3 Sums and Integrals
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Riemann Sums Fundamental Theorem of Calculus Indefinite
Riemann Sums Partition P = {x0, x1, . , xn} of an interval [a, b]. ck ∈ [xk−1, xk] Pn R(f, P, a, b) = k=1 f(ck)∆xk As the widths ∆xk of the subintervals approach 0, the Riemann Sums hopefully approach a limit, the integral of f from a to b, written R b a f(x) dx. Fundamental Theorem of Calculus Theorem 1 (FTC-Part I). If f is continuous on [a, b], then F (x) = R x 0 a f(t) dt is defined on [a, b] and F (x) = f(x). Theorem 2 (FTC-Part II). If f is continuous on [a, b] and F (x) = R R b b f(x) dx on [a, b], then a f(x) dx = F (x) a = F (b) − F (a). Indefinite Integrals Indefinite Integral: R f(x) dx = F (x) if and only if F 0(x) = f(x). In other words, the terms indefinite integral and antiderivative are synonymous. Every differentiation formula yields an integration formula. Substitution Rule For Indefinite Integrals: If u = g(x), then R f(g(x))g0(x) dx = R f(u) du. For Definite Integrals: R b 0 R g(b) If u = g(x), then a f(g(x))g (x) dx = g(a) f( u) du. Steps in Mechanically Applying the Substitution Rule Note: The variables do not have to be called x and u. (1) Choose a substitution u = g(x). du (2) Calculate = g0(x). dx du (3) Treat as if it were a fraction, a quotient of differentials, and dx du solve for dx, obtaining dx = . -
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. -
Writing Mathematical Expressions in Plain Text – Examples and Cautions Copyright © 2009 Sally J
Writing Mathematical Expressions in Plain Text – Examples and Cautions Copyright © 2009 Sally J. Keely. All Rights Reserved. Mathematical expressions can be typed online in a number of ways including plain text, ASCII codes, HTML tags, or using an equation editor (see Writing Mathematical Notation Online for overview). If the application in which you are working does not have an equation editor built in, then a common option is to write expressions horizontally in plain text. In doing so you have to format the expressions very carefully using appropriately placed parentheses and accurate notation. This document provides examples and important cautions for writing mathematical expressions in plain text. Section 1. How to Write Exponents Just as on a graphing calculator, when writing in plain text the caret key ^ (above the 6 on a qwerty keyboard) means that an exponent follows. For example x2 would be written as x^2. Example 1a. 4xy23 would be written as 4 x^2 y^3 or with the multiplication mark as 4*x^2*y^3. Example 1b. With more than one item in the exponent you must enclose the entire exponent in parentheses to indicate exactly what is in the power. x2n must be written as x^(2n) and NOT as x^2n. Writing x^2n means xn2 . Example 1c. When using the quotient rule of exponents you often have to perform subtraction within an exponent. In such cases you must enclose the entire exponent in parentheses to indicate exactly what is in the power. x5 The middle step of ==xx52− 3 must be written as x^(5-2) and NOT as x^5-2 which means x5 − 2 . -
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. -
The Definite Integrals of Cauchy and Riemann
Ursinus College Digital Commons @ Ursinus College Transforming Instruction in Undergraduate Analysis Mathematics via Primary Historical Sources (TRIUMPHS) Summer 2017 The Definite Integrals of Cauchy and Riemann Dave Ruch [email protected] Follow this and additional works at: https://digitalcommons.ursinus.edu/triumphs_analysis Part of the Analysis Commons, Curriculum and Instruction Commons, Educational Methods Commons, Higher Education Commons, and the Science and Mathematics Education Commons Click here to let us know how access to this document benefits ou.y Recommended Citation Ruch, Dave, "The Definite Integrals of Cauchy and Riemann" (2017). Analysis. 11. https://digitalcommons.ursinus.edu/triumphs_analysis/11 This Course Materials is brought to you for free and open access by the Transforming Instruction in Undergraduate Mathematics via Primary Historical Sources (TRIUMPHS) at Digital Commons @ Ursinus College. It has been accepted for inclusion in Analysis by an authorized administrator of Digital Commons @ Ursinus College. For more information, please contact [email protected]. The Definite Integrals of Cauchy and Riemann David Ruch∗ August 8, 2020 1 Introduction Rigorous attempts to define the definite integral began in earnest in the early 1800s. A major motivation at the time was the search for functions that could be expressed as Fourier series as follows: 1 a0 X f (x) = + (a cos (kw) + b sin (kw)) where the coefficients are: (1) 2 k k k=1 1 Z π 1 Z π 1 Z π a0 = f (t) dt; ak = f (t) cos (kt) dt ; bk = f (t) sin (kt) dt. 2π −π π −π π −π P k Expanding a function as an infinite series like this may remind you of Taylor series ckx from introductory calculus, except that the Fourier coefficients ak; bk are defined by definite integrals and sine and cosine functions are used instead of powers of x. -
How to Write Mathematical Papers
HOW TO WRITE MATHEMATICAL PAPERS BRUCE C. BERNDT 1. THE TITLE The title of your paper should be informative. A title such as “On a conjecture of Daisy Dud” conveys no information, unless the reader knows Daisy Dud and she has made only one conjecture in her lifetime. Generally, titles should have no more than ten words, although, admittedly, I have not followed this advice on several occasions. 2. THE INTRODUCTION The Introduction is the most important part of your paper. Although some mathematicians advise that the Introduction be written last, I advocate that the Introduction be written first. I find that writing the Introduction first helps me to organize my thoughts. However, I return to the Introduction many times while writing the paper, and after I finish the paper, I will read and revise the Introduction several times. Get to the purpose of your paper as soon as possible. Don’t begin with a pile of notation. Even at the risk of being less technical, inform readers of the purpose of your paper as soon as you can. Readers want to know as soon as possible if they are interested in reading your paper or not. If you don’t immediately bring readers to the objective of your paper, you will lose readers who might be interested in your work but, being pressed for time, will move on to other papers or matters because they do not want to read further in your paper. To state your main results precisely, considerable notation and terminology may need to be introduced. -
9.4 Arithmetic Series Notes
9.4 Arithmetic Series Notes PreAP Algebra 2 9.4 Arithmetic Series *Objective: Define arithmetic series and find their sums When you know two terms and the number of terms in a finite arithmetic sequence, you can find the sum of the terms. A series is the indicated sum of the terms of a sequence. A finite series has a first terms and a last term. An infinite series continues without end. Finite Sequence Finite Series 6, 9, 12, 15, 18 6 + 9 + 12 + 15 + 18 = 60 Infinite Sequence Infinite Series 3, 7, 11, 15, ... 3 + 7 + 11 + 15 + ... An arithmetic series is a series whose terms form an arithmetic sequence. When a series has a finite number of terms, you can use a formula involving the first and last term to evaluate the sum. The sum Sn of a finite arithmetic series a1 + a2 + a3 + ... + an is n Sn = /2 (a1 + an) a1 : is the first term an : is the last term (nth term) n : is the number of terms in the series Finding the Sum of a finite arithmetic series Ex1) a. What is the sum of the even integers from 2 to 100 b. what is the sum of the finite arithmetic series: 4 + 9 + 14 + 19 + 24 + ... + 99 c. What is the sum of the finite arithmetic series: 14 + 17 + 20 + 23 + ... + 116? Using the sum of a finite arithmetic series Ex2) A company pays $10,000 bonus to salespeople at the end of their first 50 weeks if they make 10 sales in their first week, and then improve their sales numbers by two each week thereafter. -
On the Approximation of Riemann-Liouville Integral by Fractional Nabla H-Sum and Applications L Khitri-Kazi-Tani, H Dib
On the approximation of Riemann-Liouville integral by fractional nabla h-sum and applications L Khitri-Kazi-Tani, H Dib To cite this version: L Khitri-Kazi-Tani, H Dib. On the approximation of Riemann-Liouville integral by fractional nabla h-sum and applications. 2016. hal-01315314 HAL Id: hal-01315314 https://hal.archives-ouvertes.fr/hal-01315314 Preprint submitted on 12 May 2016 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. On the approximation of Riemann-Liouville integral by fractional nabla h-sum and applications L. Khitri-Kazi-Tani∗ H. Dib y Abstract First of all, in this paper, we prove the convergence of the nabla h- sum to the Riemann-Liouville integral in the space of continuous functions and in some weighted spaces of continuous functions. The connection with time scales convergence is discussed. Secondly, the efficiency of this approximation is shown through some Cauchy fractional problems with singularity at the initial value. The fractional Brusselator system is solved as a practical case. Keywords. Riemann-Liouville integral, nabla h-sum, fractional derivatives, fractional differential equation, time scales convergence MSC (2010). 26A33, 34A08, 34K28, 34N05 1 Introduction The numerous applications of fractional calculus in the mathematical modeling of physical, engineering, economic and chemical phenomena have contributed to the rapidly growing of this theory [12, 19, 21, 18], despite the discrepancy on definitions of the fractional operators leading to nonequivalent results [6]. -
Summation and Table of Finite Sums
SUMMATION A!D TABLE OF FI1ITE SUMS by ROBERT DELMER STALLE! A THESIS subnitted to OREGON STATE COLlEGE in partial fulfillment of the requirementh for the degree of MASTER OF ARTS June l94 APPROVED: Professor of Mathematics In Charge of Major Head of Deparent of Mathematics Chairman of School Graduate Committee Dean of the Graduate School ACKOEDGE!'T The writer dshes to eicpreßs his thanks to Dr. W. E. Mime, Head of the Department of Mathenatics, who has been a constant guide and inspiration in the writing of this thesis. TABLE OF CONTENTS I. i Finite calculus analogous to infinitesimal calculus. .. .. a .. .. e s 2 Suniming as the inverse of perfornungA............ 2 Theconstantofsuirrnation......................... 3 31nite calculus as a brancn of niathematics........ 4 Application of finite 5lflITh1tiOfl................... 5 II. LVELOPMENT OF SULTION FORiRLAS.................... 6 ttethods...........................a..........,.... 6 Three genera]. sum formulas........................ 6 III S1ThATION FORMULAS DERIVED B TIlE INVERSION OF A Z FELkTION....,..................,........... 7 s urnmation by parts..................15...... 7 Ratlona]. functions................................ Gamma and related functions........,........... 9 Ecponential and logarithrnic functions...... ... Thigonoretric arÎ hyperbolic functons..........,. J-3 Combinations of elementary functions......,..... 14 IV. SUMUATION BY IfTHODS OF APPDXIMATION..............,. 15 . a a Tewton s formula a a a S a C . a e a a s e a a a a . a a 15 Extensionofpartialsunmation................a... 15 Formulas relating a sum to an ifltegral..a.aaaaaaa. 16 Sumfromeverym'thterm........aa..a..aaa........ 17 V. TABLE OFST.Thß,..,,..,,...,.,,.....,....,,,........... 18 VI. SLThMTION OF A SPECIAL TYPE OF POER SERIES.......... 26 VI BIBLIOGRAPHY. a a a a a a a a a a . a . a a a I a s . -
Using the TI-89 to Find Riemann Sums
Using the TI-89 to find Riemann sums Z b If function f is continuous on interval [a, b], f(x) dx exists and can be approximated a using either of the Riemann sums n n X X f(xi)∆x or f(xi−1)∆x i=1 i=1 (b−a) where ∆x = n and n is the number of subintervals chosen. The first of these Riemann sums evaluates function f at the right endpoint of each subinterval; the second evaluates at the left endpoint of each subinterval. n X P To evaluate f(xi) using the TI-89, go to F3 Calc and select 4: ( sum i=1 The command line should then be completed in the following form: P (f(xi), i, 1, n) The actual Riemann sum is then determined by multiplying this ans by ∆x (or incorpo- rating this multiplication into the same command line.) [Warning: Be sure to set the MODE as APPROXIMATE in this case. Otherwise, the calculator will spend an inordinate amount of time attempting to express each term of the summation in exact symbolic form.] Z 4 √ Example: To approximate 1 + x3 dx using Riemann sums with n = 100 subinter- 2 b−a 2 i vals, note first that ∆x = n = 100 = .02. Also xi = 2 + i∆x = 2 + 50 . So the right endpoint approximation will be found by entering √ P( (2 + (1 + i/50)∧3), i, 1, 100) × .02 which gives 10.7421. This is an overestimate, since the function is increasing on the given interval. To find the left endpoint approximation, replace i by (i − 1) in the square root part of the command. -
Fractional Calculus
Generalised Fractional Calculus Penelope Drastik Supervised by Marianito Rodrigo September 2018 Outline 1. Integration 2. Fractional Calculus 3. My Research Riemann sum: P tagged partition, f :[a; b] ! R n X S(f ; P) = f (ti )(xi − xi−1) i=1 The Riemann sum Partition of [a; b]: Non-overlapping intervals which cover [a; b] a = x0 < x1 < ··· < xi−1 < xi < ··· xn = b Tagged partition of [a; b]: Intervals in partition paired with tag points n P = f([xi−1; xi ]; ti )gi=1 The Riemann sum Partition of [a; b]: Non-overlapping intervals which cover [a; b] a = x0 < x1 < ··· < xi−1 < xi < ··· xn = b Tagged partition of [a; b]: Intervals in partition paired with tag points n P = f([xi−1; xi ]; ti )gi=1 Riemann sum: P tagged partition, f :[a; b] ! R n X S(f ; P) = f (ti )(xi − xi−1) i=1 The Riemann integral R b a f (x)dx = A means that: For all " > 0, there exists δ" > 0 such that if a tagged partition P satisfies 0 < xi − xi−1 < δ" for i = 1;:::; n then jS(f ; P) − Aj < " The Generalised Riemann integral R b a f (x)dx = A means that: For all " > 0, there exists a strictly positive function δ" :[a; b] ! R+ such that if a tagged partition P satisfies ti 2 [xi−1; xi ] ⊆ [ti − δ(ti ); ti + δ(ti )] for i = 1;:::; n then jS(f ; P) − Aj < " Riemann-Stieltjes integral: R b a f (x)dα(x) = A means that: For all " > 0, there exists δ" > 0 such that if a tagged partition P satisfies 0 < xi − xi−1 < δ" for i = 1;:::; n then jS(f ; P; α) − Aj < " The Riemann-Stieltjes integral Riemann-Stieltjes sum of f : Integrator α : I ! R, partition P n X S(f ; P; α) = f (ti )[α(xi -
1.1 Limits: an Informal View 4.1 Areas and Sums
Chapter 4 Integrals from Calculus: Concepts & Computation by David Betounes and Mylan Redfern | 2016 Copyright | 9781524917692 Property of Kendall Hunt Publishing 4.1 Areas and Sums 257 4 Integrals Calculus Concepts & Computation 1.1 Limits: An Informal View 4.1 Areas and Sums > with(code_ch4,circle,parabola);with(code_ch1sec1); [circle, parabola] [polygonlimit, secantlimit] This chapter begins our study of the integral calculus, which is the counter-part to the differential calculus you learned in Chapters 1–3. The topic of integrals, otherwise known as antiderivatives, was introduced in Section 3.7, and you should The General Area Problem read that discussion before continuing here. A major application of antiderivatives, or integrals, is the measurement of areas of planar regions D. In fact, a principal motive behind the invention of the integral calculus was to solve the area problem. See Figure 4.1.1. D Before we learn how to measure areas of such general regions D, it is best to think about the areas of simple regions, and, indeed, reflect on the very notion of what is meant by “area.” This we discuss here. Then, in the next two sections, Sections 4.2 and 4.3 , we look at the details of measuring areas of regions “beneath the graphs of continuous functions.” Then in Section 5.1 we tackle the task of finding area of more complicated regions, such as the region D in Figure 4.4.1. We have intuitive notions about what is meant by the area of a region. It is a positive Find the area Figure 4.1.1: number A which somehow measures the “largeness” of the region and enables us of the region D bounded by a to compare regions with different shapes.