klm Version 1.2 1106 Changes include the amendment of section 5.7 for the 2007 (onwards) specification and some minor formatting changes. Please note that these are not side-barred. GCE Mathematics (6360) Further Pure unit 3 (MFP3) Textbook The Assessment and Qualifications Alliance (AQA) is a company limited by guarantee registered in England and Wales 3644723 and a registered charity number 1073334. Registered address AQA, Devas Street, Manchester M15 6EX. Dr Michael Cresswell Director General. Copyright ' 2006 AQA and its licensors. All rights reserved. klm GCE Further Mathematics (6370) Further Pure 3 (MFP3) Textbook Further Pure 3: Contents Introduction 3 Chapter 1: Series and limits 4 1.1 The concept of a limit 5 1.2 Finding limits in simple cases 6 1.3 Maclaurin(cid:146)s series expansion 9 1.4 Range of validity of a series expansion 14 1.5 The basic series expansions 16 1.6 Use of series expansions to find limits 21 1.7 Two important limits 25 1.8 Improper integrals 29 Chapter 2: Polar coordinates 37 2.1 Cartesian and polar frames of reference 38 2.2 Restrictions on the value of θ 39 2.3 The relationship between Cartesian and polar coordinates 40 2.4 Representation of curves in polar form 41 2.5 Curve sketching 43 2.6 The area bounded by a polar curve 47 Chapter 3: Introduction to differential equations 54 3.1 The concept of a differential equation: order and linearity 55 3.2 Families of solutions, general solutions and particular solutions 57 3.3 Analytical solution of first order linear differential equations: integrating factors 61 3.4 Complementary functions and particular integrals 65 3.5 Transformations of non-linear differential equations to linear form 71 Chapter 4: Numerical methods for the solution of first order differential equations 75 4.1 Introduction 76 4.2 Euler(cid:146)s formula 78 4.3 The mid-point formula 81 4.4 The improved Euler formula 84 4.5 Error analysis: some practical considerations 89 Chapter 5: Second order differential equations 96 5.1 Introduction to complex numbers 97 5.2 Working with complex numbers 98 5.3 Euler(cid:146)s identity 101 5.4 Formation of second order differential equations 103 2 d y dy 5.5 Differential equations of the form a +b +cy =0 105 dx2 dx d2y dy 5.6 Differential equations of the form a +b +cy = f(x) 112 dx2 dx 5.7 Second order linear differential equations with variable coefficients 119 Answers to the exercises in Further Pure 3 133 2 klm GCE Further Mathematics (6370) Further Pure 3 (MFP3) Textbook Further Pure 3: Introduction The aim of this text is to provide a sound and readily accessible account of the items comprising the Further Pure Mathematics unit 3. The chapters are arranged in the same order as the five main sections of the unit. The first chapter is therefore concerned with series expansions and the evaluation of limits and improper integrals. The second covers polar coordinates and their use in curve sketching and evaluation of areas. The subject of differential equations forms a major part of this unit and Chapters 3, 4 and 5 are devoted to this topic. Chapter 3 introduces the subject and deals mainly with analytical methods for solving differential equations of first order linear form. In addition to the standard method of solution using an integrating factor, this chapter introduces the method based on finding a complementary function and a particular integral. This provides useful preparation for Chapter 5 where the same technique is used for solving second order differential equations. With the advent of modern computers, numerical methods have become an essential practical tool for solving the many differential equations which cannot be solved by analytical methods. This important subject is covered in Chapter 4 in relation to differential equations of the form y′=f(x,y). It should be appreciated that, in practice, the numerical methods described would be carried out with the aid of a computer using an appropriate program. The purpose of the worked examples and exercises in this text is to exemplify the principles of the various methods and to show how these methods work. Relatively simple functions have been chosen, as far as possible, so that the necessary calculations with a scientific calculator are not unduly tedious. Chapter 5 deals with analytical methods for solving second order differential equations and this requires some knowledge of complex numbers. Part of the required knowledge is included in the Further Pure 1 module, which is a prerequisite for studying this module, and the remainder is included in the Further Pure 2 module which is not a prerequisite. For both simplicity and completeness therefore, Chapter 5 begins with three short sections on complex numbers which cover, in a straightforward way, all that is required for the purpose of this chapter. These sections should not cause any difficulty and it is hoped that they will be found interesting as well as useful. Those who have already studied the topics covered can either pass over this work or regard it as useful revision. The main methods for solving second order linear differential equations with constant coefficients are covered in Sections 5.5. and 5.6. These methods sometimes seem difficult when first met, but students should not be discouraged by this. Useful summaries are highlighted in the text and confidence should be restored by studying how these are applied in the worked examples and by working through the exercises. The text concludes with a short section showing how some second order linear differential equations with variable coefficients can be solved by using a substitution to transform them to simpler forms. 3 klm GCE Further Mathematics (6370) Further Pure 3 (MFP3) Textbook Chapter 1: Series and Limits 1.1 The concept of a limit 1.2 Finding limits in simple cases 1.3 Maclaurin(cid:146)s series expansion 1.4 Range of validity of a series expansion 1.5 The basic series expansions 1.6 Use of series expansions to find limits 1.7 Two important limits 1.8 Improper integrals In this chapter, it is shown how series expansions are used to find limits and how improper integrals are evaluated. When you have completed it you will: • have been reminded of the concept of a limit; • have been reminded of methods for finding limits in simple cases; • know about Maclaurin(cid:146)s series expansion; • be able to use series expansions to find certain limits; • know about the limits of xke−x as x→∞ and xk lnx as x→0; • know the definition of an improper integral; • know how to evaluate improper integrals by finding a limit. 4 klm GCE Further Mathematics (6370) Further Pure 3 (MFP3) Textbook 1.1 The concept of a limit You will have already met the idea of a limit and be familiar with some of the notation used. If x is a real number which varies in such a way that it gets closer and closer to a particular value a , but is never equal to a , then this is signified by writing x→a. More precisely, the variation of x must be such that for any positive number, δ , x can be chosen so that 0< x−a <δ , no matter how small δ may be. When a function f(x) is such that f(x)→l when x→a , where l is finite, the number l is called the limit or limiting value of f(x) as x→a . This may be expressed as lim f(x)=l . x→a The statements x→∞ and f(x)→∞ mean that x and f(x) increase indefinitely (cid:150) i.e. that their values increase beyond any number we care to name, however large. Note that you should never write x=∞ or f(x)=∞ , because ∞ is not a number. Unless stated or implied otherwise, x→a means that x can approach a from either side. Occasionally however, it may be necessary to distinguish between x approaching a from the right, so that x>a always and x approaching a from the left, so that x<a always. The notation x→a+ is used to signify that x approaches a from the right, and x→a− to signify that x approaches a from the left. The two cases are illustrated in the diagram below. The distinction between the two cases is important, for instance, when we consider the 1 1 1 behaviour of as x→0 . When x→0+, →∞ ; but when x→0−, →−∞ . x x x The use of + or − attached to a is unneccessary when it is clear from the context that the approach to a can only be from one particular side. For example, since lnxis defined only for x>0 , one can write lnx→−∞ as x→0 without ambiguity: the fact that x approaches 0 from the right is implied in this case so it is unneccessary to write x→0+ . 5 klm GCE Further Mathematics (6370) Further Pure 3 (MFP3) Textbook 1.2 Finding limits in simple cases In some simple cases, it is easy to see how a function f(x) behaves as x approaches a given value and whether it has a limit. Here are three examples. 1+x 1 1. As x→0 , → because 1+x→1 and 2−x→2 as x→0 . 2−x 2 π sinx π 2. As x→ , →1 , because sinx→1 and cosx→0 as x→ . 2 1−cosx 2 1+x 3. As x→1+ , →−∞ , because 1+x→2+ and 1−x→0− as x→1+ . 1−x The first two of the above examples can be expressed as: 1+x 1 sinx lim = and lim =1 x→0 2−x 2 x→π 1−cosx 2 However, it would be wrong to state that 1+x lim =−∞ , x→1+1−x 1+x because a limit has to be finite. The function does not have a limiting value as x→1+ . 1−x Another example, not quite so straightforward as the examples above, is that of finding the 1+x limit as x→∞ of f(x)= . 1−2x ∞ As x→∞ , 1+x→∞ and 1−2x→−∞ , but the expression is meaningless. This −∞ difficulty can be overcome by first dividing the numerator and denominator of f(x) by x , giving 1 +1 x f(x)= . 1 −2 x 1 1 It can now be seen that f(x)→ as x→∞ because →0 . The limiting value of f(x) is −2 x 1 therefore − . 2 6 klm GCE Further Mathematics (6370) Further Pure 3 (MFP3) Textbook The working for this example can be presented more concisely as follows. 1 +1 1+x x f(x)= = . 1−2x 1 −2 x 1 As x→∞, →0 . Hence x 1 1 limf(x)= =− . x→∞ −2 2 There are many instances where the behaviour of a function is much more difficult to determine than in the cases considered above. For example, consider f(x)= x2lnx as x→0 . When x→0 , x2 →0 and lnx→−∞ . It is not obvious therefore what happens to the product of x2 and lnx as x→0 . Consider also the function x f(x)= . 1− 1−x 0 When x→0 , f(x)→ which is an indeterminate form having no mathematical meaning. 0 Although f(x) does not have a value at x=0 , it does approach a limiting value as x→0 . Investigating with a calculator will produce the following results, to five decimal places. f(0.1)=1.94868 , f(−0.1)=2.04881 , f(0.01)=1.99499 , f(−0.01)=2.00499 , f(0.001)=1.99950 , f(−0.001)=2.00050 . It can be seen from these results that f(x) appears to be approaching the value 2 as x→0+ and x→0− ; the limit is, in fact, exactly 2 as you would expect. However, no matter how convincing the evidence may seem, a numerical investigation of this kind does not constitute a satisfactory mathematical proof. Limits in these more difficult cases can often be found with the help of series expansions. The series expansions that we shall use are introduced in the next three sections of this chapter. 7 klm GCE Further Mathematics (6370) Further Pure 3 (MFP3) Textbook Exercise 1A 1. Write down the missing values, indicated by ∗ , in the following. 2+x 1+x (a) As x→0 , →∗ , (b) As x→2 , →∗ , 2−x 1−x π x π x (c) As x→ − , →∗ , (d) As x→ + , →∗ . 2 tanx 2 tanx 2. Explain why lnx does not have a limiting value as x→0 . 3. Write down the values of the following limits. x lnx (a) lim , (b) lim . x→π 1+sinx x→11+lnx 2 4. Find the values of the following. 3+2x x (a) lim , (b) lim , x→∞ 2+3x x→∞ 2x+3 1+x−x2 x2 +2 (c) lim , (d) lim . x→∞1−x+2x2 x→∞ x3+3 5. Use a calculator to investigate the behaviour of x0.01lnx as x→0 . You will find it difficult to guess from this investigation what happens as x→0 . Later in this chapter, it will be shown that the function tends to zero. 8 klm GCE Further Mathematics (6370) Further Pure 3 (MFP3) Textbook 1.3 Maclaurin(cid:146)s series expansion You will already be familiar with the binomial series expansion for (1+x)n : n(n−1) n(n−1)(n−2) (1+x)n =1+nx+ x2 + x3+... . 2! 3! Many other functions, such as ex , ln(1+x) , sinx and cosx can also be expressed as series in ascending powers of x . Such expansions are called Maclaurin series. The Maclaurin series for a function f(x) is given by: f′′(0) f′′′(0) f(r)(0) f(x)=f(0)+f′(0)x+ x2 + x3+...+ xr +... , 2! 3! r! where f′ , f′′ , f′′′ , (cid:133) denote the first, second, third, (cid:133) derivatives of f , respectively, and f(r) is the general derivative of order r . To derive this, the following assumptions are made. (i) The function f(x) can be expressed as a series of the form f(x)=a +a x+a x2 +a x3+a x4 +...+a xr +... , 0 1 2 3 4 r where a , a , a , a , a , (cid:133)a , (cid:133)are constants. 0 1 2 3 4 r (ii) The series can be differentiated term by term. (iii) The function f(x) and all its derivatives exist at x=0 . Succesive differentiations of each side of the equation under (i) gives f′(x)=a +2a x+3a x2 +4a x3+... , 1 2 3 4 f′′(x)=2a +2×3a x+3×4a x2 +... , 2 3 4 f′′′(x)=2×3a +2×3×4a x+... , 3 4 and, in general, f(r)(x)=2×3×...×(r−1)×ra + terms in x , x2 , x3(cid:133) . r 9 klm GCE Further Mathematics (6370) Further Pure 3 (MFP3) Textbook Putting x=0 in the expressions for f(x) and its derivatives, we see that a =f(0) , a =f′(0) 0 1 f′′(0) f′′(0) a = = , 2 2 2! f′′′(0) f′′′(0) a = = , 3 2×3 3! and, in general, f(r)(0) f(r)(0) a = = . r 1.2.3...(r−1)r r! Substituting these values into the series in (i) above gives the Maclaurin series of f(x) . The statement that f(x) can be expressed as a Maclaurin series, subject to conditions (i) (cid:150) (iii) above being satisfied, is often referred to as Maclaurin(cid:146)s theorem. The Maclaurin series has an interesting history. It is named in honour of Colin Maclaurin, a notable Scottish mathematician. Born in 1698, he was a child prodigy who entered university at the age of 11 and became a professor at the age of 19. He was personally acquainted with Newton and made significant contributions to the development of Newton(cid:146)s pioneering work in Calculus. The series which bears Maclaurin(cid:146)s name was not discovered by Maclaurin (cid:150) a fact that he readily acknowledged (cid:150) but is a special case of a more general expansion called Taylor(cid:146)s series (see exercise 1B, question 6). 10