HOME

TheInfoList




In
mathematics Mathematics (from Greek: ) includes the study of such topics as numbers (arithmetic and number theory), formulas and related structures (algebra), shapes and spaces in which they are contained (geometry), and quantities and their changes (cal ...
, tensor calculus, tensor analysis, or
Ricci calculus In mathematics Mathematics (from Greek: ) includes the study of such topics as numbers (arithmetic and number theory), formulas and related structures (algebra), shapes and spaces in which they are contained (geometry), and quantities and t ...
is an extension of
vector calculus Vector calculus, or vector analysis, is concerned with differentiation Differentiation may refer to: Business * Differentiation (economics), the process of making a product different from other similar products * Product differentiation, in ...
to
tensor field In mathematics Mathematics (from Greek: ) includes the study of such topics as numbers (arithmetic and number theory), formulas and related structures (algebra), shapes and spaces in which they are contained (geometry), and quantities and t ...
s (
tensor In mathematics Mathematics (from Greek: ) includes the study of such topics as numbers (arithmetic and number theory), formulas and related structures (algebra), shapes and spaces in which they are contained (geometry), and quantities a ...

tensor
s that may vary over a
manifold In mathematics Mathematics (from Greek: ) includes the study of such topics as numbers (arithmetic and number theory), formulas and related structures (algebra), shapes and spaces in which they are contained (geometry), and quantities a ...

manifold
, e.g. in
spacetime In physics, spacetime is any mathematical model which fuses the three-dimensional space, three dimensions of space and the one dimension of time into a single four-dimensional manifold. Minkowski diagram, Spacetime diagrams can be used to visuali ...
). Developed by
Gregorio Ricci-Curbastro Gregorio Ricci-Curbastro (; 12January 1925) was an Italian mathematician. He is most famous as the inventor of tensor calculus, but also published important works in other fields. With his former student Tullio Levi-Civita, he wrote his most f ...
and his student
Tullio Levi-Civita Tullio Levi-Civita, (, ; 29 March 1873 – 29 December 1941) was an Italians, Italian mathematician, most famous for his work on absolute differential calculus (tensor calculus) and its applications to the theory of relativity, but who also made ...
, it was used by
Albert Einstein Albert Einstein ( ; ; 14 March 1879 – 18 April 1955) was a German-born theoretical physicist, widely acknowledged to be one of the greatest physicists of all time. Einstein is known for developing the theory of relativity The theo ...

Albert Einstein
to develop his
general theory of relativity General relativity, also known as the general theory of relativity, is the geometric Geometry (from the grc, γεωμετρία; '' geo-'' "earth", '' -metron'' "measurement") is, with arithmetic, one of the oldest branches of mathema ...
. Unlike the
infinitesimal calculus Calculus, originally called infinitesimal calculus or "the calculus of infinitesimal In mathematics, infinitesimals or infinitesimal numbers are quantities that are closer to zero than any standard real number, but are not zero. They do not ex ...
, tensor calculus allows presentation of physics equations in a form that is independent of the choice of coordinates on the manifold. Tensor calculus has many applications in physics, engineering and computer science including Elasticity (physics), elasticity, continuum mechanics, electromagnetism (see mathematical descriptions of the electromagnetic field), general relativity (see mathematics of general relativity), quantum field theory, and machine learning. Working with a main proponent of the exterior calculus Elie Cartan, the influential geometer Shiing-Shen Chern summarizes the role of tensor calculus:
In our subject of differential geometry, where you talk about manifolds, one difficulty is that the geometry is described by coordinates, but the coordinates do not have meaning. They are allowed to undergo transformation. And in order to handle this kind of situation, an important tool is the so-called tensor analysis, or Ricci calculus, which was new to mathematicians. In mathematics you have a function, you write down the function, you calculate, or you add, or you multiply, or you can differentiate. You have something very concrete. In geometry the geometric situation is described by numbers, but you can change your numbers arbitrarily. So to handle this, you need the Ricci calculus.


Syntax

Tensor notation makes use of upper and lower indexes on objects that are used to label a variable object as Covariance and contravariance of vectors, covariant (lower index), Covariance and contravariance of vectors, contravariant (upper index), or mixed covariant and contravariant (having both upper and lower indexes). In fact in conventional math syntax we make use of covariant indexes when dealing with Cartesian coordinate systems (x_1, x_2, x_3) frequently without realizing this is a limited use of tensor syntax as covariant indexed components. Tensor notation allows upper index on an object that may be confused with normal power operations from conventional math syntax. For example, in normal math syntax, e=mc^2= mcc, however in tensor syntax a parenthesis should be used around an object before raising it to a power to disambiguate the use of a tensor index versus a normal power operation. In tensor syntax we would write, e=m(c^1)^2= m(c^1)(c^1) and e=m(c^2)^2= m(c^2)(c^2). The number in the inner parenthesis distinguishes the contravariant component where the outer parenthesis number distinguishes the power to raise the quantities to. Of course this is just an arbitrary equation, we could have specified that ''c'' is not a tensor and known that this particular variable does not need a parenthesis around it to take the quality ''c'' to a power of 2, however, if ''c'' were a vector, then it could be represented as a tensor and this tensor would need to be distinguished from normal math indexes that indicate raising a quantity to a power.


Key concepts


Vector decomposition

Tensors notation allows a vector (\vec) to be decomposed into an Einstein summation representing the tensor contraction of a basis vector (\vec_i or \vec^i) with a component vector (V_i or V^i). \vec = V^i \vec_i = V_i \vec^i Every vector has two different representations, one referred to as contravariant component (V^i) with a covariant basis (\vec_i), and the other as a covariant component (V_i) with a contravariant basis (\vec^i). Tensor objects with all upper indexes are referred to as contravariant, and tensor objects with all lower indexes are referred to as covariant. The need to distinguish between contravariant and covariant arises from the fact that when we dot an arbitrary vector with its basis vector related to a particular coordinate system, there are two ways of interpreting this dot product, either we view it as the projection of the basis vector onto the arbitrary vector, or we view it as the projection of the arbitrary vector onto the basis vector, both views of the dot product are entirely equivalent, but have different component elements and different basis vectors: \vec \cdot \vec_i = V_i = \vec^T \vec_i = \vec_i^T \vec = \cdot \vec_i = \cdot \vec \vec \cdot \vec^i = V^i = \vec^T \vec^i = ^T \vec = \cdot \vec^i = \cdot \vec For example, in physics you start with a vector field, you decompose it with respect to the covariant basis, and that's how you get the contravariant coordinates. For orthonormal cartesian coordinates, the covariant and contravariant basis are identical, since the basis set in this case is just the identity matrix, however, for non-affine coordinate system such as polar or spherical there is a need to distinguish between decomposition by use of contravariant or covariant basis set for generating the components of the coordinate system.


Covariant vector decomposition

\vec = V^i \vec_i


Contravariant vector decomposition

\vec = V_i \vec^i


Metric tensor

The metric tensor represents a matrix with scalar elements (Z_ or Z^) and is a tensor object which is used to raise or lower the index on another tensor object by an operation called contraction, thus allowing a covariant tensor to be converted to a contravariant tensor, and vice versa. Example of lowering index using metric tensor: T_i=Z_T^j Example of raising index using metric tensor: T^i=Z^T_j The metric tensor is defined as: Z_ = \vec_i \cdot \vec_j Z^ = \vec^i \cdot \vec^j This means that if we take every permutation of a basis vector set and dotted them against each other, and then arrange them into a square matrix, we would have a metric tensor. The caveat here is which of the two vectors in the permutation is used for projection against the other vector, that is the distinguishing property of the covariant metric tensor in comparison with the contravariant metric tensor. Two flavors of metric tensors exist: (1) the contravariant metric tensor (Z^), and (2) the covariant metric tensor (Z_). These two flavors of metric tensor are related by the identity: Z_Z^ = \delta^j_i For an orthonormal Cartesian coordinate system, the metric tensor is just the kronecker delta \delta_ or \delta^, which is just a tensor equivalent of the identity matrix, and \delta_ = \delta^ = \delta^i_j.


Jacobian

In addition a tensor can be readily converted from an unbarred(x) to a barred coordinate(\bar) system having different sets of basis vectors: f(x^1, x^2, \dots, x^n) = f\bigg(x^1(\bar), x^2(\bar), \dots, x^n(\bar)\bigg) = \bar(\bar^1, \bar^2, \dots, \bar^n)= \bar\bigg(\bar^1(x), \bar^2(x), \dots, \bar^n(x)\bigg) by use of Jacobian matrix relationships between the barred and unbarred coordinate system (\bar=J^). The Jacobian between the barred and unbarred system is instrumental in defining the covariant and contravariant basis vectors, in that in order for these vectors to exist they need to satisfy the following relationship relative to the barred and unbarred system: Contravariant vectors are required to obey the laws: v^i = \bar^r\frac \bar^i = v^r\frac Covariant vectors are required to obey the laws: v_i = \bar_r\frac \bar_i = v_r\frac There are two flavors of Jacobian matrix: 1. The J matrix representing the change from unbarred to barred coordinates. To find J, we take the "barred gradient", i.e. partial derive with respect to \bar^i: J = \bar f(x(\bar)) 2. The \bar matrix, representing the change from barred to unbarred coordinates. To find \bar, we take the "unbarred gradient", i.e. partial derive with respect to x^i: \bar = \nabla \bar(\bar(x))


Gradient vector

Tensor calculus provides a generalization to the gradient vector formula from standard calculus that works in all coordinate systems: \nabla F = \nabla_i F \vec^i Where: \nabla_i F = \frac In contrast, for standard calculus, the gradient vector formula is dependent on the coordinate system in use (example: Cartesian gradient vector formula vs. the polar gradient vector formula vs. the spherical gradient vector formula, etc.). In standard calculus, each coordinate system has its own specific formula, unlike tensor calculus that has only one gradient formula that is equivalent for all coordinate systems. This is made possible by an understanding of the metric tensor that tensor calculus makes use of.


See also

*Vector analysis *Matrix calculus *
Ricci calculus In mathematics Mathematics (from Greek: ) includes the study of such topics as numbers (arithmetic and number theory), formulas and related structures (algebra), shapes and spaces in which they are contained (geometry), and quantities and t ...
*Curvilinear coordinates **Tensors in curvilinear coordinates *Multilinear subspace learning


References


Further reading

* * * * * * *


External links

* {{Authority control Calculus Tensors