Investigation on Non-Standard Scheme Applied to Euler and Third Order Euler for Initial Value Problems
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Chapter 4 Finite Difference Gradient Information
Chapter 4 Finite Difference Gradient Information In the masters thesis Thoresson (2003), the feasibility of using gradient- based approximation methods for the optimisation of the spring and damper characteristics of an off-road vehicle, for both ride comfort and handling, was investigated. The Sequential Quadratic Programming (SQP) algorithm and the locally developed Dynamic-Q method were the two successive approximation methods used for the optimisation. The determination of the objective function value is performed using computationally expensive numerical simulations that exhibit severe inherent numerical noise. The use of forward finite differences and central finite differences for the determination of the gradients of the objective function within Dynamic-Q is also investigated. The results of this study, presented here, proved that the use of central finite differencing for gradient information improved the optimisation convergence history, and helped to reduce the difficulties associated with noise in the objective and constraint functions. This chapter presents the feasibility investigation of using gradient-based successive approximation methods to overcome the problems of poor gradient information due to severe numerical noise. The two approximation methods applied here are the locally developed Dynamic-Q optimisation algorithm of Snyman and Hay (2002) and the well known Sequential Quadratic 47 CHAPTER 4. FINITE DIFFERENCE GRADIENT INFORMATION 48 Programming (SQP) algorithm, the MATLAB implementation being used for this research (Mathworks 2000b). This chapter aims to provide the reader with more information regarding the Dynamic-Q successive approximation algorithm, that may be used as an alternative to the more established SQP method. Both algorithms are evaluated for effectiveness and efficiency in determining optimal spring and damper characteristics for both ride comfort and handling of a vehicle. -
Ordinary Differential Equations (ODE) Using Euler's Technique And
Mathematical Models and Methods in Modern Science Ordinary Differential Equations (ODE) using Euler’s Technique and SCILAB Programming ZULZAMRI SALLEH Applied Sciences and Advance Technology Universiti Kuala Lumpur Malaysian Institute of Marine Engineering Technology Bandar Teknologi Maritim Jalan Pantai Remis 32200 Lumut, Perak MALAYSIA [email protected] http://www.mimet.edu.my Abstract: - Mathematics is very important for the engineering and scientist but to make understand the mathematics is very difficult if without proper tools and suitable measurement. A numerical method is one of the algorithms which involved with computer programming. In this paper, Scilab is used to carter the problems related the mathematical models such as Matrices, operation with ODE’s and solving the Integration. It remains true that solutions of the vast majority of first order initial value problems cannot be found by analytical means. Therefore, it is important to be able to approach the problem in other ways. Today there are numerous methods that produce numerical approximations to solutions of differential equations. Here, we introduce the oldest and simplest such method, originated by Euler about 1768. It is called the tangent line method or the Euler method. It uses a fixed step size h and generates the approximate solution. The purpose of this paper is to show the details of implementing of Euler’s method and made comparison between modify Euler’s and exact value by integration solution, as well as solve the ODE’s use built-in functions available in Scilab programming. Key-Words: - Numerical Methods, Scilab programming, Euler methods, Ordinary Differential Equation. 1 Introduction availability of digital computers has led to a Numerical methods are techniques by which veritable explosion in the use and development of mathematical problems are formulated so that they numerical methods [1]. -
Numerical Methods for Ordinary Differential Equations
CHAPTER 1 Numerical Methods for Ordinary Differential Equations In this chapter we discuss numerical method for ODE . We will discuss the two basic methods, Euler’s Method and Runge-Kutta Method. 1. Numerical Algorithm and Programming in Mathcad 1.1. Numerical Algorithm. If you look at dictionary, you will the following definition for algorithm, 1. a set of rules for solving a problem in a finite number of steps; 2. a sequence of steps designed for programming a computer to solve a specific problem. A numerical algorithm is a set of rules for solving a problem in finite number of steps that can be easily implemented in computer using any programming language. The following is an algorithm for compute the root of f(x) = 0; Input f, a, N and tol . Output: the approximate solution to f(x) = 0 with initial guess a or failure message. ² Step One: Set x = a ² Step Two: For i=0 to N do Step Three - Four f(x) Step Three: Compute x = x ¡ f 0(x) Step Four: If f(x) · tol return x ² Step Five return ”failure”. In analogy, a numerical algorithm is like a cook recipe that specify the input — cooking material, the output—the cooking product, and steps of carrying computation — cooking steps. In an algorithm, you will see loops (for, while), decision making statements(if, then, else(otherwise)) and return statements. ² for loop: Typically used when specific number of steps need to be carried out. You can break a for loop with return or break statement. 1 2 1. NUMERICAL METHODS FOR ORDINARY DIFFERENTIAL EQUATIONS ² while loop: Typically used when unknown number of steps need to be carried out. -
Getting Started with Euler
Getting started with Euler Samuel Fux High Performance Computing Group, Scientific IT Services, ETH Zurich ETH Zürich | Scientific IT Services | HPC Group Samuel Fux | 19.02.2020 | 1 Outlook . Introduction . Accessing the cluster . Data management . Environment/LMOD modules . Using the batch system . Applications . Getting help ETH Zürich | Scientific IT Services | HPC Group Samuel Fux | 19.02.2020 | 2 Outlook . Introduction . Accessing the cluster . Data management . Environment/LMOD modules . Using the batch system . Applications . Getting help ETH Zürich | Scientific IT Services | HPC Group Samuel Fux | 19.02.2020 | 3 Intro > What is EULER? . EULER stands for . Erweiterbarer, Umweltfreundlicher, Leistungsfähiger ETH Rechner . It is the 5th central (shared) cluster of ETH . 1999–2007 Asgard ➔ decommissioned . 2004–2008 Hreidar ➔ integrated into Brutus . 2005–2008 Gonzales ➔ integrated into Brutus . 2007–2016 Brutus . 2014–2020+ Euler . It benefits from the 15 years of experience gained with those previous large clusters ETH Zürich | Scientific IT Services | HPC Group Samuel Fux | 19.02.2020 | 4 Intro > Shareholder model . Like its predecessors, Euler has been financed (for the most part) by its users . So far, over 100 (!) research groups from almost all departments of ETH have invested in Euler . These so-called “shareholders” receive a share of the cluster’s resources (processors, memory, storage) proportional to their investment . The small share of Euler financed by IT Services is open to all members of ETH . The only requirement -
The Original Euler's Calculus-Of-Variations Method: Key
Submitted to EJP 1 Jozef Hanc, [email protected] The original Euler’s calculus-of-variations method: Key to Lagrangian mechanics for beginners Jozef Hanca) Technical University, Vysokoskolska 4, 042 00 Kosice, Slovakia Leonhard Euler's original version of the calculus of variations (1744) used elementary mathematics and was intuitive, geometric, and easily visualized. In 1755 Euler (1707-1783) abandoned his version and adopted instead the more rigorous and formal algebraic method of Lagrange. Lagrange’s elegant technique of variations not only bypassed the need for Euler’s intuitive use of a limit-taking process leading to the Euler-Lagrange equation but also eliminated Euler’s geometrical insight. More recently Euler's method has been resurrected, shown to be rigorous, and applied as one of the direct variational methods important in analysis and in computer solutions of physical processes. In our classrooms, however, the study of advanced mechanics is still dominated by Lagrange's analytic method, which students often apply uncritically using "variational recipes" because they have difficulty understanding it intuitively. The present paper describes an adaptation of Euler's method that restores intuition and geometric visualization. This adaptation can be used as an introductory variational treatment in almost all of undergraduate physics and is especially powerful in modern physics. Finally, we present Euler's method as a natural introduction to computer-executed numerical analysis of boundary value problems and the finite element method. I. INTRODUCTION In his pioneering 1744 work The method of finding plane curves that show some property of maximum and minimum,1 Leonhard Euler introduced a general mathematical procedure or method for the systematic investigation of variational problems. -
Freemat V3.6 Documentation
FreeMat v3.6 Documentation Samit Basu November 16, 2008 2 Contents 1 Introduction and Getting Started 5 1.1 INSTALL Installing FreeMat . 5 1.1.1 General Instructions . 5 1.1.2 Linux . 5 1.1.3 Windows . 6 1.1.4 Mac OS X . 6 1.1.5 Source Code . 6 2 Variables and Arrays 7 2.1 CELL Cell Array Definitions . 7 2.1.1 Usage . 7 2.1.2 Examples . 7 2.2 Function Handles . 8 2.2.1 Usage . 8 2.3 GLOBAL Global Variables . 8 2.3.1 Usage . 8 2.3.2 Example . 9 2.4 INDEXING Indexing Expressions . 9 2.4.1 Usage . 9 2.4.2 Array Indexing . 9 2.4.3 Cell Indexing . 13 2.4.4 Structure Indexing . 14 2.4.5 Complex Indexing . 16 2.5 MATRIX Matrix Definitions . 17 2.5.1 Usage . 17 2.5.2 Examples . 17 2.6 PERSISTENT Persistent Variables . 19 2.6.1 Usage . 19 2.6.2 Example . 19 2.7 STRING String Arrays . 20 2.7.1 Usage . 20 2.8 STRUCT Structure Array Constructor . 22 2.8.1 Usage . 22 2.8.2 Example . 22 3 4 CONTENTS 3 Functions and Scripts 25 3.1 ANONYMOUS Anonymous Functions . 25 3.1.1 Usage . 25 3.1.2 Examples . 25 3.2 FUNCTION Function Declarations . 26 3.2.1 Usage . 26 3.2.2 Examples . 28 3.3 KEYWORDS Function Keywords . 30 3.3.1 Usage . 30 3.3.2 Example . 31 3.4 NARGIN Number of Input Arguments . 32 3.4.1 Usage . -
A Case Study in Fitting Area-Proportional Euler Diagrams with Ellipses Using Eulerr
A Case Study in Fitting Area-Proportional Euler Diagrams with Ellipses using eulerr Johan Larsson and Peter Gustafsson Department of Statistics, School of Economics and Management, Lund University, Lund, Sweden [email protected] [email protected] Abstract. Euler diagrams are common and user-friendly visualizations for set relationships. Most Euler diagrams use circles, but circles do not always yield accurate diagrams. A promising alternative is ellipses, which, in theory, enable accurate diagrams for a wider range of input. Elliptical diagrams, however, have not yet been implemented for more than three sets or three-set diagrams where there are disjoint or subset relationships. The aim of this paper is to present eulerr: a software package for elliptical Euler diagrams for, in theory, any number of sets. It fits Euler diagrams using numerical optimization and exact-area algorithms through a two-step procedure, first generating an initial layout using pairwise relationships and then finalizing this layout using all set relationships. 1 Background The Euler diagram, first described by Leonard Euler in 1802 [1], is a generalization of the popular Venn diagram. Venn and Euler diagrams both visualize set relationships by mapping areas in the diagram to relationships in the data. They differ, however, in that Venn diagrams require all intersections to be present| even if they are empty|whilst Euler diagrams do not, which means that Euler diagrams lend themselves well to be area-proportional. Euler diagrams may be fashioned out of any closed shape, and have been implemented for triangles [2], rectangles [2], ellipses [3], smooth curves [4], poly- gons [2], and circles [5, 2]. -
Upwind Summation by Parts Finite Difference Methods for Large Scale
Upwind summation by parts finite difference methods for large scale elastic wave simulations in 3D complex geometries ? Kenneth Durua,∗, Frederick Funga, Christopher Williamsa aMathematical Sciences Institute, Australian National University, Australia. Abstract High-order accurate summation-by-parts (SBP) finite difference (FD) methods constitute efficient numerical methods for simulating large-scale hyperbolic wave propagation problems. Traditional SBP FD operators that approximate first-order spatial derivatives with central-difference stencils often have spurious unresolved numerical wave-modes in their computed solutions. Recently derived high order accurate upwind SBP operators based non-central (upwind) FD stencils have the potential to suppress these poisonous spurious wave-modes on marginally resolved computational grids. In this paper, we demonstrate that not all high order upwind SBP FD operators are applicable. Numerical dispersion relation analysis shows that odd-order upwind SBP FD operators also support spurious unresolved high-frequencies on marginally resolved meshes. Meanwhile, even-order upwind SBP FD operators (of order 2; 4; 6) do not support spurious unresolved high frequency wave modes and also have better numerical dispersion properties. For all the upwind SBP FD operators we discretise the three space dimensional (3D) elastic wave equation on boundary-conforming curvilinear meshes. Using the energy method we prove that the semi-discrete ap- proximation is stable and energy-conserving. We derive a priori error estimate and prove the convergence of the numerical error. Numerical experiments for the 3D elastic wave equation in complex geometries corrobo- rate the theoretical analysis. Numerical simulations of the 3D elastic wave equation in heterogeneous media with complex non-planar free surface topography are given, including numerical simulations of community developed seismological benchmark problems. -
High Order Gradient, Curl and Divergence Conforming Spaces, with an Application to NURBS-Based Isogeometric Analysis
High order gradient, curl and divergence conforming spaces, with an application to compatible NURBS-based IsoGeometric Analysis R.R. Hiemstraa, R.H.M. Huijsmansa, M.I.Gerritsmab aDepartment of Marine Technology, Mekelweg 2, 2628CD Delft bDepartment of Aerospace Technology, Kluyverweg 2, 2629HT Delft Abstract Conservation laws, in for example, electromagnetism, solid and fluid mechanics, allow an exact discrete representation in terms of line, surface and volume integrals. We develop high order interpolants, from any basis that is a partition of unity, that satisfy these integral relations exactly, at cell level. The resulting gradient, curl and divergence conforming spaces have the propertythat the conservationlaws become completely independent of the basis functions. This means that the conservation laws are exactly satisfied even on curved meshes. As an example, we develop high ordergradient, curl and divergence conforming spaces from NURBS - non uniform rational B-splines - and thereby generalize the compatible spaces of B-splines developed in [1]. We give several examples of 2D Stokes flow calculations which result, amongst others, in a point wise divergence free velocity field. Keywords: Compatible numerical methods, Mixed methods, NURBS, IsoGeometric Analyis Be careful of the naive view that a physical law is a mathematical relation between previously defined quantities. The situation is, rather, that a certain mathematical structure represents a given physical structure. Burke [2] 1. Introduction In deriving mathematical models for physical theories, we frequently start with analysis on finite dimensional geometric objects, like a control volume and its bounding surfaces. We assign global, ’measurable’, quantities to these different geometric objects and set up balance statements. -
The Python Interpreter
The Python interpreter Remi Lehe Lawrence Berkeley National Laboratory (LBNL) US Particle Accelerator School (USPAS) Summer Session Self-Consistent Simulations of Beam and Plasma Systems S. M. Lund, J.-L. Vay, R. Lehe & D. Winklehner Colorado State U, Ft. Collins, CO, 13-17 June, 2016 Python interpreter: Outline 1 Overview of the Python language 2 Python, numpy and matplotlib 3 Reusing code: functions, modules, classes 4 Faster computation: Forthon Overview Scientific Python Reusing code Forthon Overview of the Python programming language Interpreted language (i.e. not compiled) ! Interactive, but not optimal for computational speed Readable and non-verbose No need to declare variables Indentation is enforced Free and open-source + Large community of open-souce packages Well adapted for scientific and data analysis applications Many excellent packages, esp. numerical computation (numpy), scientific applications (scipy), plotting (matplotlib), data analysis (pandas, scikit-learn) 3 Overview Scientific Python Reusing code Forthon Interfaces to the Python language Scripting Interactive shell Code written in a file, with a Obtained by typing python or text editor (gedit, vi, emacs) (better) ipython Execution via command line Commands are typed in and (python + filename) executed one by one Convenient for exploratory work, Convenient for long-term code debugging, rapid feedback, etc... 4 Overview Scientific Python Reusing code Forthon Interfaces to the Python language IPython (a.k.a Jupyter) notebook Notebook interface, similar to Mathematica. Intermediate between scripting and interactive shell, through reusable cells Obtained by typing jupyter notebook, opens in your web browser Convenient for exploratory work, scientific analysis and reports 5 Overview Scientific Python Reusing code Forthon Overview of the Python language This lecture Reminder of the main points of the Scipy lecture notes through an example problem. -
The Pascal Matrix Function and Its Applications to Bernoulli Numbers and Bernoulli Polynomials and Euler Numbers and Euler Polynomials
The Pascal Matrix Function and Its Applications to Bernoulli Numbers and Bernoulli Polynomials and Euler Numbers and Euler Polynomials Tian-Xiao He ∗ Jeff H.-C. Liao y and Peter J.-S. Shiue z Dedicated to Professor L. C. Hsu on the occasion of his 95th birthday Abstract A Pascal matrix function is introduced by Call and Velleman in [3]. In this paper, we will use the function to give a unified approach in the study of Bernoulli numbers and Bernoulli poly- nomials. Many well-known and new properties of the Bernoulli numbers and polynomials can be established by using the Pascal matrix function. The approach is also applied to the study of Euler numbers and Euler polynomials. AMS Subject Classification: 05A15, 65B10, 33C45, 39A70, 41A80. Key Words and Phrases: Pascal matrix, Pascal matrix func- tion, Bernoulli number, Bernoulli polynomial, Euler number, Euler polynomial. ∗Department of Mathematics, Illinois Wesleyan University, Bloomington, Illinois 61702 yInstitute of Mathematics, Academia Sinica, Taipei, Taiwan zDepartment of Mathematical Sciences, University of Nevada, Las Vegas, Las Vegas, Nevada, 89154-4020. This work is partially supported by the Tzu (?) Tze foundation, Taipei, Taiwan, and the Institute of Mathematics, Academia Sinica, Taipei, Taiwan. The author would also thank to the Institute of Mathematics, Academia Sinica for the hospitality. 1 2 T. X. He, J. H.-C. Liao, and P. J.-S. Shiue 1 Introduction A large literature scatters widely in books and journals on Bernoulli numbers Bn, and Bernoulli polynomials Bn(x). They can be studied by means of the binomial expression connecting them, n X n B (x) = B xn−k; n ≥ 0: (1) n k k k=0 The study brings consistent attention of researchers working in combi- natorics, number theory, etc. -
Freemat V4.0 Documentation
FreeMat v4.0 Documentation Samit Basu October 4, 2009 2 Contents 1 Introduction and Getting Started 39 1.1 INSTALL Installing FreeMat . 39 1.1.1 General Instructions . 39 1.1.2 Linux . 39 1.1.3 Windows . 40 1.1.4 Mac OS X . 40 1.1.5 Source Code . 40 2 Variables and Arrays 41 2.1 CELL Cell Array Definitions . 41 2.1.1 Usage . 41 2.1.2 Examples . 41 2.2 Function Handles . 42 2.2.1 Usage . 42 2.3 GLOBAL Global Variables . 42 2.3.1 Usage . 42 2.3.2 Example . 42 2.4 INDEXING Indexing Expressions . 43 2.4.1 Usage . 43 2.4.2 Array Indexing . 43 2.4.3 Cell Indexing . 46 2.4.4 Structure Indexing . 47 2.4.5 Complex Indexing . 49 2.5 MATRIX Matrix Definitions . 49 2.5.1 Usage . 49 2.5.2 Examples . 49 2.6 PERSISTENT Persistent Variables . 51 2.6.1 Usage . 51 2.6.2 Example . 51 2.7 STRUCT Structure Array Constructor . 51 2.7.1 Usage . 51 2.7.2 Example . 52 3 4 CONTENTS 3 Functions and Scripts 55 3.1 ANONYMOUS Anonymous Functions . 55 3.1.1 Usage . 55 3.1.2 Examples . 55 3.2 FUNCTION Function Declarations . 56 3.2.1 Usage . 56 3.2.2 Examples . 57 3.3 KEYWORDS Function Keywords . 60 3.3.1 Usage . 60 3.3.2 Example . 60 3.4 NARGIN Number of Input Arguments . 61 3.4.1 Usage . 61 3.4.2 Example . 61 3.5 NARGOUT Number of Output Arguments .