- #1
yuiop
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While posting a reply in another thread, I had an inspiration for a device to measure spacetime curvature. It is well know that we can measure this curvature by measuring the angles of a large triangle or comparing the circumference of a circle to its radius, but his device may may be simpler or more portable.
The device requires two rulers, one 10 meters long and the other 1 meter long. Reflectors are placed at the ends of each ruler and the other ends are aligned with each other and common signal emitter is placed there. The light path on the short ruler is arranged so that signal bounces to and fro ten times before returning to an interferometer. The light path on the longer ruler does one round trip before being routed to the interferometer. In flat space the signals should return at the same time and there will be no interference detected when tuned and calibrated correctly. Now if the device is placed in a gravitational field or in the pseudo gravitational field of a linearly or rotationally accelerating frame the device will detect curvature as an interference pattern (although it might be argued that it is detecting proper acceleration and is simply acting as a relativistic accelerometer with no moving parts).
A similar device might have the short ruler connected at right angles to the longer ruler. Rotating this device slowly to different orientations in curved space will produce changes in the interference pattern.
Yet another device will simply have identical signal sources placed a fixed distance from each other and detect the difference in redshift between the two sources as an indication of curvature (or acceleration?).
Any thoughts on the workings or the interpretations of the indications?
I am also curious if such devices would detect any curvature when in free fall in a gravitational field, assuming the device is sufficiently rigid to maintain reasonably constant proper length?
The device requires two rulers, one 10 meters long and the other 1 meter long. Reflectors are placed at the ends of each ruler and the other ends are aligned with each other and common signal emitter is placed there. The light path on the short ruler is arranged so that signal bounces to and fro ten times before returning to an interferometer. The light path on the longer ruler does one round trip before being routed to the interferometer. In flat space the signals should return at the same time and there will be no interference detected when tuned and calibrated correctly. Now if the device is placed in a gravitational field or in the pseudo gravitational field of a linearly or rotationally accelerating frame the device will detect curvature as an interference pattern (although it might be argued that it is detecting proper acceleration and is simply acting as a relativistic accelerometer with no moving parts).
A similar device might have the short ruler connected at right angles to the longer ruler. Rotating this device slowly to different orientations in curved space will produce changes in the interference pattern.
Yet another device will simply have identical signal sources placed a fixed distance from each other and detect the difference in redshift between the two sources as an indication of curvature (or acceleration?).
Any thoughts on the workings or the interpretations of the indications?
I am also curious if such devices would detect any curvature when in free fall in a gravitational field, assuming the device is sufficiently rigid to maintain reasonably constant proper length?