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In mathematics, a tensor is a certain kind of geometrical entity which generalizes the concepts of scalar, vector (spatial) and linear operator in a way that is independent of any chosen frame of reference. Tensors are of importance in physics and engineering.
While tensors can be represented by multi-dimensional arrays of components, the point of having a tensor theory is to explain the further implications of saying that a quantity is a tensor, beyond that specifying it requires a number of indexed components. In particular, tensors behave in special ways under coordinate transformations.
This article attempts to provide a non-technical introduction to the idea of tensors, and to provide an introduction to the articles which describe different, complementary treatments of the theory of tensors in detail.
The word tensor was introduced by William Rowan Hamilton in 1846, but he used the word for what is now called modulus. The word was used in its current meaning by Woldemar Voigt in 1899.
The notation was developed around 1890 by Gregorio Ricci-Curbastro under the title absolute differential geometry, and made accessible to many mathematicians by the publication of Tullio Levi-CivitaTullio Levi-Civit ( March 29, 1873 December 29, 1941) was an Italian mathematician, most famous for his work on tensor calculus but who also made significant contributions in other areas, some related to this work and some not. He was a pupil of Gregorio's classic text The Absolute Differential Calculus in 1900 (in Italian; translations followed). The tensor calculus achieved broader acceptance with the introduction of Einstein's theory of general relativityGeneral relativity (GR or general relativity theory (GRT is the theory of gravitation published by Albert Einstein in 1915. The conceptual core of general relativity, from which its other consequences largely follow, is the Principle of Equivalence which, around 1915. General Relativity is formulated completely in the language of tensors, which Einstein had learned from Levi-Civita himself with great difficulty. But tensors are used also within other fields such as continuum mechanicsContinuum mechanics is a branch of physics (specifically mechanics) that deals with continuous matter, including both solids and fluids (i. liquids and gases). The fact that matter is made of atoms and that it commonly has some sort of heterogeneous micro, for example the strain tensorThe strain tensor [ε] is a symmetric tensor used to quantify the strain of an object undergoing a 3-dimensional deformation: the diagonal coefficients ε are the relative change in length in the direction of the i direction (along the x axi, (see linear elasticityContinuum mechanics Linear elasticity The linear theory of elasticity models the macroscopic mechanical properties of solids assuming "small" deformations. Basic equations Linear elastodynamics is based on three tensor equations: dynamic equation constitu).
Note that the word "tensor" is often used as a shorthand for tensor fieldDifferential geometry Differential topology 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 genera, which is a tensor value defined at every point in a manifold. To understand tensor fields, you need to first understand the basic idea of tensors.
There are two ways of approaching the definition of tensors: