Jökull


Jökull - 01.12.1973, Side 42

Jökull - 01.12.1973, Side 42
represent a set of m linear equations with n unknowns. The coefficients aik are assumed to be real. In the following it is convenient to assume that the equations have been normalized such that the h-norm of the row-vectors is unity, viz. If jrj| zjí= 1 this can always be achieved by dividing each equation by jr±J. The underdeter- mined, well posed and overdetermined cases are then characterized by m < n, m = n, and m > n respectively. It is also convenient to rewrite (8) in vector-matrix language. Let x be the un- known n-vector (xk), b the given m-vector (bj), and A = (alk) be the m x n matrix of the en- tries aik where i = 1, 2,. . ., m, and k=l,2, . . ., n. The system (8) can then be written Ax = b (10) Let A' be the n x m transpose or adjoint of A and x • y denote the scalar product of two vectors x and y. The adjoint satisfies the identity x • Ay = A'x • y (11) for any m-vector x and n-vector y. The product matrix AA' is m x m and A'A is n x n. These two matrices are symmetric. In the following we will assume that our basic matrix A is such that both AA' and A'A are non-singular and hence invertible. The identity (11) shows that the range of A' is orthogonal to the null-space of A and vice versa. Hence, any solution of the homogeneous equations (10) has to be ortho- gonal to the range of the adjoint A'. The underdetermined case Let equations (10) represent an underdeter- mined case where m < n. Adopting the solu- tion method indicated by equations (2) and (3) above, we will assume that the solution n- vectors of (10) can be represented x = x0 + s (12) 40 JÖKULL 23. ÁR where x0 is the least 12-norm vector satisfying (10) and the vector s lies wholly within the null-space N of A, viz. As = 0 (13) for any s in N. The decomposition (12) prc- supposes the orthogonality of x0 and s, which will be verified below, and hence, |X|2=|X0|2+ |S|2 (14) The vector x0 is consequently to be found as the solution of the following minimum pro- blem [x|2 = min. (15) for all x which satisfy equations (10). This problem is solved by a standard variational technique, that is, we minimize the following expression M = |x|2 + 2a • (b — Ax) (16) where a is the Lagrange m-vector multiplier which is to be determined. The factor 2 in equation (16) is introduced for convenience. Let <3x be an arbitrary small n-vector and c a scalar. The vector gx is introduced into (16) as the variation of x, that is, we replace x in (16) by x + c ðx and minimize M with respect to c at c = 0, viz. = 2x-8x-2a-A8x = 0 (17) c = 0 The second term on the right of (17) can be written with the help of the adjoint A' a-A8x = A'a-8x (18) and hence (17) can be rewritten (x — A' a) • 8x = 0 (19) This equation has to hold for an arbitrary 8x, viz. our solution x0 = A' a 3M 9c (20)
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