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SOLUTIONS TO 18.01 EXERCISES 2. Applications of Differentiation 2A. Approximation d √ b √ b 2A-1 dx a + bx = √ ⇒ f(x) ≈ a + √ x by formula. 2 a + bx 2 a � √ √ bx √ bx By algebra: a + bx = a 1+ ≈ a(1 + ), same as above. a 2a 2A-2 D( 1 ) = −b ⇒ f(x) ≈ 1 − b x; OR: 1 = 1/a ≈ 2 2 a + bx (a + bx) a a a + bx 1+ b/ax 1 b (1 − x). a a 3/2 3 3/2 3/2 (1 + x) (1+2x) · 2 · (1 + x) − (1 + x) · 2 � 1 2A-3 D( 1+2x )= (1 + 2x)2 ⇒ f (0) = − 2 3/2 1 (1 + x) 3 1 ⇒ f(x) ≈ 1− x; OR, by algebra, ≈ (1+ x)(1−2x) ≈ 1− x. 2 1 + 2x 2 2 h g 2 2h 2A-4 Put R = �; then w = (1+ �)2 ≈ g(1 − �) ≈ g(1 − 2�) = g(1 − R ). 2A-5 A reasonable assumption is that w is propotional to volume v, which is in turn proportional to the cube of a linear dimension, i.e., a given person remains 3; since 5 feet = 60 similar to him/herself, for small weight changes.) Thus w = Ch inches, we get w(60 + �) C(60 + �)3 � 3 3� 1 = 3 = (1+ ) ⇒ w(60+�) ≈ w(60)·(1+ ) ≈ 120·(1+ ) ≈ 126. w(60) C(60) 60 60 20 [Or you can calculate the linearization of w(h) arround h = 60 using derivatives, and using the value w(60) to determine C. getting w(h) ≈ 120 + 6(h − 60) COPYRIGHT DAVID JERISON AND MIT 1996, 2003 1 E. Solutions to 18.01 Exercises 2. Applications of Differentiation 2A-6 tan θ = sin θ ≈ θ ≈ θ(1 + θ2//2) ≈ θ cos θ 1 − θ2/2 sec x 1 1 1 2 2A-7 √ 2 = √ 2 ≈ 1 2 1 2 ≈ 1 − x2 ≈ 1+ x 1 − x cos x 1 − x (1 − x )(1 − x ) 2 2 2A-8 1 = 1 = 1 = 2 1 − x 1 1 1 − 2Δx 1 − ( +Δx) − Δx 2 2 2 1 1 2 ≈ 2(1 + 2Δx + 4(Δx) ) ≈ 2 + 4(x − ) + 8(x − ) 2 2 r � r−1 �� r−2 2A-10 y = (1+ x) ,y = r(1 + x) , y = r(r − 1)(1 + x) � �� r Therefore y(0) = 1,y (0) = r,y (0) = r(r − 1), giving (1 + x) ≈ 1 + rx + r(r − 1) 2 2 x . k −k −k −k Δv −k 2A-11 pv = c ⇒ p = cv = c((v +Δv) = cv (1 + ) 0 0 v 0 c Δv k(k + 1) Δv 2 ≈ v k (1 − k v + 2 ( v ) ) 0 0 0 ex x2 5 2 2 2A-12 a) ≈ (1 + x + )(1 + x + x ) ≈ 1 +2x + x 1 − x 2 2 b) ln(1 + x) ≈ x ≈ 1 − x x xe x(1 + x) 2 −x 2 x c) e ≈ 1 − x [Substitute into e ≈ 1+ x] x2 x2 d) ln(cos x) ≈ ln(1 − 2 ) ≈ − 2 [since ln(1 + h) ≈ h] 2 2 e) x ln x = (1 + h) ln(1 + h) ≈ (1 + h)(h − h ) ≈ h + h ⇒ x ln x ≈ 2 2 2 (x − 1) + (x − 1) 2 2A-13 Finding the linear and quadratic approximation 2 2. Applications of Differentiation E. Solutions to 18.01 Exercises a) 2x (both linear and quadratic) b) 1, 1 − 2x2 2 −1 2 c) 1, 1 + x /2 (Use (1 + u) ≈ 1 − u with u = x /2: sec x = 1/ cos x 2 2 −1 2 ≈ 1/(1 − x /2) = (1 − x /2) ≈ 1+ x /2 d) 1, 1 + x2 −1 2 e) Use (1 + u) ≈ 1 − u + u : −1 −1 −1 −1 2 (a + bx) = a (1 + (bx/a)) ≈ a (1 − bx/a +(bx/a) ) Linear approximation: (1/a) 2 − (b/a )x 2 2 3 2 Quadratic approximation: (1/a) − (b/a )x +(b /a )x � −2 �� 2 −3 f) f(x) = 1/(a + bx) so that f (1) = −b(a + b) and f (1) = 2b /(a + b) . We need to assume that these numbers are defined, in other words that a + b �= 0. Then the linear approximation is 1/(a + b) 2 − (b/(a + b) )(x − 1) and the quadratic approximation is 1/(a + b) 2 3 2 − (b/(a + b) )(x − 1) + (b/(a + b) )(x − 1) Method 2: Write 1/(a + bx) = 1/(a + b + b(x − 1)) Then use the expansion of problem (e) with a+b in place of a and b in place of b and − 1) in place of x. The requirement a �= 0 in (e) corresponds to the restriction (x a + b �= 0 in (f). 2A-15 f(x) = cos(3x), f�(x) = −3sin(3x), f��(x) = −9cos(3x). Thus, (1) f(0) = 1, f(π/6) = cos(π/2) = 0, f(π/3) = cos π = −1 (2) f�(0) = −3sin0 = 0, f�(π/6) = −3sin(π/2) = −3, f�(π/3) = −3sin π = 0 (3) f��(0) = −9, f��(π/6) = 0, f��(π/3) = 9 Using these values, the linear and quadratic approximations are respectively: 2 (4) for x ≈ 0 : f(x) ≈ 1 and f(x) ≈ 1 − (9/2)x (5) for x ≈ π/6 : both are f(x) ≈ −3(x − π/6) (6) for x ≈ π/3 : f(x) ≈ −1 and f(x) ≈ −1 + (9/2)(x − π/3)2 3 E. Solutions to 18.01 Exercises 2. Applications of Differentiation 2A-16 a) The law of cosines says that for a triangle with sides a, b, and c, with θ opposite the side of length c, 2 2 2 c = a + b − 2ab cos θ Apply it to one of the n triangles with vertex at the origin: a = b = 1 and θ = 2π/n. So the formula is � c = 2 − 2cos(2π/n) � b) The perimeter is n 2 − 2cos(2π/n). The quadratic approximation to cos θ near 0 is cos θ ≈ 1 − θ2/2 Therefore, as n → ∞ and θ = 2π/n → 0, � � 2 � 2 n 2 − 2cos(2π/n) ≈ n 2 − 2(1 − (1/2)(2π/n) ) = n (2π/n) = n(2π/n) = 2π In other words, � lim n 2 − 2cos(2π/n) = 2π, n→∞ the circumference of the circle of radius 1. 2B. Curve Sketching 3 � 2 � 2B-1 a) y = x − 3x + 1, y = 3x − 3 = 3(x − 1)(x + 1). y = 0 =⇒ x = ±1. Endpoint values: y → −∞ as x → −∞, and y → ∞ as x → ∞. Critical values: y(−1) = 3, y(1) = −1. Increasing on: −∞ < x < −1, 1 < x < ∞. Decreasing on: −1 < x < 1. Graph: (−∞, −∞) � (−1, 3) � (1, −1) � (∞, ∞), crossing the xaxis three times. (-1, 3) 1a (1,-1) 4 � 3 � 1/3 b) y = x − 4x + 1, y = x − 4. y = 0 =⇒ x = 4 . 4
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