A First Course in Complex Analysis
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Calculus 1 to 4 (2004–2006)
Calculus 1 to 4 (2004–2006) Axel Schuler¨ January 3, 2007 2 Contents 1 Real and Complex Numbers 11 Basics .......................................... 11 Notations ..................................... 11 SumsandProducts ................................ 12 MathematicalInduction. 12 BinomialCoefficients............................... 13 1.1 RealNumbers................................... 15 1.1.1 OrderedSets ............................... 15 1.1.2 Fields................................... 17 1.1.3 OrderedFields .............................. 19 1.1.4 Embedding of natural numbers into the real numbers . ....... 20 1.1.5 The completeness of Ê .......................... 21 1.1.6 TheAbsoluteValue............................ 22 1.1.7 SupremumandInfimumrevisited . 23 1.1.8 Powersofrealnumbers.. .. .. .. .. .. .. 24 1.1.9 Logarithms ................................ 26 1.2 Complexnumbers................................. 29 1.2.1 TheComplexPlaneandthePolarform . 31 1.2.2 RootsofComplexNumbers . 33 1.3 Inequalities .................................... 34 1.3.1 MonotonyofthePowerand ExponentialFunctions . ...... 34 1.3.2 TheArithmetic-Geometricmeaninequality . ...... 34 1.3.3 TheCauchy–SchwarzInequality . .. 35 1.4 AppendixA.................................... 36 2 Sequences and Series 43 2.1 ConvergentSequences .. .. .. .. .. .. .. .. 43 2.1.1 Algebraicoperationswithsequences. ..... 46 2.1.2 Somespecialsequences . .. .. .. .. .. .. 49 2.1.3 MonotonicSequences .. .. .. .. .. .. .. 50 2.1.4 Subsequences............................... 51 2.2 CauchySequences -
Math 137 Calculus 1 for Honours Mathematics Course Notes
Math 137 Calculus 1 for Honours Mathematics Course Notes Barbara A. Forrest and Brian E. Forrest Version 1.61 Copyright c Barbara A. Forrest and Brian E. Forrest. All rights reserved. August 1, 2021 All rights, including copyright and images in the content of these course notes, are owned by the course authors Barbara Forrest and Brian Forrest. By accessing these course notes, you agree that you may only use the content for your own personal, non-commercial use. You are not permitted to copy, transmit, adapt, or change in any way the content of these course notes for any other purpose whatsoever without the prior written permission of the course authors. Author Contact Information: Barbara Forrest ([email protected]) Brian Forrest ([email protected]) i QUICK REFERENCE PAGE 1 Right Angle Trigonometry opposite ad jacent opposite sin θ = hypotenuse cos θ = hypotenuse tan θ = ad jacent 1 1 1 csc θ = sin θ sec θ = cos θ cot θ = tan θ Radians Definition of Sine and Cosine The angle θ in For any θ, cos θ and sin θ are radians equals the defined to be the x− and y− length of the directed coordinates of the point P on the arc BP, taken positive unit circle such that the radius counter-clockwise and OP makes an angle of θ radians negative clockwise. with the positive x− axis. Thus Thus, π radians = 180◦ sin θ = AP, and cos θ = OA. 180 or 1 rad = π . The Unit Circle ii QUICK REFERENCE PAGE 2 Trigonometric Identities Pythagorean cos2 θ + sin2 θ = 1 Identity Range −1 ≤ cos θ ≤ 1 −1 ≤ sin θ ≤ 1 Periodicity cos(θ ± 2π) = cos θ sin(θ ± 2π) = sin -
G-Convergence and Homogenization of Some Sequences of Monotone Differential Operators
Thesis for the degree of Doctor of Philosophy Östersund 2009 G-CONVERGENCE AND HOMOGENIZATION OF SOME SEQUENCES OF MONOTONE DIFFERENTIAL OPERATORS Liselott Flodén Supervisors: Associate Professor Anders Holmbom, Mid Sweden University Professor Nils Svanstedt, Göteborg University Professor Mårten Gulliksson, Mid Sweden University Department of Engineering and Sustainable Development Mid Sweden University, SE‐831 25 Östersund, Sweden ISSN 1652‐893X, Mid Sweden University Doctoral Thesis 70 ISBN 978‐91‐86073‐36‐7 i Akademisk avhandling som med tillstånd av Mittuniversitetet framläggs till offentlig granskning för avläggande av filosofie doktorsexamen onsdagen den 3 juni 2009, klockan 10.00 i sal Q221, Mittuniversitetet, Östersund. Seminariet kommer att hållas på svenska. G-CONVERGENCE AND HOMOGENIZATION OF SOME SEQUENCES OF MONOTONE DIFFERENTIAL OPERATORS Liselott Flodén © Liselott Flodén, 2009 Department of Engineering and Sustainable Development Mid Sweden University, SE‐831 25 Östersund Sweden Telephone: +46 (0)771‐97 50 00 Printed by Kopieringen Mittuniversitetet, Sundsvall, Sweden, 2009 ii Tothememoryofmyfather G-convergence and Homogenization of some Sequences of Monotone Differential Operators Liselott Flodén Department of Engineering and Sustainable Development Mid Sweden University, SE-831 25 Östersund, Sweden Abstract This thesis mainly deals with questions concerning the convergence of some sequences of elliptic and parabolic linear and non-linear oper- ators by means of G-convergence and homogenization. In particular, we study operators with oscillations in several spatial and temporal scales. Our main tools are multiscale techniques, developed from the method of two-scale convergence and adapted to the problems stud- ied. For certain classes of parabolic equations we distinguish different cases of homogenization for different relations between the frequen- cies of oscillations in space and time by means of different sets of local problems. -
Generalizations of the Riemann Integral: an Investigation of the Henstock Integral
Generalizations of the Riemann Integral: An Investigation of the Henstock Integral Jonathan Wells May 15, 2011 Abstract The Henstock integral, a generalization of the Riemann integral that makes use of the δ-fine tagged partition, is studied. We first consider Lebesgue’s Criterion for Riemann Integrability, which states that a func- tion is Riemann integrable if and only if it is bounded and continuous almost everywhere, before investigating several theoretical shortcomings of the Riemann integral. Despite the inverse relationship between integra- tion and differentiation given by the Fundamental Theorem of Calculus, we find that not every derivative is Riemann integrable. We also find that the strong condition of uniform convergence must be applied to guarantee that the limit of a sequence of Riemann integrable functions remains in- tegrable. However, by slightly altering the way that tagged partitions are formed, we are able to construct a definition for the integral that allows for the integration of a much wider class of functions. We investigate sev- eral properties of this generalized Riemann integral. We also demonstrate that every derivative is Henstock integrable, and that the much looser requirements of the Monotone Convergence Theorem guarantee that the limit of a sequence of Henstock integrable functions is integrable. This paper is written without the use of Lebesgue measure theory. Acknowledgements I would like to thank Professor Patrick Keef and Professor Russell Gordon for their advice and guidance through this project. I would also like to acknowledge Kathryn Barich and Kailey Bolles for their assistance in the editing process. Introduction As the workhorse of modern analysis, the integral is without question one of the most familiar pieces of the calculus sequence. -
Conceptual Power Series Knowledge of STEM Majors
Paper ID #21246 Conceptual Power Series Knowledge of STEM Majors Dr. Emre Tokgoz, Quinnipiac University Emre Tokgoz is currently the Director and an Assistant Professor of Industrial Engineering at Quinnipiac University. He completed a Ph.D. in Mathematics and another Ph.D. in Industrial and Systems Engineer- ing at the University of Oklahoma. His pedagogical research interest includes technology and calculus education of STEM majors. He worked on several IRB approved pedagogical studies to observe under- graduate and graduate mathematics and engineering students’ calculus and technology knowledge since 2011. His other research interests include nonlinear optimization, financial engineering, facility alloca- tion problem, vehicle routing problem, solar energy systems, machine learning, system design, network analysis, inventory systems, and Riemannian geometry. c American Society for Engineering Education, 2018 Mathematics & Engineering Majors’ Conceptual Cognition of Power Series Emre Tokgöz [email protected] Industrial Engineering, School of Engineering, Quinnipiac University, Hamden, CT, 08518 Taylor series expansion of functions has important applications in engineering, mathematics, physics, and computer science; therefore observing responses of graduate and senior undergraduate students to Taylor series questions appears to be the initial step for understanding students’ conceptual cognitive reasoning. These observations help to determine and develop a successful teaching methodology after weaknesses of the students are investigated. Pedagogical research on understanding mathematics and conceptual knowledge of physics majors’ power series was conducted in various studies ([1-10]); however, to the best of our knowledge, Taylor series knowledge of engineering majors was not investigated prior to this study. In this work, the ability of graduate and senior undergraduate engineering and mathematics majors responding to a set of power series questions are investigated. -
Sequences, Series and Taylor Approximation (Ma2712b, MA2730)
Sequences, Series and Taylor Approximation (MA2712b, MA2730) Level 2 Teaching Team Current curator: Simon Shaw November 20, 2015 Contents 0 Introduction, Overview 6 1 Taylor Polynomials 10 1.1 Lecture 1: Taylor Polynomials, Definition . .. 10 1.1.1 Reminder from Level 1 about Differentiable Functions . .. 11 1.1.2 Definition of Taylor Polynomials . 11 1.2 Lectures 2 and 3: Taylor Polynomials, Examples . ... 13 x 1.2.1 Example: Compute and plot Tnf for f(x) = e ............ 13 1.2.2 Example: Find the Maclaurin polynomials of f(x) = sin x ...... 14 2 1.2.3 Find the Maclaurin polynomial T11f for f(x) = sin(x ) ....... 15 1.2.4 QuestionsforChapter6: ErrorEstimates . 15 1.3 Lecture 4 and 5: Calculus of Taylor Polynomials . .. 17 1.3.1 GeneralResults............................... 17 1.4 Lecture 6: Various Applications of Taylor Polynomials . ... 22 1.4.1 RelativeExtrema .............................. 22 1.4.2 Limits .................................... 24 1.4.3 How to Calculate Complicated Taylor Polynomials? . 26 1.5 ExerciseSheet1................................... 29 1.5.1 ExerciseSheet1a .............................. 29 1.5.2 FeedbackforSheet1a ........................... 33 2 Real Sequences 40 2.1 Lecture 7: Definitions, Limit of a Sequence . ... 40 2.1.1 DefinitionofaSequence .......................... 40 2.1.2 LimitofaSequence............................. 41 2.1.3 Graphic Representations of Sequences . .. 43 2.2 Lecture 8: Algebra of Limits, Special Sequences . ..... 44 2.2.1 InfiniteLimits................................ 44 1 2.2.2 AlgebraofLimits.............................. 44 2.2.3 Some Standard Convergent Sequences . .. 46 2.3 Lecture 9: Bounded and Monotone Sequences . ..... 48 2.3.1 BoundedSequences............................. 48 2.3.2 Convergent Sequences and Closed Bounded Intervals . .... 48 2.4 Lecture10:MonotoneSequences . -
Euler's Calculation of the Sum of the Reciprocals of the Squares
Euler's Calculation of the Sum of the Reciprocals of the Squares Kenneth M. Monks ∗ August 5, 2019 A central theme of most second-semester calculus courses is that of infinite series. Simply put, to study infinite series is to attempt to answer the following question: What happens if you add up infinitely many numbers? How much sense humankind made of this question at different points throughout history depended enormously on what exactly those numbers being summed were. As far back as the third century bce, Greek mathematician and engineer Archimedes (287 bce{212 bce) used his method of exhaustion to carry out computations equivalent to the evaluation of an infinite geometric series in his work Quadrature of the Parabola [Archimedes, 1897]. Far more difficult than geometric series are p-series: series of the form 1 X 1 1 1 1 = 1 + + + + ··· np 2p 3p 4p n=1 for a real number p. Here we show the history of just two such series. In Section 1, we warm up with Nicole Oresme's treatment of the harmonic series, the p = 1 case.1 This will lessen the likelihood that we pull a muscle during our more intense Section 3 excursion: Euler's incredibly clever method for evaluating the p = 2 case. 1 Oresme and the Harmonic Series In roughly the year 1350 ce, a University of Paris scholar named Nicole Oresme2 (1323 ce{1382 ce) proved that the harmonic series does not sum to any finite value [Oresme, 1961]. Today, we would say the series diverges and that 1 1 1 1 + + + + ··· = 1: 2 3 4 His argument was brief and beautiful! Let us admire it below. -
1 Infinite Sequences and Series
1 Infinite Sequences and Series In experimental science and engineering, as well as in everyday life, we deal with integers, or at most rational numbers. Yet in theoretical analysis, we use real and complex numbers, as well as far more abstract mathematical constructs, fully expecting that this analysis will eventually provide useful models of natural phenomena. Hence we proceed through the con- struction of the real and complex numbers starting from the positive integers1. Understanding this construction will help the reader appreciate many basic ideas of analysis. We start with the positive integers and zero, and introduce negative integers to allow sub- traction of integers. Then we introduce rational numbers to permit division by integers. From arithmetic we proceed to analysis, which begins with the concept of convergence of infinite sequences of (rational) numbers, as defined here by the Cauchy criterion. Then we define irrational numbers as limits of convergent (Cauchy) sequences of rational numbers. In order to solve algebraic equations in general, we must introduce complex numbers and the representation of complex numbers as points in the complex plane. The fundamental theorem of algebra states that every polynomial has at least one root in the complex plane, from which it follows that every polynomial of degree n has exactly n roots in the complex plane when these roots are suitably counted. We leave the proof of this theorem until we study functions of a complex variable at length in Chapter 4. Once we understand convergence of infinite sequences, we can deal with infinite series of the form ∞ xn n=1 and the closely related infinite products of the form ∞ xn n=1 Infinite series are central to the study of solutions, both exact and approximate, to the differ- ential equations that arise in every branch of physics. -
(Sn) Converges to a Real Number S If ∀Ε > 0, ∃Ns.T
32 MATH 3333{INTERMEDIATE ANALYSIS{BLECHER NOTES 4. Sequences 4.1. Convergent sequences. • A sequence (sn) converges to a real number s if 8 > 0, 9Ns:t: jsn − sj < 8n ≥ N. Saying that jsn−sj < is the same as saying that s− < sn < s+. • If (sn) converges to s then we say that s is the limit of (sn) and write s = limn sn, or s = limn!1 sn, or sn ! s as n ! 1, or simply sn ! s. • If (sn) does not converge to any real number then we say that it diverges. • A sequence (sn) is called bounded if the set fsn : n 2 Ng is a bounded set. That is, there are numbers m and M such that m ≤ sn ≤ M for all n 2 N. This is the same as saying that fsn : n 2 Ng ⊂ [m; M]. It is easy to see that this is equivalent to: there exists a number K ≥ 0 such that jsnj ≤ K for all n 2 N. (See the first lines of the last Section.) Fact 1. Any convergent sequence is bounded. Proof: Suppose that sn ! s as n ! 1. Taking = 1 in the definition of convergence gives that there exists a number N 2 N such that jsn −sj < 1 whenever n ≥ N. Thus jsnj = jsn − s + sj ≤ jsn − sj + jsj < 1 + jsj whenever n ≥ N. Now let M = maxfjs1j; js2j; ··· ; jsN j; 1 + jsjg. We have jsnj ≤ M if n = 1; 2; ··· ;N, and jsnj ≤ M if n ≥ N. So (sn) is bounded. • A sequence (an) is called nonnegative if an ≥ 0 for all n 2 N. -
BAIRE ONE FUNCTIONS 1. History Baire One Functions Are Named in Honor of René-Louis Baire (1874- 1932), a French Mathematician
BAIRE ONE FUNCTIONS JOHNNY HU Abstract. This paper gives a general overview of Baire one func- tions, including examples as well as several interesting properties involving bounds, uniform convergence, continuity, and Fσ sets. We conclude with a result on a characterization of Baire one func- tions in terms of the notion of first return recoverability, which is a topic of current research in analysis [6]. 1. History Baire one functions are named in honor of Ren´e-Louis Baire (1874- 1932), a French mathematician who had research interests in continuity of functions and the idea of limits [1]. The problem of classifying the class of functions that are convergent sequences of continuous functions was first explored in 1897. According to F.A. Medvedev in his book Scenes from the History of Real Functions, Baire was interested in the relationship between the continuity of a function of two variables in each argument separately and its joint continuity in the two variables [2]. Baire showed that every function of two variables that is continuous in each argument separately is not pointwise continuous with respect to the two variables jointly [2]. For instance, consider the function xy f(x; y) = : x2 + y2 Observe that for all points (x; y) =6 0, f is continuous and so, of course, f is separately continuous. Next, we see that, xy xy lim = lim = 0 (x;0)!(0;0) x2 + y2 (0;y)!(0;0) x2 + y2 as (x; y) approaches (0; 0) along the x-axis and y-axis respectively. However, as (x; y) approaches (0; 0) along the line y = x, we have xy 1 lim = : (x;x)!(0;0) x2 + y2 2 Hence, f is continuous along the lines y = 0 and x = 0, but is discon- tinuous overall at (0; 0). -
Complex Analysis Mario Bonk
Complex Analysis Mario Bonk Course notes for Math 246A and 246B University of California, Los Angeles Contents Preface 6 1 Algebraic properties of complex numbers 8 2 Topological properties of C 18 3 Differentiation 26 4 Path integrals 38 5 Power series 43 6 Local Cauchy theorems 55 7 Power series representations 62 8 Zeros of holomorphic functions 68 9 The Open Mapping Theorem 74 10 Elementary functions 79 11 The Riemann sphere 86 12 M¨obiustransformations 92 13 Schwarz's Lemma 105 14 Winding numbers 113 15 Global Cauchy theorems 122 16 Isolated singularities 129 17 The Residue Theorem 142 18 Normal families 152 19 The Riemann Mapping Theorem 161 3 CONTENTS 4 20 The Cauchy transform 170 21 Runge's Approximation Theorem 179 References 187 Preface These notes cover the material of a course on complex analysis that I taught repeatedly at UCLA. In many respects I closely follow Rudin's book on \Real and Complex Analysis". Since Walter Rudin is the unsurpassed master of mathematical exposition for whom I have great admiration, I saw no point in trying to improve on his presentation of subjects that are relevant for the course. The notes give a fairly accurate account of the material covered in class. They are rather terse as oral discussions that gave further explanations or put results into perspective are mostly omitted. In addition, all pictures and diagrams are currently missing as it is much easier to produce them on the blackboard than to put them into print. 6 1 Algebraic properties of complex numbers 1.1. -
Sequences and Their Limits
Sequences and their limits c Frank Zorzitto, Faculty of Mathematics University of Waterloo The limit idea For the purposes of calculus, a sequence is simply a list of numbers x1; x2; x3; : : : ; xn;::: that goes on indefinitely. The numbers in the sequence are usually called terms, so that x1 is the first term, x2 is the second term, and the entry xn in the general nth position is the nth term, naturally. The subscript n = 1; 2; 3;::: that marks the position of the terms will sometimes be called the index. We shall deal only with real sequences, namely those whose terms are real numbers. Here are some examples of sequences. • the sequence of positive integers: 1; 2; 3; : : : ; n; : : : • the sequence of primes in their natural order: 2; 3; 5; 7; 11; ::: • the decimal sequence that estimates 1=3: :3;:33;:333;:3333;:33333;::: • a binary sequence: 0; 1; 0; 1; 0; 1;::: • the zero sequence: 0; 0; 0; 0;::: • a geometric sequence: 1; r; r2; r3; : : : ; rn;::: 1 −1 1 (−1)n • a sequence that alternates in sign: 2 ; 3 ; 4 ;:::; n ;::: • a constant sequence: −5; −5; −5; −5; −5;::: 1 2 3 4 n • an increasing sequence: 2 ; 3 ; 4 ; 5 :::; n+1 ;::: 1 1 1 1 • a decreasing sequence: 1; 2 ; 3 ; 4 ;:::; n ;::: 3 2 4 3 5 4 n+1 n • a sequence used to estimate e: ( 2 ) ; ( 3 ) ; ( 4 ) :::; ( n ) ::: 1 • a seemingly random sequence: sin 1; sin 2; sin 3;:::; sin n; : : : • the sequence of decimals that approximates π: 3; 3:1; 3:14; 3:141; 3:1415; 3:14159; 3:141592; 3:1415926; 3:14159265;::: • a sequence that lists all fractions between 0 and 1, written in their lowest form, in groups of increasing denominator with increasing numerator in each group: 1 1 2 1 3 1 2 3 4 1 5 1 2 3 4 5 6 1 3 5 7 1 2 4 5 ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ; ;::: 2 3 3 4 4 5 5 5 5 6 6 7 7 7 7 7 7 8 8 8 8 9 9 9 9 It is plain to see that the possibilities for sequences are endless.