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Simple Nature - Light and Matter

Simple Nature - Light and Matter

Simple Nature - Light and Matter

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Although the light rays in figure n don’t speed up or slow down,they do experience gravitational Doppler shifts. If a light ray isemitted from just above the event horizon, then it will escape to aninfinite distance, but it will suffer an extreme Doppler shift towardlow frequencies. A distant observer also has the option of interpretingthis as a gravitational time dilation that greatly lowers thefrequency of the oscillating electric charges that produced the ray.If the point of emission is made closer <strong>and</strong> closer to the horizon,the frequency <strong>and</strong> energy measured by a distant observer approachzero, making the ray impossible to observe.n / The equivalence principle tellsus that spacetime locally has thesame structure as in special relativity,so we can draw the familiarparallelogram of x − t coordinatesat each point near the blackhole. Superimposed on each littlegrid is a pair of lines representingmotion at the speed oflight in both directions, inward <strong>and</strong>outward. Because spacetime iscurved, these lines do not appearto be at 45-degree angles,but to an observer in that region,they would appear to be. Whenlight rays are emitted inward <strong>and</strong>outward from a point outside theevent horizon, one escapes <strong>and</strong>one plunges into the black hole.On this diagram, they look likethey are decelerating <strong>and</strong> accelerating,but local observers comparingthem to their own coordinategrids would always see themas moving at exactly c. Whenrays are emitted from a point insidethe event horizon, neither escapes;the distortion is so severethat “outward” is really inward.Information paradoxBlack holes have some disturbing implications for the kind ofuniverse that in the Age of the Enlightenment was imagined to havebeen set in motion initially <strong>and</strong> then left to run forever like clockwork.Newton’s laws have built into them the implicit assumption thatomniscience is possible, at least in principle. For example, Newton’sdefinition of an inertial frame of reference leads to an infinite regress,as described on p. 429. For Newton this isn’t a problem, becausein principle an omnisicient observer can know the location of everymass in the universe. In this conception of the cosmos, thereare no theoretical limits on human knowledge, only practical ones;if we could gather sufficiently precise data about the state of theuniverse at one time, <strong>and</strong> if we could carry out all the calculationsto extrapolate into the future, then we could know everything thatwould ever happen. (See the famous quote by Laplace on p. 16.)But the existence of event horizons surrounding black holes makesSection 7.4 ⋆ General Relativity 431

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