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Orthogonality

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orthogonality

In mathematics, a property synonymous with perpendicularity when applied to vectors but applicable more generally to functions. Two elements of an inner product space are orthogonal when their inner product—for vectors, the dot product (see vector operations); for functions, the definite integral of their product—is zero. A set of orthogonal vectors or functions can serve as the basis of an inner product space, meaning that any element of the space can be formed from a linear combination (see linear transformation) of the elements of such a set.


orthogonality [ȯr‚thäg·ə′nal·əd·ē]
(mathematics)
Two geometric objects have this property if they are perpendicular.

Orthogonality 

a generalization and often a synonym of the concept of perpendicularity. If two vectors in three-dimensional space are perpendicular, their scalar product is equal to zero. This fact permits us to generalize the concept of perpendicularity by extending it to vectors in any linear space, where a scalar product is defined with the usual properties. Thus two vectors are said to be orthogonal if their scalar product is equal to zero. In particular, let us define the scalar product in the space of complex-valued functions on the interval [a, b] by the formula

where ρ(x) ≥ 0. Then, if (f, ϕ)ρ = 0, that is,

f(x) and ϕ(x) are said to be orthogonal with respect to the weight function ρ(x). Two linear subspaces are termed orthogonal if every vector in one of them is orthogonal to every vector in the other. This concept generalizes the concept of the perpendicularity of two lines or of a line and a plane in three-dimensional space but not the concept of the perpendicularity of two planes. Curves that intersect at right angles, as measured by the angle between the tangents at the point of intersection, are called orthogonal curves.



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The analogue transform we employ to make our construction is based on some q-Bessel functions and orthogonality results from (14), which have important applications to q-deformed mechanics.
As each transmitting waveform is assigned to a distinct channel, orthogonality holds for all the transmitting signals.
 
 
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