Each diagonal element is solved for, and an approximate value plugged in.

The diagonal elements of the stress tensor are changed by a constant amount.

The diagonal elements must be real, as they must be their own complex conjugate.

The missing diagonal elements were then added afterwards.

These diagonal elements are called the principal moments of the gyration tensor.

(b) Let us add 2 to each diagonal element of A, to give.

No scanning is needed in the third variant, where the diagonal elements are prescribed.

We may first note that the product of the diagonal elements of the leading matrix in (1) is evidently.

P is usually chosen so that the diagonal elements of R are non-increasing:

As it is an orthogonal matrix these diagonal elements are either 1 or 1.