Difference between revisions of "Interval"
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In general relativity theory one considers the interval between two infinitesimally-close events: | In general relativity theory one considers the interval between two infinitesimally-close events: | ||
− | $$ds=\sqrt{-g_{ik}dx^ | + | $$ds=\sqrt{-g_{ik}\,dx^i\,dx^k},$$ |
where $dx^i$ is the infinitesimal difference of the space-time coordinates of these events and $g_{ik}$ is the metric tensor. | where $dx^i$ is the infinitesimal difference of the space-time coordinates of these events and $g_{ik}$ is the metric tensor. |
Latest revision as of 14:51, 30 December 2018
See Interval and segment.
A space-time interval is a quantity characterizing the relation between two events separated by a spatial distance and a time duration. In special relativity theory the square of an interval is
$$s^2=c^2(t_2-t_1)^2-(x_2-x_1)^2-(y_2-y_1)^2-(z_2-z_1)^2,$$
where $c$ is the velocity of light, $x_i,y_i,z_i$ are the space coordinates and $t_i$ are the corresponding points in time (for more details, see Minkowski space).
In general relativity theory one considers the interval between two infinitesimally-close events:
$$ds=\sqrt{-g_{ik}\,dx^i\,dx^k},$$
where $dx^i$ is the infinitesimal difference of the space-time coordinates of these events and $g_{ik}$ is the metric tensor.
Comments
A space-time interval with $s^2>0$ is called a time-like space-time interval, and one with $s^2<0$ is called a space-like space-time interval.
References
[a1] | D.F. Lawden, "An introduction to tensor calculus and relativity" , Methuen (1962) |
[a2] | R.K. Sachs, H. Wu, "General relativity for mathematicians" , Springer (1977) |
[a3] | E. Tocaci, "Relativistic mechanics, time, and inertia" , Reidel (1985) pp. Sect. A.II.1.4 |
Interval. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Interval&oldid=43587