AN INTRODUCTION TO NUMERICAL METHODS USING MATHCAD. Mathcad Release 13. Khyruddin Akbar Ansari, Ph.D., P.E.
|
|
- Jean Campbell
- 5 years ago
- Views:
Transcription
1 AN INTRODUCTION TO NUMERICAL METHODS USING MATHCAD Mathca Release 13 Khyruin Akbar Ansari, Ph.D., P.E. Professor of Mechanical Engineering School of Engineering Gonzaga University SDC PUBLICATIONS Schroff Development Corporation
2 Chapter 2: Introuction to Numerical Methos 43 C H A P T E R 2 INTRODUCTION TO NUMERICAL METHODS 2.1 THE USE OF NUMERICAL METHODS IN SCIENCE AND ENGINEERING Analysis of problems in engineering an the physical sciences typically involves four steps as follows. (1) Development of a suitable mathematical moel that realistically represents a given physical system. (2) Derivation of the system governing equations using physical laws such as Newton's laws of motion, conservation of energy, the laws governing electrical circuits etc. (3) Solution of the governing equations, an (4) Interpretation of the results. Because real worl problems are generally quite complex with the generation of close-form analytical solutions becoming impossible in many situations, there exists, most efinitely, a nee for the proper utilization of computer-base techniques in the solution of practical problems. The avancement of computer technology has mae the effective use of numerical methos an computer-base techniques very feasible, an thus, solutions can now be obtaine much faster than ever before an with much better than acceptable accuracy. However, there are avantages as well as isavantages associate with any numerical proceure that is resorte to, an these must be kept in min when using it. 2.2 COMPARISON OF NUMERICAL METHODS WITH ANALYTICAL METHODS While an analytical solution will be exact if it exists, a numerical metho, on the other han, will generally require iterations to generate a solution, which is only an approximation an which certainly cannot be consiere exact by any means. A isavantage associate with analytical solution techniques is that they are generally applicable only to very special cases of problems. Numerical solutions, on the contrary, will solve complex situations as well. While numerical techniques have several avantages incluing easy programming on a computer an the convenience with which they hanle complex problems, the initial estimate of the solution along with the many number of iterations that are sometimes require to generate a solution can be looke upon as isavantages.
3 44 AN INTRODUCTION TO NUMERICAL METHODS USING MATHCAD 2.3 SOURCES OF NUMERICAL ERRORS AND THEIR COMPUTATION It is inee possible for miscalculations to creep into a numerical solution because of various sources of error. These inclue inaccurate mathematical moeling, wrong programming, wrong input, rouning off of numbers an truncation of an infinite series. Roun-off error is the general name given to inaccuracies that affect the calculation scene when a finite number of igits are assigne to represent an actual number. In a long sequence of calculations, this roun-off error can accumulate, then propagate through the process of calculation an finally grow very rapily to a significant number. A truncation error results when an infinite series is approximate by a finite number of terms, an, typically, upper bouns are place on the size of this error. The true error is efine as the ifference between the compute value an the true value of a number. E True = X Comp X True (2.1) while the relative true error is the error relative to the true value X Comp X True e r = X True (2.2) Expresse as a percentage, the relative true error is written as X Comp X True e r = 1 (%) (2.3) X True 2.4 TAYLOR SERIES EXPANSION The Taylor series is consiere as a basis of approximation in numerical analysis. If the value of a function of x is provie at " x ", then the Taylor series provies a means of evaluating the function at " x + h", where " x " is the starting value of the inepenent variable an " h " is the ifference between the starting value an the new value at which the function is to be approximate ( ) = fx ( ) + h fx + h ( ) fx x + h 2 2 2! 2 x fx ( ) h fx ( 3! 3 ) +... x (2.4) This equation can be use for generating various s of approximations as shown below. The of approximation is efine by the highest erivative inclue in the series. For example, If only terms up to the secon erivative are retaine in the series, the result is a secon approximation.
4 Chapter 2: Introuction to Numerical Methos 4 First approximation: ( ) = fx ( ) + h fx + h x fx ( ) (2.) Secon approximation: ( ) = fx ( ) + h fx + h x fx ( ) + h 2 2 2! 2 x fx ( ) (2.6) Thir approximation: ( ) = fx ( ) + h fx + h x fx ( ) + h 2 2 2! 2 x fx ( ) + h 3 3 3! 3 x fx ( ) (2.7) It is to note that the significance of the higher terms in the Taylor series increases with the nonlinearity of the function involve as well as the ifference between the " starting x" value an the "x" value at which the function is to be approximate. Thus, the fewer the terms that are inclue in the series, the larger will be the error associate with the computation of the function value. If the function is linear, however, only terms up to the first erivative term nee to be inclue. Example 2.1 Using the Taylor series expansion for f(x) = -.1 x x x x + etermine the zeroth, first, secon, thir, fourth an fifth approximations of f(x + h ) where x = an h = 1,2, 3, 4, an compare these with the exact solutions. h=1.: Put in the function an generate its erivatives: fx ( ) :=.1 x 4.17 x 3.2 x 2.2x + x := h:= 1. fprime( x) :=.6x 3.1x 2.x.2 <--Generate erivatives f2prime( x) := 1.8x 2 1.2x. f3prime( x) := 3.6x 1.2 f4prime( x) := 3.6 fprime( x) :=.
5 46 AN INTRODUCTION TO NUMERICAL METHODS USING MATHCAD h 2 term1 := f( x) term2 := hfprime( x) term3 := f2prime x 2 ( ) h 3 term4 := f3prime x 6 ( ) term h 4 := f4prime x 24 ( ) term6 h := fprime x 12 ( ) ftaylor := term1 <---- one-term or zero- approximation ftaylor1 := term1 + term2 <---- first approximation with two terms ftaylor2 := term1 + term2 + term3 <---secon approximation with 3 terms ftaylor3 := term1 + term2 + term3 + term4 <---thir approximation with 4 terms ftaylor4 := term1 + term2 + term3 + term4 + term <---fourth approximation with terms ftaylor := term1 + term2 + term3 + term4 + term + term6 <----- fifth approximation with 6 terms x := x + h x = 1 ftaylor = ftaylor1 = 1 ftaylor2.7 ftaylor3 =.8 ftaylor4 =.43 ftaylor =.43 = These are the zero- fifth <-- approximations of the given function f(x) using the Taylor series. f1 ( ) =.43 <---EXACT ANSWER USING FUNCTION GIVEN. err := f( x) ftaylor err =.82 err1 := f( x) ftaylor1 err1 =.7 err2 := f( x) ftaylor2 err2 =.32 These are errors ( ifferences between exact <-- values an approximations ) for the above zero - fifth approximations. err3 := f( x) ftaylor3 err3 =.1 err4 := f( x) ftaylor4 err4 = err := f( x) ftaylor err = Similarly, by using h= 2, 3, 4,, the zeroth- fifth approximations for f(2), f(3), f(4), f() an the associate errors can be etermine. These are given in Tables 2.1 an 2.2 Plots of the various Taylor series approximations of the given function an associate errors are generate below an are presente in Figs. 2.1 an 2.2
6 Chapter 2: Introuction to Numerical Methos 47 x := x :=,.1.. ftaylor( x) := fx ( ) <-- zeroth- approximation ftaylor1( x) := ftaylor( x) + ( x x) fprime( x) <---first- approximation ( x x) 2 ftaylor2( x) := ftaylor1( x) + f2prime( x) <--secon- approximation 2 ( x x) 3 ftaylor3( x) := ftaylor2( x) + f3prime( x) <---thir- approximation 6 ( x x) 4 ftaylor4( x) := ftaylor3( x) + f4prime( x) <---fourth- approximation 24 ( x x) ftaylor ( x) := ftaylor4( x) + fprime( x) <---fifth- approximation 12 Errors generate with the various approximations are as follows Zero approximation: err( x) := fx ( ) ftaylor( x) First approximation: err1( x) := fx ( ) ftaylor1( x) Secon approximation: err2( x) := fx ( ) ftaylor2( x) Thir approximation: err3( x) := fx ( ) ftaylor3( x) Fourth approximation: err4( x) := fx ( ) ftaylor4( x) Fifth approximation: err ( x) := fx ( ) ftaylor ( x) The various approximations generate by the above calculations an the associate errors are compare in Table 2.1.
7 48 AN INTRODUCTION TO NUMERICAL METHODS USING MATHCAD Taylor series approx of given function Function approximate by Taylor series ftaylor( x) ftaylor3( x) ftaylor( x) 1 Zeroth approx Thir approx Fifth approx/ given function x x- value Figure 2.1. Taylor series approximation of given function x :=,.1.. Errors gen ue to Taylor-series approx errors as function of x err( x) err3( x) err( x) 1 Zero approx Thir approx Fifth approx x x- value Figure 2.2. Errors associate with the various Taylor series approximations
8 Chapter 2: Introuction to Numerical Methos 49 The various approximations generate by the above calculations an the associate errors are compare in the following tables. Table 2.1 h := 1.. x :=, 1.. Various s of approximation generate by Taylor series approach versus true values of given function zeroth first secon thir fourth fifth True Value h = x = ftaylor( x) ftaylor1 = ( x) =ftaylor2( x) ftaylor3 = ( x) =ftaylor4( x) =ftaylor ( x) =f( x) = Table 2.2 Errors associate with the ifferent s of approximation zeroth first secon thir fourth fifth h = x = err( x) = err1( x) = err2( x) = err3( x) = err4( x) = err ( x) = PROBLEMS 2.1. Using the Taylor series expansion for cos x, which is given as f(x) = cos x = 1- x 2 / 2 + x 4 / 24, etermine the one-term, two-term an three-term approximations of f(x + h ), where x =
9 AN INTRODUCTION TO NUMERICAL METHODS USING MATHCAD ra an h =. 1, ra, an compare these with the exact solution. Using Mathca, generate plots of the various Taylor series approximations an associate errors as functions of the inepenent variable x. 2.2 Develop a Taylor series expansion of the following function: f(x) = x - 6 x 4 + 3x Use x =3 as the base an h as the increment. Using Mathca, evaluate the series for h=.1, , aing terms incrementally as in Problem 2.1. Compare the various Taylor series approximations obtaine with true values in a table. Generate plots of the approximations an associate errors as functions of x. 2.3 Given the following function: f(x) = x 3-3 x 2 + x + 1, etermine f ( x + h ) with the help of a Taylor series expansion, where x = 2 an h =.4. Compare the true value of f ( 2.4 ) with estimates obtaine by resorting to (a) one term only (b) two terms (c) three terms an () four terms of the series. 2.4 Given the following function fx ( ) = 3x 3 6x x + 2 use a Taylor series expansion to etermine the zeroth, first, secon an thir approximations of f(x +h) where x = 2 an h =.. Compare these with the exact solution. 2. By eveloping a Taylor series expansion for f(x) = e x about x =, etermine the fourth- approximation of e 2. an compare it with the exact solution By eveloping a Taylor series expansion for f(x) = ln(2-x) about x =, etermine the fourth- approximation of ln (.) an compare it with the exact solution
10 Chapter 2: Introuction to Numerical Methos By eveloping a Taylor series expansion for f(x) = x 3 e - x about x = 1, etermine the thir- approximation of f(1.2) an compare it with the exact solution By eveloping a Taylor series expansion for f(x) = e cos x about x =, etermine the fourth- approximation of f (2π) an compare it with the exact solution By eveloping a Taylor series expansion for f(x) = (x - 2) 1/2 about x = 3, etermine the thir- approximation of f (2.2), that is, (.2) 1/2, an compare it with the exact solution Given the function f(x) = x 2 - x. + 6, use a Taylor series expansion to etermine the first, secon, thir an fourth approximations of f (2. ) by resorting to x = 2 an h =.. Compare these with the exact solution Given the function f(x) = 6 x 3-9 x 2 +2 x + 4, use a Taylor series expansion to etermine the zeroth, first, secon an thir approximations of f (x + h ) where x = 3 an h = 1. Compare these with the exact solution Given the function f(x) = 4 x 4-7 x 3 + x 2-6 x + 9 use a Taylor series expansion to etermine the zeroth, first, secon, thir an fourth
11 2 AN INTRODUCTION TO NUMERICAL METHODS USING MATHCAD approximations of f (x + h ) ) where x = 3 an h =.. Compare these with the exact solution. Calculate errors an generate calculations to three ecimal places Given the function f(x) = 8 x 3-1 x x + 4, use a Taylor series expansion to etermine the zeroth, first, secon an thir approximations of f (x + h ) where x = 2 an h = 1. Compare these with the exact solution Given the function f(x) = 1 + x + x 2 / 2! + x 3 / 3! +x 4 / 4! use a Taylor series expansion to etermine the zeroth, first, secon, thir an fourth approximations of f (x + h ) where x = an h =.. Compare these with the exact solution. Generate answers correct to four ecimal places Given the function f(x) = x + x 3 / x / 1 use a Taylor series expansion to etermine the zeroth, first, secon, thir an fourth approximations of f (x + h ) where x = an h =.8. Compare these with the exact solution by computing percentage errors. Generate answers correct to four ecimal places Given the function f(x) = sin (x) use a Taylor series expansion to etermine the fifth approximation of f (x + h ) where x = an h =.2 raians. Compare your answer with the true value. Generate answers correct to four ecimal places Given the function f(x) = 3 x 2-6 x. + 9, use a Taylor series expansion to etermine the zeroth, first, secon, thir an fourth approximations of f (x + h ) whereo x = 3 an h = 1. Compare these with the exact solution by computing percentage errors. Generate answers correct to four ecimal places.
AN INTRODUCTION TO NUMERICAL METHODS USING MATHCAD. Mathcad Release 14. Khyruddin Akbar Ansari, Ph.D., P.E.
AN INTRODUCTION TO NUMERICAL METHODS USING MATHCAD Mathca Release 14 Khyruin Akbar Ansari, Ph.D., P.E. Professor of Mechanical Engineering School of Engineering an Applie Science Gonzaga University SDC
More informationTAYLOR S POLYNOMIAL APPROXIMATION FOR FUNCTIONS
MISN-0-4 TAYLOR S POLYNOMIAL APPROXIMATION FOR FUNCTIONS f(x ± ) = f(x) ± f ' (x) + f '' (x) 2 ±... 1! 2! = 1.000 ± 0.100 + 0.005 ±... TAYLOR S POLYNOMIAL APPROXIMATION FOR FUNCTIONS by Peter Signell 1.
More informationOptimization of Geometries by Energy Minimization
Optimization of Geometries by Energy Minimization by Tracy P. Hamilton Department of Chemistry University of Alabama at Birmingham Birmingham, AL 3594-140 hamilton@uab.eu Copyright Tracy P. Hamilton, 1997.
More informationJUST THE MATHS UNIT NUMBER DIFFERENTIATION 2 (Rates of change) A.J.Hobson
JUST THE MATHS UNIT NUMBER 10.2 DIFFERENTIATION 2 (Rates of change) by A.J.Hobson 10.2.1 Introuction 10.2.2 Average rates of change 10.2.3 Instantaneous rates of change 10.2.4 Derivatives 10.2.5 Exercises
More informationAN INTRODUCTION TO NUMERICAL METHODS USING MATHCAD. Mathcad Release 14. Khyruddin Akbar Ansari, Ph.D., P.E.
AN INTRODUCTION TO NUMERICAL METHODS USING MATHCAD Mathcad Release 14 Khyruddin Akbar Ansari, Ph.D., P.E. Professor of Mechanical Engineering School of Engineering and Applied Science Gonzaga University
More informationSolutions to MATH 271 Test #3H
Solutions to MATH 71 Test #3H This is the :4 class s version of the test. See pages 4 7 for the 4:4 class s. (1) (5 points) Let a k = ( 1)k. Is a k increasing? Decreasing? Boune above? Boune k below? Convergant
More informationThe derivative of a function f(x) is another function, defined in terms of a limiting expression: f(x + δx) f(x)
Y. D. Chong (2016) MH2801: Complex Methos for the Sciences 1. Derivatives The erivative of a function f(x) is another function, efine in terms of a limiting expression: f (x) f (x) lim x δx 0 f(x + δx)
More informationThe Principle of Least Action
Chapter 7. The Principle of Least Action 7.1 Force Methos vs. Energy Methos We have so far stuie two istinct ways of analyzing physics problems: force methos, basically consisting of the application of
More informationSurvey Sampling. 1 Design-based Inference. Kosuke Imai Department of Politics, Princeton University. February 19, 2013
Survey Sampling Kosuke Imai Department of Politics, Princeton University February 19, 2013 Survey sampling is one of the most commonly use ata collection methos for social scientists. We begin by escribing
More informationDifferentiation ( , 9.5)
Chapter 2 Differentiation (8.1 8.3, 9.5) 2.1 Rate of Change (8.2.1 5) Recall that the equation of a straight line can be written as y = mx + c, where m is the slope or graient of the line, an c is the
More informationLagrangian and Hamiltonian Mechanics
Lagrangian an Hamiltonian Mechanics.G. Simpson, Ph.. epartment of Physical Sciences an Engineering Prince George s Community College ecember 5, 007 Introuction In this course we have been stuying classical
More informationLectures - Week 10 Introduction to Ordinary Differential Equations (ODES) First Order Linear ODEs
Lectures - Week 10 Introuction to Orinary Differential Equations (ODES) First Orer Linear ODEs When stuying ODEs we are consiering functions of one inepenent variable, e.g., f(x), where x is the inepenent
More informationECE 422 Power System Operations & Planning 7 Transient Stability
ECE 4 Power System Operations & Planning 7 Transient Stability Spring 5 Instructor: Kai Sun References Saaat s Chapter.5 ~. EPRI Tutorial s Chapter 7 Kunur s Chapter 3 Transient Stability The ability of
More informationSingle Variable Calculus Warnings
Single Variable Calculus Warnings These notes highlight number of common, but serious, first year calculus errors. Warning. The formula g(x) = g(x) is vali only uner the hypothesis g(x). Discussion. In
More informationLinear and quadratic approximation
Linear an quaratic approximation November 11, 2013 Definition: Suppose f is a function that is ifferentiable on an interval I containing the point a. The linear approximation to f at a is the linear function
More information1 dx. where is a large constant, i.e., 1, (7.6) and Px is of the order of unity. Indeed, if px is given by (7.5), the inequality (7.
Lectures Nine an Ten The WKB Approximation The WKB metho is a powerful tool to obtain solutions for many physical problems It is generally applicable to problems of wave propagation in which the frequency
More informationChapter 2 Lagrangian Modeling
Chapter 2 Lagrangian Moeling The basic laws of physics are use to moel every system whether it is electrical, mechanical, hyraulic, or any other energy omain. In mechanics, Newton s laws of motion provie
More informationMATH , 06 Differential Equations Section 03: MWF 1:00pm-1:50pm McLaury 306 Section 06: MWF 3:00pm-3:50pm EEP 208
MATH 321-03, 06 Differential Equations Section 03: MWF 1:00pm-1:50pm McLaury 306 Section 06: MWF 3:00pm-3:50pm EEP 208 Instructor: Brent Deschamp Email: brent.eschamp@ssmt.eu Office: McLaury 316B Phone:
More informationELEC3114 Control Systems 1
ELEC34 Control Systems Linear Systems - Moelling - Some Issues Session 2, 2007 Introuction Linear systems may be represente in a number of ifferent ways. Figure shows the relationship between various representations.
More informationMath 342 Partial Differential Equations «Viktor Grigoryan
Math 342 Partial Differential Equations «Viktor Grigoryan 6 Wave equation: solution In this lecture we will solve the wave equation on the entire real line x R. This correspons to a string of infinite
More informationLinear First-Order Equations
5 Linear First-Orer Equations Linear first-orer ifferential equations make up another important class of ifferential equations that commonly arise in applications an are relatively easy to solve (in theory)
More informationECEn 621 Computer Arithmetic. Method Comparisons
ECEn 61 Computer Arithmetic Chapter 7: Iterative Approximation Slie #1 Metho Comparisons Digit Recurrence Metho Computes Multiplication Division/Square Root Log/Exp Operations Use Shifting Aition Simple
More information2Algebraic ONLINE PAGE PROOFS. foundations
Algebraic founations. Kick off with CAS. Algebraic skills.3 Pascal s triangle an binomial expansions.4 The binomial theorem.5 Sets of real numbers.6 Surs.7 Review . Kick off with CAS Playing lotto Using
More informationExamining Geometric Integration for Propagating Orbit Trajectories with Non-Conservative Forcing
Examining Geometric Integration for Propagating Orbit Trajectories with Non-Conservative Forcing Course Project for CDS 05 - Geometric Mechanics John M. Carson III California Institute of Technology June
More informationCalculus of Variations
16.323 Lecture 5 Calculus of Variations Calculus of Variations Most books cover this material well, but Kirk Chapter 4 oes a particularly nice job. x(t) x* x*+ αδx (1) x*- αδx (1) αδx (1) αδx (1) t f t
More informationSYNCHRONOUS SEQUENTIAL CIRCUITS
CHAPTER SYNCHRONOUS SEUENTIAL CIRCUITS Registers an counters, two very common synchronous sequential circuits, are introuce in this chapter. Register is a igital circuit for storing information. Contents
More informationA Weak First Digit Law for a Class of Sequences
International Mathematical Forum, Vol. 11, 2016, no. 15, 67-702 HIKARI Lt, www.m-hikari.com http://x.oi.org/10.1288/imf.2016.6562 A Weak First Digit Law for a Class of Sequences M. A. Nyblom School of
More information3.2 Differentiability
Section 3 Differentiability 09 3 Differentiability What you will learn about How f (a) Might Fail to Eist Differentiability Implies Local Linearity Numerical Derivatives on a Calculator Differentiability
More informationMore from Lesson 6 The Limit Definition of the Derivative and Rules for Finding Derivatives.
Math 1314 ONLINE More from Lesson 6 The Limit Definition of the Derivative an Rules for Fining Derivatives Eample 4: Use the Four-Step Process for fining the erivative of the function Then fin f (1) f(
More informationNew Statistical Test for Quality Control in High Dimension Data Set
International Journal of Applie Engineering Research ISSN 973-456 Volume, Number 6 (7) pp. 64-649 New Statistical Test for Quality Control in High Dimension Data Set Shamshuritawati Sharif, Suzilah Ismail
More information1 The Derivative of ln(x)
Monay, December 3, 2007 The Derivative of ln() 1 The Derivative of ln() The first term or semester of most calculus courses will inclue the it efinition of the erivative an will work out, long han, a number
More informationDerivative of a Constant Multiple of a Function Theorem: If f is a differentiable function and if c is a constant, then
Bob Brown Math 51 Calculus 1 Chapter 3, Section Complete 1 Review of the Limit Definition of the Derivative Write the it efinition of the erivative function: f () Derivative of a Constant Multiple of a
More informationYORK UNIVERSITY. Faculty of Science Department of Mathematics and Statistics. MATH A Test #2. June 25, 2014 SOLUTIONS
YORK UNIVERSITY Faculty of Science Department of Mathematics an Statistics MATH 505 6.00 A Test # June 5, 04 SOLUTIONS Family Name (print): Given Name: Stuent No: Signature: INSTRUCTIONS:. Please write
More informationModule 2. DC Circuit. Version 2 EE IIT, Kharagpur
Moule 2 DC Circuit Lesson 9 Analysis of c resistive network in presence of one non-linear element Objectives To unerstan the volt (V ) ampere ( A ) characteristics of linear an nonlinear elements. Concept
More informationLecture 2 Lagrangian formulation of classical mechanics Mechanics
Lecture Lagrangian formulation of classical mechanics 70.00 Mechanics Principle of stationary action MATH-GA To specify a motion uniquely in classical mechanics, it suffices to give, at some time t 0,
More informationTIME-DELAY ESTIMATION USING FARROW-BASED FRACTIONAL-DELAY FIR FILTERS: FILTER APPROXIMATION VS. ESTIMATION ERRORS
TIME-DEAY ESTIMATION USING FARROW-BASED FRACTIONA-DEAY FIR FITERS: FITER APPROXIMATION VS. ESTIMATION ERRORS Mattias Olsson, Håkan Johansson, an Per öwenborg Div. of Electronic Systems, Dept. of Electrical
More informationTable of Common Derivatives By David Abraham
Prouct an Quotient Rules: Table of Common Derivatives By Davi Abraham [ f ( g( ] = [ f ( ] g( + f ( [ g( ] f ( = g( [ f ( ] g( g( f ( [ g( ] Trigonometric Functions: sin( = cos( cos( = sin( tan( = sec
More informationAn inductance lookup table application for analysis of reluctance stepper motor model
ARCHIVES OF ELECTRICAL ENGINEERING VOL. 60(), pp. 5- (0) DOI 0.478/ v07-0-000-y An inuctance lookup table application for analysis of reluctance stepper motor moel JAKUB BERNAT, JAKUB KOŁOTA, SŁAWOMIR
More information6 Wave equation in spherical polar coordinates
6 Wave equation in spherical polar coorinates We now look at solving problems involving the Laplacian in spherical polar coorinates. The angular epenence of the solutions will be escribe by spherical harmonics.
More informationFall 2016: Calculus I Final
Answer the questions in the spaces provie on the question sheets. If you run out of room for an answer, continue on the back of the page. NO calculators or other electronic evices, books or notes are allowe
More informationEuler equations for multiple integrals
Euler equations for multiple integrals January 22, 2013 Contents 1 Reminer of multivariable calculus 2 1.1 Vector ifferentiation......................... 2 1.2 Matrix ifferentiation........................
More informationd dx But have you ever seen a derivation of these results? We ll prove the first result below. cos h 1
Lecture 5 Some ifferentiation rules Trigonometric functions (Relevant section from Stewart, Seventh Eition: Section 3.3) You all know that sin = cos cos = sin. () But have you ever seen a erivation of
More informationThe total derivative. Chapter Lagrangian and Eulerian approaches
Chapter 5 The total erivative 51 Lagrangian an Eulerian approaches The representation of a flui through scalar or vector fiels means that each physical quantity uner consieration is escribe as a function
More informationThe Exact Form and General Integrating Factors
7 The Exact Form an General Integrating Factors In the previous chapters, we ve seen how separable an linear ifferential equations can be solve using methos for converting them to forms that can be easily
More informationTransmission Line Matrix (TLM) network analogues of reversible trapping processes Part B: scaling and consistency
Transmission Line Matrix (TLM network analogues of reversible trapping processes Part B: scaling an consistency Donar e Cogan * ANC Eucation, 308-310.A. De Mel Mawatha, Colombo 3, Sri Lanka * onarecogan@gmail.com
More informationChapter 4. Electrostatics of Macroscopic Media
Chapter 4. Electrostatics of Macroscopic Meia 4.1 Multipole Expansion Approximate potentials at large istances 3 x' x' (x') x x' x x Fig 4.1 We consier the potential in the far-fiel region (see Fig. 4.1
More informationModule FP2. Further Pure 2. Cambridge University Press Further Pure 2 and 3 Hugh Neill and Douglas Quadling Excerpt More information
5548993 - Further Pure an 3 Moule FP Further Pure 5548993 - Further Pure an 3 Differentiating inverse trigonometric functions Throughout the course you have graually been increasing the number of functions
More informationLeast-Squares Regression on Sparse Spaces
Least-Squares Regression on Sparse Spaces Yuri Grinberg, Mahi Milani Far, Joelle Pineau School of Computer Science McGill University Montreal, Canaa {ygrinb,mmilan1,jpineau}@cs.mcgill.ca 1 Introuction
More informationOutline. MS121: IT Mathematics. Differentiation Rules for Differentiation: Part 1. Outline. Dublin City University 4 The Quotient Rule
MS2: IT Mathematics Differentiation Rules for Differentiation: Part John Carroll School of Mathematical Sciences Dublin City University Pattern Observe You may have notice the following pattern when we
More informationPolynomial Inclusion Functions
Polynomial Inclusion Functions E. e Weert, E. van Kampen, Q. P. Chu, an J. A. Muler Delft University of Technology, Faculty of Aerospace Engineering, Control an Simulation Division E.eWeert@TUDelft.nl
More informationLINEAR DIFFERENTIAL EQUATIONS OF ORDER 1. where a(x) and b(x) are functions. Observe that this class of equations includes equations of the form
LINEAR DIFFERENTIAL EQUATIONS OF ORDER 1 We consier ifferential equations of the form y + a()y = b(), (1) y( 0 ) = y 0, where a() an b() are functions. Observe that this class of equations inclues equations
More informationAverage value of position for the anharmonic oscillator: Classical versus quantum results
verage value of position for the anharmonic oscillator: Classical versus quantum results R. W. Robinett Department of Physics, The Pennsylvania State University, University Park, Pennsylvania 682 Receive
More informationWe G Model Reduction Approaches for Solution of Wave Equations for Multiple Frequencies
We G15 5 Moel Reuction Approaches for Solution of Wave Equations for Multiple Frequencies M.Y. Zaslavsky (Schlumberger-Doll Research Center), R.F. Remis* (Delft University) & V.L. Druskin (Schlumberger-Doll
More informationMath Chapter 2 Essentials of Calculus by James Stewart Prepared by Jason Gaddis
Math 231 - Chapter 2 Essentials of Calculus by James Stewart Prepare by Jason Gais Chapter 2 - Derivatives 21 - Derivatives an Rates of Change Definition A tangent to a curve is a line that intersects
More informationSection 7.1: Integration by Parts
Section 7.1: Integration by Parts 1. Introuction to Integration Techniques Unlike ifferentiation where there are a large number of rules which allow you (in principle) to ifferentiate any function, the
More information11.7. Implicit Differentiation. Introduction. Prerequisites. Learning Outcomes
Implicit Differentiation 11.7 Introuction This Section introuces implicit ifferentiation which is use to ifferentiate functions expresse in implicit form (where the variables are foun together). Examples
More informationConstruction of the Electronic Radial Wave Functions and Probability Distributions of Hydrogen-like Systems
Construction of the Electronic Raial Wave Functions an Probability Distributions of Hyrogen-like Systems Thomas S. Kuntzleman, Department of Chemistry Spring Arbor University, Spring Arbor MI 498 tkuntzle@arbor.eu
More informationModeling time-varying storage components in PSpice
Moeling time-varying storage components in PSpice Dalibor Biolek, Zenek Kolka, Viera Biolkova Dept. of EE, FMT, University of Defence Brno, Czech Republic Dept. of Microelectronics/Raioelectronics, FEEC,
More informationThermal runaway during blocking
Thermal runaway uring blocking CES_stable CES ICES_stable ICES k 6.5 ma 13 6. 12 5.5 11 5. 1 4.5 9 4. 8 3.5 7 3. 6 2.5 5 2. 4 1.5 3 1. 2.5 1. 6 12 18 24 3 36 s Thermal runaway uring blocking Application
More informationMATH2231-Differentiation (2)
-Differentiation () The Beginnings of Calculus The prime occasion from which arose my iscovery of the metho of the Characteristic Triangle, an other things of the same sort, happene at a time when I ha
More informationState-Space Model for a Multi-Machine System
State-Space Moel for a Multi-Machine System These notes parallel section.4 in the text. We are ealing with classically moele machines (IEEE Type.), constant impeance loas, an a network reuce to its internal
More informationMathcad Lecture #5 In-class Worksheet Plotting and Calculus
Mathca Lecture #5 In-class Worksheet Plotting an Calculus At the en of this lecture, you shoul be able to: graph expressions, functions, an matrices of ata format graphs with titles, legens, log scales,
More informationx f(x) x f(x) approaching 1 approaching 0.5 approaching 1 approaching 0.
Engineering Mathematics 2 26 February 2014 Limits of functions Consier the function 1 f() = 1. The omain of this function is R + \ {1}. The function is not efine at 1. What happens when is close to 1?
More informationTutorial on Maximum Likelyhood Estimation: Parametric Density Estimation
Tutorial on Maximum Likelyhoo Estimation: Parametric Density Estimation Suhir B Kylasa 03/13/2014 1 Motivation Suppose one wishes to etermine just how biase an unfair coin is. Call the probability of tossing
More informationSolutions to the Exercises of Chapter 9
9A. Vectors an Forces Solutions to the Exercises of Chapter 9. F = 5 sin 5.9 an F = 5 cos 5 4.8.. a. By the Pythagorean theorem, the length of the vector from to (, ) is + = 5. So the magnitue of the force
More informationExam 2 Answers Math , Fall log x dx = x log x x + C. log u du = 1 3
Exam Answers Math -, Fall 7. Show, using any metho you like, that log x = x log x x + C. Answer: (x log x x+c) = x x + log x + = log x. Thus log x = x log x x+c.. Compute these. Remember to put boxes aroun
More informationx f(x) x f(x) approaching 1 approaching 0.5 approaching 1 approaching 0.
Engineering Mathematics 2 26 February 2014 Limits of functions Consier the function 1 f() = 1. The omain of this function is R + \ {1}. The function is not efine at 1. What happens when is close to 1?
More informationLie symmetry and Mei conservation law of continuum system
Chin. Phys. B Vol. 20, No. 2 20 020 Lie symmetry an Mei conservation law of continuum system Shi Shen-Yang an Fu Jing-Li Department of Physics, Zhejiang Sci-Tech University, Hangzhou 3008, China Receive
More informationImplicit Differentiation
Implicit Differentiation Implicit Differentiation Using the Chain Rule In the previous section we focuse on the erivatives of composites an saw that THEOREM 20 (Chain Rule) Suppose that u = g(x) is ifferentiable
More informationCalculus Math Fall 2012 (Cohen) Lecture Notes
Calculus Math 70.200 Fall 202 (Cohen) Lecture Notes For the purposes of this class, we will regar calculus as the stuy of limits an limit processes. Without yet formally recalling the efinition of a limit,
More informationC6-1 Differentiation 2
C6-1 Differentiation 2 the erivatives of sin, cos, a, e an ln Pre-requisites: M5-4 (Raians), C5-7 (General Calculus) Estimate time: 2 hours Summary Lea-In Learn Solve Revise Answers Summary The erivative
More informationQubit channels that achieve capacity with two states
Qubit channels that achieve capacity with two states Dominic W. Berry Department of Physics, The University of Queenslan, Brisbane, Queenslan 4072, Australia Receive 22 December 2004; publishe 22 March
More informationWITH high operating frequencies and scaled geometries,
IEEE TRANSACTIONS ON CIRCUITS AND SYSTEMS II: EXPRESS BRIEFS, VOL. 56, NO. 7, JULY 2009 585 Inuctance Moel of Interigitate Power an Groun Distribution Networks Renatas Jakushokas, Stuent Member, IEEE,
More information'HVLJQ &RQVLGHUDWLRQ LQ 0DWHULDO 6HOHFWLRQ 'HVLJQ 6HQVLWLYLW\,1752'8&7,21
Large amping in a structural material may be either esirable or unesirable, epening on the engineering application at han. For example, amping is a esirable property to the esigner concerne with limiting
More informationFebruary 21 Math 1190 sec. 63 Spring 2017
February 21 Math 1190 sec. 63 Spring 2017 Chapter 2: Derivatives Let s recall the efinitions an erivative rules we have so far: Let s assume that y = f (x) is a function with c in it s omain. The erivative
More informationImplicit Differentiation
Implicit Differentiation Thus far, the functions we have been concerne with have been efine explicitly. A function is efine explicitly if the output is given irectly in terms of the input. For instance,
More informationScott E. Grasman 1, Zaki Sari 2 and Tewfik Sari 3
RAIRO Operations Research RAIRO Oper. Res. 41 (27) 455 464 DOI: 1.151/ro:2731 NEWSVENDOR SOLUTIONS WITH GENERAL RANDOM YIELD DISTRIBUTIONS Scott E. Grasman 1, Zaki Sari 2 an Tewfik Sari 3 Abstract. Most
More informationFinal Exam Study Guide and Practice Problems Solutions
Final Exam Stuy Guie an Practice Problems Solutions Note: These problems are just some of the types of problems that might appear on the exam. However, to fully prepare for the exam, in aition to making
More informationAdaptive Gain-Scheduled H Control of Linear Parameter-Varying Systems with Time-Delayed Elements
Aaptive Gain-Scheule H Control of Linear Parameter-Varying Systems with ime-delaye Elements Yoshihiko Miyasato he Institute of Statistical Mathematics 4-6-7 Minami-Azabu, Minato-ku, okyo 6-8569, Japan
More information18 EVEN MORE CALCULUS
8 EVEN MORE CALCULUS Chapter 8 Even More Calculus Objectives After stuing this chapter you shoul be able to ifferentiate an integrate basic trigonometric functions; unerstan how to calculate rates of change;
More informationA Comparison between a Conventional Power System Stabilizer (PSS) and Novel PSS Based on Feedback Linearization Technique
J. Basic. Appl. Sci. Res., ()9-99,, TextRoa Publication ISSN 9-434 Journal of Basic an Applie Scientific Research www.textroa.com A Comparison between a Conventional Power System Stabilizer (PSS) an Novel
More informationThe Sokhotski-Plemelj Formula
hysics 24 Winter 207 The Sokhotski-lemelj Formula. The Sokhotski-lemelj formula The Sokhotski-lemelj formula is a relation between the following generalize functions (also calle istributions), ±iǫ = iπ(),
More informationDesigning of Acceptance Double Sampling Plan for Life Test Based on Percentiles of Exponentiated Rayleigh Distribution
International Journal of Statistics an Systems ISSN 973-675 Volume, Number 3 (7), pp. 475-484 Research Inia Publications http://www.ripublication.com Designing of Acceptance Double Sampling Plan for Life
More informationSeparation of Variables
Physics 342 Lecture 1 Separation of Variables Lecture 1 Physics 342 Quantum Mechanics I Monay, January 25th, 2010 There are three basic mathematical tools we nee, an then we can begin working on the physical
More informationEquations of lines in
Roberto s Notes on Linear Algebra Chapter 6: Lines, planes an other straight objects Section 1 Equations of lines in What ou nee to know alrea: The ot prouct. The corresponence between equations an graphs.
More informationChapter 2 Derivatives
Chapter Derivatives Section. An Intuitive Introuction to Derivatives Consier a function: Slope function: Derivative, f ' For each, the slope of f is the height of f ' Where f has a horizontal tangent line,
More informationThe Chain Rule. d dx x(t) dx. dt (t)
The Chain Rule The Problem You alreay routinely use the one imensional chain rule t f xt = f x xt x t t in oing computations like t sint2 = cost 2 2t In this example, fx = sinx an xt = t 2. We now generalize
More informationLecture Introduction. 2 Examples of Measure Concentration. 3 The Johnson-Lindenstrauss Lemma. CS-621 Theory Gems November 28, 2012
CS-6 Theory Gems November 8, 0 Lecture Lecturer: Alesaner Mąry Scribes: Alhussein Fawzi, Dorina Thanou Introuction Toay, we will briefly iscuss an important technique in probability theory measure concentration
More information1 Lecture 13: The derivative as a function.
1 Lecture 13: Te erivative as a function. 1.1 Outline Definition of te erivative as a function. efinitions of ifferentiability. Power rule, erivative te exponential function Derivative of a sum an a multiple
More information4. Important theorems in quantum mechanics
TFY4215 Kjemisk fysikk og kvantemekanikk - Tillegg 4 1 TILLEGG 4 4. Important theorems in quantum mechanics Before attacking three-imensional potentials in the next chapter, we shall in chapter 4 of this
More informationHyperbolic Systems of Equations Posed on Erroneous Curved Domains
Hyperbolic Systems of Equations Pose on Erroneous Curve Domains Jan Norström a, Samira Nikkar b a Department of Mathematics, Computational Mathematics, Linköping University, SE-58 83 Linköping, Sween (
More informationLaplace s Equation in Cylindrical Coordinates and Bessel s Equation (II)
Laplace s Equation in Cylinrical Coorinates an Bessel s Equation (II Qualitative properties of Bessel functions of first an secon kin In the last lecture we foun the expression for the general solution
More informationMULTIFRACTAL NETWORK GENERATORS
MULTIFRACTAL NETWORK GENERATORS AUSTIN R. BENSON, CARLOS RIQUELME, SVEN P. SCHMIT (0) Abstract. Generating ranom graphs to moel networks has a rich history. In this paper, we explore a recent generative
More informationQ(s, t) = S M = S M [ G 1 (t) G 2 (t) G 3 1(t) G 4 (t) ] T
Curves an Surfaces: Parametric Bicubic Surfaces - Intro Surfaces are generalizations of curves Use s in place of t in parametric equation: Q(s) = S M G where S equivalent to T in Q(t) = T M G If G is parameterize
More informationAn Analytical Expression of the Probability of Error for Relaying with Decode-and-forward
An Analytical Expression of the Probability of Error for Relaying with Decoe-an-forwar Alexanre Graell i Amat an Ingmar Lan Department of Electronics, Institut TELECOM-TELECOM Bretagne, Brest, France Email:
More informationPARALLEL-PLATE CAPACITATOR
Physics Department Electric an Magnetism Laboratory PARALLEL-PLATE CAPACITATOR 1. Goal. The goal of this practice is the stuy of the electric fiel an electric potential insie a parallelplate capacitor.
More informationFurther Differentiation and Applications
Avance Higher Notes (Unit ) Prerequisites: Inverse function property; prouct, quotient an chain rules; inflexion points. Maths Applications: Concavity; ifferentiability. Real-Worl Applications: Particle
More informationIMPLICIT DIFFERENTIATION
IMPLICIT DIFFERENTIATION CALCULUS 3 INU0115/515 (MATHS 2) Dr Arian Jannetta MIMA CMath FRAS Implicit Differentiation 1/ 11 Arian Jannetta Explicit an implicit functions Explicit functions An explicit function
More informationA PAC-Bayesian Approach to Spectrally-Normalized Margin Bounds for Neural Networks
A PAC-Bayesian Approach to Spectrally-Normalize Margin Bouns for Neural Networks Behnam Neyshabur, Srinah Bhojanapalli, Davi McAllester, Nathan Srebro Toyota Technological Institute at Chicago {bneyshabur,
More informationThe Press-Schechter mass function
The Press-Schechter mass function To state the obvious: It is important to relate our theories to what we can observe. We have looke at linear perturbation theory, an we have consiere a simple moel for
More information