Proper length
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Proper length is a relativity concept. It is an invariant quantity which is the rod distance between spacelike events in a frame of reference in which the events are simultaneous. (Unlike classical mechanics, simultaneity is relative in relativity. See relativity of simultaneity for more infomation.)
In special relativity, the proper length L between spacelike events is
<math>L=\sqrt{-c^2 \Delta t^2 + \Delta x^2 + \Delta y^2 + \Delta z^2}<math>,
where
- t is the temporal coordinates of the events for an observer,
- x, y, and z are the linear, orthogonal, spatial coordinates of the events for the same observer,
- c is the speed of light, and
- Δ stands for "difference in".
Along an arbitrary spacelike path P in either special relativity or general relativity, the proper length is given in tensor syntax by the path integral
<math>L = c \int_P \sqrt{-g_{\mu\nu} dx^\mu dx^\nu} <math>,
where
- gμν is the metric tensor for the current spacetime and coordinate mapping,
- dxμ is the coordinate separation between neighboring events along the path P,
- the +--- metric signature is used, and
- gμν has been normalized to return a time instead of a distance1.
Proper length is analogous to proper time. The difference is that proper length is the invariant interval of a spacelike path while proper time is the invariant interval of a timelike path. For more information on the used of the path integral above and examples of its use, see the proper time article.
Notes
- Note 1: By mutiplying or dividing by c2, a metric can be made to produce an invariant interval in units of either space or time. For convenience, physicists often avoid this issue by using geometrized coordinates, which are set up so that c=G=1.