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5.6: 18 Use the substitution formula in Theorem 7 to evaluate the integral: 3π/2 Z cot5 (θ/6) sec2 (θ/6) dθ. π Sometimes its just best to simplify first. Recall that cot x = cos x/ sin x, and that sec x = 1/ cos x. Then we can reduce this to: Z 3π/2 Z 3π/2 −1 5 2 3 2 cot (θ/6) sec (θ/6) dθ = −6 cot (θ/6) csc (θ/6) dθ 6 π π d cot x = − csc2 x. Then we see that we should let u = cot(θ/6), whereby du = − 16 csc2 (θ/6) dθ. Recall that dx Then upon the use of the substitution formula: 1 Z 3π/2 Z u(3π/2) −1 u4 3 2 3 −6 cot (θ/6) = 12. csc (θ/6) dθ = −6 u du = 6 4 √3 π u(π/2) 5.6: 32 Use the substitution formula in Theorem 7 to evaluate the integral: Z 16 dx √ . 2x ln x 2 Here we let u = ln x, so du = 1 x Z dx: 16 2 dx 1 √ = 2 2x ln x Z u ln 16 (2)u(16) u−1/2 du = u1/2 . ln 2 4 Before simplifying further, notice that ln 16 = ln 2 = 4 ln 2. Then: ln 16 √ √ √ 1/2 = 4 ln 2 − ln 2 = ln 2. u ln 2 5.6: 52 Find the area shown in the book. The formula for the area will be: π/3 Z A= −π/3 1 2 2 sec t − −4 sin t dt 2 Simplifying a little bit, we get: A= 1 2 Z π/3 sec2 t dt + 4 Z π/3 −π/3 −π/3 1 sin2 t dt. The first integral can be evaluated as follows: Z π/3 π/3 √ sec t dt = tan t = 2 3. 2 −π/3 −π/3 The second integral requires the use of a half angle formula: Z π/3 sin2 t dt = −π/3 1 2 Z π/3 (1 − cos 2t) dt = −π/3 √ 1 4π − 3 3 . 12 Combining these results, we get: A= √ 4π 1 √ 1 2 3 +4 4π − 3 3 = . 2 12 3 5.6: 100 Find the area of the “triangular” region in the first quadrant that is bounded above by the curve y = ex/2 , below by the curve y = e−x/2 , and on the right by the line 2 ln 2. Be sure that, for a problem of this form, you can sketch the given regions and understand what they look like. The area is given by: Z 2 ln 2 A= e x/2 −e −x/2 dx = 2e x/2 + 2e −x/2 0 2 ln 2 1 = 2 2 − 1 + − 1 = 1. 2 0 5.6: 114 (a) Show that if f is odd on [−a, a], then Z a f (x) dx = 0. −a (b) Test the result in part (a) with f (x) = sin x and a = π/2. I’ll verify part (a). Part (b) should be fairly straightforward. Let’s try to compute substitution u = −x, du = −dx: Z 0 Z u(0) f (x) dx = −a Z u(−a) 0 a −a f (x) dx by using the a Z f (u) du = − f (−u) (−du) = R0 f (u) du. 0 The second to last step follows from the fact that since f is an odd function, f (−u) = −f (u), and the last step from inverting the order of the bounds. Now u is just a dummy index, so we can relabel it x if we like. Then: Z a Z 0 Z a Z a Z a f (x) dx = f (x) dx + f (x) dx = − f (x) dx + f (x) dx = 0. −a −a 0 0 2 0