curvature of space-time xamidegi-ye fazâ-zamân (#) Fr.: courbure de l'espace-temps According to → general relativity, → space-time is curved by the presence of → matter. The curvature is described in terms of → Riemann's geometry. In → cosmological models three types of curvature are considered: positive (spherical, → closed Universe), zero (Euclidean, → flat Universe), and negative (hyperbolic, → open Universe). See also → curvature constant. → curvature; → space-time. |
Minkowski space-time fazâ-zamân-e Minkowski (#) Fr.: espace-temps de Minkowski A completely flat four-dimensional space, which contains no gravitating matter, used in the theory of special relativity. → Minkowski metric; → space-time. |
space-time fazâ-zamân (#) Fr.: espace-temps A physical entity resulting from the union of space and time concepts. In its most simple version space-time is the four-dimensional continuum, having three spatial coordinates and one temporal coordinate, in which any → event or physical object is located. In → special relativity it is Minkowski's flat space-time. In → general relativity, it is described by a curved entity characterized by a → metric. Free-fall motion describes the → geodesic of this curved space-time. It may have additional dimensions in the context of speculative theories, such as → string theory. |
space-time curvature xamidegi-ye fazâ-zamân Fr.: courbure de l'espace-temps |
space-time diagram nemudâr-e fazâ-zamân (#) Fr.: diagramme espace-temps A simple way of representing the → space-time continuum, usually including time and only one spatial dimension. The curve of a particle's equation of motion on a space-time diagram is called a → world line. Same as → Minkowski diagram. |
space-time interval andarvâr-e fazâ-zamân Fr.: intervalle espace-temps 1) In Einstein's → theory of relativity,
ds2 = c2dt2 -
dx2 - dy2 - dz2. → space-time; → interval. |