MA1102R Calculus AY 2013/2014 Sem 2 NATIONAL UNIVERSITY OF SINGAPORE MATHEMATICS SOCIETY PAST YEAR PAPER SOLUTIONS MA1102R Calculus AY 2013/2014 Sem 2 Version 1: November 19, 2014 Written by Sherman Yuen Audited by Henry Morco Contributors – Question 1 (a) (i) Since x2 and cos x − 1 are both equal to 0 when x = 0, we may use the L’Hˆopital’s Rule. So, x2 2x = lim x→0 cos x − 1 x→0 − sin x if the latter limit exists. Similarly, since 2x and − sin x are both equal to 0 when x = 0, we may apply the L’Hˆ opital’s Rule again. lim 2 2 2x = lim = = −2 x→0 − cos x x→0 − sin x −1 lim Therefore we have x2 = −2 x→0 cos x − 1 lim (ii) We may use the substitution y = 1/x. 2 1 3 y + 5 sin 2y 3 + 5y 2 sin 2y (3x2 + 5) sin x2 lim = lim = lim x→∞ 5x + 3 5y + 3y 2 y→0+ y→0+ 5 y1 + 3 Since both the numerator and denominator equal to 0 when y = 0, we may use the L’Hˆopital’s Rule. So, 3 + 5y 2 sin 2y 10y sin 2y + (3 + 5y 2 )(2 cos 2y) 0 + (3 + 0)(2) 6 lim = lim = = 2 + + 5y + 3y 5 + 6y 5+0 5 y→0 y→0 Therefore we have (3x2 + 5) sin x2 6 = x→∞ 5x + 3 5 lim (iii) lim x→0 1 + 2 x + 3x 3 1 x ln = lim e 1 1+2x +3x x 3 x→0 1 = lim e x ln 1+2x +3x 3 x→0 =e limx→0 1 x ln 1+2x +3x 3 The limits are the same as e is a continuous function everywhere. We may now apply L’Hˆopital’s x x Rule because ln 1+2 3+3 and x are both equal to 0 when x = 0. We have 2x ln 2+3x ln 3 √ 1 1 + 2 x + 3x 2x ln 2 + 3x ln 3 ln 2 + ln 3 1 3 3 lim ln = lim = lim = = ln 6 = ln 6 x +3x 1+2 x→0 x x→0 x→0 1 + 2x + 3x 3 3 3 3 Therefore, lim x→0 1 + 2 x + 3x 3 NUS Math LATEXify Proj Team 1 x =e limx→0 1 x ln Page 1 of 8 1+2x +3x 3 = eln √ 3 6 = √ 3 6 NUS Mathematics Society MA1102R Calculus AY 2013/2014 Sem 2 (b) 2 2 x − 2x x − 6 x − 2x − 3x − 6 x2 − 5x − 6 (x + 1)(x − 6) = = |x + 1| x + 2 − 3 = x+2 = x + 2 x+2 x+2 Whenever |x + 1| < 12 , that is, − 21 < x + 1 < 1 2 13 (i) − 32 < x < − 12 ⇒ − 15 ⇒ 2 <x−6<− 2 (ii) − 32 < x < − 21 ⇒ 1 2 <x+2< 3 2 ⇒ 1 2 or − 32 < x < − 12 , we must have: 13 2 < |x − 6| < < |x + 2| < 3 2 ⇒ 15 2 1 2 ⇒ |x − 6| < 15 2 < |x + 2| Let > 0 be given. Choose δ = min{ 12 , 15 }. Then 2 x − 2x x − 6 < |x + 1| 15/2 = |x + 1| × 15 < × 15 = 0 < |x + 1| < δ ⇒ − 3 = |x + 1| x+2 x + 2 1/2 15 Question 2 (a) Let g(x) = |f (x)| and let g 0 (0) = L. We have g(x) − g(0) g(x) − 0 g(x) = lim = lim x→0 x→0 x − 0 x→0 x x−0 L = lim By taking limits for the positive side, we get g(x) g(x) |g(x)| g(x) L = lim = lim = lim = lim = |L| x x→0+ x x→0+ x x→0+ |x| x→0+ By taking limits for the negative side, we get g(x) g(x) |g(x)| g(x) L = lim = lim = lim − = − lim = −|L| x x→0− x x→0− −|x| x→0− x→0− x So we have −|L| = |L|, which means L = 0. So g 0 (0) = 0. Now we want to show that f 0 (0) = 0. Let > 0 be given. Then there exists a δ > 0 such that g(x) − 0 < 0 < |x − 0| < δ ⇒ x |f (x)| < ⇒ x f (x) < ⇒ x f (x) − 0 ⇒ − 0 < x−0 f (x) − f (0) ⇒ − 0 < x−0 This shows that f 0 (0) = 0. NUS Math LATEXify Proj Team Page 2 of 8 NUS Mathematics Society MA1102R Calculus AY 2013/2014 Sem 2 (b) Since f is continuous at 0, we have f (0) = lim f (x) = lim x→0 x→0 f (x) f (x) × x = lim × lim x = 2 × 0 = 0 x→0 x→0 x x By using the definition of the derivative, f (x) − f (0) f (x) − 0 f (x) = lim = lim =2 x→0 x→0 x→0 x x−0 x f 0 (0) = lim (c) Z 5x 2 Z 5x 2 sin(t )dt = cos x Z 0 sin(t )dt + 0 2 Z Z 2 cos x sin(t )dt − sin(t )dt = cos x 5x 0 sin(t2 )dt 0 By using the Fundamental Theorem of Calculus, we have Z 5x Z 5x Z cos x d d d 2 2 sin(t )dt = sin(t )dt − sin(t2 )dt = 5 sin((5x)2 ) − sin(cos2 x)(− sin x) dx cos x dx 0 dx 0 So, d dx Z 5x sin(t2 )dt = 5 sin(25x2 ) + sin x sin(cos2 x) cos x Question 3 (a) Since f is differentiable at 1, the function must be continuous at 1. πx π f (1) = lim f (x) = lim x cos = lim 1 cos =0 2 2 x→1− x→1− x→1− So we must have f (1) = 0. Since 0 = f (1) = a(1)2 + b = a + b, we have b = −a. The limit of the difference quotient must also exist at 1. f 0 (1) = lim x→1+ ax2 + b − 0 ax2 + b f (x) − f (1) = lim = lim x−1 x−1 x→1+ x→1+ x − 1 We may substitute b = −a into the equation to obtain f 0 (1) = lim x→1+ ax2 − a a(x + 1)(x − 1) = lim = lim a(x + 1) = 2a + x−1 x−1 x→1 x→1+ By looking at the left-hand limit, we get πx x cos πx − 0 x cos f (x) − f (1) 2 2 f (1) = lim = lim = lim x−1 x−1 x−1 x→1− x→1− x→1− 0 We will use L’Hˆ opital’s Rule since both the numerator and denominator are equal to 0 π πx π π π cos πx + x(− sin π 0 2 2 2 ) f (1) = lim = cos − sin =− − 1 2 2 2 2 x→1 So we obtain 2a = − π2 , giving us a = − π4 , b = π4 . NUS Math LATEXify Proj Team Page 3 of 8 NUS Mathematics Society MA1102R Calculus AY 2013/2014 Sem 2 (b) We have f (2) = (2 − 2)g(2) = 0. So, f 0 (x) = lim x→2 (x − 2)g(x) − 0 f (x) − f (2) = lim = lim g(x) = g(2) = 1 x→2 x→2 x−2 x−2 since g is continuous at 2. (c) Z π 4 √ ln( 1 + tan x)dx = Z 0 π 4 0 r Z π r 4 π π ln 1 + tan ( − t) (−1)dt = 1 + tan ( − t) dt ln 4 4 0 We use the trigonometric addition formula, tan(A − B) = 1 + tan ( tan(A)−tan(B) 1+tan(A) tan(B) , to get tan π4 − tan t π 1 − tan t 1 + tan t + 1 − tan t 2 =1+ − t) = 1 + = = π 4 1 + tan 4 tan t 1 + 1 · tan t 1 + tan t 1 + tan t This gives π 4 Z I:= 0 π 4 Z = 0 π 4 Z = 0 π 4 Z = 0 π 4 Z = √ ln( 1 + tan x)dx r π ln 1 + tan ( − t) dt 4 ! r 2 ln dt 1 + tan t ! √ 2 ln √ dt 1 + tan t √ √ ln 2 − ln( 1 + tan t)dt 0 π 4 Z = √ Z ln 2dt − 0 = √ ln( 1 + tan t)dt 0 π 4 Z π 4 √ ln 2dt − I 0 where we have made the remarkable observation that the last integral is also exactly equal to I! Hence we must have π Z π √ 4 4 1 π ln 2 2I = ln 2dt = t ln 2 = 2 8 0 0 π R √ ln 2 Hence 04 ln( 1 + tan x)dx = I = π 16 . Question 4 (a) (i) Z 1 00 Z x(1 − x)f (x)dx = 0 1 00 Z xf (x)dx − 0 1 x2 f 00 (x)dx 0 For the first integral, we can integrate by parts to get Z 1 Z 1 0 1 00 xf (x)dx = xf (x) 0 − f 0 (x)dx = (1 · f 0 (1) − 0 · f 0 (0)) − (f (1) − f (0)) = f 0 (1) 0 NUS Math LATEXify Proj Team 0 Page 4 of 8 NUS Mathematics Society MA1102R Calculus AY 2013/2014 Sem 2 For the second integral, we may integrate by parts repeatedly on the given integral Z 1 f (x)dx 1= 0 Z 1 1 xf 0 (x)dx = [xf (x)]0 − 0 ! 1 Z 1 1 2 0 1 2 00 = (1 · f (1) − 0 · f (0)) − x f (x) − x f (x)dx 2 0 2 0 Z 1 1 1 2 00 = (0 − 0) − ( f 0 (1) − 0 · f 0 (0)) − x f (x)dx 2 0 2 Z 1 0 f (1) 1 2 00 x f (x)dx − = 2 0 2 R1 So we have 0 x2 f 00 (x)dx = 2 + f 0 (1). Therefore, Z 1 x(1 − x)f 00 (x)dx = 0 Z 1 xf 00 (x)dx − 0 Z 1 x2 f 00 (x)dx = f 0 (1) − (2 + f 0 (1)) = −2 0 (ii) It suffices to find a c ∈ [0, 1] such that f 00 (c) = −12. Define g(x) = −6x2 + 6x − f (x). Note that g(x) is twice differentiable such that its second derivative is continuous. Let G(x) be an anti-derivative of g(x). Then, by the Fundamental Theorem of Calculus, Z 1 G(1) − G(0) = g(x)dx 0 Z 1 −6x2 + 6x − f (x)dx 0 Z 1 3 2 1 = −2x + 3x |0 − f (x)dx = 0 = (−2 + 3) − 1 =0 This means that G(0) = G(1). By the Mean Value Theorem, there exists d ∈ (0, 1) such that g(d) = G0 (d) = G(1) − G(0) =0 1−0 Now, by direct calculations, we also have g(0) = g(1) = 0. So by Mean Value Theorem again, there exists a ∈ (0, d) and b ∈ (d, 1) such that g 0 (a) = g(d) − g(0) = 0, d−0 g 0 (b) = g(1) − g(d) =0 1−d And by the Mean Value Theorem one more time, there exists c ∈ (a, b) such that g 00 (c) = g 0 (b) − g 0 (a) =0 b−a Now, since g(x) = −6x2 + 6x − f (x), we have g 0 (x) = −12x + 6 − f 0 (x) and g 00 (x) = −12 − f 00 (x). So this gives 0 = g 00 (c) = −12 − f 00 (c) ⇒ f 00 (c) = −12 This completes the proof. NUS Math LATEXify Proj Team Page 5 of 8 NUS Mathematics Society MA1102R Calculus AY 2013/2014 Sem 2 (b) Let F (x) be an anti-derivative of f (x) and G(x) be an anti-derivative of F (x) (so G0 (x) = F (x) and F 0 (x) = f (x)). Integrating by parts, we get Z 1 0= 0 1 Z xf (x)dx = xF (x) − 1 0 0 1 F (x)dx = 1F (1) − 0F (0) − G(x) = F (1) − (G(1) − G(0)) 0 This gives G(1) − G(0) = F (1). By the Mean Value Theorem, there exists c ∈ (0, 1) such that F (c) = G0 (c) = F (1) G(1) − G(0) = = F (1) 1−0 1 Also, we have 1 Z 0= 0 1 f (x)dx = F (x) = F (1) − F (0) 0 So altogether we obtain F (0) = F (c) = F (1) for some c ∈ (0, 1). By Rolle’s Theorem, there exists a ∈ (0, c) and b ∈ (c, 1) such that F 0 (a) = 0, F 0 (b) = 0. So f (a) = f (b) = 0. (c) Z Volume of solid = 4 √ 4 Z 2 π( x) dx = 0 0 4 1 2 πxdx = πx = 8π 2 0 Question 5 (a) dy dv =v+x dx dx So, by substituting this into the equation, we get dy + x2 + y 2 dx dv 2 + x2 + (vx)2 = (x − x(vx)) v + x dx dv 2 = x (1 − v) v + x + x2 + v 2 x2 dx dv = x2 (1 − v) v + x + 1 + v2 dx 0 = (x2 − xy) But x 6= 0. So we may divide x2 from both sides. dv + 1 + v2 0 = (1 − v) v + x dx dv dv = v − v2 + x − vx + 1 + v2 dx dx dv dv =v+x − vx +1 dx dx dv = x(1 − v) +1+v dx This gives 1 = x NUS Math LATEXify Proj Team v−1 v+1 dv = dx 1− Page 6 of 8 2 v+1 dv dx NUS Mathematics Society MA1102R Calculus AY 2013/2014 Sem 2 Integrating both sides with respect to x, we get Z Z 2 1 1− dv dx = x v+1 ln x = v − 2 ln (v + 1) + C y y ln x = − 2 ln +1 +C x x Substituting x = 1, y = 0, we get 0 = 0 − 2 ln 1 + C = C. So y y ln x = − 2 ln +1 x x (b) An integrating factor of the first order linear differential equation is e R −(1+ x3 )dx = e−x−3 ln x = e−x eln x −3 = x−3 e−x So we have 3 dy − (1 + )y = x + 2 dx x dy 3 x−3 e−x − x−3 e−x (1 + )y = x−3 e−x (x + 2) dx x d −3 −x x e y = x−3 e−x (x + 2) dx Integrating both sides with respect to x, we get Z x−3 e−x y = x−3 e−x (x + 2)dx To integrate the RHS, we make the observation that x−3 e−x (x + 2) = Quotient Rule, looks like some form of the derivative of e−x . x2 e−x (x2 +2x) (x2 )2 which, by using Indeed, d e−x −x2 (e−x ) − 2x(e−x ) = = −x−3 e−x (x + 2) dx x2 (x2 )2 Therefore, we have x −3 −x e Z y=− −x−3 e−x (x + 2)dx e−x +C x2 y = −x + Cx3 ex x−3 e−x y = − where C is an arbitrary constant. Substitute the initial value and we get C = 1. Therefore we have y = x3 e x − x END OF SOLUTIONS NUS Math LATEXify Proj Team Page 7 of 8 NUS Mathematics Society MA1102R Calculus AY 2013/2014 Sem 2 Any Mistakes? 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