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Page 367

At time t the electron's rest frame K' and the laboratory frame K are related by a

Lorentz

now changed to K", related to K by a Lorentz

At time t the electron's rest frame K' and the laboratory frame K are related by a

Lorentz

**transformation**with velocity v. At time t + 6t the electron's rest frame hasnow changed to K", related to K by a Lorentz

**transformation**with velocity v + 6v.Page 370

is an invariant under Lorentz

that Lorentz

or, more correctly, are orthogonal

is an invariant under Lorentz

**transformations**. This is then exactly the requirementthat Lorentz

**transformations**are rotations in a four-dimensional Euclidean spaceor, more correctly, are orthogonal

**transformations**in four dimensions.Page

0 (11.112) Al 11.10

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

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

from a ...

0 (11.112) Al 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,za, Fa, (11.113) With

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

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### Contents

Introduction to Electrostatics | 1 |

Nš 3 | 3 |

Greens theorem | 14 |

Copyright | |

30 other sections not shown

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