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・ Membrane fluidity
・ Membrane fouling
・ Membrane fusion protein
・ Membrane gas separation
・ Membrane glucocorticoid receptor
・ Membrane glycoproteins
・ Membrane keyboard
・ Membrane lipids
・ Membrane method
・ Membrane mineralocorticoid receptor
・ Membrane mirror
・ Membrane models
・ Membrane nanotube
・ Membrane osmometer
・ Membrane oxygenator
Membrane paradigm
・ Membrane potential
・ Membrane Pro-X carboxypeptidase
・ Membrane progesterone receptor
・ Membrane protein
・ Membrane Protein Structural Dynamics Consortium
・ Membrane reactor
・ Membrane roofing
・ Membrane ruffling
・ Membrane sex steroid receptor
・ Membrane stabilizing effect
・ Membrane steroid receptor
・ Membrane structure
・ Membrane switch
・ Membrane technology


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Membrane paradigm : ウィキペディア英語版
Membrane paradigm
In black hole theory, the black hole membrane paradigm is a useful "toy model" method or "engineering approach" for visualising and calculating the effects predicted by quantum mechanics for the exterior physics of black holes, without using quantum-mechanical principles or calculations. It models a black hole as a thin classically-radiating surface (or membrane) at or vanishingly close to the black hole's event horizon. This approach to the theory of black holes was created by Kip S. Thorne, R. H. Price and D. A. Macdonald.
The results of the membrane paradigm are generally considered to be "safe".
==Electrical resistance==
Thorne (1994) relates that this approach to studying black holes was prompted by the realisation by Hanni, Ruffini, Wald and Cohen in the early 1970s that since an electrically charged pellet dropped into a black hole should still ''appear'' to a distant outsider to be remaining just outside the event horizon, if its image persists, its electrical fieldlines ought to persist too, and ought to point to the location of the "frozen" image (1994, pp. 406). If the black hole rotates, and the image of the pellet is pulled around, the associated electrical fieldlines ought to be pulled around with it to create basic "electrical dynamo" effects (''see:'' dynamo theory).
Further calculations yielded properties for a black hole such as apparent electrical resistance (pp. 408). Since these fieldline properties seemed to be exhibited down to the event horizon, and general relativity insisted that no dynamic exterior interactions could extend ''through'' the horizon, it was considered convenient to invent a surface ''at'' the horizon that these electrical properties could be said to belong to.

抄文引用元・出典: フリー百科事典『 ウィキペディア(Wikipedia)
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