## Classical Electrodynamics |

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Page 357

11.5 With the definition that x = [(v. x)w]|vo and x = x – x, equations (11.20) can be

combined to yield the general

? t;2 1 – = 1–3 1 x • W (11.21) r--H(-o) It should be noted that (11.21) represents ...

11.5 With the definition that x = [(v. x)w]|vo and x = x – x, equations (11.20) can be

combined to yield the general

**Lorentz transformation**:* x = x + –––. ** v--—w p? p? t;2 1 – = 1–3 1 x • W (11.21) r--H(-o) It should be noted that (11.21) represents ...

Page 371

If slo -> 0, the events are said to have a space-like separation, because it is

always possible to find a

where (t1' – ta) = 0 and siz” = (x1' – 22')* + (y1' – yo)” + (21' – 2,')* > 0 (11.65) That

is, ...

If slo -> 0, the events are said to have a space-like separation, because it is

always possible to find a

**Lorentz transformation**to a new coordinate system K'where (t1' – ta) = 0 and siz” = (x1' – 22')* + (y1' – yo)” + (21' – 2,')* > 0 (11.65) That

is, ...

Page 372

This is then exactly the requirement that

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

transformation.

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.

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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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