Read e-book online Engineering applications of noncommutative harmonic analysis PDF

By Chirikjian G.S., Kyatkin A.B.

ISBN-10: 0849307481

ISBN-13: 9780849307485

The classical Fourier remodel is among the most generally used mathematical instruments in engineering. despite the fact that, few engineers comprehend that extensions of harmonic research to capabilities on teams holds nice capability for fixing difficulties in robotics, picture research, mechanics, and different components. for those who can be conscious of its strength worth, there's nonetheless no position they could flip to for a transparent presentation of the historical past they should observe the concept that to engineering problems.Engineering purposes of Noncommutative Harmonic research brings this robust device to the engineering international. Written in particular for engineers and computing device scientists, it bargains a pragmatic remedy of harmonic research within the context of specific Lie teams (rotation and Euclidean motion). It offers just a restricted variety of proofs, focusing as a substitute on supplying a overview of the basic mathematical effects unknown to such a lot engineers and exact discussions of particular applications.Advances in natural arithmetic can result in very tangible advances in engineering, yet provided that they're to be had and obtainable to engineers. Engineering functions of Noncommutative Harmonic research presents the potential for including this worthwhile and powerful strategy to the engineer's toolbox.

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This includes everything from satellites in space to the dynamics of liquid crystals composed of many molecules modeled as identical rigid bodies. Regardless 12 ENGINEERING APPLICATIONS OF NONCOMMUTATIVE HARMONIC ANALYSIS of the particular physical situation, they have the common feature that they are described by linear partial differential equations describing processes which evolve on the group of rotations in three dimensional space. In this context, noncommutative harmonic analysis provides a tool for converting partial differential equations into systems of ordinary differential equations in a different domain.

Both functions return real numbers. Explicitly we write (f1 ∗ f2 )(g(x1 , x2 , 0)) as f˜1 ∗ f˜2 (x1 , x2 ) = ∞ ∞ π a1 =−∞ a2 =−∞ α=−π f˜1 (a1 , a2 , α) · f˜2 ((x1 − a1 ) cos α + (x2 − a2 ) sin α, − (x1 − a1 ) sin α + (x2 − a2 ) cos α) da1 da2 dα, which is interpreted as the function f2 being swept by f1 . We can think of this as copies of f2 which are translated and rotated and then deposited on the plane with an intensity governed by f1 . With a slight modification, so that g1 = g(x1 , x2 , θ) and f2 (g(x1 , x2 , θ)) = f˜2 (x1 , x2 , θ), the result is precisely a convolution of functions on the group of rigid-body motions of the plane.

If c + fˆ(ω) = 0 for all values of ω, one can apply the Fourier inversion formula to find u(x) = F −1 g(ω) ˆ . c + fˆ(ω) In the case when c + fˆ(ω) = 0 for one or more values of ω a regularization technique is required. ” One popular method is zeroth order Tikhonov regularization [15]. In this method, one seeks a solution to the modified problem of minimization of the functional4 F = cu + f ∗ u − g 2 2 + 2 u 2 2 3 The subject of inverse problems is more general than the solution of integral equations, but all of the inverse problems encountered in this book are integral equations.

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Engineering applications of noncommutative harmonic analysis by Chirikjian G.S., Kyatkin A.B.

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