mutually orthogonal वाक्य
उदाहरण वाक्य
मोबाइल
- In general an orthant in " n "-dimensions can be considered the intersection of " n " mutually orthogonal half-spaces.
- Then the row vectors of U ^ {-1 } B are mutually orthogonal and their squared norms are the eigenvalues of A ( in order ).
- A left hand can be held, as shown in the illustration, so as to represent three mutually orthogonal axes on the thumb, first finger and middle finger.
- Furthermore, as all functions in the basis are mutually orthogonal and are not associated with any particular atom, plane-wave basis sets do not exhibit basis-set superposition error.
- Blocks, monolithic or not, are irrelevant in this or any other discussion, because the concept of a " block " and the concept of " logic " are mutually orthogonal.
- They are sometimes referred to as the versors of the coordinate system, and they form a set of mutually orthogonal unit vectors, typically referred to as a standard basis in linear algebra.
- The grand antiprism may be obtained by another diminishing of the 600-cell : removing 20 vertices that lie on two mutually orthogonal rings and taking the convex hull of the remaining vertices.
- The normalized cross product corrects for this varying length, and yields the mutually orthogonal unit vector to the two inputs, applying the right-hand rule to resolve one of two possible directions.
- A set of Latin squares of the same order forms a set of "'mutually orthogonal Latin squares ( MOLS ) "'if every pair of Latin squares in the set are orthogonal.
- Due to the PCA properties : eigenvectors are mutually orthogonal, form a basis of the training set cloud in the shape space, and cross at the 0 in this space, which represents the mean shape.
- Computationally speaking, this diminishing may be realized by removing two rings of vertices from the 600-cell, each ring having 10 vertices, and each lying in mutually orthogonal planes, and taking the convex hull of the remaining vertices.
- In fact,, ? 1 and ? 8 are three mutually orthogonal linear combinations of the quark pairs, and; they are at the centre of the pseudo-scalar nonet of mesons with all the main quantum numbers equal to zero.
- The latin squares produced in this way from an orthogonal array will be orthogonal latin squares, so the " k " " 2 columns other than the indexing columns will produce a set of " k " " 2 mutually orthogonal latin squares.
- :: Under the circumstances, " A " can be always taken to be a symmetric matrix, in which case the spectral theorem can be applied : any such matrix is diagonalizable, with real eigenvalues, and mutually orthogonal eigenvectors . talk ) 19 : 47, 23 November 2008 ( UTC)
- He is notable for his breakthrough work along with R . C . Bose and S . S . Shrikhande in their disproof of the famous conjecture made by Leonhard Euler dated 1782 that there do not exist two mutually orthogonal latin squares of order 4 " n " + 2 for every " n ".
- In both cases, the transverse directions are unaffected and the three planes meeting at each corner of the cuboids are " mutually orthogonal " ( in the sense of "'E "'1, 2 at right, and in the sense of "'E "'3 at left ).
- Due to the mutually orthogonal property, there is exactly one instance somewhere in the table for any pair of elements, such as ( white foreground, monospace ), or ( " fjords ", navy background ) etc ., and also all possible such pairs of values of distinct " dimensions " are represented exactly once each.
- We all know that given x, y, z etc that the square root of the sum of the squares ( x ^ 2 + y ^ 2 + z ^ 2 ) ^ 1 / 2 is a metric that equates to the distance between points 0, 0, 0 and x, y, z in a mutually orthogonal geometry.
- To illustrate, suppose we have a system of N bosons that occupy mutually orthogonal single-particle states | \ phi _ 1 \ rang, | \ phi _ 2 \ rang, | \ phi _ 3 \ rang, etc . Using the usual representation, we demonstrate the system by assigning a state to each particle and then imposing exchange symmetry.
- Here we utilized the cross-normalization condition l ^ an _ a = n ^ al _ a =-1 as well as the requirement that g _ { ab } + l _ an _ b + n _ al _ b should span the induced metric h _ { AB } for cross-sections of { v = constant, r = constant }, where dv and dr are not mutually orthogonal.
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