By Menas Kafatos

ISBN-10: 0792304969

ISBN-13: 9780792304968

Bell's Theorem and its linked implications for the character of the actual global stay subject matters of serious curiosity. for that reason many conferences were lately hung on the translation of quantum conception and the results of Bell's Theorem. commonly those conferences were held essentially for quantum physicists and philosophers of technology who've been or are actively engaged on the subject. however, different philosophers of technological know-how, mathematicians, engineers in addition to contributors of most people have more and more taken curiosity in Bell's Theorem and its implications. the autumn Workshop held at George Mason college on October 21 and 22, 1988 and titled "Bell's Theorem, Quantum conception and Conceptions of the Universe" used to be of a extra basic scope. not just it attracted specialists within the box, it additionally lined different themes similar to the results of quantum non-locality for the character of awareness, cosmology, the anthropic precept, and so forth. themes frequently no longer lined in prior conferences of this sort. The assembly was once attended through multiple hundred ten experts and different humans from world wide. the aim of the assembly used to be to not offer a definitive resolution to the overall questions raised through Bell's Theorem. it's most probably that the talk will move on for rather decades. quite, it used to be intended to give a contribution to the real discussion among various disciplines.

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Extra info for Bell's Theorem, Quantum Theory and Conceptions of the Universe (Fundamental Theories of Physics)

Example text

Das Ringintegral des H-Feldes ist (s. Kap. 2) ˛ NI : H ds D H ` D N I ) H D ` Das Magnetfeld wird 0N I : ` Diese Gleichung gilt in guter Näherung auch für eine lange gerade Spule. 46) 26 1 Grundlagen von Elektrizität und Magnetismus Dipolmagnet Als zweites Beispiel berechnen wir das Feld eines Dipolmagneten in einem Kreisbeschleuniger. Das Eisenjoch hat einen Luftspalt der Höhe h, die Feldlinien stehen senkrecht auf den Polschuhen. Auf das Joch ist eine Spule mit N Windungen ge¸ wickelt. Das Ringintegral des erregenden Feldes hat wieder den Wert H d s D N I , aber im Unterschied zur Toroidspule ist H nicht mehr konstant auf dem Integrationsweg.

22) Hier haben wir benutzt, dass man Integral- und Summenzeichen vertauschen darf. Der elektrische Fluss des Gesamtfeldes ist gleich der Summe der Flüsse der Einzelfelder (Abb. 11). Das bedeutet: Pman kann alle Ladungen innerhalb des Volumens zu einer Gesamtladung Qges D j Qj zusammenfassen und den elektrischen Fluss des Gesamtfeldes als Qges ="0 schreiben. 2 Integralsatz von Gauß, Divergenz eines Vektorfeldes 45 Abb. 11 Der Fluss der elektrischen Feldstärke durch eine Kugelfläche S1 ist gleich dem Fluss durch eine beliebig geformte geschlossene Oberfläche S2 .

Die Quellen des magnetisierenden (erregenden) Feldes H sind die „freien“ Ströme in Magnetspulen, die der Experimentator nach Belieben einstellen und messen kann. Die Quellen des Magnetfeldes B hingegen sind sowohl die Ströme in Spulen als auch die Magnetisierung der Materie, und letztere ist nicht beliebig einstellbar oder kontrollierbar. Bei der Berechnung eines Elektromagneten mit Eisenkern benötigt man daher das H -Feld. Dafür geben wir im nächsten Abschnitt zwei Beispiele. Es gibt eine historisch bedingte und durch unglückliche Maßsysteme4 geförderte Begriffsverwirrung bei der Bezeichnung von Magnetfeldern.

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Bell's Theorem, Quantum Theory and Conceptions of the Universe (Fundamental Theories of Physics) by Menas Kafatos


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