second order tensor: symmetric and skew-symmetric parts


We shall prove the following theoremMathworldPlanetmath on existence and uniqueness. (Here, we assime that the ground field has characteristic different from 2. This hypothesisMathworldPlanetmathPlanetmath is satisfied for the cases of greatest interest, namely real and complex ground fields.)

Theorem 1.

Every covariant and contravariant tensor of second rank may be expressed univocally as the sum of a symmetricPlanetmathPlanetmathPlanetmathPlanetmath and skew-symmetric tensor.

Proof.

Let us consider a contravariant tensor.

1. Existence.  Put

Ui⁢j=12⁢(Ti⁢j+Tj⁢i),Wi⁢j=12⁢(Ti⁢j-Tj⁢i).

Then Ui⁢j=Uj⁢i is symmetric, Wi⁢j=-Wj⁢i is skew-symmetric, and

Ti⁢j=Ui⁢j+Wi⁢j.

2. Uniqueness.  Let us suppose that Ti⁢j admits the decompositions

Ti⁢j=Ui⁢j+Wi⁢j=U′⁣i⁢j+W′⁣i⁢j.

By taking the transposesMathworldPlanetmath

Tj⁢i=Uj⁢i+Wj⁢i=U′⁣j⁢i+W′⁣j⁢i,

we separate the symmetric and skew-symmetric parts in both equations and making use of their symmetry properties, we have

Ui⁢j-U′⁣i⁢j = W′⁣i⁢j-Wi⁢j
=Uj⁢i-U′⁣j⁢i = W′⁣j⁢i-Wj⁢i
=Wi⁢j-W′⁣i⁢j = U′⁣i⁢j-Ui⁢j
=-(Ui⁢j-U′⁣i⁢j) = 0,

which shows uniqueness of each part. mutatis mutandis  for a covariant tensor Ti⁢j. ∎

Title second orderPlanetmathPlanetmath tensor: symmetric and skew-symmetric parts
Canonical name SecondOrderTensorSymmetricAndSkewsymmetricParts
Date of creation 2013-03-22 15:51:32
Last modified on 2013-03-22 15:51:32
Owner rspuzio (6075)
Last modified by rspuzio (6075)
Numerical id 18
Author rspuzio (6075)
Entry type Theorem
Classification msc 15A69