| | #Unlike most well-tested fundamental physical theories, the theory of relativity violates conditions of a conservative field. Path independence, for example, is lacking under the theory of relativity, as in the "twin paradox" whereby the age of each twin under the theory is dependent on the path he traveled.<ref>In defense of the theory, it is noted that it mandates conservation of the matter-stress-energy tensor (the only way to get ''real'' conservation, since matter and energy are interchangeable.) This follows from the "contracted Bianchi identity". [http://www.mth.uct.ac.za/omei/gr/chap6/node14.html] Also, the curl of the "gravitational field vector" is exactly zero in the absence of moving sources, due to symmetries of [[Riemann]]'s tensor. It follows, from [[Stokes' Theorem]], that the gravitational field is conservative and has a potential function. Energy is conserved.</ref> | | #Unlike most well-tested fundamental physical theories, the theory of relativity violates conditions of a conservative field. Path independence, for example, is lacking under the theory of relativity, as in the "twin paradox" whereby the age of each twin under the theory is dependent on the path he traveled.<ref>In defense of the theory, it is noted that it mandates conservation of the matter-stress-energy tensor (the only way to get ''real'' conservation, since matter and energy are interchangeable.) This follows from the "contracted Bianchi identity". [http://www.mth.uct.ac.za/omei/gr/chap6/node14.html] Also, the curl of the "gravitational field vector" is exactly zero in the absence of moving sources, due to symmetries of [[Riemann]]'s tensor. It follows, from [[Stokes' Theorem]], that the gravitational field is conservative and has a potential function. Energy is conserved.</ref> |
| | #The Ehrenfest Paradox: Consider a spinning hoop, where the tangential velocity is near the speed of light. In this case, the circumference (<math>2 \pi R</math>) is length-contracted. However, since <math>R</math> is always perpendicular to the motion, it is not contracted. This leads to a paradox: does the radius of the accelerating hoop equal <math>R</math>, or is it less than <math>R</math>? | | #The Ehrenfest Paradox: Consider a spinning hoop, where the tangential velocity is near the speed of light. In this case, the circumference (<math>2 \pi R</math>) is length-contracted. However, since <math>R</math> is always perpendicular to the motion, it is not contracted. This leads to a paradox: does the radius of the accelerating hoop equal <math>R</math>, or is it less than <math>R</math>? |
| | + | #The Twin Paradox: Consider twins who are separated with one traveling at a very high speed such that his "clock" (age) slows down, so that when he returns he has a younger age than the twin; this violates Relativity because ''both'' twins should expect the other to be younger, if motion is relative. Einstein himself admitted that this contradicts Relativity.<ref>Einstein attempted to explain the paradox based on the acceleration that one twin uniquely undergoes, but the length of travel can simply be extended to the point where any effect from acceleration would be ''de minimis''.</ref> |
| | + | #Relativity predicted that clocks at the Earth's equator would be slower than clocks at the North Pole, due to different velocities; in fact, all clocks at sea level measure time at the same rate, and Relativitists made new assumptions about the Earth's shape to justify this contradiction of the theory. |