Gaussian Quadrature 1 Gaussian Quadrature
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Fortran Resources 1
Fortran Resources 1 Ian D Chivers Jane Sleightholme May 7, 2021 1The original basis for this document was Mike Metcalf’s Fortran Information File. The next input came from people on comp-fortran-90. Details of how to subscribe or browse this list can be found in this document. If you have any corrections, additions, suggestions etc to make please contact us and we will endeavor to include your comments in later versions. Thanks to all the people who have contributed. Revision history The most recent version can be found at https://www.fortranplus.co.uk/fortran-information/ and the files section of the comp-fortran-90 list. https://www.jiscmail.ac.uk/cgi-bin/webadmin?A0=comp-fortran-90 • May 2021. Major update to the Intel entry. Also changes to the editors and IDE section, the graphics section, and the parallel programming section. • October 2020. Added an entry for Nvidia to the compiler section. Nvidia has integrated the PGI compiler suite into their NVIDIA HPC SDK product. Nvidia are also contributing to the LLVM Flang project. Updated the ’Additional Compiler Information’ entry in the compiler section. The Polyhedron benchmarks discuss automatic parallelisation. The fortranplus entry covers the diagnostic capability of the Cray, gfortran, Intel, Nag, Oracle and Nvidia compilers. Updated one entry and removed three others from the software tools section. Added ’Fortran Discourse’ to the e-lists section. We have also made changes to the Latex style sheet. • September 2020. Added a computer arithmetic and IEEE formats section. • June 2020. Updated the compiler entry with details of standard conformance. -
The Legendre Transform Ross Bannister, May 2005 Orthogonality of the Legendre Polynomials the Legendre Polynomials Satisfy the Following Orthogonality Property [1], 1
The Legendre Transform Ross Bannister, May 2005 Orthogonality of the Legendre polynomials The Legendre polynomials satisfy the following orthogonality property [1], 1 2 ¥ ¥§¦ ¥ ¤ ¤ d x Pn ¤ x Pm x mn 1 © 2n ¨ 1 x ¡£¢ 1 ¥ where Pn ¤ x is the nth order Legendre polynomial. In meteorology it is sometimes convenient to integrate over the latitude domain, , instead of over x. This is achieved with the following transform, d x ¦ ¦ ¦ ¥ ¤ x sin cos d x cos d 2 d In latitude (measured in radians), Eq. (1) becomes, /2 2 ¥ ¥ ¥§¦ ¤ ¤ d cos Pn ¤ Pm mn 3 ¨ © 2n 1 ¡£¢ /2 The Legendre transform and its inverse convert to and from the latitudinal and Legendre polynomial representations of functions (I call this these transforms a Legendre transform pair). In the following we shall develop these transforms in matrix form. The matrix form of the transforms is a compact and convenient means of performing summations over and over n (we shall assume that functions are represented discreetly in space and so integrals are represented by summations). In the notation to follow, functions are represented as vectors. A function in space shall be denoted by the vector x, and a function in n space shall be denoted by p. Let the matrix consisting of columns of Legendre polynomials be F. The orthogonality condition, Eq. (3), in matrix form is, T ¦ ¥ ¤ F PF 4 where P is the so-called diagonal inner product matrix whose diagonal elements are cos and is the ¨ ¥ diagonal matrix whose diagonal elements are the normalizations 2 / ¤ 2n 1 . Legendre transform pair ('unbalanced' version) The orthogonality condition, Eq. -
Calculation of Highly Oscillatory Integrals by Quadrature Methods
CALCULATION OF HIGHLY OSCILLATORY INTEGRALS BY QUADRATURE METHODS A Senior Scholars Thesis by KRISHNA THAPA Submitted to Honors and Undergraduate Research Texas A&M University in partial fulfillment of the requirements for the designation as UNDERGRADUATE RESEARCH SCHOLAR May 2012 Major: Physics CALCULATION OF HIGHLY OSCILLATORY INTEGRALS BY QUADRATURE METHODS A Senior Scholars Thesis by KRISHNA THAPA Submitted to Honors and Undergraduate Research Texas A&M University in partial fulfillment of the requirements for the designation as UNDERGRADUATE RESEARCH SCHOLAR Approved by: Research Advisor: Stephen Fulling Associate Director, Honors and Undergraduate Research: Duncan MacKenzie May 2012 Major: Physics iii ABSTRACT Calculation of Highly Oscillatory Integrals by Quadrature Methods. (May 2012) Krishna Thapa Department of Physics Texas A&M University Research Advisor: Dr. Stephen Fulling Department of Mathematics R 1 i!g(x) Highly oscillatory integrals of the form I(f) = 0 dxf(x)e arise in various problems in dynamics, image analysis, optics, and other fields of physics and math- ematics. Conventional approximation methods for such highly oscillatory integrals tend to give huge errors as frequency (!) ! 1. Over years, various attempts have been made to get over this flaw by considering alternative quadrature methods for integration. One such method was developed by Filon in 1928, which Iserles et al. have recently extended. Using this method, Iserles et al. show that as ! ! 1, the error decreases further as the error is inversely proportional to !. We use methods developed by Iserles' group, along with others like Newton-Cotes, Clenshaw-Curtis and Levin's methods with the aid of Mathematica. Our aim is to find a systematic way of calculating highly oscillatory integrals. -
Numerical Construction of Gaussian Quadrature Formulas For
mathematics of computation, VOLUME 27, NUMBER 124, OCTOBER 1973 Numerical Construction of Gaussian Quadrature Formulas for / (-Log *)• xa-f(x)-dx and / Em(x)-j(x)-dx Jo Jo By Bernard Danloy Abstract. Most nonclassical Gaussian quadrature rules are difficult to construct because of the loss of significant digits during the generation of the associated orthogonal poly- nomials. But, in some particular cases, it is possible to develop stable algorithms. This is true for at least two well-known integrals, namely ¡l-(Loêx)-x°f(x)dx and ¡Ô Em(x)f(x)-dx. A new approach is presented, which makes use of known classical Gaussian quadratures and is remarkably well-conditioned since the generation of the orthogonal polynomials requires only the computation of discrete sums of positive quantities. Finally, some numerical results are given. 1. Introduction. Let w(x) be a nonnegative weight function on (a, b) such that all its moments (1.1) M*= / w(x)-x"-dx, k = 0, 1, 2, ••■ , exist. The «-point Gaussian quadrature rule associated with w(x) and (a, b) is that uniquely defined linear functional (1.2) G„-/= ¿X, •/(*,) ¿-i which satisfies (1.3) G„/ = [ w(x)-j(x)-dx Ja whenever / is a polynomial of degree ^ 2n — 1. It is a well-known result [8] that the Gaussian abscissas *¿ are the roots of the polynomials orthogonal on (a, b) with respect to w(x), and that the associated coeffi- cients X,, called Christoffel constants, can also be expressed in terms of these poly- nomials. A direct exploitation of these results is still the most widely recommended procedure, even though alternative approaches have been suggested by Rutishauser [7], Golub and Welsch [6]. -
Evolving Software Repositories
1 Evolving Software Rep ositories http://www.netli b.org/utk/pro ject s/esr/ Jack Dongarra UniversityofTennessee and Oak Ridge National Lab oratory Ron Boisvert National Institute of Standards and Technology Eric Grosse AT&T Bell Lab oratories 2 Pro ject Fo cus Areas NHSE Overview Resource Cataloging and Distribution System RCDS Safe execution environments for mobile co de Application-l evel and content-oriented to ols Rep ository interop erabili ty Distributed, semantic-based searching 3 NHSE National HPCC Software Exchange NASA plus other agencies funded CRPC pro ject Center for ResearchonParallel Computation CRPC { Argonne National Lab oratory { California Institute of Technology { Rice University { Syracuse University { UniversityofTennessee Uniform interface to distributed HPCC software rep ositories Facilitation of cross-agency and interdisciplinary software reuse Material from ASTA, HPCS, and I ITA comp onents of the HPCC program http://www.netlib.org/nhse/ 4 Goals: Capture, preserve and makeavailable all software and software- related artifacts pro duced by the federal HPCC program. Soft- ware related artifacts include algorithms, sp eci cations, designs, do cumentation, rep ort, ... Promote formation, growth, and interop eration of discipline-oriented rep ositories that organize, evaluate, and add value to individual contributions. Employ and develop where necessary state-of-the-art technologies for assisting users in nding, understanding, and using HPCC software and technologies. 5 Bene ts: 1. Faster development of high-quality software so that scientists can sp end less time writing and debugging programs and more time on research problems. 2. Less duplication of software development e ort by sharing of soft- ware mo dules. -
Handout on Gaussian Quadrature, Parts I and II
Theoretical foundations of Gaussian quadrature 1 Inner product vector space Definition 1. A vector space (or linear space) is a set V = {u, v, w,...} in which the following two operations are defined: (A) Addition of vectors: u + v ∈ V , which satisfies the properties (A1) associativity: u + (v + w) = (u + v) + w ∀ u, v, w in V ; (A2) existence of a zero vector: ∃ 0 ∈ V such that u + 0 = u ∀u ∈ V ; (A3) existence of an opposite element: ∀u ∈ V ∃(−u) ∈ V such that u + (−u) = 0; (A4) commutativity: u + v = v + u ∀ u, v in V ; (B) Multiplication of a number and a vector: αu ∈ V for α ∈ R, which satisfies the properties (B1) α(u + v) = αu + αv ∀ α ∈ R, ∀u, v ∈ V ; (B2) (α + β)u = αu + βu ∀ α, β ∈ R, ∀u ∈ V ; (B3) (αβ)u = α(βu) ∀ α, β ∈ R, ∀u ∈ V ; (B4) 1u = u ∀u ∈ V . Definition 2. An inner product linear space is a linear space V with an operation (·, ·) satisfying the properties (a) (u, v) = (v, u) ∀ u, v in V ; (b) (u + v, w) = (u, w) + (v, w) ∀ u, v, w in V ; (c) (αu, v) = α(u, v) ∀α ∈ R, ∀ u, v, w in V ; (d) (u, u) ≥ 0 ∀u ∈ V ; moreover, (u, u) = 0 if and only if u = 0. d Example. The “standard” inner product of the vectors u = (u1, u2, . , ud) ∈ R and d v = (v1, v2, . , vd) ∈ R is given by d X (u, v) = uivi . i=1 1 Example. Let G be a symmetric positive-definite matrix, for example 5 4 1 G = (gij) = 4 7 0 . -
[Draft] 4.4.3. Examples of Gaussian Quadrature. Gauss–Legendre
CAAM 453 · NUMERICAL ANALYSIS I Lecture 26: More on Gaussian Quadrature [draft] 4.4.3. Examples of Gaussian Quadrature. Gauss{Legendre quadrature. The best known Gaussian quadrature rule integrates functions over the interval [−1; 1] with the trivial weight function w(x) = 1. As we saw in Lecture 19, the orthogonal polynomials for this interval and weight are called Legendre polynomials. To construct a Gaussian quadrature rule with n + 1 points, we must determine the roots of the degree-(n + 1) Legendre polynomial, then find the associated weights. First, consider the case of n = 1. The quadratic Legendre polynomial is 2 φ2(x) = x − 1=3; and from this polynomialp one can derive the 2-point quadrature rule that is exact for cubic poly- nomials, with roots ±1= 3. This agrees with the special 2-point rule derived in Section 4.4.1. The values for the weights follow simply, w0 = w1 = 1, giving the 2-point Gauss{Legendre rule p p I(f) = f(−1= 3) + f(1= 3): For Gauss{Legendre quadrature rules based on larger numbers of points, there are various ways to compute the nodes and weights. Traditionally, one would consult a book of mathematical tables, such as the venerable Handbook of Mathematical Functions, edited by Milton Abramowitz and Irene Stegun for the National Bureau of Standards in the early 1960s. Now, one can look up these quadrature nodes and weights on web sites, or determine them to high precision using a symbolic mathematics package such as Mathematica. Most effective of all, one can compute these nodes and weights by solving a symmetric tridiagonal eigenvalue problem. -
Scipy 1.0: Fundamental Algorithms for Scientific Computing in Python
PERSPECTIVE https://doi.org/10.1038/s41592-019-0686-2 SciPy 1.0: fundamental algorithms for scientific computing in Python Pauli Virtanen1, Ralf Gommers 2*, Travis E. Oliphant2,3,4,5,6, Matt Haberland 7,8, Tyler Reddy 9, David Cournapeau10, Evgeni Burovski11, Pearu Peterson12,13, Warren Weckesser14, Jonathan Bright15, Stéfan J. van der Walt 14, Matthew Brett16, Joshua Wilson17, K. Jarrod Millman 14,18, Nikolay Mayorov19, Andrew R. J. Nelson 20, Eric Jones5, Robert Kern5, Eric Larson21, C J Carey22, İlhan Polat23, Yu Feng24, Eric W. Moore25, Jake VanderPlas26, Denis Laxalde 27, Josef Perktold28, Robert Cimrman29, Ian Henriksen6,30,31, E. A. Quintero32, Charles R. Harris33,34, Anne M. Archibald35, Antônio H. Ribeiro 36, Fabian Pedregosa37, Paul van Mulbregt 38 and SciPy 1.0 Contributors39 SciPy is an open-source scientific computing library for the Python programming language. Since its initial release in 2001, SciPy has become a de facto standard for leveraging scientific algorithms in Python, with over 600 unique code contributors, thou- sands of dependent packages, over 100,000 dependent repositories and millions of downloads per year. In this work, we provide an overview of the capabilities and development practices of SciPy 1.0 and highlight some recent technical developments. ciPy is a library of numerical routines for the Python program- has become the standard others follow and has seen extensive adop- ming language that provides fundamental building blocks tion in research and industry. Sfor modeling and solving scientific problems. SciPy includes SciPy’s arrival at this point is surprising and somewhat anoma- algorithms for optimization, integration, interpolation, eigenvalue lous. -
Section “Creating R Packages” in Writing R Extensions
Writing R Extensions Version 3.0.0 RC (2013-03-28) R Core Team Permission is granted to make and distribute verbatim copies of this manual provided the copyright notice and this permission notice are preserved on all copies. Permission is granted to copy and distribute modified versions of this manual under the con- ditions for verbatim copying, provided that the entire resulting derived work is distributed under the terms of a permission notice identical to this one. Permission is granted to copy and distribute translations of this manual into another lan- guage, under the above conditions for modified versions, except that this permission notice may be stated in a translation approved by the R Core Team. Copyright c 1999{2013 R Core Team i Table of Contents Acknowledgements ::::::::::::::::::::::::::::::::: 1 1 Creating R packages:::::::::::::::::::::::::::: 2 1.1 Package structure :::::::::::::::::::::::::::::::::::::::::::::: 3 1.1.1 The `DESCRIPTION' file :::::::::::::::::::::::::::::::::::: 4 1.1.2 Licensing:::::::::::::::::::::::::::::::::::::::::::::::::: 9 1.1.3 The `INDEX' file :::::::::::::::::::::::::::::::::::::::::: 10 1.1.4 Package subdirectories:::::::::::::::::::::::::::::::::::: 11 1.1.5 Data in packages ::::::::::::::::::::::::::::::::::::::::: 14 1.1.6 Non-R scripts in packages :::::::::::::::::::::::::::::::: 15 1.2 Configure and cleanup :::::::::::::::::::::::::::::::::::::::: 16 1.2.1 Using `Makevars'::::::::::::::::::::::::::::::::::::::::: 19 1.2.1.1 OpenMP support:::::::::::::::::::::::::::::::::::: 22 1.2.1.2 -
Numerical Quadrature
Numerical Integration Numerical Differentiation Richardson Extrapolation Outline 1 Numerical Integration 2 Numerical Differentiation 3 Richardson Extrapolation Michael T. Heath Scientific Computing 2 / 61 Main Ideas ❑ Quadrature based on polynomial interpolation: ❑ Methods: ❑ Method of undetermined coefficients (e.g., Adams-Bashforth) ❑ Lagrangian interpolation ❑ Rules: ❑ Midpoint, Trapezoidal, Simpson, Newton-Cotes ❑ Gaussian Quadrature ❑ Quadrature based on piecewise polynomial interpolation ❑ Composite trapezoidal rule ❑ Composite Simpson ❑ Richardson extrapolation ❑ Differentiation ❑ Taylor series / Richardson extrapolation ❑ Derivatives of Lagrange polynomials ❑ Derivative matrices Quadrature Examples b = ecos x dx •I Za Di↵erential equations: n u(x)= u φ (x) XN j j 2 j=1 X Find u(x)suchthat du r(x)= f(x) XN dx − ? Numerical Integration Quadrature Rules Numerical Differentiation Adaptive Quadrature Richardson Extrapolation Other Integration Problems Integration For f : R R, definite integral over interval [a, b] ! b I(f)= f(x) dx Za is defined by limit of Riemann sums n R = (x x ) f(⇠ ) n i+1 − i i Xi=1 Riemann integral exists provided integrand f is bounded and continuous almost everywhere Absolute condition number of integration with respect to perturbations in integrand is b a − Integration is inherently well-conditioned because of its smoothing effect Michael T. Heath Scientific Computing 3 / 61 Numerical Integration Quadrature Rules Numerical Differentiation Adaptive Quadrature Richardson Extrapolation Other Integration Problems Numerical Quadrature Quadrature rule is weighted sum of finite number of sample values of integrand function To obtain desired level of accuracy at low cost, How should sample points be chosen? How should their contributions be weighted? Computational work is measured by number of evaluations of integrand function required Michael T. -
Gaussian Quadrature for Computer Aided Robust Design
Page 1 of 88 Gaussian Quadrature for Computer Aided Robust Design by Geoffrey Scott Reber S.B. Aeronautics and Astronautics Massachusetts Institute of Technology, 2000 Submitted to the Department of Aeronautics and Astronautics in partial fulfillment of the requirements for the degree of Masters of Science in Aeronautics and Astronautics at the Massachusetts Institute of Technology OF TECHN3LOGY JUL 0 1 2004 June, 2004 LIBRARIES © 2004 Massachusetts Institute of Technology. All rights reserved t AERO Signature of Author: Department o auticsd Astronautics -Myay 7, 2004 Certified by: aniel Frey Professor of Mechan' al Engineering Thesis Supervisor Approved by: Edward Greitzer H.N. Slater Professor of Aeronautics and Astronautics Chair, Committee on Graduate Students Page 2 of 88 Gaussian Quadrature for Computer Aided Robust Design by Geoffrey Scott Reber Submitted to the Department of Aeronautics and Astronautics on May 7, 2004 in partial fulfillment of the requirements for the degree of Master of Science in Aeronautics and Astronautics ABSTRACT Computer aided design has allowed many design decisions to be made before hardware is built through "virtual" prototypes: computer simulations of an engineering design. To produce robust systems noise factors must also be considered (robust design), and should they should be considered as early as possible to reduce the impact of late design changes. Robust design on the computer requires a method to analyze the effects of uncertainty. Unfortunately, the most commonly used computer uncertainty analysis technique (Monte Carlo Simulation) requires thousands more simulation runs than needed if noises are ignored. For complex simulations such as Computational Fluid Dynamics, such a drastic increase in the time required to evaluate an engineering design may be probative early in the design process. -
A. an Introduction to Scientific Computing with Python
August 30, 2013 Time: 06:43pm appendixa.tex A. An Introduction to Scientific Computing with Python “The world’s a book, writ by the eternal art – Of the great author printed in man’s heart, ’Tis falsely printed, though divinely penned, And all the errata will appear at the end.” (Francis Quarles) n this appendix we aim to give a brief introduction to the Python language1 and Iits use in scientific computing. It is intended for users who are familiar with programming in another language such as IDL, MATLAB, C, C++, or Java. It is beyond the scope of this book to give a complete treatment of the Python language or the many tools available in the modules listed below. The number of tools available is large, and growing every day. For this reason, no single resource can be complete, and even experienced scientific Python programmers regularly reference documentation when using familiar tools or seeking new ones. For that reason, this appendix will emphasize the best ways to access documentation both on the web and within the code itself. We will begin with a brief history of Python and efforts to enable scientific computing in the language, before summarizing its main features. Next we will discuss some of the packages which enable efficient scientific computation: NumPy, SciPy, Matplotlib, and IPython. Finally, we will provide some tips on writing efficient Python code. Some recommended resources are listed in §A.10. A.1. A brief history of Python Python is an open-source, interactive, object-oriented programming language, cre- ated by Guido Van Rossum in the late 1980s.