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In mathematics, physics and engineering, a tensor field is a very general concept of variable geometric quantity. It is used in differential geometry and the theory of manifolds, in algebraic geometry, in general relativity, in the analysis of stress and strain in materials, and in numerous applications in the physical sciences and engineering. It is a generalisation of the idea of vector field, which can be thought of as a 'vector that varies from point to point'.
It should also be noted that many mathematical structures informally called 'tensors' are actually 'tensor fields', fields defined over a manifold which define a tensor at every point of the manifold. See the tensor article for an elementary introduction to tensors.
The geometric intuition for a vector field is of an 'arrow' attached to each point of a region, with variable length and direction. Our idea of a vector field on some curved space is supported by the example of a weather map showing horizontal wind velocity, at each point of the Earth's surface.
The general idea of tensor field combines the requirement of richer geometry - for example an ellipse varying from point to point - with the idea that we don't want our notion to depend on the particular method of mapping the surface. It should exist independently of latitude and longitude, or whatever particular 'cartographic projection' we are using to introduce numerical co-ordinates.
The contemporary mathematical expression of the idea of tensor field breaks it down into a two-step concept.
There is the idea of vector bundle, which is a natural idea of ' vector space depending on parameters' - the parameters being in a manifold. For example a vector space of one dimension depending on an angle could look like a Möbius band as well as a cylinderThe word cylinder has several meanings. For the geometric object, see Cylinder (geometry . For the engine component, see Cylinder (engine . In firearms the cylinder is the rotating device that contains the firing chambers of a revolver. The phonograph cyl. Given a vector bundle V over M, the corresponding field concept is called a section of the bundle: for m varying over M, a choice of vector vm in Vm, the vector space 'at' m.
Since the tensor productAbstract algebra Algebra In mathematics, the tensor product denoted by , may be applied in different contexts to vectors, matrices, tensors and vector spaces. In each case the significance of the symbol is the same: the most general bilinear operation. concept is independent of any choice of basis, taking the tensor product of two vector bundles on M is routine. Starting with the tangent bundleIn mathematics, the tangent bundle of a manifold is a vector bundle which as a set is the disjoint union of all the tangent spaces at every point in the manifold with natural topology and smooth structure. The tangent bundle of manifold M is usually denot (the bundle of tangent spaceDifferential topology Differential geometry In differential geometry, one can attach to every point p of a differentiable manifold a tangent space a real vector space which intuitively contains the possible "directions" in which one can pass through p''.s) the whole apparatus explained at component-free treatment of tensors carries over in a routine way - again independently of co-ordinates, as mentioned in the introduction.
In the end, we can give a definition of tensor field, namely as a sectionSection can be: A cross section (in the common sense or the physics sense) In mathematics: A conic section A section of a fiber bundle or sheaf A Caesarean section In UK law, Section 28 In the fictional Star Trek universe, Section 31 A military unit A sec of some tensor bundle. This is then guaranteed geometric content, since everything has been done in an intrinsic way.
See also jet bundleIn differential geometry, the jet bundle is a certain construction which makes a new smooth fiber bundle out of a given smooth fiber bundle. It makes it possible to write differential equations on sections of a fiber bundle in an invariant form. Historica.
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