Taylor Polynomials and Infinite Series a Chapter for a First-Year Calculus Course
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Ch. 15 Power Series, Taylor Series
Ch. 15 Power Series, Taylor Series 서울대학교 조선해양공학과 서유택 2017.12 ※ 본 강의 자료는 이규열, 장범선, 노명일 교수님께서 만드신 자료를 바탕으로 일부 편집한 것입니다. Seoul National 1 Univ. 15.1 Sequences (수열), Series (급수), Convergence Tests (수렴판정) Sequences: Obtained by assigning to each positive integer n a number zn z . Term: zn z1, z 2, or z 1, z 2 , or briefly zn N . Real sequence (실수열): Sequence whose terms are real Convergence . Convergent sequence (수렴수열): Sequence that has a limit c limznn c or simply z c n . For every ε > 0, we can find N such that Convergent complex sequence |zn c | for all n N → all terms zn with n > N lie in the open disk of radius ε and center c. Divergent sequence (발산수열): Sequence that does not converge. Seoul National 2 Univ. 15.1 Sequences, Series, Convergence Tests Convergence . Convergent sequence: Sequence that has a limit c Ex. 1 Convergent and Divergent Sequences iin 11 Sequence i , , , , is convergent with limit 0. n 2 3 4 limznn c or simply z c n Sequence i n i , 1, i, 1, is divergent. n Sequence {zn} with zn = (1 + i ) is divergent. Seoul National 3 Univ. 15.1 Sequences, Series, Convergence Tests Theorem 1 Sequences of the Real and the Imaginary Parts . A sequence z1, z2, z3, … of complex numbers zn = xn + iyn converges to c = a + ib . if and only if the sequence of the real parts x1, x2, … converges to a . and the sequence of the imaginary parts y1, y2, … converges to b. Ex. -
Topic 7 Notes 7 Taylor and Laurent Series
Topic 7 Notes Jeremy Orloff 7 Taylor and Laurent series 7.1 Introduction We originally defined an analytic function as one where the derivative, defined as a limit of ratios, existed. We went on to prove Cauchy's theorem and Cauchy's integral formula. These revealed some deep properties of analytic functions, e.g. the existence of derivatives of all orders. Our goal in this topic is to express analytic functions as infinite power series. This will lead us to Taylor series. When a complex function has an isolated singularity at a point we will replace Taylor series by Laurent series. Not surprisingly we will derive these series from Cauchy's integral formula. Although we come to power series representations after exploring other properties of analytic functions, they will be one of our main tools in understanding and computing with analytic functions. 7.2 Geometric series Having a detailed understanding of geometric series will enable us to use Cauchy's integral formula to understand power series representations of analytic functions. We start with the definition: Definition. A finite geometric series has one of the following (all equivalent) forms. 2 3 n Sn = a(1 + r + r + r + ::: + r ) = a + ar + ar2 + ar3 + ::: + arn n X = arj j=0 n X = a rj j=0 The number r is called the ratio of the geometric series because it is the ratio of consecutive terms of the series. Theorem. The sum of a finite geometric series is given by a(1 − rn+1) S = a(1 + r + r2 + r3 + ::: + rn) = : (1) n 1 − r Proof. -
Line Integrals for Work, Circulation, and Plane Flux
Classroom Tips and Techniques: Line Integrals for Work, Circulation, and Plane Flux Robert J. Lopez Emeritus Professor of Mathematics and Maple Fellow © Maplesoft, a division of Waterloo Maple Inc., 2005 Introduction In our last column, we discussed how to address the iterated integral in Maple 9.5. This month, we will continue discussing integrals that arise in the subject area of vector calculus. In particular, we will discuss line integrals of the tangential and normal components of a vector field. The line integral of the tangential component of a force field produces the work done by the force on a particle of unit mass, as the mass moves along a specified curve. For the tangential component of the velocity field of a planar fluid flow, the line integral around a closed curve - typically a circle - is the circulation of the flow. The line integral of the normal component of a vector field is the flux of the field through the curve, and is a measure of the net "flow" of the field in the direction of the normal. If F = i + j represents the vector field in Cartesian coordinates, and is a planar curve parametrized by the equations then work (or circulation), the line integral of the tangential component of F along , is given by + or Flux, the line integral of the normal component of F along , is given by or (The mnemonic I always provided my students for the flux integral in the plane is that the form starts and ends with the same letters as the word "flux" and has a minus sign in the middle, thus determining where the letters and must go.) All of these physically meaningful quantities can be computed with the LineInt command in Maple's VectorCalculus package. -
3.3 Convergence Tests for Infinite Series
3.3 Convergence Tests for Infinite Series 3.3.1 The integral test We may plot the sequence an in the Cartesian plane, with independent variable n and dependent variable a: n X The sum an can then be represented geometrically as the area of a collection of rectangles with n=1 height an and width 1. This geometric viewpoint suggests that we compare this sum to an integral. If an can be represented as a continuous function of n, for real numbers n, not just integers, and if the m X sequence an is decreasing, then an looks a bit like area under the curve a = a(n). n=1 In particular, m m+2 X Z m+1 X an > an dn > an n=1 n=1 n=2 For example, let us examine the first 10 terms of the harmonic series 10 X 1 1 1 1 1 1 1 1 1 1 = 1 + + + + + + + + + : n 2 3 4 5 6 7 8 9 10 1 1 1 If we draw the curve y = x (or a = n ) we see that 10 11 10 X 1 Z 11 dx X 1 X 1 1 > > = − 1 + : n x n n 11 1 1 2 1 (See Figure 1, copied from Wikipedia) Z 11 dx Now = ln(11) − ln(1) = ln(11) so 1 x 10 X 1 1 1 1 1 1 1 1 1 1 = 1 + + + + + + + + + > ln(11) n 2 3 4 5 6 7 8 9 10 1 and 1 1 1 1 1 1 1 1 1 1 1 + + + + + + + + + < ln(11) + (1 − ): 2 3 4 5 6 7 8 9 10 11 Z dx So we may bound our series, above and below, with some version of the integral : x If we allow the sum to turn into an infinite series, we turn the integral into an improper integral. -
1 Approximating Integrals Using Taylor Polynomials 1 1.1 Definitions
Seunghee Ye Ma 8: Week 7 Nov 10 Week 7 Summary This week, we will learn how we can approximate integrals using Taylor series and numerical methods. Topics Page 1 Approximating Integrals using Taylor Polynomials 1 1.1 Definitions . .1 1.2 Examples . .2 1.3 Approximating Integrals . .3 2 Numerical Integration 5 1 Approximating Integrals using Taylor Polynomials 1.1 Definitions When we first defined the derivative, recall that it was supposed to be the \instantaneous rate of change" of a function f(x) at a given point c. In other words, f 0 gives us a linear approximation of f(x) near c: for small values of " 2 R, we have f(c + ") ≈ f(c) + "f 0(c) But if f(x) has higher order derivatives, why stop with a linear approximation? Taylor series take this idea of linear approximation and extends it to higher order derivatives, giving us a better approximation of f(x) near c. Definition (Taylor Polynomial and Taylor Series) Let f(x) be a Cn function i.e. f is n-times continuously differentiable. Then, the n-th order Taylor polynomial of f(x) about c is: n X f (k)(c) T (f)(x) = (x − c)k n k! k=0 The n-th order remainder of f(x) is: Rn(f)(x) = f(x) − Tn(f)(x) If f(x) is C1, then the Taylor series of f(x) about c is: 1 X f (k)(c) T (f)(x) = (x − c)k 1 k! k=0 Note that the first order Taylor polynomial of f(x) is precisely the linear approximation we wrote down in the beginning. -
On a Series of Goldbach and Euler Llu´Is Bibiloni, Pelegr´I Viader, and Jaume Parad´Is
On a Series of Goldbach and Euler Llu´ıs Bibiloni, Pelegr´ı Viader, and Jaume Parad´ıs 1. INTRODUCTION. Euler’s paper Variae observationes circa series infinitas [6] ought to be considered important for several reasons. It contains the first printed ver- sion of Euler’s product for the Riemann zeta-function; it definitely establishes the use of the symbol π to denote the perimeter of the circle of diameter one; and it introduces a legion of interesting infinite products and series. The first of these is Theorem 1, which Euler says was communicated to him and proved by Goldbach in a letter (now lost): 1 = 1. n − m,n≥2 m 1 (One must avoid repetitions in this sum.) We refer to this result as the “Goldbach-Euler Theorem.” Goldbach and Euler’s proof is a typical example of what some historians consider a misuse of divergent series, for it starts by assigning a “value” to the harmonic series 1/n and proceeds by manipulating it by substraction and replacement of other series until the desired result is reached. This unchecked use of divergent series to obtain valid results was a standard procedure in the late seventeenth and early eighteenth centuries. It has provoked quite a lot of criticism, correction, and, why not, praise of the audacity of the mathematicians of the time. They were led by Euler, the “Master of Us All,” as Laplace christened him. We present the original proof of the Goldbach- Euler theorem in section 2. Euler was obviously familiar with other instances of proofs that used divergent se- ries. -
Series, Cont'd
Jim Lambers MAT 169 Fall Semester 2009-10 Lecture 5 Notes These notes correspond to Section 8.2 in the text. Series, cont'd In the previous lecture, we defined the concept of an infinite series, and what it means for a series to converge to a finite sum, or to diverge. We also worked with one particular type of series, a geometric series, for which it is particularly easy to determine whether it converges, and to compute its limit when it does exist. Now, we consider other types of series and investigate their behavior. Telescoping Series Consider the series 1 X 1 1 − : n n + 1 n=1 If we write out the first few terms, we obtain 1 X 1 1 1 1 1 1 1 1 1 − = 1 − + − + − + − + ··· n n + 1 2 2 3 3 4 4 5 n=1 1 1 1 1 1 1 = 1 + − + − + − + ··· 2 2 3 3 4 4 = 1: We see that nearly all of the fractions cancel one another, revealing the limit. This is an example of a telescoping series. It turns out that many series have this property, even though it is not immediately obvious. Example The series 1 X 1 n(n + 2) n=1 is also a telescoping series. To see this, we compute the partial fraction decomposition of each term. This decomposition has the form 1 A B = + : n(n + 2) n n + 2 1 To compute A and B, we multipy both sides by the common denominator n(n + 2) and obtain 1 = A(n + 2) + Bn: Substituting n = 0 yields A = 1=2, and substituting n = −2 yields B = −1=2. -
Mathematics 1
Mathematics 1 MATH 1141 Calculus I for Chemistry, Engineering, and Physics MATHEMATICS Majors 4 Credits Prerequisite: Precalculus. This course covers analytic geometry, continuous functions, derivatives Courses of algebraic and trigonometric functions, product and chain rules, implicit functions, extrema and curve sketching, indefinite and definite integrals, MATH 1011 Precalculus 3 Credits applications of derivatives and integrals, exponential, logarithmic and Topics in this course include: algebra; linear, rational, exponential, inverse trig functions, hyperbolic trig functions, and their derivatives and logarithmic and trigonometric functions from a descriptive, algebraic, integrals. It is recommended that students not enroll in this course unless numerical and graphical point of view; limits and continuity. Primary they have a solid background in high school algebra and precalculus. emphasis is on techniques needed for calculus. This course does not Previously MA 0145. count toward the mathematics core requirement, and is meant to be MATH 1142 Calculus II for Chemistry, Engineering, and Physics taken only by students who are required to take MATH 1121, MATH 1141, Majors 4 Credits or MATH 1171 for their majors, but who do not have a strong enough Prerequisite: MATH 1141 or MATH 1171. mathematics background. Previously MA 0011. This course covers applications of the integral to area, arc length, MATH 1015 Mathematics: An Exploration 3 Credits and volumes of revolution; integration by substitution and by parts; This course introduces various ideas in mathematics at an elementary indeterminate forms and improper integrals: Infinite sequences and level. It is meant for the student who would like to fulfill a core infinite series, tests for convergence, power series, and Taylor series; mathematics requirement, but who does not need to take mathematics geometry in three-space. -
Appendix a Short Course in Taylor Series
Appendix A Short Course in Taylor Series The Taylor series is mainly used for approximating functions when one can identify a small parameter. Expansion techniques are useful for many applications in physics, sometimes in unexpected ways. A.1 Taylor Series Expansions and Approximations In mathematics, the Taylor series is a representation of a function as an infinite sum of terms calculated from the values of its derivatives at a single point. It is named after the English mathematician Brook Taylor. If the series is centered at zero, the series is also called a Maclaurin series, named after the Scottish mathematician Colin Maclaurin. It is common practice to use a finite number of terms of the series to approximate a function. The Taylor series may be regarded as the limit of the Taylor polynomials. A.2 Definition A Taylor series is a series expansion of a function about a point. A one-dimensional Taylor series is an expansion of a real function f(x) about a point x ¼ a is given by; f 00ðÞa f 3ðÞa fxðÞ¼faðÞþf 0ðÞa ðÞþx À a ðÞx À a 2 þ ðÞx À a 3 þÁÁÁ 2! 3! f ðÞn ðÞa þ ðÞx À a n þÁÁÁ ðA:1Þ n! © Springer International Publishing Switzerland 2016 415 B. Zohuri, Directed Energy Weapons, DOI 10.1007/978-3-319-31289-7 416 Appendix A: Short Course in Taylor Series If a ¼ 0, the expansion is known as a Maclaurin Series. Equation A.1 can be written in the more compact sigma notation as follows: X1 f ðÞn ðÞa ðÞx À a n ðA:2Þ n! n¼0 where n ! is mathematical notation for factorial n and f(n)(a) denotes the n th derivation of function f evaluated at the point a. -
Convergence Tests: Divergence, Integral, and P-Series Tests
Convergence Tests: Divergence, Integral, and p-Series Tests SUGGESTED REFERENCE MATERIAL: As you work through the problems listed below, you should reference your lecture notes and the relevant chapters in a textbook/online resource. EXPECTED SKILLS: • Recognize series that cannot converge by applying the Divergence Test. • Use the Integral Test on appropriate series (all terms positive, corresponding function is decreasing and continuous) to make a conclusion about the convergence of the series. • Recognize a p-series and use the value of p to make a conclusion about the convergence of the series. • Use the algebraic properties of series. PRACTICE PROBLEMS: For problems 1 { 9, apply the Divergence Test. What, if any, conlcusions can you draw about the series? 1 X 1. (−1)k k=1 lim (−1)k DNE and thus is not 0, so by the Divergence Test the series diverges. k!1 Also, recall that this series is a geometric series with ratio r = −1, which confirms that it must diverge. 1 X 1 2. (−1)k k k=1 1 lim (−1)k = 0, so the Divergence Test is inconclusive. k!1 k 1 X ln k 3. k k=3 ln k lim = 0, so the Divergence Test is inconclusive. k!1 k 1 1 X ln 6k 4. ln 2k k=1 ln 6k lim = 1 6= 0 [see Sequences problem #26], so by the Divergence Test the series diverges. k!1 ln 2k 1 X 5. ke−k k=1 lim ke−k = 0 [see Limits at Infinity Review problem #6], so the Divergence Test is k!1 inconclusive. -
Operations on Power Series Related to Taylor Series
Operations on Power Series Related to Taylor Series In this problem, we perform elementary operations on Taylor series – term by term differen tiation and integration – to obtain new examples of power series for which we know their sum. Suppose that a function f has a power series representation of the form: 1 2 X n f(x) = a0 + a1(x − c) + a2(x − c) + · · · = an(x − c) n=0 convergent on the interval (c − R; c + R) for some R. The results we use in this example are: • (Differentiation) Given f as above, f 0(x) has a power series expansion obtained by by differ entiating each term in the expansion of f(x): 1 0 X n−1 f (x) = a1 + a2(x − c) + 2a3(x − c) + · · · = nan(x − c) n=1 • (Integration) Given f as above, R f(x) dx has a power series expansion obtained by by inte grating each term in the expansion of f(x): 1 Z a1 a2 X an f(x) dx = C + a (x − c) + (x − c)2 + (x − c)3 + · · · = C + (x − c)n+1 0 2 3 n + 1 n=0 for some constant C depending on the choice of antiderivative of f. Questions: 1. Find a power series representation for the function f(x) = arctan(5x): (Note: arctan x is the inverse function to tan x.) 2. Use power series to approximate Z 1 2 sin(x ) dx 0 (Note: sin(x2) is a function whose antiderivative is not an elementary function.) Solution: 1 For question (1), we know that arctan x has a simple derivative: , which then has a power 1 + x2 1 2 series representation similar to that of , where we subsitute −x for x. -
Problem Set 1
Mathematics 41C - 43C Mathematics Department Phillips Exeter Academy Exeter, NH August 2019 Table of Contents 41C Laboratory 0: Graphing . 6 Problem Set 1 . 9 Laboratory 1: Differences . 13 Problem Set 2 . .15 Laboratory 2: Functions and Rate of Change Graphs . 19 Problem Set 3 . .21 Laboratory 3: Approximating Instantaneous Rate of Change . 28 Problem Set 4 . .29 Laboratory 4: Linear Approximation . 34 Problem Set 5 . .36 Laboratory 5: Transformations and Derivatives . 41 Problem Set 6 . .43 Laboratory 6: Addition Rule and Product Rule for Derivatives . 47 Problem Set 7 . .49 Laboratory 7: Graphs and the Derivative . .53 Problem Set 8 . .54 Laboratory 8: The Most Exciting Moment on the Tilt-a-Whirl . 58 42C Laboratory 9: Graphs and the Second Derivative . 62 Problem Set 10 . .63 Laboratory 10: The Chain Rule for Derivatives . 66 Problem Set 11 . .69 Laboratory 11: Discovering Differential Equations . 74 Problem Set 12 . .76 Laboratory 12: Projectile Motion . .80 Problem Set 13 . .81 Laboratory 13: Introducing Slope Fields . .84 Problem Set 14 . .86 Laboratory 14: Introducing Euler's Method . 89 Problem Set 15 . .91 Laboratory 15: Skydiving . 95 Problem Set 16 . .97 43C Problem Set 17 . 102 Laboratory 17: The Gini Index . .107 Problem Set 18 . 111 Laboratory 18: Integration as Accumulation . .115 Problem Set 19 . 117 Laboratory 19: Geometric Probability . 120 Problem Set 20 . 121 August 2019 3 Phillips Exeter Academy Table of Contents Laboratory 20: The Normal Curve . 124 Problem Set 21 . 126 Laboratory 21: The Exponential Distribution . 129 Problem Set 22 . 131 Laboratory 22: Calculus and Data Analysis . 134 Problem Set 23 . 138 Laboratory 23: Predator/Prey Model .