Terrell rotation
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This article includes a list of references, related reading or external links, but its sources remain unclear because it lacks inline citations. Please improve this article by introducing more precise citations. (March 2010) |
Terrell rotation is the name of a mathematical and physical effect. Specifically, Terrell rotation is the distortion that a passing object would appear to undergo, according to the special theory of relativity if it were travelling a significant fraction of the speed of light. This behaviour was described independently by both James Terrell and Roger Penrose in pieces published in 1959.
Due to an early dispute about priority and correct attribution, the effect is also sometimes referred to as the Penrose-Terrell effect, the Terrell-Penrose effect, or just as the Terrell effect.
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Terrell's paper pointed out that although special relativity appeared to describe an "observed contraction" in moving objects, these interpreted "observations" were not to be confused with the theory's literal predictions for the visible appearance of a moving object. Thanks to the differential timelag effects in signals reaching the observer from the object's different parts, a receding object would appear contracted, an approaching object would appear elongated (even under special relativity) and the geometry of a passing object would appear skewed, as if rotated.
For images of passing objects, the apparent contraction of distances between points on the object's transverse surface could then be interpreted as being due to an apparent change in viewing angle, and the image of the object could be interpreted as appearing instead to be rotated. A previously-popular description of special relativity's predictions, in which an observer sees a passing object to be contracted (for instance, from a sphere to a flattened ellipsoid), was wrong.
Terrell's piece prompted a number of followup papers, mostly in the American Journal of Physics, exploring the consequences of this correction. Terrell's paper pointed out that some existing discussions of special relativity were flawed and "explained" effects that the theory did not actually predict - while his paper did not change the actual mathematical structure of special relativity in any way, it did correct a popular misconception regarding the theory's predictions.
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[edit] References and further reading
- James Terrell (1959). "Invisibility of the Lorentz Contraction". Physical Review 116 (4): 1041–1045. Bibcode 1959PhRv..116.1041T. doi:10.1103/PhysRev.116.1041.
- Roger Penrose (1959). "The Apparent Shape of a Relativistically Moving Sphere". Proceedings of the Cambridge Philosophical Society 55 (01): 137–139. Bibcode 1959PCPS...55..137P. doi:10.1017/S0305004100033776.
- Mary L. Boas (1961). "Apparent shape of large objects at relativistic speeds". American Journal of Physics 29 (5): 283–286. Bibcode 1961AmJPh..29..283B. doi:10.1119/1.1937751.
- Eric Sheldon (1988). "The twists and turns of the Terrell Effect". American Journal of Physics 56 (3): 199–200. Bibcode 1988AmJPh..56..199S. doi:10.1119/1.15687.
- James Terrell (1989). "The Terrell Effect". American Journal of Physics 57 (1): 9–10. Bibcode 1989AmJPh..57....9T. doi:10.1119/1.16131.
- Eric Sheldon (1989). "The Terrell Effect: Eppure si contorce!". American Journal of Physics 57 (6): 487. Bibcode 1989AmJPh..57..487S. doi:10.1119/1.16144.
- John Robert Burke and Frank J. Strode (1991). "Classroom exercises with the Terrell effect". American Journal of Physics 59 (10): 912–915. Bibcode 1991AmJPh..59..912B. doi:10.1119/1.16670.