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Integration Techniques: Substitution and Integration by Parts, Study notes of Calculus

Two integration techniques: substitution and integration by parts. The substitution method involves changing the variable of integration and adjusting the limits accordingly. The integration by parts formula allows us to express an integral as the product of two functions, their antiderivatives, and a constant. Examples and step-by-step calculations are provided for better understanding.

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Pre 2010

Uploaded on 03/10/2009

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koofers-user-eub 🇺🇸

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Download Integration Techniques: Substitution and Integration by Parts and more Study notes Calculus in PDF only on Docsity! LECTURE THIRTEEN Recall the following result from previous lectures. Corollary 1. Let f(t) be a continuous function [a, b]. If G is an antiderivative of f on [a, b], then b ∫ a f(t)dt = [G(x)]ba = G(b) − G(a). Example: Let m, n be positive integers such that m n 6= −1 and n 6= 0. Then, Since G(x) = ( 1 m n +1 ) x m n +1 is an antiderivative of the function f(x) = x m n , we have that 2 ∫ 1 x m n dx = [( 1 m n + 1 ) x m n +1 ]2 1 = ( 1 m n + 1 ) 2 m n +1− ( 1 m n + 1 ) 1 m n +1 = ( 1 m n + 1 ) (2 m n +1−1). So far we only know the following antiderivatives. (1) ∫ αdx = αx + c, where α is a constant. (2) ∫ x m n dx = 1m n +1 x m n +1 + c. (3) ∫ 1 x dx = ln |x| + c. (4) ∫ exdx = ex + c. Using the above known antiderivatives, we can find the antiderivatives of other func- tions, for example, ∫ (2x + 5 + ex)dx = x2 + 5x + ex + C. So, we have that 1 ∫ 0 2x + 5 + exdx = [ x2 + 5x + ex ]1 0 = (12 + 5(1) + e1) − (02 + 5(0) + e0) = 5 + e. 1. Substitution: Change of Variables Let g be a continuous function on [a, b] such that the derivative g′ is also continuous on [a, b]. Let f be a function which is continuous on g([a, b]). Then, (1.1) b ∫ x=a f(g(x))g′(x)dx = g(b) ∫ u=g(a) f(u)du, 1 2 LECTURE THIRTEEN Example: Evaluate 2 ∫ 1 2x √ x2 − 1dx. We apply the formula (1.1). Let g(x) = x2 − 1, and let f(x) = √x. Then we have that 2 ∫ 1 2x √ x2 − 1dx = 2 ∫ 1 f(g(x))g′(x)dx. Also, F (x) = 2 3 x 3 2 is an antiderivative for f(x) = √ x. Note that, g(1) = 0, g(2) = 3, and g′(x) = 2x So by applying the formula (1.1), we get 2 ∫ 1 2x √ x2 − 1dx = 2 ∫ x=1 f(g(x))g′(x)dx = 3 ∫ u=0 f(u)du = 3 ∫ u=0 u 1 2 du = [ 2 3 u 3 2 ]3 0 = 2 3 [ 3 3 2 − 0 32 ] = 2 3 3 3 2 . In practice, If we have to find an integral of the form (1.2) b ∫ x=a f(g(x))g′(x)dx, then it is helpful to follow the following steps. We let u = g(x), and then du = g′(x)dx, and we change the limits of integration a and b by g(a) and g(b). Then the integral equals g(b) ∫ u=g(a) f(u)du. Example: Evaluate 2 ∫ x=1 2xex 2 dx Let u = x2. Then du = 2xdx, and 2 ∫ x=1 2xex2dx = 4 ∫ u=1 eudu = [eu]41 = e 4 − e1 = e4 − e. Remark: The above method can also be used to find antiderivatives. Note that an antiderivative of a function of the form f(g(x))g′(x) is F (g(x) where F (x) is an antiderivative of f(x). This follows from the chain rule. We write this in the following way. ∫ f(g(x))g′(x)dx = F (g(x) + c. In practice it is helpful to follow the steps below in order to find the antiderivative ∫ f(g(x))g′(x)dx. We let u = g(x) and then du = g′(x)dx, to get ∫ f(g(x))g′(x)dx = ∫ f(u)du = F (u) + c = F (g(x)) + c.
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