pole tensorowe

Explicitly, let T be a tensor field of type (p,q).

This identity hold for tensor fields of all orders.

It is therefore a tensor field of rank three.

Note that the tensor field only needs to be defined on the curve for this definition to make sense.

A tensor field is an element of this set.

The same is true in general relativity, of tensor fields describing a physical property.

It is also possible for a tensor field to have a "density".

The solution is a metric tensor field, rather than a wavefunction.

The theory seems to contain an asymmetric tensor field and a source current vector.

The result can be generalized to higher rank symmetric tensor fields.