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Further Calculus — Diagnostic Tests

Unit Tests

UT-1: Improper Integrals

Question: (a) Evaluate 11x2dx\int_1^{\infty} \frac{1}{x^2}\,dx. (b) Determine whether 11xdx\int_1^{\infty} \frac{1}{x}\,dx converges or diverges. (c) Evaluate 01LB1RB◆◆LBxRBdx\int_0^1 \frac◆LB◆1◆RB◆◆LB◆\sqrt{x}◆RB◆\,dx. (d) Explain the difference between a convergent and divergent improper integral.

Solution:

(a) 11x2dx=limb[1x]1b=limb(1b+1)=0+1=1\int_1^{\infty} \frac{1}{x^2}\,dx = \lim_{b \to \infty}\left[-\frac{1}{x}\right]_1^b = \lim_{b \to \infty}\left(-\frac{1}{b} + 1\right) = 0 + 1 = 1. Converges to 1.

(b) 11xdx=limb[lnx]1b=limb(lnb0)=\int_1^{\infty} \frac{1}{x}\,dx = \lim_{b \to \infty}[\ln x]_1^b = \lim_{b \to \infty}(\ln b - 0) = \infty. Diverges.

(c) 01LB1RB◆◆LBxRBdx=lima0+[2x]a1=lima0+(22a)=20=2\int_0^1 \frac◆LB◆1◆RB◆◆LB◆\sqrt{x}◆RB◆\,dx = \lim_{a \to 0^+}[2\sqrt{x}]_a^1 = \lim_{a \to 0^+}(2 - 2\sqrt{a}) = 2 - 0 = 2. Converges to 2.

(d) A convergent improper integral has a finite value -- the limit exists and equals a real number. A divergent improper integral approaches infinity (or does not approach a limit), meaning the area under the curve is infinite.

UT-2: Volumes of Revolution

Question: (a) Find the volume generated when the curve y=xy = \sqrt{x} is rotated 2π2\pi radians about the xx-axis between x=0x = 0 and x=4x = 4. (b) Find the volume generated when x=y2x = y^2 (for y0y \ge 0) is rotated about the yy-axis between y=0y = 0 and y=2y = 2. (c) The region bounded by y=x2y = x^2, y=0y = 0, and x=1x = 1 is rotated about the yy-axis. Calculate the volume using the shell method: V=2πabxydxV = 2\pi\int_a^b xy\,dx.

Solution:

(a) V=π04y2dx=π04xdx=π[x22]04=π×8=8πV = \pi\int_0^4 y^2\,dx = \pi\int_0^4 x\,dx = \pi\left[\frac{x^2}{2}\right]_0^4 = \pi \times 8 = 8\pi.

(b) V=π02x2dy=π02y4dy=π[y55]02=π×325=LB32πRB◆◆LB5RBV = \pi\int_0^2 x^2\,dy = \pi\int_0^2 y^4\,dy = \pi\left[\frac{y^5}{5}\right]_0^2 = \pi \times \frac{32}{5} = \frac◆LB◆32\pi◆RB◆◆LB◆5◆RB◆.

(c) V=2π01xx2dx=2π01x3dx=2π[x44]01=2π×14=LBπRB◆◆LB2RBV = 2\pi\int_0^1 x \cdot x^2\,dx = 2\pi\int_0^1 x^3\,dx = 2\pi\left[\frac{x^4}{4}\right]_0^1 = 2\pi \times \frac{1}{4} = \frac◆LB◆\pi◆RB◆◆LB◆2◆RB◆.

UT-3: Parametric Differentiation

Question: A curve is given parametrically by x=t2+1x = t^2 + 1, y=t3ty = t^3 - t. (a) Find dydx\frac{dy}{dx} in terms of tt. (b) Find the coordinates of the stationary points. (c) Find d2ydx2\frac{d^2y}{dx^2} and determine the nature of each stationary point. (d) Find the equation of the normal to the curve at the point where t=2t = 2.

Solution:

(a) dxdt=2t\frac{dx}{dt} = 2t, dydt=3t21\frac{dy}{dt} = 3t^2 - 1. dydx=3t212t\frac{dy}{dx} = \frac{3t^2 - 1}{2t}.

(b) Stationary points: dydx=0\frac{dy}{dx} = 0, so 3t21=03t^2 - 1 = 0, t=±LB1RB◆◆LB3RBt = \pm\frac◆LB◆1◆RB◆◆LB◆\sqrt{3}◆RB◆.

t=LB1RB◆◆LB3RBt = \frac◆LB◆1◆RB◆◆LB◆\sqrt{3}◆RB◆: x=43x = \frac{4}{3}, y=LB1RB◆◆LB33RBLB1RB◆◆LB3RB=LB2RB◆◆LB33RBy = \frac◆LB◆1◆RB◆◆LB◆3\sqrt{3}◆RB◆ - \frac◆LB◆1◆RB◆◆LB◆\sqrt{3}◆RB◆ = -\frac◆LB◆2◆RB◆◆LB◆3\sqrt{3}◆RB◆. t=LB1RB◆◆LB3RBt = -\frac◆LB◆1◆RB◆◆LB◆\sqrt{3}◆RB◆: x=43x = \frac{4}{3}, y=LB1RB◆◆LB33RB+LB1RB◆◆LB3RB=LB2RB◆◆LB33RBy = -\frac◆LB◆1◆RB◆◆LB◆3\sqrt{3}◆RB◆ + \frac◆LB◆1◆RB◆◆LB◆\sqrt{3}◆RB◆ = \frac◆LB◆2◆RB◆◆LB◆3\sqrt{3}◆RB◆.

(c) d2ydx2=ddt(3t212t)/dxdt=LB6t2t(3t21)2RB◆◆LB4t2RB/2t=12t26t2+24t212t=6t2+28t3\frac{d^2y}{dx^2} = \frac{d}{dt}\left(\frac{3t^2-1}{2t}\right) \Big/ \frac{dx}{dt} = \frac◆LB◆6t \cdot 2t - (3t^2-1) \cdot 2◆RB◆◆LB◆4t^2◆RB◆ \Big/ 2t = \frac{12t^2 - 6t^2 + 2}{4t^2} \cdot \frac{1}{2t} = \frac{6t^2 + 2}{8t^3}.

At t=LB1RB◆◆LB3RBt = \frac◆LB◆1◆RB◆◆LB◆\sqrt{3}◆RB◆: d2ydx2=LB6/3+2RB◆◆LB8/(33)RB=LB4RB◆◆LB8/(33)RB=LB123RB◆◆LB8RB=LB33RB◆◆LB2RB>0\frac{d^2y}{dx^2} = \frac◆LB◆6/3 + 2◆RB◆◆LB◆8/(3\sqrt{3})◆RB◆ = \frac◆LB◆4◆RB◆◆LB◆8/(3\sqrt{3})◆RB◆ = \frac◆LB◆12\sqrt{3}◆RB◆◆LB◆8◆RB◆ = \frac◆LB◆3\sqrt{3}◆RB◆◆LB◆2◆RB◆ \gt 0: minimum.

At t=LB1RB◆◆LB3RBt = -\frac◆LB◆1◆RB◆◆LB◆\sqrt{3}◆RB◆: d2ydx2=LB6/3+2RB◆◆LB8/(33)RB=LB33RB◆◆LB2RB<0\frac{d^2y}{dx^2} = \frac◆LB◆6/3 + 2◆RB◆◆LB◆8/(-3\sqrt{3})◆RB◆ = -\frac◆LB◆3\sqrt{3}◆RB◆◆LB◆2◆RB◆ \lt 0: maximum.

(d) At t=2t = 2: x=5x = 5, y=6y = 6. dydx=1214=114\frac{dy}{dx} = \frac{12-1}{4} = \frac{11}{4}.

Normal gradient =411= -\frac{4}{11}. Equation: y6=411(x5)y - 6 = -\frac{4}{11}(x - 5), i.e., 11y66=4x+2011y - 66 = -4x + 20, so 4x+11y=864x + 11y = 86.


Integration Tests

IT-1: Calculus in Context (with Differential Equations)

Question: A population grows according to dPdt=kP(1000P)\frac{dP}{dt} = kP(1000 - P) where PP is the population and k=0.001k = 0.001. Initial population P(0)=100P(0) = 100. (a) Identify the type of differential equation. (b) Solve by separating variables. (c) Find PP when t=5t = 5. (d) Describe the long-term behaviour of the population.

Solution:

(a) This is a separable first-order differential equation and a logistic growth equation.

(b) dPP(1000P)=0.001dt\frac{dP}{P(1000-P)} = 0.001\,dt. Using partial fractions: 1P(1000P)=1/1000P+1/10001000P\frac{1}{P(1000-P)} = \frac{1/1000}{P} + \frac{1/1000}{1000-P}.

11000lnP1000P=0.001t+C\frac{1}{1000}\ln\left|\frac{P}{1000-P}\right| = 0.001t + C. lnP1000P=t+C\ln\left|\frac{P}{1000-P}\right| = t + C'.

P1000P=Aet\frac{P}{1000-P} = Ae^t. At t=0t = 0: 100900=A\frac{100}{900} = A, so A=1/9A = 1/9.

P1000P=et9\frac{P}{1000-P} = \frac{e^t}{9}. P=1000et9+etP = \frac{1000e^t}{9 + e^t}.

(c) P(5)=1000e59+e5=1000(148.4)157.4=942.8P(5) = \frac{1000e^5}{9 + e^5} = \frac{1000(148.4)}{157.4} = 942.8.

(d) As tt \to \infty: P1000P \to 1000. The population approaches the carrying capacity of 1000. The growth is initially approximately exponential when PP is small, but slows as PP approaches 1000.

IT-2: Integration Techniques (with Maclaurin Series)

Question: (a) Evaluate 0π/2xsinxdx\int_0^{\pi/2} x\sin x\,dx using integration by parts. (b) Use the Maclaurin series for exe^x to evaluate 00.1ex2dx\int_0^{0.1} e^{-x^2}\,dx correct to 4 decimal places. (c) Evaluate 1x29dx\int \frac{1}{x^2 - 9}\,dx using partial fractions. (d) Evaluate 0xexdx\int_0^{\infty} xe^{-x}\,dx.

Solution:

(a) u=xu = x, dv=sinxdxdv = \sin x\,dx. du=dxdu = dx, v=cosxv = -\cos x. 0π/2xsinxdx=[xcosx]0π/2+0π/2cosxdx=0+[sinx]0π/2=1\int_0^{\pi/2} x\sin x\,dx = [-x\cos x]_0^{\pi/2} + \int_0^{\pi/2} \cos x\,dx = 0 + [\sin x]_0^{\pi/2} = 1.

(b) ex2=1x2+x42x66+e^{-x^2} = 1 - x^2 + \frac{x^4}{2} - \frac{x^6}{6} + \cdots 00.1ex2dx=[xx33+x510x742]00.1\int_0^{0.1} e^{-x^2}\,dx = \left[x - \frac{x^3}{3} + \frac{x^5}{10} - \frac{x^7}{42}\right]_0^{0.1} =0.10.0013+0.00001100.000000142= 0.1 - \frac{0.001}{3} + \frac{0.00001}{10} - \frac{0.0000001}{42} =0.10.000333+0.0000010.0000000024=0.0996680.0997= 0.1 - 0.000333 + 0.000001 - 0.0000000024 = 0.099668 \approx 0.0997.

(c) 1x29=1(x3)(x+3)=1/6x31/6x+3\frac{1}{x^2 - 9} = \frac{1}{(x-3)(x+3)} = \frac{1/6}{x-3} - \frac{1/6}{x+3}. =16lnx316lnx+3+C=16lnx3x+3+C\int = \frac{1}{6}\ln|x-3| - \frac{1}{6}\ln|x+3| + C = \frac{1}{6}\ln\left|\frac{x-3}{x+3}\right| + C.

(d) Integration by parts: u=xu = x, dv=exdxdv = e^{-x}\,dx. du=dxdu = dx, v=exv = -e^{-x}. 0xexdx=[xex]0+0exdx=0+[ex]0=0+1=1\int_0^{\infty} xe^{-x}\,dx = [-xe^{-x}]_0^{\infty} + \int_0^{\infty} e^{-x}\,dx = 0 + [-e^{-x}]_0^{\infty} = 0 + 1 = 1.

(This is the gamma function Γ(2)=1!=1\Gamma(2) = 1! = 1.)

IT-3: Arc Length and Surface Area (with Geometry)

Question: (a) Find the arc length of the curve y=23x3/2y = \frac{2}{3}x^{3/2} from x=0x = 0 to x=3x = 3. (b) Find the surface area generated when this curve is rotated about the xx-axis. (c) A curve is given by x=2cosθx = 2\cos\theta, y=2sinθy = 2\sin\theta. Find the arc length for one complete revolution (0θ2π0 \le \theta \le 2\pi). (d) Explain why the arc length formula involves LB1+(dydx)2RB\sqrt◆LB◆1 + \left(\frac{dy}{dx}\right)^2◆RB◆.

Solution:

(a) Arc length s=abLB1+(dydx)2RBdxs = \int_a^b \sqrt◆LB◆1 + \left(\frac{dy}{dx}\right)^2◆RB◆\,dx. dydx=x1/2\frac{dy}{dx} = x^{1/2}. s=031+xdx=[23(1+x)3/2]03=23(81)=143s = \int_0^3 \sqrt{1 + x}\,dx = \left[\frac{2}{3}(1+x)^{3/2}\right]_0^3 = \frac{2}{3}(8 - 1) = \frac{14}{3}.

(b) Surface area =2π03yLB1+(dydx)2RBdx=2π0323x3/21+xdx= 2\pi\int_0^3 y\sqrt◆LB◆1 + \left(\frac{dy}{dx}\right)^2◆RB◆\,dx = 2\pi\int_0^3 \frac{2}{3}x^{3/2}\sqrt{1+x}\,dx.

Let u=1+xu = 1 + x, du=dxdu = dx, x=u1x = u - 1: =LB4πRB◆◆LB3RB14(u1)3/2u1/2du= \frac◆LB◆4\pi◆RB◆◆LB◆3◆RB◆\int_1^4 (u-1)^{3/2}u^{1/2}\,du.

This integral requires expanding (u1)3/2=u3/23u1/2+3u1/2u3/2(u-1)^{3/2} = u^{3/2} - 3u^{1/2} + 3u^{-1/2} - u^{-3/2}, then multiplying by u1/2u^{1/2} and integrating term by term.

=LB4πRB◆◆LB3RB14(u23u+3u1)du=LB4πRB◆◆LB3RB[u333u22+3ulnu]14= \frac◆LB◆4\pi◆RB◆◆LB◆3◆RB◆\int_1^4 (u^2 - 3u + 3 - u^{-1})\,du = \frac◆LB◆4\pi◆RB◆◆LB◆3◆RB◆\left[\frac{u^3}{3} - \frac{3u^2}{2} + 3u - \ln u\right]_1^4

=LB4πRB◆◆LB3RB[(64324+12ln4)(1332+30)]=LB4πRB◆◆LB3RB(63312+932ln4)= \frac◆LB◆4\pi◆RB◆◆LB◆3◆RB◆\left[\left(\frac{64}{3} - 24 + 12 - \ln 4\right) - \left(\frac{1}{3} - \frac{3}{2} + 3 - 0\right)\right] = \frac◆LB◆4\pi◆RB◆◆LB◆3◆RB◆\left(\frac{63}{3} - 12 + 9 - \frac{3}{2} - \ln 4\right)

=LB4πRB◆◆LB3RB(2112+91.51.386)=LB4πRB◆◆LB3RB(15.114)=63.3= \frac◆LB◆4\pi◆RB◆◆LB◆3◆RB◆(21 - 12 + 9 - 1.5 - 1.386) = \frac◆LB◆4\pi◆RB◆◆LB◆3◆RB◆(15.114) = 63.3.

(c) LBdxRB◆◆LBdθRB=2sinθ\frac◆LB◆dx◆RB◆◆LB◆d\theta◆RB◆ = -2\sin\theta, LBdyRB◆◆LBdθRB=2cosθ\frac◆LB◆dy◆RB◆◆LB◆d\theta◆RB◆ = 2\cos\theta. LB(2sinθ)2+(2cosθ)2RB=4=2\sqrt◆LB◆(-2\sin\theta)^2 + (2\cos\theta)^2◆RB◆ = \sqrt{4} = 2. s=02π2dθ=4πs = \int_0^{2\pi} 2\,d\theta = 4\pi. This is a circle of radius 2, so circumference =2π(2)=4π= 2\pi(2) = 4\pi.

(d) The formula comes from approximating the curve by many small line segments of length Δs=LB(Δx)2+(Δy)2RB\Delta s = \sqrt◆LB◆(\Delta x)^2 + (\Delta y)^2◆RB◆. Dividing by Δx\Delta x: Δs=LB1+(LBΔyRB◆◆LBΔxRB)2RBΔx\Delta s = \sqrt◆LB◆1 + \left(\frac◆LB◆\Delta y◆RB◆◆LB◆\Delta x◆RB◆\right)^2◆RB◆\Delta x. In the limit as Δx0\Delta x \to 0: ds=1+(dy/dx)2dxds = \sqrt{1 + (dy/dx)^2}\,dx. Integrating gives the total arc length.