Lecture 22 Appendix B (More on Legendre Polynomials and Associated Legendre functions)
|
|
- Meagan Gilmore
- 5 years ago
- Views:
Transcription
1 Lecture Appendix B (More on Legendre Polynomials and Associated Legendre functions) Ex.7: Let's use Mathematica to solve the equation and then verify orthogonality. First In[]:= Out[]= DSolve y'' x n^y x, y x, x y x C Cos nx C Sin nx y x C Cos nx C Sin nx As - expected the sines and cosines. Then consider the pair-wise integrals (the dot products) In[]:= Out[]= In[]:= Integrate Sin mx Sin nx, x,, ncos n Sin m mcos m Sin n m n ncos n Sin m mcos m Sin n m n FullSimplify, Assumptions m, n Integers Out[]= Interesting for m n, but how about m = n In[]:= Out[]= Integrate Sin mx Sin mx, x,, Sin m m Sin m m In[]:= Out[]= FullSimplify, Assumptions m Integers In[6]:= FullSimplify Integrate Cos mx Cos nx, x,,, Assumptions m, n Integers Out[6]= In[7]:= Out[7]= FullSimplify Integrate Cos mx Cos mx, x,,, Assumptions m Integers Finally
2 Lec App B.nb In[]:= Out[]= FullSimplify Integrate Sin mx Cos nx, x,,, Assumptions m, n Integers In[]:= FullSimplify Integrate Sin mx Cos mx, x,,, Assumptions m Integers Out[]= So always get zero here. Ex.7: Now consider the integrals with the Legendre polynomials In[]:= Integrate x^mlegendrep l, x, x,, Out[]= x m LegendreP l, x x Can't do the generic case. Make a table In[]:= TableForm Table m, l, Integrate x^mlegendrep l, x, x,,, m,,, l,, Out[]//TableForm= So, as expected, the integral is non-zero only when l m and both are either even or odd. The same structure for polynomials is
3 Lec App B.nb In[]:= TableForm Table m, l, Integrate LegendreP m, x LegendreP l, x, x,,, m,,, l,, Out[]//TableForm= So non-zero only for l = m. Ex.: Now expand a function with Legendre polynomials. Consider the function In[]:= In[]:= Out[]= F x : Sign x Plot F x, x,,, AxesLabel x, "F",. F..... x.. The expansion coefficients are given by
4 Lec App B.nb In[]:= In[6]:= c m : m Integrate LegendreP m, x F x, x,, Out[6]//TableForm= TableForm Table m, c m, m,, As expected, only the odd terms are non-zero. We can compare the values to our analytic results In[7]:= TableForm Table m, ^mgamma m m, m,, 7 Gamma m Gamma Out[7]//TableForm= Clearly in agreement. Next look at the truncated sums In[]:= In[]:= Out[]= FA N, x : Sum c m LegendreP m, x, m,, N FA, x x 7 6 x x
5 Lec App B.nb In[]:= Out[]= Not so good Plot, x,,, AxesLabel x, "F ", F x. In[]:= In[]:= Out[]= FA, x ; Plot, x,,, AxesLabel x, "F ", F x. Better In[]:= FA, x ;
6 6 Lec App B.nb In[]:= Out[]= Plot, x,,, AxesLabel x, "F ", F.... x OK, except for the issues at the endpoints. Ex.: 6 Consider the following function (singular at the origin) In[]:= In[6]:= Out[6]= F x : UnitStep x Log x ^ Plot F x, x,,, AxesLabel x, "F", LabelStyle Large, PlotStyle Thick, Exclusions None, PlotRange, F x Expand in Legendre polynomials In[7]:= c m : m Integrate LegendreP m, x F x, x,,
7 Lec App B.nb 7 In[]:= Out[]//TableForm= TableForm Table m, c m, m,, These results agree with the analytic ones - but it is clearly easier to use Mathematica here. In[]:= In[]:= In[]:= Out[]= FA N, x : Sum c m LegendreP m, x, m,, N FA, x ; Plot, x,,, AxesLabel x, "F ", F.... x Clearly need more terms, as expected due to the singular behavior. Ex.: Here we consider the polynomial In[]:= In[]:= F x : 7x^ x c m : m Integrate LegendreP m, x F x, x,,
8 Lec App B.nb In[]:= Out[]//TableForm= TableForm Table m, c m, m,, 6 7 All zero above as expected. In[]:= In[6]:= Out[6]= In[7]:= FA N, x : Sum c m LegendreP m, x, m,, N FA, x x x x x Simplify Out[7]= x 7x The desired polynomial. Ex.: Here we consider the polynomial In[]:= In[]:= In[]:= F x : x x^ c m : m Integrate LegendreP m, x F x, x,, TableForm Table m, c m, m,, Out[]//TableForm= 6 7 All zero above as expected, and only odd.
9 Lec App B.nb In[]:= FA N, x : Sum c m LegendreP m, x, m,, N In[]:= Out[]= In[]:= FA, x x x x Simplify Out[]= x x The desired polynomial. Ex.: Here we consider the function In[]:= F x : Abs x The coefficients in the expansion are In[]:= In[6]:= c m : m Integrate LegendreP m, x F x, x,, TableForm Table m, c m, m,, Out[6]//TableForm= Only the even terms are non-zero as expected. So the best fit quadratic polynomial is In[7]:= In[]:= Out[]= In[]:= Out[]= FA N, x : Sum c m LegendreP m, x, m,, N FA, x 6 x Simplify 6 x Make a comparison
10 Lec App B.nb In[]:= Out[]= Plot, Abs x, x,,, AxesLabel x, "F", F x Clearly a pretty good fit, but misses the details. Ex.: Now we want to consider the Associated Legendre function In[]:= LegendreP,, Cos Out[]= Cos Cos 7Cos By inspection this is what we obtained analytically except for the differing minus sign convention in Mathematica.
Mathematica examples relevant to Legendre functions
Mathematica eamples relevant to Legendre functions Legendre Polynomials are built in Here is Legendre s equation, and Mathematica recognizes as being solved by Legendre polynomials (LegendreP) and the
More informationfirst define colors for future graphics red RGBColor 1, 0, 0 ; green RGBColor 0, 1, 0 ; blue RGBColor 0, 0, 1 ; black RGBColor 0, 0, 0 ;
In[1]:= note: to simplifynotations all periodic functions of x are expected to have a period of 2 Pi, as Ch. 11.1 by KR. If a function has a period "2L" as in his later sections, one can always switch
More informationTOPIC 3. Taylor polynomials. Mathematica code. Here is some basic mathematica code for plotting functions.
TOPIC 3 Taylor polynomials Main ideas. Linear approximating functions: Review Approximating polynomials Key formulas: P n (x) =a 0 + a (x x )+ + a n (x x ) n P n (x + x) =a 0 + a ( x)+ + a n ( x) n where
More informationExamples of the Fourier Theorem (Sect. 10.3). The Fourier Theorem: Continuous case.
s of the Fourier Theorem (Sect. 1.3. The Fourier Theorem: Continuous case. : Using the Fourier Theorem. The Fourier Theorem: Piecewise continuous case. : Using the Fourier Theorem. The Fourier Theorem:
More informationPhysics 6303 Lecture 11 September 24, LAST TIME: Cylindrical coordinates, spherical coordinates, and Legendre s equation
Physics 6303 Lecture September 24, 208 LAST TIME: Cylindrical coordinates, spherical coordinates, and Legendre s equation, l l l l l l. Consider problems that are no axisymmetric; i.e., the potential depends
More informationA Library of Functions
LibraryofFunctions.nb 1 A Library of Functions Any study of calculus must start with the study of functions. Functions are fundamental to mathematics. In its everyday use the word function conveys to us
More information14 Fourier analysis. Read: Boas Ch. 7.
14 Fourier analysis Read: Boas Ch. 7. 14.1 Function spaces A function can be thought of as an element of a kind of vector space. After all, a function f(x) is merely a set of numbers, one for each point
More informationA small note on the statistical method of moments for fitting a probability model to data
A small note on the statistical method of moments for fitting a probability model to data by Nasser Abbasi, Nov 16, 2007 Mathematics 502 probability and statistics, CSUF, Fall 2007 f x x Μ 2 2 Σ 2 2 Π
More informationNonhomogeneous Linear Differential Equations with Constant Coefficients - (3.4) Method of Undetermined Coefficients
Nonhomogeneous Linear Differential Equations with Constant Coefficients - (3.4) Method of Undetermined Coefficients Consider an nth-order nonhomogeneous linear differential equation with constant coefficients:
More informationSection 5.2 Series Solution Near Ordinary Point
DE Section 5.2 Series Solution Near Ordinary Point Page 1 of 5 Section 5.2 Series Solution Near Ordinary Point We are interested in second order homogeneous linear differential equations with variable
More informationRolle s Theorem and the Mean Value Theorem. By Tuesday J. Johnson
Rolle s Theorem and the Mean Value Theorem By Tuesday J. Johnson 1 Suggested Review Topics Algebra skills reviews suggested: None Trigonometric skills reviews suggested: None 2 Applications of Differentiation
More informationLecture 4: Series expansions with Special functions
Lecture 4: Series expansions with Special functions 1. Key points 1. Legedre polynomials (Legendre functions) 2. Hermite polynomials(hermite functions) 3. Laguerre polynomials (Laguerre functions) Other
More information5.4 Bessel s Equation. Bessel Functions
SEC 54 Bessel s Equation Bessel Functions J (x) 87 # with y dy>dt, etc, constant A, B, C, D, K, and t 5 HYPERGEOMETRIC ODE At B (t t )(t t ), t t, can be reduced to the hypergeometric equation with independent
More informationMa 530 Power Series II
Ma 530 Power Series II Please note that there is material on power series at Visual Calculus. Some of this material was used as part of the presentation of the topics that follow. Operations on Power Series
More informationVectors in Function Spaces
Jim Lambers MAT 66 Spring Semester 15-16 Lecture 18 Notes These notes correspond to Section 6.3 in the text. Vectors in Function Spaces We begin with some necessary terminology. A vector space V, also
More informationTaylor and Maclaurin Series. Copyright Cengage Learning. All rights reserved.
11.10 Taylor and Maclaurin Series Copyright Cengage Learning. All rights reserved. We start by supposing that f is any function that can be represented by a power series f(x)= c 0 +c 1 (x a)+c 2 (x a)
More informationMathematica for Calculus II (Version 9.0)
Mathematica for Calculus II (Version 9.0) C. G. Melles Mathematics Department United States Naval Academy December 31, 013 Contents 1. Introduction. Volumes of revolution 3. Solving systems of equations
More information1 Solutions in cylindrical coordinates: Bessel functions
1 Solutions in cylindrical coordinates: Bessel functions 1.1 Bessel functions Bessel functions arise as solutions of potential problems in cylindrical coordinates. Laplace s equation in cylindrical coordinates
More informationTAYLOR AND MACLAURIN SERIES
TAYLOR AND MACLAURIN SERIES. Introduction Last time, we were able to represent a certain restricted class of functions as power series. This leads us to the question: can we represent more general functions
More informationLimits at Infinity. Horizontal Asymptotes. Definition (Limits at Infinity) Horizontal Asymptotes
Limits at Infinity If a function f has a domain that is unbounded, that is, one of the endpoints of its domain is ±, we can determine the long term behavior of the function using a it at infinity. Definition
More informationd 1 µ 2 Θ = 0. (4.1) consider first the case of m = 0 where there is no azimuthal dependence on the angle φ.
4 Legendre Functions In order to investigate the solutions of Legendre s differential equation d ( µ ) dθ ] ] + l(l + ) m dµ dµ µ Θ = 0. (4.) consider first the case of m = 0 where there is no azimuthal
More information8.5 Taylor Polynomials and Taylor Series
8.5. TAYLOR POLYNOMIALS AND TAYLOR SERIES 50 8.5 Taylor Polynomials and Taylor Series Motivating Questions In this section, we strive to understand the ideas generated by the following important questions:
More informationLecture 32: Taylor Series and McLaurin series We saw last day that some functions are equal to a power series on part of their domain.
Lecture 32: Taylor Series and McLaurin series We saw last day that some functions are equal to a power series on part of their domain. For example f(x) = 1 1 x = 1 + x + x2 + x 3 + = ln(1 + x) = x x2 2
More information7 PDES, FOURIER SERIES AND TRANSFORMS Last Updated: July 16, 2012
Problem List 7.1 Fourier series expansion of absolute value function 7.2 Fourier series expansion of step function 7.3 Orthogonality of functions 7.4 Fourier transform of sinusoidal pulse 7.5 Introducing
More informationMath 205, Winter 2018, Assignment 3
Math 05, Winter 08, Assignment 3 Solutions. Calculate the following integrals. Show your steps and reasoning. () a) ( + + )e = ( + + )e ( + )e = ( + + )e ( + )e + e = ( )e + e + c = ( + )e + c This uses
More informationAnalysis II: Basic knowledge of real analysis: Part V, Power Series, Differentiation, and Taylor Series
.... Analysis II: Basic knowledge of real analysis: Part V, Power Series, Differentiation, and Taylor Series Kenichi Maruno Department of Mathematics, The University of Texas - Pan American March 4, 20
More informationPhysics 229& 100 Homework #1 Name: Nasser Abbasi
Physics 229& 100 Homework #1 Name: Nasser Abbasi (converted to 6.0) 1. Practice in transcribing expressions into Mathematica syntax a) Find the determinant of this matrix: In[94]:= a = {{1, 2, 3, 4}, {1,
More informationBessel s and legendre s equations
Chapter 12 Bessel s and legendre s equations 12.1 Introduction Many linear differential equations having variable coefficients cannot be solved by usual methods and we need to employ series solution method
More informationFourier Sin and Cos Series and Least Squares Convergence
Fourier and east Squares Convergence James K. Peterson Department of Biological Sciences and Department of Mathematical Sciences Clemson University May 7, 28 Outline et s look at the original Fourier sin
More informationProperties of a Taylor Polynomial
3.4.4: Still Better Approximations: Taylor Polynomials Properties of a Taylor Polynomial Constant: f (x) f (a) Linear: f (x) f (a) + f (a)(x a) Quadratic: f (x) f (a) + f (a)(x a) + 1 2 f (a)(x a) 2 3.4.4:
More informationMath 651 Introduction to Numerical Analysis I Fall SOLUTIONS: Homework Set 1
ath 651 Introduction to Numerical Analysis I Fall 2010 SOLUTIONS: Homework Set 1 1. Consider the polynomial f(x) = x 2 x 2. (a) Find P 1 (x), P 2 (x) and P 3 (x) for f(x) about x 0 = 0. What is the relation
More informationDecember 18, 2017 Section W Nandyalam
Mathematica Gift #11 Problem Complete the following 15 exercises in a Mathematica notebook. You should write the problem in a text cell and show your work below the question. Questions Question 1 Compute
More informationMath 421 Homework 1. Paul Hacking. September 22, 2015
Math 421 Homework 1 Paul Hacking September 22, 2015 (1) Compute the following products of complex numbers. Express your answer in the form x + yi where x and y are real numbers. (a) (2 + i)(5 + 3i) (b)
More informationStudents should read Sections of Rogawski's Calculus [1] for a detailed discussion of the material presented in this section.
Chapter 3 Differentiation ü 3.1 The Derivative Students should read Sections 3.1-3.5 of Rogawski's Calculus [1] for a detailed discussion of the material presented in this section. ü 3.1.1 Slope of Tangent
More informationTwo special equations: Bessel s and Legendre s equations. p Fourier-Bessel and Fourier-Legendre series. p
LECTURE 1 Table of Contents Two special equations: Bessel s and Legendre s equations. p. 259-268. Fourier-Bessel and Fourier-Legendre series. p. 453-460. Boundary value problems in other coordinate system.
More informationMore on Fourier Series
More on Fourier Series R. C. Trinity University Partial Differential Equations Lecture 6.1 New Fourier series from old Recall: Given a function f (x, we can dilate/translate its graph via multiplication/addition,
More informationName: Date: Practice Midterm Exam Sections 1.2, 1.3, , ,
Name: Date: Practice Midterm Exam Sections 1., 1.3,.1-.7, 6.1-6.5, 8.1-8.7 a108 Please develop your one page formula sheet as you try these problems. If you need to look something up, write it down on
More informationFourier-Bessel series
Bessel Series 2.nb Fourier-Bessel series Orthogonality of J 0 Bessel functions This is what the J 0 Bessel function looks like. Plot#BesselJ#0, x', x, 0, 5' - 2 4 6 8 0 2 4 - We see there are zeros of
More informationPHYS 301 HOMEWORK #8
PHYS 301 HOMEWORK #8 Due : 5 April 2017 1. Find the recursion relation and general solution near x = 2 of the differential equation : In this case, the solution will be of the form: y'' - (x - 2) y' +
More informationA Summary of Contour Integration
A Summary of Contour Integration vs 0., 5//08 ' Niels Walet, University of Manchester In this document I will summarise some very simple results of contour integration. The Basics The key word linked to
More informationPower series solutions for 2nd order linear ODE s (not necessarily with constant coefficients) a n z n. n=0
Lecture 22 Power series solutions for 2nd order linear ODE s (not necessarily with constant coefficients) Recall a few facts about power series: a n z n This series in z is centered at z 0. Here z can
More informationExample 1 Which of these functions are polynomials in x? In the case(s) where f is a polynomial,
1. Polynomials A polynomial in x is a function of the form p(x) = a 0 + a 1 x + a 2 x 2 +... a n x n (a n 0, n a non-negative integer) where a 0, a 1, a 2,..., a n are constants. We say that this polynomial
More informationUsing Mathematica to study series (part II)
Using Mathematica to study series (part II) Truncation errors Example of exponential; first consider x>0 Remainder if use only first 3 terms in power series for exponential: PlotExpx1xx ^,x, 0,, PlotStyleThick,
More informationLecture 5: Function Approximation: Taylor Series
1 / 10 Lecture 5: Function Approximation: Taylor Series MAR514 Geoffrey Cowles Department of Fisheries Oceanography School for Marine Science and Technology University of Massachusetts-Dartmouth Better
More informationScientific Computing
2301678 Scientific Computing Chapter 2 Interpolation and Approximation Paisan Nakmahachalasint Paisan.N@chula.ac.th Chapter 2 Interpolation and Approximation p. 1/66 Contents 1. Polynomial interpolation
More informationn=1 ( 2 3 )n (a n ) converges by direct comparison to
. (a) n = a n converges, so we know that a n =. Therefore, for n large enough we know that a n
More informationReview for Exam 2. Review for Exam 2.
Review for Exam 2. 5 or 6 problems. No multiple choice questions. No notes, no books, no calculators. Problems similar to homeworks. Exam covers: Regular-singular points (5.5). Euler differential equation
More informationSUMMATION TECHNIQUES
SUMMATION TECHNIQUES MATH 53, SECTION 55 (VIPUL NAIK) Corresponding material in the book: Scattered around, but the most cutting-edge parts are in Sections 2.8 and 2.9. What students should definitely
More informationswapneel/207
Partial differential equations Swapneel Mahajan www.math.iitb.ac.in/ swapneel/207 1 1 Power series For a real number x 0 and a sequence (a n ) of real numbers, consider the expression a n (x x 0 ) n =
More information1 A complete Fourier series solution
Math 128 Notes 13 In this last set of notes I will try to tie up some loose ends. 1 A complete Fourier series solution First here is an example of the full solution of a pde by Fourier series. Consider
More information1 Boas, problem p.564,
Physics 6C Solutions to Homewor Set # Fall 0 Boas, problem p.564,.- Solve the following differential equations by series and by another elementary method and chec that the results agree: xy = xy +y ()
More informationMath 112 Rahman. Week Taylor Series Suppose the function f has the following power series:
Math Rahman Week 0.8-0.0 Taylor Series Suppose the function f has the following power series: fx) c 0 + c x a) + c x a) + c 3 x a) 3 + c n x a) n. ) Can we figure out what the coefficients are? Yes, yes
More informationThe Solow model - analytical solution, linearization, shooting, relaxation (complete)
The Solow model - analytical solution, linearization, shooting, relaxation (complete) (Quantitative Dynamic Macroeconomics, Lecture Notes, Thomas Steger, University of Leipzig). Solow model: analytical
More informationObjective Mathematics
Multiple choice questions with ONE correct answer : ( Questions No. 1-5 ) 1. If the equation x n = (x + ) is having exactly three distinct real solutions, then exhaustive set of values of 'n' is given
More informationThe Ramsey model - linearization, backward integration, relaxation (complete)
The Ramsey model - linearization, backward integration, relaxation (complete) (Quantitative Dynamic Macroeconomics, Lecture Notes, Thomas Steger, University of Leipzig) Ramsey Model: linearized version
More informationf (x) = k=0 f (0) = k=0 k=0 a k k(0) k 1 = a 1 a 1 = f (0). a k k(k 1)x k 2, k=2 a k k(k 1)(0) k 2 = 2a 2 a 2 = f (0) 2 a k k(k 1)(k 2)x k 3, k=3
1 M 13-Lecture Contents: 1) Taylor Polynomials 2) Taylor Series Centered at x a 3) Applications of Taylor Polynomials Taylor Series The previous section served as motivation and gave some useful expansion.
More informationFourier series
11.1-11.2. Fourier series Yurii Lyubarskii, NTNU September 5, 2016 Periodic functions Function f defined on the whole real axis has period p if Properties f (t) = f (t + p) for all t R If f and g have
More informationMathematical Economics: Lecture 2
Mathematical Economics: Lecture 2 Yu Ren WISE, Xiamen University September 25, 2012 Outline 1 Number Line The number line, origin (Figure 2.1 Page 11) Number Line Interval (a, b) = {x R 1 : a < x < b}
More informationThe standard form for a general polynomial of degree n is written. Examples of a polynomial in standard form
Section 4 1A: The Rational Zeros (Roots) of a Polynomial The standard form for a general polynomial of degree n is written f (x) = a n x n + a n 1 x n 1 +... + a 1 x + a 0 where the highest degree term
More informationPHYS 502 Lecture 3: Fourier Series
PHYS 52 Lecture 3: Fourier Series Fourier Series Introduction In mathematics, a Fourier series decomposes periodic functions or periodic signals into the sum of a (possibly infinite) set of simple oscillating
More informationEx. 3. Mathematica knows about all standard probability distributions. c) The probability is just the pdf integrated over the interval
Ex. 3 Mathematica knows about all standard probability distributions a) In[336]:= p.4; n 6; r 5; PDF BinomialDistribution n, p r BarChart Table PDF BinomialDistribution n, p, k, k,, n Out[339]=.36864.3.25.2
More informationTaylor Series. Math114. March 1, Department of Mathematics, University of Kentucky. Math114 Lecture 18 1/ 13
Taylor Series Math114 Department of Mathematics, University of Kentucky March 1, 2017 Math114 Lecture 18 1/ 13 Given a function, can we find a power series representation? Math114 Lecture 18 2/ 13 Given
More informationTo get horizontal and slant asymptotes algebraically we need to know about end behaviour for rational functions.
Concepts: Horizontal Asymptotes, Vertical Asymptotes, Slant (Oblique) Asymptotes, Transforming Reciprocal Function, Sketching Rational Functions, Solving Inequalities using Sign Charts. Rational Function
More informationMath 255 Honors: Gram-Schmidt Orthogonalization on the Space of Polynomials
Math 55 Honors: Gram-Schmidt Orthogonalization on the Space of Polynomials David Moore May, 03 Abstract Gram-Schmidt Orthogonalization is a process to construct orthogonal vectors from some basis for a
More informationq-series Michael Gri for the partition function, he developed the basic idea of the q-exponential. From
q-series Michael Gri th History and q-integers The idea of q-series has existed since at least Euler. In constructing the generating function for the partition function, he developed the basic idea of
More information(a) Determine the general solution for φ(ρ) near ρ = 0 for arbitary values E. (b) Show that the regular solution at ρ = 0 has the series expansion
Problem 1. Curious Wave Functions The eigenfunctions of a D7 brane in a curved geometry lead to the following eigenvalue equation of the Sturm Liouville type ρ ρ 3 ρ φ n (ρ) = E n w(ρ)φ n (ρ) w(ρ) = where
More informationClass 4: More Pendulum results
Class 4: More Pendulum results The pendulum is a mechanical problem with a long and interesting history, from Galileo s first ansatz that the period was independent of the amplitude based on watching priests
More information1. An Introduction to Mathematica (complete)
1. An Introduction to Mathematica (complete) (Lecture Notes, Thomas Steger, University of Leipzig, summer term 11) This chapter provides a concise introduction to Mathematica. Instead of giving a rigorous
More informationContinuity and One-Sided Limits
Continuity and One-Sided Limits 1. Welcome to continuity and one-sided limits. My name is Tuesday Johnson and I m a lecturer at the University of Texas El Paso. 2. With each lecture I present, I will start
More informationMODULE 1: FOUNDATIONS OF MATHEMATICS
MODULE 1: FOUNDATIONS OF MATHEMATICS GENERAL OBJECTIVES On completion of this Module, students should: 1. acquire competency in the application of algebraic techniques; 2. appreciate the role of exponential
More informationPhysics 250 Green s functions for ordinary differential equations
Physics 25 Green s functions for ordinary differential equations Peter Young November 25, 27 Homogeneous Equations We have already discussed second order linear homogeneous differential equations, which
More informationLecture 16: Bessel s Inequality, Parseval s Theorem, Energy convergence
Introductory lecture notes on Partial Differential Equations - c Anthony Peirce. ot to be copied, used, or revised without explicit written permission from the copyright owner. ecture 6: Bessel s Inequality,
More information1 angle.mcd Inner product and angle between two vectors. Note that a function is a special case of a vector. Instructor: Nam Sun Wang. x.
angle.mcd Inner product and angle between two vectors. Note that a function is a special case of a vector. Instructor: Nam Sun Wang Define angle between two vectors & y:. y. y. cos( ) (, y). y. y Projection
More informationSection 9.7 and 9.10: Taylor Polynomials and Approximations/Taylor and Maclaurin Series
Section 9.7 and 9.10: Taylor Polynomials and Approximations/Taylor and Maclaurin Series Power Series for Functions We can create a Power Series (or polynomial series) that can approximate a function around
More informationTrig Identities. or (x + y)2 = x2 + 2xy + y 2. Dr. Ken W. Smith Other examples of identities are: (x + 3)2 = x2 + 6x + 9 and
Trig Identities An identity is an equation that is true for all values of the variables. Examples of identities might be obvious results like Part 4, Trigonometry Lecture 4.8a, Trig Identities and Equations
More informationTHE KENNESAW STATE UNIVERSITY HIGH SCHOOL MATHEMATICS COMPETITION PART II Calculators are NOT permitted Time allowed: 2 hours
THE 018-019 KENNESAW STATE UNIVERSITY HIGH SCHOOL MATHEMATICS COMPETITION PART II Calculators are NOT permitted Time allowed: hours 1 Let m be a three-digit integer with distinct digits Find all such integers
More informationMath 489AB A Very Brief Intro to Fourier Series Fall 2008
Math 489AB A Very Brief Intro to Fourier Series Fall 8 Contents Fourier Series. The coefficients........................................ Convergence......................................... 4.3 Convergence
More informationFOURIER SERIES, TRANSFORMS, AND BOUNDARY VALUE PROBLEMS
fc FOURIER SERIES, TRANSFORMS, AND BOUNDARY VALUE PROBLEMS Second Edition J. RAY HANNA Professor Emeritus University of Wyoming Laramie, Wyoming JOHN H. ROWLAND Department of Mathematics and Department
More informationAnalytic Trigonometry. Copyright Cengage Learning. All rights reserved.
Analytic Trigonometry Copyright Cengage Learning. All rights reserved. 7.4 Basic Trigonometric Equations Copyright Cengage Learning. All rights reserved. Objectives Basic Trigonometric Equations Solving
More informationmultiply both sides of eq. by a and projection overlap
Fourier Series n x n x f xa ancos bncos n n periodic with period x consider n, sin x x x March. 3, 7 Any function with period can be represented with a Fourier series Examples (sawtooth) (square wave)
More information3.2. The Ramsey model - linearization, backward integration, relaxation (complete)
3.. The Ramsey model - linearization, backward integration, relaxation (complete) (Quantitative Dynamic Macroeconomics, Lecture Notes, Thomas Steger, University of Leipzig, winter term /3) Ramsey Model:
More informationPolynomial Chaos and Karhunen-Loeve Expansion
Polynomial Chaos and Karhunen-Loeve Expansion 1) Random Variables Consider a system that is modeled by R = M(x, t, X) where X is a random variable. We are interested in determining the probability of the
More informationMathematical methods and its applications Dr. S. K. Gupta Department of Mathematics Indian Institute of Technology, Roorkee
Mathematical methods and its applications Dr. S. K. Gupta Department of Mathematics Indian Institute of Technology, Roorkee Lecture - 56 Fourier sine and cosine transforms Welcome to lecture series on
More informationLegendre s Equation. PHYS Southern Illinois University. October 18, 2016
Legendre s Equation PHYS 500 - Southern Illinois University October 18, 2016 PHYS 500 - Southern Illinois University Legendre s Equation October 18, 2016 1 / 11 Legendre s Equation Recall We are trying
More information9.3. Total number of phonon modes, total energy and heat capacity
Phys50.nb 6 E = n = n = exp - (9.9) 9... History of the Planck distribution or the Bose-Einstein distribution. his distribution was firstly discovered by Planck in the study of black-body radiation. here,
More informationLEAST SQUARES APPROXIMATION
LEAST SQUARES APPROXIMATION One more approach to approximating a function f (x) on an interval a x b is to seek an approximation p(x) with a small average error over the interval of approximation. A convenient
More informationProcedure for Graphing Polynomial Functions
Procedure for Graphing Polynomial Functions P(x) = a nx n + a n-1x n-1 + + a 1x + a 0 To graph P(x): As an example, we will examine the following polynomial function: P(x) = 2x 3 3x 2 23x + 12 1. Determine
More informationChapter 2: Functions, Limits and Continuity
Chapter 2: Functions, Limits and Continuity Functions Limits Continuity Chapter 2: Functions, Limits and Continuity 1 Functions Functions are the major tools for describing the real world in mathematical
More informationMath Lecture 36
Math 80 - Lecture 36 Dylan Zwick Fall 013 Today, we re going to examine the solutions to the differential equation x y + xy + (x p )y = 0, which is called Bessel s equation of order p 0. The solutions
More informationPeriodic functions: simple harmonic oscillator
Periodic functions: simple harmonic oscillator Recall the simple harmonic oscillator (e.g. mass-spring system) d 2 y dt 2 + ω2 0y = 0 Solution can be written in various ways: y(t) = Ae iω 0t y(t) = A cos
More information11.10a Taylor and Maclaurin Series
11.10a 1 11.10a Taylor and Maclaurin Series Let y = f(x) be a differentiable function at x = a. In first semester calculus we saw that (1) f(x) f(a)+f (a)(x a), for all x near a The right-hand side of
More information2014 Summer Review for Students Entering Algebra 2. TI-84 Plus Graphing Calculator is required for this course.
1. Solving Linear Equations 2. Solving Linear Systems of Equations 3. Multiplying Polynomials and Solving Quadratics 4. Writing the Equation of a Line 5. Laws of Exponents and Scientific Notation 6. Solving
More informationSpecial Functions of Mathematical Physics
Arnold F. Nikiforov Vasilii B. Uvarov Special Functions of Mathematical Physics A Unified Introduction with Applications Translated from the Russian by Ralph P. Boas 1988 Birkhäuser Basel Boston Table
More information3.4 Introduction to power series
3.4 Introduction to power series Definition 3.4.. A polynomial in the variable x is an expression of the form n a i x i = a 0 + a x + a 2 x 2 + + a n x n + a n x n i=0 or a n x n + a n x n + + a 2 x 2
More informationA-Level Maths Revision notes 2014
A-Level Maths Revision notes 2014 Contents Coordinate Geometry... 2 Trigonometry... 4 Basic Algebra... 7 Advanced Algebra... 9 Sequences and Series... 11 Functions... 12 Differentiation... 14 Integration...
More informationPhysics 342 Lecture 23. Radial Separation. Lecture 23. Physics 342 Quantum Mechanics I
Physics 342 Lecture 23 Radial Separation Lecture 23 Physics 342 Quantum Mechanics I Friday, March 26th, 2010 We begin our spherical solutions with the simplest possible case zero potential. Aside from
More informationQualification Exam: Mathematical Methods
Qualification Exam: Mathematical Methods Name:, QEID#41534189: August, 218 Qualification Exam QEID#41534189 2 1 Mathematical Methods I Problem 1. ID:MM-1-2 Solve the differential equation dy + y = sin
More informationADVANCED ENGINEERING MATHEMATICS
ADVANCED ENGINEERING MATHEMATICS DENNIS G. ZILL Loyola Marymount University MICHAEL R. CULLEN Loyola Marymount University PWS-KENT O I^7 3 PUBLISHING COMPANY E 9 U Boston CONTENTS Preface xiii Parti ORDINARY
More informationChapter 6. Legendre and Bessel Functions
Chapter 6 Legendre and Bessel Functions Legendre's Equation Legendre's Equation (order n): legendre d K y''k y'c n n C y = : is an important ode in applied mathematics When n is a non-negative integer,
More informationMATH1190 CALCULUS 1 - NOTES AND AFTERNOTES
MATH90 CALCULUS - NOTES AND AFTERNOTES DR. JOSIP DERADO. Historical background Newton approach - from physics to calculus. Instantaneous velocity. Leibniz approach - from geometry to calculus Calculus
More information