Semester University of Sheffield. School of Mathematics and Statistics

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University of Sheffield School of Mathematics and Statistics MAS140: Mathematics (Chemical) MAS15: Civil Engineering Mathematics MAS15: Essential Mathematical Skills & Techniques MAS156: Mathematics (Electrical and Aerospace) MAS161: General Engineering Mathematics Semester 1 017 18 Outline Syllabus Functions of a real variable. The concept of a function; odd, even and periodic functions; continuity. Binomial theorem. Elementary functions. Circular functions and their inverses. Polynomials. Exponential, logarithmic and hyperbolic functions. Differentiation. Basic rules of differentiation: maxima, minima and curve sketching. Partial differentiation. First and second derivatives, geometrical interpretation. Series. Taylor and Maclaurin series, L Hôpital s rule. Complex numbers. basic manipulation, Argand diagram, de Moivre s theorem, Euler s relation. Vectors. Vector algebra, dot and cross products, differentiation. Module Materials These notes supplement the video lectures. All course materials, including examples sheets (with worked solutions), are available on the course webpage, http://engmaths.group.shef.ac.uk/mas140/ http://engmaths.group.shef.ac.uk/mas151/ http://engmaths.group.shef.ac.uk/mas15/ http://engmaths.group.shef.ac.uk/mas156/ http://engmaths.group.shef.ac.uk/mas161/ which can also be accessed through MOLE. 1

1 Maclaurin and Taylor Series 1.1 Maclaurin Series We say that a function possesses a power series expansion if there exist numbers a 0, a 1 etc., which are independent of x, such that = a 0 + a 1 x + a x + a 3 x 3 (1.1) Suppose that does possess a power series expansion. Then setting x = 0 gives a 0 = f(0). If we further assume that the power series expansion can be differentiated, we have f (x) = a 1 + a x + 3a 3 x, and setting x = 0 in this expression gives a 1 = f (0). Repeating the process (of differentiating and then setting x = 0), we have f (x) = a + 3.a 3 x a = f (0) f (x) = 3.a 3 + 4.3.a 4 x a 3 = f (0) 3. f (4) (x) = 4.3.a 4 a 4 = f (4) (0) 4.3.. The general coefficient in the power series is a n = f (n) (0) for n = 0, 1,, 3,... (Recall that 0!=1 and f (n) is the nth derivative of f.) Having obtained an expression for all the a n, we can substitute these into Eq. (1.1) to obtain = f(0) + f (0)x + f (0) x + f (3) (0) x3 3! = This is the Maclaurin series (or expansion) of f. Examples 1. = e x f (x) = e x f (n) (x) = e x Thus f (n) (0) = 1 for n = 0, 1,,..., and so e x = x n = 1 + x + x + x3 3! f (n) (0)x n

. = sin x f (x) = cos x, f () (x) = sin x, f (3) (x) = cos x, f (4) (x) = sin x,... Therefore f(0) = 0, f (1) (0) = 1, f () (0) = 0, f (3) (0) = 1. Hence Similarly sin x = x x3 3! + x5 5! x7 7! cos x = 1 x + x4 4! x6 6! 3. = (1 + x) 1 Notes f (x) = (1 + x), f () (x) = (1 + x) 3, f (3) (x) =.3(1 + x) 4,... Generally, f (n) (x) = ( 1) n (1 + x) n 1. Hence f (n) (0) = ( 1) n and (1 + x) 1 = 1 x + x x 3 + x 4, (1.) which is just the binomial expansion of (1 + x) 1. The expansion (1.) is only valid for 1 < x < 1. Sometimes the Maclaurin expansion will only be valid for a certain range of x (in extreme cases, only for x = 0). Not all functions have Maclaurin expansions (e.g. x and ln x.) Clearly f must have derivatives of all orders existing at x = 0 in order to have a Maclaurin series (i.e. it must be infinitely differentiable at x = 0). The first few terms of the Maclaurin expansion of a function can give a good approximation to the function for small values of x. This can be of great use in finding approximate solutions to equations. 3

1. Taylor Series The Maclaurin expansion is a special case of Taylor s theorem, which states that f (n) (a)(x a) n = (1.3) for any value of the constant a. Choosing a = 0 results in the Maclaurin expansion. The series (1.3) is referred to as the Taylor expansion (or series) of f about x = a. An equivalent form of the Taylor expansion of about x = a is f (n) (a)x n f(a + x) =. Taylor s theorem can be verified in the same way as the Maclaurin series, by differentiating a power series expansion of (in powers of (x a)) and setting x = a. Notes The functions x does not have a Maclaurin series but does have a Taylor series: x = 1 + x 1 (x 1) 8 + (x 1)3 16 While the function ln x does not have a Maclaurin series, ln(1 + x) does have such an expansion. This is equivalent to the Taylor series of ln x about x = 1: ln(1 + x) = x x + x3 3 x4 4 This is valid for 1 < x 1. If f has a Maclaurin or Taylor series, then that series can always be differentiated (or integrated) any number of times. If the original series is valid for x a < k then all of the series obtained will also be valid for x a < k. 4

1.3 L Hôpital s Rule When evaluating the derivative of a function from first principles, we have to evaluate the it of a ratio of functions that both tend to zero. More generally, we often need to evaluate its of the form x a g(x) when f(a) = 0 = g(a). If both and g(x) are differentiable, and f(a) = 0 = g(a), l Hôpital s rule states that x a g(x) = f (x) x a g (x). Note that one differentiates top and bottom separately. In particular, if g (a) is not zero, then x a g(x) = f (a) g (a). The rule may be proved by using Taylor s theorem. If and g(x) have a Taylor expansion about x = a, then since f(a) = 0 = g(a) we have = f (a)(x a) + f () (a)(x a) g(x) = g (a)(x a) + g() (a)(x a) and so f f () (a)(x a) (a) + g(x) =. g (a) + g() (a)(x a) If g (a) is not zero, then the result follows. If g (a) = 0 then, for the it to exist, f (a) must also be zero and so g(x) = f () (a) g () (a) + f (3) (a)(x a) 3! + g(3) (a)(x a) 3! The validity of the rule can now be seen.. In practice, one continues to differentiate the numerator and denominator until the expression is no longer of the form 0/0. Do not differentiate the expression as a quotient. Differentiate the numerator and denominator separately. 5

The rule also applies when both f and g approach ± as x approaches a. The rule also applies when x ±, i.e. to its of the form x g(x) when f and g either both approach zero as x or both approach infinity as x. If the given problem involves the indeterminate form 0, then this can usually be solved by using some preinary algebra to get the expression into the required form. The rule can be applied to the indeterminate forms 0 0, 0 and 1 by first taking logarithms. The form will certainly require some preinary algebra to cast it into a form suitable for L Hôpital s Rule. Examples 1. sin x x. e x 1 x = cos x 1 e x = 1 3. x 1 x 3 3x + 1 1 + cos(πx) 4. x ex x = 5. x ( 1 x 1 ) x sin x = 1 = x 1 = x e x = 6x 6x π sin(πx) = x 1 x x e x = 1x 6 π cos(πx) = 6 π x sin x x = x sin x cos x 1 = x cos x + x sin x = = ln(sin x) 6. x ln(sin x) = + + x 1 1 = sin x. cos x + x ( x ) = x. + sin x. cos x = 0.1.1 = 0 e x = 0 sin x x sin x + 4x cos x + sin x cos x x cos x 6x sin x + 6 cos x = 1 6 6