MAT 1332, Assignment #2 Solutions [5] 1. If you simply integrate, the answer is zero. So that obviously isn’t right. It’s best to sketch the two graphs. See Figure 1. 1 sin(2x) A cos(2x) 0.5 B 0 C −0.5 −1 0 π /8 π /4 π /2 5π /8 π 3π /4 Figure 1: Area between sin(2x) and cos(2x). Clearly the area between them isn’t zero. In fact, it’s area A, plus area B, plus area C on the graph. And before we can find them, we need to find the points of intersection. That is, the values of x where sin(2x) = cos(2x). If you look at Figure 1 again, you may be able to subtly discern these. But let’s figure them out: sin(2x) = cos(2x) tan(2x) = 1 (dividing both sides by cos(2x)) 7π 3π π 5π 9π 2x = ... − , − , , , ... 4 4 4 4 4 7π 3π π 5π 9π x = ... − , − , , , ... 8 8 8 8 8 Actually, since 0 ≤ x ≤ π, we only need values that fall into this range. So the points of intersection within this range are x = π8 and x = 5π 8 . Now we’re ready to integrate. The area is the sum of areas A, B and C, so we have Area = A + B + C = Z π/8 0 (cos(2x) − sin(2x)) dx + Z 5π/8 π/8 (sin(2x) − cos(2x)) dx + 1 Z π 5π/8 (cos(2x) − sin(2x)) dx · = sin(2x) cos(2x) + 2 2 ¸π/8 ·µ · + − 0 ¶ µ cos(2x) sin(2x) − 2 2 ¸5π/8 ¶¸ · + π/8 ·µ sin(2x) cos(2x) + 2 2 ¸π 5π/8 ¶ sin(π/4) cos(π/4) sin(0) cos(0) cos(5π/4) sin(5π/4) = + − + + − − 2 2 2 2 2 2 µ ¶¸ ·µ ¶ µ ¶¸ cos(π/4) sin(π/4) sin(2π) cos(2π) sin(5π/4) cos(5π/4) − + + − − + − 2 2 2 2 2 2 ·µ ¶ µ ¶¸ ·µ ¶ µ ¶¸ 1 1 1 1 1 1 1 √ + √ √ + √ − 0+ + − − √ − √ = 2 2 2 2 2 2 2 2 2 2 2 2 2 ·µ ¶ µ ¶¸ 1 1 1 + 0+ − − √ − √ 2 2 2 2 2 4 = √ = 2.828 units2 . 2 2. Once again, it’s a good idea to draw a sketch. In this case it’s a cubic, with positive leading term and the hint has kindly given us the places where it crosses the x-axis, so it’s quite easy to draw. For the absolute value part, we turn the negative piece upside down, so it looks like Figure 2. 1000 |360t−39t2+t3| 500 0 2 3 360t−39t +t −500 0 5 10 15 20 25 Figure 2: Graph of |g(x)| (solid curve) and g(x) (dotted curve). Since we have an absolute value, we need to split it into two pieces. The split occurs at x = 15, so the first part is the regular (positive) function and the second is the negative of the (negative) function. Thus, the total energy is Total = ·Z 15 ³ " = 0 2 360t − 39t + t t4 180t − 13t + 4 2 #15 3 3 ´ dt + Z 24 ³ 15 " 2 39t − 360t − t t4 + 13t − 180t − 4 3 0 2 #24 2 15 3 ¸ ´ dt = [9281.25 − 0] + [−6912 − (−9281.25)] = 11650.5 joules/hour . 3. The derivative is ρ0 (x) = 4 × 10−8 x(240 − x) − 2 × 10−8 x2 −6 = 9.6 × 10 −6 = 9.6 × 10 −8 2 x − 4 × 10 (using the chain rule) −8 2 x − 2 × 10 x −8 2 x − 6 × 10 x . The turning points occur when ρ0 (x) = 0. Thus x = 0 and x = 9.6×10−6 6×10−8 = 160. Since ρ(0) = 1 and ρ(160) = 1.04096, it’s clear that the minimum occurs at x = 0 and the maximum occurs at x = 160. (You could also use the second derivative test here if you like.) (a) Thus, the maximum is 1.04096. (b) The minimum is 1. (c) The maximum occurs at x = 160. (d) The total mass is Z 200 Total mass = 0 ρ(x)dx Z 200 h = 0 Z 200 h = h 0 (remember 2m=200cm) i 1 + 2 × 10−8 x2 (240 − x) dx i 1 + 4.8 × 10−6 x2 − 2 × 10−8 x3 ) dx i200 x + 1.6 × 10−6 x3 − 5 × 10−9 x4 ) = 0 = 200 + 12.8 − 8 = 204.8 g . (e) The average mass is just 204.8 200 = 1.024. (f) The graph is shown in Figure 3. [5] 4. The volume obtained by rotating f (x) = sin V ¡x¢ 4 around the x-axis, between −π and π is given by the formula = π = π Z π −π Z π −π [f (x)]2 dx µ ¶ sin 2 x dx . 4 We can’t integrate sin2 θ directly, so we have to use our long-forgotten-but-recently-looked-up-in-the-textbook trigonemetric identities. Thus cos 2θ = cos2 θ − sin2 θ = (1 − sin2 θ) − sin2 θ (since cos2 θ + sin2 θ = 1) = 1 − 2 sin2 θ . Thus sin2 θ = 3 1 − cos 2θ . 2 1.045 density 1.04 1.035 average 1.03 1.025 1.02 1.015 1.01 1.005 1 0 20 40 60 80 100 120 140 160 180 Figure 3: The density (solid curve) and average (dotted curve). Substituting this into the integral, we have V = π = = = = = ¡ ¢ Z π 1 − cos 2 x4 −π Z π µ 2 ¶ dx π x 1 − cos dx 2 −π 2 · ¸ π x π x − 2 sin 2 2 −π ·µ ¶ µ µ ¶¶¸ π π π π − 2 sin − −π − 2 sin − 2 2 2 π (2π − 4) 2 π 2 − 2π units3 = 3.586 units3 . 4 200
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