17.02.2014 Views

Mathematical Methods for Physicists: A concise introduction - Site Map

Mathematical Methods for Physicists: A concise introduction - Site Map

Mathematical Methods for Physicists: A concise introduction - Site Map

SHOW MORE
SHOW LESS

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

VECTOR AND TENSOR ANALYSIS<br />

(2) Addition (subtraction): The sum (di€erence) of two or more tensors of the<br />

same type and rank is also a tensor of the same type and rank. Addition of<br />

tensors is commutative and associative.<br />

(3) Outer product of tensors: The product of two tensors is a tensor whose rank<br />

is the sum of the ranks of the given two tensors. This product involves<br />

ordinary multiplication of the components of the tensor and it is called<br />

the outer product. For example, A B ˆ C <br />

is the outer product<br />

of A and B .<br />

(4) Contraction: If a covariant and a contravariant index of a mixed tensor are<br />

set equal, a summation over the equal indices is to be taken according to the<br />

summation convention. The resulting tensor is a tensor of rank two less than<br />

that of the original tensor. This process is called contraction. For example, if<br />

we start with a fourth-order tensor T , one way of contracting it is to set<br />

ˆ , which gives the second rank tensor T . We could contract it again<br />

to get the scalar T .<br />

(5) Inner product of tensors: The inner product of two tensors is produced by<br />

contracting the outer product of the tensors. For example, given two tensors<br />

A and B , the outer product is A B . Setting ˆ , we obtain the<br />

inner product A B .<br />

(6) Symmetric and antisymmetric tensors: A tensor is called symmetric with<br />

respect to two contravariant or two covariant indices if its components<br />

remain unchanged upon interchange of the indices:<br />

A ˆ A ; A ˆ A :<br />

A tensor is called anti-symmetric with respect to two contravariant or two<br />

covariant indices if its components change sign upon interchange of the<br />

indices:<br />

A ˆA ; A ˆA :<br />

Symmetry and anti-symmetry can be de®ned only <strong>for</strong> similar indices, not<br />

when one index is up and the other is down.<br />

Quotient law<br />

A quantity Q ... ... with various up and down indexes may or may not be a tensor.<br />

We can test whether it is a tensor or not by using the quotient law, which can be<br />

stated as follows:<br />

Suppose it is not known whether a quantity X is a tensor or not.<br />

If an inner product of X with an arbitrary tensor is a tensor, then<br />

X is also a tensor.<br />

50

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!