INTRODUCTION to ANALYSIS (MATH 420) Contents References 4
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Calculus for the Life Sciences I Lecture Notes – Limits, Continuity, and the Derivative
Limits Continuity Derivative Calculus for the Life Sciences I Lecture Notes – Limits, Continuity, and the Derivative Joseph M. Mahaffy, [email protected] Department of Mathematics and Statistics Dynamical Systems Group Computational Sciences Research Center San Diego State University San Diego, CA 92182-7720 http://www-rohan.sdsu.edu/∼jmahaffy Spring 2013 Lecture Notes – Limits, Continuity, and the Deriv Joseph M. Mahaffy, [email protected] — (1/24) Limits Continuity Derivative Outline 1 Limits Definition Examples of Limit 2 Continuity Examples of Continuity 3 Derivative Examples of a derivative Lecture Notes – Limits, Continuity, and the Deriv Joseph M. Mahaffy, [email protected] — (2/24) Limits Definition Continuity Examples of Limit Derivative Introduction Limits are central to Calculus Lecture Notes – Limits, Continuity, and the Deriv Joseph M. Mahaffy, [email protected] — (3/24) Limits Definition Continuity Examples of Limit Derivative Introduction Limits are central to Calculus Present definitions of limits, continuity, and derivative Lecture Notes – Limits, Continuity, and the Deriv Joseph M. Mahaffy, [email protected] — (3/24) Limits Definition Continuity Examples of Limit Derivative Introduction Limits are central to Calculus Present definitions of limits, continuity, and derivative Sketch the formal mathematics for these definitions Lecture Notes – Limits, Continuity, and the Deriv Joseph M. Mahaffy, [email protected] — (3/24) Limits Definition Continuity Examples of Limit Derivative Introduction Limits -
Hegel on Calculus
HISTORY OF PHILOSOPHY QUARTERLY Volume 34, Number 4, October 2017 HEGEL ON CALCULUS Ralph M. Kaufmann and Christopher Yeomans t is fair to say that Georg Wilhelm Friedrich Hegel’s philosophy of Imathematics and his interpretation of the calculus in particular have not been popular topics of conversation since the early part of the twenti- eth century. Changes in mathematics in the late nineteenth century, the new set-theoretical approach to understanding its foundations, and the rise of a sympathetic philosophical logic have all conspired to give prior philosophies of mathematics (including Hegel’s) the untimely appear- ance of naïveté. The common view was expressed by Bertrand Russell: The great [mathematicians] of the seventeenth and eighteenth cen- turies were so much impressed by the results of their new methods that they did not trouble to examine their foundations. Although their arguments were fallacious, a special Providence saw to it that their conclusions were more or less true. Hegel fastened upon the obscuri- ties in the foundations of mathematics, turned them into dialectical contradictions, and resolved them by nonsensical syntheses. .The resulting puzzles [of mathematics] were all cleared up during the nine- teenth century, not by heroic philosophical doctrines such as that of Kant or that of Hegel, but by patient attention to detail (1956, 368–69). Recently, however, interest in Hegel’s discussion of calculus has been awakened by an unlikely source: Gilles Deleuze. In particular, work by Simon Duffy and Henry Somers-Hall has demonstrated how close Deleuze and Hegel are in their treatment of the calculus as compared with most other philosophers of mathematics. -
Limits and Derivatives 2
57425_02_ch02_p089-099.qk 11/21/08 10:34 AM Page 89 FPO thomasmayerarchive.com Limits and Derivatives 2 In A Preview of Calculus (page 3) we saw how the idea of a limit underlies the various branches of calculus. Thus it is appropriate to begin our study of calculus by investigating limits and their properties. The special type of limit that is used to find tangents and velocities gives rise to the central idea in differential calcu- lus, the derivative. We see how derivatives can be interpreted as rates of change in various situations and learn how the derivative of a function gives information about the original function. 89 57425_02_ch02_p089-099.qk 11/21/08 10:35 AM Page 90 90 CHAPTER 2 LIMITS AND DERIVATIVES 2.1 The Tangent and Velocity Problems In this section we see how limits arise when we attempt to find the tangent to a curve or the velocity of an object. The Tangent Problem The word tangent is derived from the Latin word tangens, which means “touching.” Thus t a tangent to a curve is a line that touches the curve. In other words, a tangent line should have the same direction as the curve at the point of contact. How can this idea be made precise? For a circle we could simply follow Euclid and say that a tangent is a line that intersects the circle once and only once, as in Figure 1(a). For more complicated curves this defini- tion is inadequate. Figure l(b) shows two lines and tl passing through a point P on a curve (a) C. -
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. -
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. -
Limits of Functions
Chapter 2 Limits of Functions In this chapter, we define limits of functions and describe some of their properties. 2.1. Limits We begin with the ϵ-δ definition of the limit of a function. Definition 2.1. Let f : A ! R, where A ⊂ R, and suppose that c 2 R is an accumulation point of A. Then lim f(x) = L x!c if for every ϵ > 0 there exists a δ > 0 such that 0 < jx − cj < δ and x 2 A implies that jf(x) − Lj < ϵ. We also denote limits by the `arrow' notation f(x) ! L as x ! c, and often leave it to be implicitly understood that x 2 A is restricted to the domain of f. Note that we exclude x = c, so the function need not be defined at c for the limit as x ! c to exist. Also note that it follows directly from the definition that lim f(x) = L if and only if lim jf(x) − Lj = 0: x!c x!c Example 2.2. Let A = [0; 1) n f9g and define f : A ! R by x − 9 f(x) = p : x − 3 We claim that lim f(x) = 6: x!9 To prove this, let ϵ >p 0 be given. For x 2 A, we have from the difference of two squares that f(x) = x + 3, and p x − 9 1 jf(x) − 6j = x − 3 = p ≤ jx − 9j: x + 3 3 Thus, if δ = 3ϵ, then jx − 9j < δ and x 2 A implies that jf(x) − 6j < ϵ. -
(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). -
MATH M25BH: Honors: Calculus with Analytic Geometry II 1
MATH M25BH: Honors: Calculus with Analytic Geometry II 1 MATH M25BH: HONORS: CALCULUS WITH ANALYTIC GEOMETRY II Originator brendan_purdy Co-Contributor(s) Name(s) Abramoff, Phillip (pabramoff) Butler, Renee (dbutler) Balas, Kevin (kbalas) Enriquez, Marcos (menriquez) College Moorpark College Attach Support Documentation (as needed) Honors M25BH.pdf MATH M25BH_state approval letter_CCC000621759.pdf Discipline (CB01A) MATH - Mathematics Course Number (CB01B) M25BH Course Title (CB02) Honors: Calculus with Analytic Geometry II Banner/Short Title Honors: Calc/Analy Geometry II Credit Type Credit Start Term Fall 2021 Catalog Course Description Reviews integration. Covers area, volume, arc length, surface area, centers of mass, physics applications, techniques of integration, improper integrals, sequences, series, Taylor’s Theorem, parametric equations, polar coordinates, and conic sections with translations. Honors work challenges students to be more analytical and creative through expanded assignments and enrichment opportunities. Additional Catalog Notes Course Credit Limitations: 1. Credit will not be awarded for both the honors and regular versions of a course. Credit will be awarded only for the first course completed with a grade of "C" or better or "P". Honors Program requires a letter grade. 2. MATH M16B and MATH M25B or MATH M25BH combined: maximum one course for transfer credit. Taxonomy of Programs (TOP) Code (CB03) 1701.00 - Mathematics, General Course Credit Status (CB04) D (Credit - Degree Applicable) Course Transfer Status (CB05)