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Euclidean vectors

The examinations will be accomplished in the three-dimensional Euclidean vector space, where the scalar product of vectors is defined beyond the prop -erties of the afline space. Cartesian coordinates with their orthogonal, straight, and normalized base are sufficient for the problems at hand and therefore will be used. [Pg.19]

Brockmaim, Theory of Adaptive Fiber Composites, Solid Mechanics and Its Applications 161, [Pg.19]

The scalar or dot product processes two vectors, for example v and w, of arbitrary dimension into a scalar. The scalar product is commutative  [Pg.20]

The vector or cross product determines a so-called axial vector with orthogonal orientation from two spatial vectors. The vector product is anti-commutative  [Pg.20]


The euclidean norm of a matrix considered as a vector in m2-space is a matrix norm that is consistent with the euclidean vector norm. This is perhaps the matrix norm that occurs most frequently in the literature. But the euclidean norm of I is n112 > 1 when n > 1, hence it is not a sup. In fact,... [Pg.57]

Suppose that V is a finite-dimensional complex vector space. By the definition this means that V has a finite basis. It turns out that all the different bases of V must be the same size. This is geometrically plausible for real Euclidean vector spaces, where one can visualize a basis of size one determiiung a line, a basis of size two determining a plane, and so on. The same is true for complex vector spaces. A key part of the proof, useful in its own right, is the following fact. [Pg.46]

Thus far the discussion has been largely confined to a specific set of reference intensities and extensities. However, equations such as (11.10) make clear the possibility of treating more general types of thermodynamic variations. Transformations among thermodynamic variables will correspond to ordinary Euclidean vector transformations, which can therefore be treated simply and systematically in Ms-... [Pg.357]

It is a remarkable fact that properties (13.4a-c) are necessary and sufficient to give Euclidean geometry. In other words, if any rule can be found that associates a number (say, (X Y)) with each pair of abstract objects ( vectors X), Y)) of the manifold in a way that satisfies (13.4a-c), then the manifold is isomorphic to a corresponding Euclidean vector space. We introduced a rather unconventional rule for the scalar products (X Y) [recognizing that (13.4a-c) are guaranteed by the laws of thermodynamics] to construct the abstract Euclidean metric space Ms for an equilibrium state of a system S, characterized by a metric matrix M. This geometry allows the thermodynamic state description to be considerably simplified, as demonstrated in Chapters 9-12. [Pg.425]

The least squares solution x of an unsolvable linear system Ax = b such as our system is the vector x that minimizes the error Ax — 6 in the euclidean vector norm a defined by x Jx +. .. + x% when the vector x has n real entries x. ... [Pg.18]

A graphic that can be produced to better describe the actual situation is the plot of b against y-y, where symbolizes the Euclidean vector norm [4CM16], As Figure 5.14 discloses, an /.-shaped curve results with the best model occurring at the bend, which reflects a harmonious model with the least amount of compromise in the trade-off between minimization of the residual and regression vector norms. The regression vector norm acts as an indicator of variance for the... [Pg.144]

Secondly, the commutator is the Lie product33 of the operators X Xs and Xu this choice of multiplication is particularly appropriate when one realizes that the X XS are the generators of the semisimple compact Lie group U , which is associated with the infinitesimal unitary transformations of the Euclidean vector space R (e.g., the space of the creation operators).34 With the preceding comments, the action of the transformation operator on the creation operators can formally be written in the usual form of the transformation law for covariant vectors,33... [Pg.216]

First it will be shown that for any real nonsingular matrix A of order n, there exists a particular vector Xx such that jXj = 1 and flAXj = A. The matrix norm so constructed is said to be subordinate to the given vector norm. Then it will be shown that the matrix norm so constructed satisfies the four conditions required of a matrix norm as well as the compatibility relationship. Only the matrix norm subordinate to the euclidean vector norm X , given by Eq. (A-26) is considered. Now consider the vector AX, whose vector norm as given by Eq. (A-26), is... [Pg.590]

Now it will be shown that the Hilbert matrix norm and the euclidean vector norm satisfy the four requirements as well as the compatibility relationship. To show that the first condition is satisfied, let A be any real nonsingular, nonzero matrix (A 0). Then there exists a vector X such that X , = 1 and such that the euclidean norm of the vector AX is a maximum and nonzero. Moreover, the particular vector X that satisfies these conditions is the eigenvector Xt corresponding to the largest eigenvalue That is... [Pg.591]

Since there exists an X having a euclidean norm of unity for which the euclidean vector norm of AX is a maximum, it follows that... [Pg.591]

In the - = Xi ctor interpretation the vector space is the m-dimen-sional Euclidean vector space spanned by the AIM basis vectors i > = c, and the scalar (inner) product = aibi, where (ai, bj are components of (3, b) on e. The occupation interpretation calls for the m-dimensional function space spanned by the corresponding AIM function vectors, 11> = 1with the appropriate definition of the scalar product, = J PJ Ppdt. [Pg.181]

Formally, a vector is a set of two or more variable values, but our use of the term will be restricted to Euclidean vectors, which are governed by the following definitions and rules ... [Pg.11]

Here we consider the Euclidean vector space p and assume that the components of an arbitrary vector IR3 are its Cartesian components with respect to a fixed orthonormal basis where the former are denoted by Xj =x,X2 = y, X3 = z, respectively. Accordingly a tensor of rank [m is defined as follows ... [Pg.1181]


See other pages where Euclidean vectors is mentioned: [Pg.658]    [Pg.57]    [Pg.425]    [Pg.542]    [Pg.425]    [Pg.5]    [Pg.324]    [Pg.591]    [Pg.6]    [Pg.494]    [Pg.494]    [Pg.529]    [Pg.19]    [Pg.723]   
See also in sourсe #XX -- [ Pg.11 ]

See also in sourсe #XX -- [ Pg.19 ]




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Euclidean

Feature vectors Euclidean

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