Contravariant Tensor (original) (raw)
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A contravariant tensor is a tensor having specific transformation properties (cf., a covariant tensor). To examine the transformation properties of a contravariant tensor, first consider a tensor of rank 1 (a vector)
(1) |
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for which
(2) |
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Now let , then any set of quantities
which transform according to
(3) |
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or, defining
(4) |
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according to
(5) |
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is a contravariant tensor. Contravariant tensors are indicated with raised indices, i.e., .
Covariant tensors are a type of tensor with differing transformation properties, denoted . However, in three-dimensional Euclidean space,
(6) |
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for , 2, 3, meaning that contravariant and covariant tensors are equivalent. Such tensors are known as Cartesian tensor. The two types of tensors do differ in higher dimensions, however.
Contravariant four-vectors satisfy
(7) |
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where is a Lorentz tensor.
To turn a covariant tensor into a contravariant tensor
(index raising), use themetric tensor
to write
(8) |
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Covariant and contravariant indices can be used simultaneously in a mixed tensor.
See also
Cartesian Tensor, Contravariant Vector, Covariant Tensor, Four-Vector,Index Raising, Lorentz Tensor, Metric Tensor, Mixed Tensor, Tensor
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References
Arfken, G. "Noncartesian Tensors, Covariant Differentiation." ยง3.8 in Mathematical Methods for Physicists, 3rd ed. Orlando, FL: Academic Press, pp. 158-164, 1985.Morse, P. M. and Feshbach, H. Methods of Theoretical Physics, Part I. New York: McGraw-Hill, pp. 44-46, 1953.Weinberg, S. Gravitation and Cosmology: Principles and Applications of the General Theory of Relativity. New York: Wiley, 1972.
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Cite this as:
Weisstein, Eric W. "Contravariant Tensor." From MathWorld--A Wolfram Web Resource. https://mathworld.wolfram.com/ContravariantTensor.html