BSM510 Numerical Analysis

Size: px
Start display at page:

Download "BSM510 Numerical Analysis"

Transcription

1 BSM510 Numerica Anaysis Roots: Bracketing methods : Open methods Prof. Manar Mohaisen Department of EEC Engineering

2 Lecture Content v Introduction v Bracketing methods v Open methods v MATLAB hints 2

3 Introduction f() roots f() v Roots of a function The points at which Numerica methods q Bracketing methods: initia guess that brackets the root q Open methods: one/more initia guesses but no need for them to bracket the root v Loca/goba maimums f '( ) = 0 and f ''( ) < 0 The points at which f( ) = 0 v Loca/goba minimums The points at which f '( ) = 0 and f ''( ) > 0 3

4 Bracketing methods v Method I: Incrementa search Check the occurrence of sign change in the given range with a predefined increment ength q Large increment ength might ead the search to miss roots q Sma increment ength sows down the search Check Fig. 5.4 in the tet book (run the code) 2 1 ns = 10, brackets = 5 ns = 50, brackets = 5 ns = 100, brackets = 9 f()

5 Bracketing methods contd. v Method II: Bisection Good method to ocate the interva of a root Sow q It is foowed by a fast converging method to find the vaue of the root Stage I q Make a guess on the interva of the root Stage II q Cacuate the midpoint r q If r and have the same sign = r, don t modify u q If r and have opposite signs Continue u = r, don t modify q same as in stage II ti a tight interva is found I = [, ] r = e = a u + 2 u new r r - od r new 100% 5

6 Bracketing methods contd. v Method III: Fase position Same as the bisection method with the difference that r = - u f( u)( - u) f( ) - f( ) u q The computed r repaces whether or u q The resuting function vaue has same sign of f( r ) q or u aways bracket the true root 6

7 Bracketing methods contd. v Numerica eampe Function æ ö f( ) = sin ç 2p + cos( p ) è ø f() v Bisection Fase position method is very simiar f( ) f( ) < 0 = r u r f ( ) f ( ) > 0 = r f( ) f( ) < 0 = r r u r f ( ) ( ) 0 f r > = f( ) f( ) < 0 = r u r f ( ) f ( ) > 0 = f( ) f( ) < 0 = r r r r u r Iteration u r e a % % % 7

8 Bracketing methods contd. v Comparison between methods A methods q Generay, converge to the root s interva, more iterations à tighter interva Incrementa search q Locates the interva(s) of sign change q The choice of increment ength is critica (sma à sow, argeà miss a toot) Bisection (modification of IS) q The interva is aways divided in haf to ocate the root ocation q Sow but certainy converges q Convergence is generay independent of the function s curvature Fase Position (modification of bisection) q Generay, faster convergence q However, for functions with significant curvature Fase position method is sower than bisection method 8

9 Open methods v Bracketing methods Require two initia points bracketing the root Converge Sow v Open methods Require one or two points Empoy a formua to predict the root Therefore, q Since root is not bounded, Methods might diverge If they converge q They converge fast 9

10 Open methods contd. v Method I: Simpe fied-point iteration Step I: Rearrange the function f()=0 so that is on the eft side q f() = 0 means the ocation of a root q Eampe = g( ) f( ) = 2 - f( ) = 0 = g( ) = 2 Step II: a new estimate of the root is then given by i g( ) 1 i + = f() = e - - f() root: e - =

11 Open methods contd. v Method I: Simpe fied-point iteration Aternative graphica approach q Step I: Spit f()=0 into two functions y 1 () = y 2 () q Step II: The root is the intersection of these two functions y 1 (), y 2 ()

12 Open methods contd. v Method I: Simpe fied-point iteration Convergence q Error at (i+1)th iteration q If E ' i 1 g + = E g'( ) ³ 1 ( ) i The method diverges q If '( ) 1 g < The method converges 12

13 Open methods contd. v Method I: Simpe fied-point iteration Root for the function f( ) = e- - f( ) = 0 = e - i i e a % e t % e t i / e t i

14 Open methods contd. v Method II: Newton-Raphson method The update formua f( ) - 0 f( ) ( ) f '( ) = i i i - = - i+ 1 i ' i i+ 1 f i q The 0 is the epected vaue of f( i+1 ). Eampe f( ) = e- - e- - = i+ 1 i e- 1 i i e t % <

15 Open methods contd. v Method II: Newton-Raphson method NR method performs poory for the functions in the figure q Remedy: Have a guess cose to the root Good aspect q The error of the i+1 th iteration is roughy proportiona to the square of the error of the ith iteration - this is caed quadratic convergence 15

16 Open methods contd. v Method III: Secant methods Drawback of NP method q The derivative might be hard to compute or to evauate The derivative is therefore approimated as (using 2 points) f( ) - f( ) f( )( - ) f ( = = - ( ) ( ) ' i-1 i i i-1 i - i+ 1 i i-1 i f - f i-1 i Same can be done with a point and a fraction of it as foows d f( ) ( ) ( ) i i i+ 1 = i - f + d - f i i i q Other properties are same as those of NR method 16

17 MATLAB Code v fzero fzero(@() func, 0) q Tries to find a zero of the function func near the point 0 Eampe q fzero(@() ep(-) -, 0.8) v roots roots(c) q Find the roots of the poynomia whose coefficients are the vector c Eampe q roots([1-2 -1]) q ans: ,

18 Lecture Summary v Introduction v Bracketing methods v Open methods v MATLAB hints 18

SOLVING EQUATIONS OF ONE VARIABLE

SOLVING EQUATIONS OF ONE VARIABLE 1 SOLVING EQUATIONS OF ONE VARIABLE ELM1222 Numerical Analysis Some of the contents are adopted from Laurene V. Fausett, Applied Numerical Analysis using MATLAB. Prentice Hall Inc., 1999 2 Today s lecture

More information

NON-LINEAR ALGEBRAIC EQUATIONS Lec. 5.1: Nonlinear Equation in Single Variable

NON-LINEAR ALGEBRAIC EQUATIONS Lec. 5.1: Nonlinear Equation in Single Variable NON-LINEAR ALGEBRAIC EQUATIONS Lec. 5.1: Nonlinear Equation in Single Variable Dr. Niket Kaisare Department of Chemical Engineering IIT Madras NPTEL Course: MATLAB Programming for Numerical Computations

More information

BSM510 Numerical Analysis

BSM510 Numerical Analysis BSM510 Numerical Analysis Polynomial Interpolation Prof. Manar Mohaisen Department of EEC Engineering Review of Precedent Lecture Polynomial Regression Multiple Linear Regression Nonlinear Regression Lecture

More information

Numerical Analysis Fall. Roots: Open Methods

Numerical Analysis Fall. Roots: Open Methods Numerical Analysis 2015 Fall Roots: Open Methods Open Methods Open methods differ from bracketing methods, in that they require only a single starting value or two starting values that do not necessarily

More information

Laplace Examples, Inverse, Rational Form

Laplace Examples, Inverse, Rational Form Lecture 20 Outine: Lapace Eampe, Invere, Rationa Form Announcement: HW 5 poted, due Friday ore Lapace Tranform Eampe Invere Lapace Tranform Rationa Lapace Tranform ROC for Right/Left/Toided Signa agnitude/phae

More information

F O R SOCI AL WORK RESE ARCH

F O R SOCI AL WORK RESE ARCH 7 TH EUROPE AN CONFERENCE F O R SOCI AL WORK RESE ARCH C h a l l e n g e s i n s o c i a l w o r k r e s e a r c h c o n f l i c t s, b a r r i e r s a n d p o s s i b i l i t i e s i n r e l a t i o n

More information

Numerical Methods. Root Finding

Numerical Methods. Root Finding Numerical Methods Solving Non Linear 1-Dimensional Equations Root Finding Given a real valued function f of one variable (say ), the idea is to find an such that: f() 0 1 Root Finding Eamples Find real

More information

Numerical Methods School of Mechanical Engineering Chung-Ang University

Numerical Methods School of Mechanical Engineering Chung-Ang University Part 2 Chapter 5 Roots: Bracketing Methods Prof. Hae-Jin Choi hjchoi@cau.ac.kr 1 Overview of Part 2 l To find the roots of general second order polynomial, the quadratic formula is used b b 2 2 - ± - 4ac

More information

1. Measurements and error calculus

1. Measurements and error calculus EV 1 Measurements and error cacuus 11 Introduction The goa of this aboratory course is to introduce the notions of carrying out an experiment, acquiring and writing up the data, and finay anayzing the

More information

Finding Roots of Equations

Finding Roots of Equations Finding Roots of Equations Solution Methods Overview Bisection/Half-interval Search Method of false position/regula Falsi Secant Method Newton Raphson Iteration Method Many more. Open Methods Bracketing

More information

Finding roots. Lecture 4

Finding roots. Lecture 4 Finding roots Lecture 4 Finding roots: Find such that 0 or given. Bisection method: The intermediate value theorem states the obvious: i a continuous unction changes sign within a given interval, it has

More information

Numerical Methods Lecture 3

Numerical Methods Lecture 3 Numerical Methods Lecture 3 Nonlinear Equations by Pavel Ludvík Introduction Definition (Root or zero of a function) A root (or a zero) of a function f is a solution of an equation f (x) = 0. We learn

More information

MATH 3795 Lecture 12. Numerical Solution of Nonlinear Equations.

MATH 3795 Lecture 12. Numerical Solution of Nonlinear Equations. MATH 3795 Lecture 12. Numerical Solution of Nonlinear Equations. Dmitriy Leykekhman Fall 2008 Goals Learn about different methods for the solution of f(x) = 0, their advantages and disadvantages. Convergence

More information

ab = c a If the coefficients a,b and c are real then either α and β are real or α and β are complex conjugates

ab = c a If the coefficients a,b and c are real then either α and β are real or α and β are complex conjugates Further Pure Summary Notes. Roots of Quadratic Equations For a quadratic equation ax + bx + c = 0 with roots α and β Sum of the roots Product of roots a + b = b a ab = c a If the coefficients a,b and c

More information

Numerical Solution of f(x) = 0

Numerical Solution of f(x) = 0 Numerical Solution of f(x) = 0 Gerald W. Recktenwald Department of Mechanical Engineering Portland State University gerry@pdx.edu ME 350: Finding roots of f(x) = 0 Overview Topics covered in these slides

More information

Chapter 4. Solution of a Single Nonlinear Algebraic Equation

Chapter 4. Solution of a Single Nonlinear Algebraic Equation Single Nonlinear Algebraic Equation - 56 Chapter 4. Solution of a Single Nonlinear Algebraic Equation 4.1. Introduction Life, my fris, is nonlinear. As such, in our roles as problem-solvers, we will be

More information

TWO METHODS FOR OF EQUATIONS

TWO METHODS FOR OF EQUATIONS TWO METHODS FOR FINDING ROOTS OF EQUATIONS Closed (Bracketing) Methods Open Methods Motivation: i In engineering applications, it is often necessary to determine the rootofan of equation when a formula

More information

Brine Discharge Plumes on a Sloping Beach

Brine Discharge Plumes on a Sloping Beach Brine Discharge Pumes on a Soping Beach H.H. AL-BARWANI, Anton PURNAMA Department of Mathematics and Statistics, Coege of Science Sutan Qaboos Universit, PO Bo 6, A-Khod 1, Muscat, Sutanate of Oman E-mai:

More information

Finding the Roots of f(x) = 0. Gerald W. Recktenwald Department of Mechanical Engineering Portland State University

Finding the Roots of f(x) = 0. Gerald W. Recktenwald Department of Mechanical Engineering Portland State University Finding the Roots of f(x) = 0 Gerald W. Recktenwald Department of Mechanical Engineering Portland State University gerry@me.pdx.edu These slides are a supplement to the book Numerical Methods with Matlab:

More information

Finding the Roots of f(x) = 0

Finding the Roots of f(x) = 0 Finding the Roots of f(x) = 0 Gerald W. Recktenwald Department of Mechanical Engineering Portland State University gerry@me.pdx.edu These slides are a supplement to the book Numerical Methods with Matlab:

More information

18-660: Numerical Methods for Engineering Design and Optimization

18-660: Numerical Methods for Engineering Design and Optimization 8-660: Numerica Methods for Engineering esign and Optimization in i epartment of ECE Carnegie Meon University Pittsburgh, PA 523 Side Overview Conjugate Gradient Method (Part 4) Pre-conditioning Noninear

More information

6.1 The function can be set up for fixed-point iteration by solving it for x

6.1 The function can be set up for fixed-point iteration by solving it for x 1 CHAPTER 6 6.1 The function can be set up for fied-point iteration by solving it for 1 sin i i Using an initial guess of 0 = 0.5, the first iteration yields 1 sin 0.5 0.649637 a 0.649637 0.5 100% 3% 0.649637

More information

Math 124B January 31, 2012

Math 124B January 31, 2012 Math 124B January 31, 212 Viktor Grigoryan 7 Inhomogeneous boundary vaue probems Having studied the theory of Fourier series, with which we successfuy soved boundary vaue probems for the homogeneous heat

More information

CS 221 Lecture 9. Tuesday, 1 November 2011

CS 221 Lecture 9. Tuesday, 1 November 2011 CS 221 Lecture 9 Tuesday, 1 November 2011 Some slides in this lecture are from the publisher s slides for Engineering Computation: An Introduction Using MATLAB and Excel 2009 McGraw-Hill Today s Agenda

More information

Nonlinear Equations. Chapter The Bisection Method

Nonlinear Equations. Chapter The Bisection Method Chapter 6 Nonlinear Equations Given a nonlinear function f(), a value r such that f(r) = 0, is called a root or a zero of f() For eample, for f() = e 016064, Fig?? gives the set of points satisfying y

More information

12.2. Maxima and Minima. Introduction. Prerequisites. Learning Outcomes

12.2. Maxima and Minima. Introduction. Prerequisites. Learning Outcomes Maima and Minima 1. Introduction In this Section we anayse curves in the oca neighbourhood of a stationary point and, from this anaysis, deduce necessary conditions satisfied by oca maima and oca minima.

More information

T i t l e o f t h e w o r k : L a M a r e a Y o k o h a m a. A r t i s t : M a r i a n o P e n s o t t i ( P l a y w r i g h t, D i r e c t o r )

T i t l e o f t h e w o r k : L a M a r e a Y o k o h a m a. A r t i s t : M a r i a n o P e n s o t t i ( P l a y w r i g h t, D i r e c t o r ) v e r. E N G O u t l i n e T i t l e o f t h e w o r k : L a M a r e a Y o k o h a m a A r t i s t : M a r i a n o P e n s o t t i ( P l a y w r i g h t, D i r e c t o r ) C o n t e n t s : T h i s w o

More information

by Martin Mendez, UASLP Copyright 2006 The McGraw-Hill Companies, Inc. Permission required for reproduction or display.

by Martin Mendez, UASLP Copyright 2006 The McGraw-Hill Companies, Inc. Permission required for reproduction or display. Chapter 5 by Martin Mendez, 1 Roots of Equations Part Why? b m b a + b + c = 0 = aa 4ac But a 5 4 3 + b + c + d + e + f = 0 sin + = 0 =? =? by Martin Mendez, Nonlinear Equation Solvers Bracketing Graphical

More information

Numerical Methods. Roots of Equations

Numerical Methods. Roots of Equations Roots of Equations by Norhayati Rosli & Nadirah Mohd Nasir Faculty of Industrial Sciences & Technology norhayati@ump.edu.my, nadirah@ump.edu.my Description AIMS This chapter is aimed to compute the root(s)

More information

arxiv:quant-ph/ v3 6 Jan 1995

arxiv:quant-ph/ v3 6 Jan 1995 arxiv:quant-ph/9501001v3 6 Jan 1995 Critique of proposed imit to space time measurement, based on Wigner s cocks and mirrors L. Diósi and B. Lukács KFKI Research Institute for Partice and Nucear Physics

More information

Haar Decomposition and Reconstruction Algorithms

Haar Decomposition and Reconstruction Algorithms Jim Lambers MAT 773 Fa Semester 018-19 Lecture 15 and 16 Notes These notes correspond to Sections 4.3 and 4.4 in the text. Haar Decomposition and Reconstruction Agorithms Decomposition Suppose we approximate

More information

Candidate Number. General Certificate of Education Advanced Level Examination June 2010

Candidate Number. General Certificate of Education Advanced Level Examination June 2010 Centre Number Surname Candidate Number For Examiner s Use Other Names Candidate Signature Examiner s Initias Genera Certificate of Education Advanced Leve Examination June 2010 Question 1 2 Mark Physics

More information

Goals for This Lecture:

Goals for This Lecture: Goals for This Lecture: Learn the Newton-Raphson method for finding real roots of real functions Learn the Bisection method for finding real roots of a real function Look at efficient implementations of

More information

p 1 p 0 (p 1, f(p 1 )) (p 0, f(p 0 )) The geometric construction of p 2 for the se- cant method.

p 1 p 0 (p 1, f(p 1 )) (p 0, f(p 0 )) The geometric construction of p 2 for the se- cant method. 80 CHAP. 2 SOLUTION OF NONLINEAR EQUATIONS f (x) = 0 y y = f(x) (p, 0) p 2 p 1 p 0 x (p 1, f(p 1 )) (p 0, f(p 0 )) The geometric construction of p 2 for the se- Figure 2.16 cant method. Secant Method The

More information

Introduction to Simulation - Lecture 14. Multistep Methods II. Jacob White. Thanks to Deepak Ramaswamy, Michal Rewienski, and Karen Veroy

Introduction to Simulation - Lecture 14. Multistep Methods II. Jacob White. Thanks to Deepak Ramaswamy, Michal Rewienski, and Karen Veroy Introduction to Simuation - Lecture 14 Mutistep Methods II Jacob White Thans to Deepa Ramaswamy, Micha Rewiensi, and Karen Veroy Outine Sma Timestep issues for Mutistep Methods Reminder about LTE minimization

More information

The distribution of the number of nodes in the relative interior of the typical I-segment in homogeneous planar anisotropic STIT Tessellations

The distribution of the number of nodes in the relative interior of the typical I-segment in homogeneous planar anisotropic STIT Tessellations Comment.Math.Univ.Caroin. 51,3(21) 53 512 53 The distribution of the number of nodes in the reative interior of the typica I-segment in homogeneous panar anisotropic STIT Tesseations Christoph Thäe Abstract.

More information

Solution of Algebric & Transcendental Equations

Solution of Algebric & Transcendental Equations Page15 Solution of Algebric & Transcendental Equations Contents: o Introduction o Evaluation of Polynomials by Horner s Method o Methods of solving non linear equations o Bracketing Methods o Bisection

More information

cha1873x_p02.qxd 3/21/05 1:01 PM Page 104 PART TWO

cha1873x_p02.qxd 3/21/05 1:01 PM Page 104 PART TWO cha1873x_p02.qxd 3/21/05 1:01 PM Page 104 PART TWO ROOTS OF EQUATIONS PT2.1 MOTIVATION Years ago, you learned to use the quadratic formula x = b ± b 2 4ac 2a to solve f(x) = ax 2 + bx + c = 0 (PT2.1) (PT2.2)

More information

Expectation-Maximization for Estimating Parameters for a Mixture of Poissons

Expectation-Maximization for Estimating Parameters for a Mixture of Poissons Expectation-Maximization for Estimating Parameters for a Mixture of Poissons Brandon Maone Department of Computer Science University of Hesini February 18, 2014 Abstract This document derives, in excrutiating

More information

Differentiating Functions & Expressions - Edexcel Past Exam Questions

Differentiating Functions & Expressions - Edexcel Past Exam Questions - Edecel Past Eam Questions. (a) Differentiate with respect to (i) sin + sec, (ii) { + ln ()}. 5-0 + 9 Given that y =, ¹, ( -) 8 (b) show that = ( -). (6) June 05 Q. f() = e ln, > 0. (a) Differentiate

More information

Section 2: Basic Algebra

Section 2: Basic Algebra Section : Basic Aebra Aebra ike arithmetic deas with numbers Both subjects empoy the fundamenta operations of addition, subtraction, mutipication, division, raisin to a power and takin a root In both,

More information

THE THREE POINT STEINER PROBLEM ON THE FLAT TORUS: THE MINIMAL LUNE CASE

THE THREE POINT STEINER PROBLEM ON THE FLAT TORUS: THE MINIMAL LUNE CASE THE THREE POINT STEINER PROBLEM ON THE FLAT TORUS: THE MINIMAL LUNE CASE KATIE L. MAY AND MELISSA A. MITCHELL Abstract. We show how to identify the minima path network connecting three fixed points on

More information

V.B The Cluster Expansion

V.B The Cluster Expansion V.B The Custer Expansion For short range interactions, speciay with a hard core, it is much better to repace the expansion parameter V( q ) by f( q ) = exp ( βv( q )), which is obtained by summing over

More information

Assignment 7 Due Tuessday, March 29, 2016

Assignment 7 Due Tuessday, March 29, 2016 Math 45 / AMCS 55 Dr. DeTurck Assignment 7 Due Tuessday, March 9, 6 Topics for this week Convergence of Fourier series; Lapace s equation and harmonic functions: basic properties, compuations on rectanges

More information

Numerical simulation of javelin best throwing angle based on biomechanical model

Numerical simulation of javelin best throwing angle based on biomechanical model ISSN : 0974-7435 Voume 8 Issue 8 Numerica simuation of javein best throwing ange based on biomechanica mode Xia Zeng*, Xiongwei Zuo Department of Physica Education, Changsha Medica University, Changsha

More information

Roots of Equations. ITCS 4133/5133: Introduction to Numerical Methods 1 Roots of Equations

Roots of Equations. ITCS 4133/5133: Introduction to Numerical Methods 1 Roots of Equations Roots of Equations Direct Search, Bisection Methods Regula Falsi, Secant Methods Newton-Raphson Method Zeros of Polynomials (Horner s, Muller s methods) EigenValue Analysis ITCS 4133/5133: Introduction

More information

Separation of Variables and a Spherical Shell with Surface Charge

Separation of Variables and a Spherical Shell with Surface Charge Separation of Variabes and a Spherica She with Surface Charge In cass we worked out the eectrostatic potentia due to a spherica she of radius R with a surface charge density σθ = σ cos θ. This cacuation

More information

INTRODUCTION TO NUMERICAL ANALYSIS

INTRODUCTION TO NUMERICAL ANALYSIS INTRODUCTION TO NUMERICAL ANALYSIS Cho, Hyoung Kyu Department of Nuclear Engineering Seoul National University 3. SOLVING NONLINEAR EQUATIONS 3.1 Background 3.2 Estimation of errors in numerical solutions

More information

A proposed nonparametric mixture density estimation using B-spline functions

A proposed nonparametric mixture density estimation using B-spline functions A proposed nonparametric mixture density estimation using B-spine functions Atizez Hadrich a,b, Mourad Zribi a, Afif Masmoudi b a Laboratoire d Informatique Signa et Image de a Côte d Opae (LISIC-EA 4491),

More information

IMPROVEMENT OF THE SHAPE FUNCTION IN THE STOCHASTIC SIMULATION METHOD AND REPRODUCTION OF HIGH-FREQUENCY MOTION RECORDINGS OF THE KOBE EARTHQUAKE

IMPROVEMENT OF THE SHAPE FUNCTION IN THE STOCHASTIC SIMULATION METHOD AND REPRODUCTION OF HIGH-FREQUENCY MOTION RECORDINGS OF THE KOBE EARTHQUAKE IMPROVEMENT OF THE SHAPE FUNCTION IN THE STOCHASTIC SIMULATION METHOD AND REPRODUCTION OF HIGH-FREQUENCY MOTION RECORDINGS OF THE KOBE EARTHQUAKE ABSTRACT: Masanori Horike 1 and Yoshihiro Onishi 1 Professor,

More information

NUMERICAL METHODS FOR SOLVING EQUATIONS

NUMERICAL METHODS FOR SOLVING EQUATIONS Mathematics Revision Guides Numerical Methods for Solving Equations Page of M.K. HOME TUITION Mathematics Revision Guides Level: AS / A Level AQA : C3 Edecel: C3 OCR: C3 NUMERICAL METHODS FOR SOLVING EQUATIONS

More information

MATH 350: Introduction to Computational Mathematics

MATH 350: Introduction to Computational Mathematics MATH 350: Introduction to Computational Mathematics Chapter IV: Locating Roots of Equations Greg Fasshauer Department of Applied Mathematics Illinois Institute of Technology Spring 2011 fasshauer@iit.edu

More information

Queens College, CUNY, Department of Computer Science Numerical Methods CSCI 361 / 761 Spring 2018 Instructor: Dr. Sateesh Mane.

Queens College, CUNY, Department of Computer Science Numerical Methods CSCI 361 / 761 Spring 2018 Instructor: Dr. Sateesh Mane. Queens College, CUNY, Department of Computer Science Numerical Methods CSCI 361 / 761 Spring 2018 Instructor: Dr. Sateesh Mane c Sateesh R. Mane 2018 3 Lecture 3 3.1 General remarks March 4, 2018 This

More information

2-loop additive mass renormalization with clover fermions and Symanzik improved gluons

2-loop additive mass renormalization with clover fermions and Symanzik improved gluons 2-oop additive mass renormaization with cover fermions and Symanzik improved guons Apostoos Skouroupathis Department of Physics, University of Cyprus, Nicosia, CY-1678, Cyprus E-mai: php4as01@ucy.ac.cy

More information

Homework #04 Answers and Hints (MATH4052 Partial Differential Equations)

Homework #04 Answers and Hints (MATH4052 Partial Differential Equations) Homework #4 Answers and Hints (MATH452 Partia Differentia Equations) Probem 1 (Page 89, Q2) Consider a meta rod ( < x < ), insuated aong its sides but not at its ends, which is initiay at temperature =

More information

2.29 Numerical Fluid Mechanics Spring 2015 Lecture 4

2.29 Numerical Fluid Mechanics Spring 2015 Lecture 4 2.29 Spring 2015 Lecture 4 Review Lecture 3 Truncation Errors, Taylor Series and Error Analysis Taylor series: 2 3 n n i1 i i i i i n f( ) f( ) f '( ) f ''( ) f '''( )... f ( ) R 2! 3! n! n1 ( n1) Rn f

More information

Introduction to Simulation - Lecture 13. Convergence of Multistep Methods. Jacob White. Thanks to Deepak Ramaswamy, Michal Rewienski, and Karen Veroy

Introduction to Simulation - Lecture 13. Convergence of Multistep Methods. Jacob White. Thanks to Deepak Ramaswamy, Michal Rewienski, and Karen Veroy Introduction to Simuation - Lecture 13 Convergence of Mutistep Methods Jacob White Thans to Deepa Ramaswamy, Micha Rewiensi, and Karen Veroy Outine Sma Timestep issues for Mutistep Methods Loca truncation

More information

Lec7p1, ORF363/COS323

Lec7p1, ORF363/COS323 Lec7 Page 1 Lec7p1, ORF363/COS323 This lecture: One-dimensional line search (root finding and minimization) Bisection Newton's method Secant method Introduction to rates of convergence Instructor: Amir

More information

Part A. z-transform. 1. z-transform

Part A. z-transform. 1. z-transform Chapter 6 ztransform Part A ztransform Contents Part A: ztransform Part B: Inverse ztransform Part C: Transfer Function Part A: ztransform 1. ztransform 1. ztransform ztransform Reion of Converence (ROC)

More information

General Certificate of Education Advanced Level Examination June 2010

General Certificate of Education Advanced Level Examination June 2010 Genera Certificate of Education Advanced Leve Examination June 2010 Human Bioogy HBI6T/Q10/task Unit 6T A2 Investigative Skis Assignment Task Sheet The effect of using one or two eyes on the perception

More information

V.B The Cluster Expansion

V.B The Cluster Expansion V.B The Custer Expansion For short range interactions, speciay with a hard core, it is much better to repace the expansion parameter V( q ) by f(q ) = exp ( βv( q )) 1, which is obtained by summing over

More information

Methods for Advanced Mathematics (C3) Coursework Numerical Methods

Methods for Advanced Mathematics (C3) Coursework Numerical Methods Woodhouse College 0 Page Introduction... 3 Terminolog... 3 Activit... 4 Wh use numerical methods?... Change of sign... Activit... 6 Interval Bisection... 7 Decimal Search... 8 Coursework Requirements on

More information

14-6 The Equation of Continuity

14-6 The Equation of Continuity 14-6 The Equation of Continuity 14-6 The Equation of Continuity Motion of rea fuids is compicated and poory understood (e.g., turbuence) We discuss motion of an idea fuid 1. Steady fow: Laminar fow, the

More information

The EM Algorithm applied to determining new limit points of Mahler measures

The EM Algorithm applied to determining new limit points of Mahler measures Contro and Cybernetics vo. 39 (2010) No. 4 The EM Agorithm appied to determining new imit points of Maher measures by Souad E Otmani, Georges Rhin and Jean-Marc Sac-Épée Université Pau Veraine-Metz, LMAM,

More information

arxiv: v1 [hep-th] 10 Dec 2018

arxiv: v1 [hep-th] 10 Dec 2018 Casimir energy of an open string with ange-dependent boundary condition A. Jahan 1 and I. Brevik 2 1 Research Institute for Astronomy and Astrophysics of Maragha (RIAAM, Maragha, Iran 2 Department of Energy

More information

Gauss Law. 2. Gauss s Law: connects charge and field 3. Applications of Gauss s Law

Gauss Law. 2. Gauss s Law: connects charge and field 3. Applications of Gauss s Law Gauss Law 1. Review on 1) Couomb s Law (charge and force) 2) Eectric Fied (fied and force) 2. Gauss s Law: connects charge and fied 3. Appications of Gauss s Law Couomb s Law and Eectric Fied Couomb s

More information

2.3 The Fixed-Point Algorithm

2.3 The Fixed-Point Algorithm .3 The Fied-Point Algorithm 1. Mean Value Theorem: Theorem Rolle stheorem: Suppose that f is continuous on a, b and is differentiable on a, b. If f a f b, then there eists a number c in a, b such that

More information

Some Measures for Asymmetry of Distributions

Some Measures for Asymmetry of Distributions Some Measures for Asymmetry of Distributions Georgi N. Boshnakov First version: 31 January 2006 Research Report No. 5, 2006, Probabiity and Statistics Group Schoo of Mathematics, The University of Manchester

More information

Root Finding Convergence Analysis

Root Finding Convergence Analysis Root Finding Convergence Analysis Justin Ross & Matthew Kwitowski November 5, 2012 There are many different ways to calculate the root of a function. Some methods are direct and can be done by simply solving

More information

Matrices and Determinants

Matrices and Determinants Matrices and Determinants Teaching-Learning Points A matri is an ordered rectanguar arra (arrangement) of numbers and encosed b capita bracket [ ]. These numbers are caed eements of the matri. Matri is

More information

MATH 350: Introduction to Computational Mathematics

MATH 350: Introduction to Computational Mathematics MATH 350: Introduction to Computational Mathematics Chapter IV: Locating Roots of Equations Greg Fasshauer Department of Applied Mathematics Illinois Institute of Technology Spring 2011 fasshauer@iit.edu

More information

Theme 1: Solving Nonlinear Equations

Theme 1: Solving Nonlinear Equations Theme 1: Solving Nonlinear Equations Prof. Mapundi K. Banda (Tuks) WTW263 Semester II 1 / 22 Sources of Errors Finite decimal representation (Rounding): Finite decimal representation will be used to represent

More information

Week 6 Lectures, Math 6451, Tanveer

Week 6 Lectures, Math 6451, Tanveer Fourier Series Week 6 Lectures, Math 645, Tanveer In the context of separation of variabe to find soutions of PDEs, we encountered or and in other cases f(x = f(x = a 0 + f(x = a 0 + b n sin nπx { a n

More information

Multiple Beam Interference

Multiple Beam Interference MutipeBeamInterference.nb James C. Wyant 1 Mutipe Beam Interference 1. Airy's Formua We wi first derive Airy's formua for the case of no absorption. ü 1.1 Basic refectance and transmittance Refected ight

More information

Strain Energy in Linear Elastic Solids

Strain Energy in Linear Elastic Solids Strain Energ in Linear Eastic Soids CEE L. Uncertaint, Design, and Optimiation Department of Civi and Environmenta Engineering Duke Universit Henri P. Gavin Spring, 5 Consider a force, F i, appied gradua

More information

The Hydrogen Atomic Model Based on the Electromagnetic Standing Waves and the Periodic Classification of the Elements

The Hydrogen Atomic Model Based on the Electromagnetic Standing Waves and the Periodic Classification of the Elements Appied Physics Research; Vo. 4, No. 3; 0 ISSN 96-9639 -ISSN 96-9647 Pubished by Canadian Center of Science and ducation The Hydrogen Atomic Mode Based on the ectromagnetic Standing Waves and the Periodic

More information

CLASS NOTES Computational Methods for Engineering Applications I Spring 2015

CLASS NOTES Computational Methods for Engineering Applications I Spring 2015 CLASS NOTES Computational Methods for Engineering Applications I Spring 2015 Petros Koumoutsakos Gerardo Tauriello (Last update: July 2, 2015) IMPORTANT DISCLAIMERS 1. REFERENCES: Much of the material

More information

Root Finding (and Optimisation)

Root Finding (and Optimisation) Root Finding (and Optimisation) M.Sc. in Mathematical Modelling & Scientific Computing, Practical Numerical Analysis Michaelmas Term 2018, Lecture 4 Root Finding The idea of root finding is simple we want

More information

Lobontiu: System Dynamics for Engineering Students Website Chapter 3 1. z b z

Lobontiu: System Dynamics for Engineering Students Website Chapter 3 1. z b z Chapter W3 Mechanica Systems II Introduction This companion website chapter anayzes the foowing topics in connection to the printed-book Chapter 3: Lumped-parameter inertia fractions of basic compiant

More information

Topic 4b. Open Methods for Root Finding

Topic 4b. Open Methods for Root Finding Course Instructor Dr. Ramond C. Rump Oice: A 337 Phone: (915) 747 6958 E Mail: rcrump@utep.edu Topic 4b Open Methods or Root Finding EE 4386/5301 Computational Methods in EE Outline Open Methods or Root

More information

Module 22: Simple Harmonic Oscillation and Torque

Module 22: Simple Harmonic Oscillation and Torque Modue : Simpe Harmonic Osciation and Torque.1 Introduction We have aready used Newton s Second Law or Conservation of Energy to anayze systems ike the boc-spring system that osciate. We sha now use torque

More information

4 Separation of Variables

4 Separation of Variables 4 Separation of Variabes In this chapter we describe a cassica technique for constructing forma soutions to inear boundary vaue probems. The soution of three cassica (paraboic, hyperboic and eiptic) PDE

More information

An explicit Jordan Decomposition of Companion matrices

An explicit Jordan Decomposition of Companion matrices An expicit Jordan Decomposition of Companion matrices Fermín S V Bazán Departamento de Matemática CFM UFSC 88040-900 Forianópois SC E-mai: fermin@mtmufscbr S Gratton CERFACS 42 Av Gaspard Coriois 31057

More information

MA 201: Partial Differential Equations Lecture - 10

MA 201: Partial Differential Equations Lecture - 10 MA 201: Partia Differentia Equations Lecture - 10 Separation of Variabes, One dimensiona Wave Equation Initia Boundary Vaue Probem (IBVP) Reca: A physica probem governed by a PDE may contain both boundary

More information

Paraxial Beam, Gaussian Basics

Paraxial Beam, Gaussian Basics Paraxia Beam, Gaussian Basics ECE 5368/6358 han q e - copyrighted Use soey for students registered for UH ECE 6358/5368 during courses - DO NOT distributed (copyrighted materias). Introduction. Paraxia

More information

Root finding. Eugeniy E. Mikhailov. Lecture 06. The College of William & Mary. Eugeniy Mikhailov (W&M) Practical Computing Lecture 06 1 / 10

Root finding. Eugeniy E. Mikhailov. Lecture 06. The College of William & Mary. Eugeniy Mikhailov (W&M) Practical Computing Lecture 06 1 / 10 Root finding Eugeniy E. Mikhailov The College of William & Mary Lecture 06 Eugeniy Mikhailov (W&M) Practical Computing Lecture 06 1 / 10 Root finding problem Generally we want to solve the following canonical

More information

Numerical Methods I Solving Nonlinear Equations

Numerical Methods I Solving Nonlinear Equations Numerical Methods I Solving Nonlinear Equations Aleksandar Donev Courant Institute, NYU 1 donev@courant.nyu.edu 1 MATH-GA 2011.003 / CSCI-GA 2945.003, Fall 2014 October 16th, 2014 A. Donev (Courant Institute)

More information

PhysicsAndMathsTutor.com

PhysicsAndMathsTutor.com . Two points A and B ie on a smooth horizonta tabe with AB = a. One end of a ight eastic spring, of natura ength a and moduus of easticity mg, is attached to A. The other end of the spring is attached

More information

3.1 Introduction. Solve non-linear real equation f(x) = 0 for real root or zero x. E.g. x x 1.5 =0, tan x x =0.

3.1 Introduction. Solve non-linear real equation f(x) = 0 for real root or zero x. E.g. x x 1.5 =0, tan x x =0. 3.1 Introduction Solve non-linear real equation f(x) = 0 for real root or zero x. E.g. x 3 +1.5x 1.5 =0, tan x x =0. Practical existence test for roots: by intermediate value theorem, f C[a, b] & f(a)f(b)

More information

BEKG 2452 NUMERICAL METHODS Solution of Nonlinear Equations

BEKG 2452 NUMERICAL METHODS Solution of Nonlinear Equations BEKG 2452 NUMERICAL METHODS Solution of Nonlinear Equations Ser Lee Loh a, Wei Sen Loi a a Fakulti Kejuruteraan Elektrik Universiti Teknikal Malaysia Melaka Lesson Outcome Upon completion of this lesson,

More information

CS229 Lecture notes. Andrew Ng

CS229 Lecture notes. Andrew Ng CS229 Lecture notes Andrew Ng Part IX The EM agorithm In the previous set of notes, we taked about the EM agorithm as appied to fitting a mixture of Gaussians. In this set of notes, we give a broader view

More information

An H 2 type Riemannian metric on the space of planar curves

An H 2 type Riemannian metric on the space of planar curves An H 2 type Riemannian metric on the space of panar curves Jayant hah Mathematics Department, Northeastern University, Boston MA emai: shah@neu.edu Abstract An H 2 type metric on the space of panar curves

More information

Chapter 6. Nonlinear Equations. 6.1 The Problem of Nonlinear Root-finding. 6.2 Rate of Convergence

Chapter 6. Nonlinear Equations. 6.1 The Problem of Nonlinear Root-finding. 6.2 Rate of Convergence Chapter 6 Nonlinear Equations 6. The Problem of Nonlinear Root-finding In this module we consider the problem of using numerical techniques to find the roots of nonlinear equations, f () =. Initially we

More information

SydU STAT3014 (2015) Second semester Dr. J. Chan 18

SydU STAT3014 (2015) Second semester Dr. J. Chan 18 STAT3014/3914 Appied Stat.-Samping C-Stratified rand. sampe Stratified Random Samping.1 Introduction Description The popuation of size N is divided into mutuay excusive and exhaustive subpopuations caed

More information

Chapter 1. Root Finding Methods. 1.1 Bisection method

Chapter 1. Root Finding Methods. 1.1 Bisection method Chapter 1 Root Finding Methods We begin by considering numerical solutions to the problem f(x) = 0 (1.1) Although the problem above is simple to state it is not always easy to solve analytically. This

More information

CHAPTER-II ROOTS OF EQUATIONS

CHAPTER-II ROOTS OF EQUATIONS CHAPTER-II ROOTS OF EQUATIONS 2.1 Introduction The roots or zeros of equations can be simply defined as the values of x that makes f(x) =0. There are many ways to solve for roots of equations. For some

More information

Related Topics Maxwell s equations, electrical eddy field, magnetic field of coils, coil, magnetic flux, induced voltage

Related Topics Maxwell s equations, electrical eddy field, magnetic field of coils, coil, magnetic flux, induced voltage Magnetic induction TEP Reated Topics Maxwe s equations, eectrica eddy fied, magnetic fied of cois, coi, magnetic fux, induced votage Principe A magnetic fied of variabe frequency and varying strength is

More information

Figure 1: Graph of y = x cos(x)

Figure 1: Graph of y = x cos(x) Chapter The Solution of Nonlinear Equations f(x) = 0 In this chapter we will study methods for find the solutions of functions of single variables, ie values of x such that f(x) = 0 For example, f(x) =

More information

Chemical Kinetics Part 2. Chapter 16

Chemical Kinetics Part 2. Chapter 16 Chemica Kinetics Part 2 Chapter 16 Integrated Rate Laws The rate aw we have discussed thus far is the differentia rate aw. Let us consider the very simpe reaction: a A à products The differentia rate reates

More information

Today s class. Numerical differentiation Roots of equation Bracketing methods. Numerical Methods, Fall 2011 Lecture 4. Prof. Jinbo Bi CSE, UConn

Today s class. Numerical differentiation Roots of equation Bracketing methods. Numerical Methods, Fall 2011 Lecture 4. Prof. Jinbo Bi CSE, UConn Today s class Numerical differentiation Roots of equation Bracketing methods 1 Numerical Differentiation Finite divided difference First forward difference First backward difference Lecture 3 2 Numerical

More information