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Further Calculus -- Diagnostic Tests

This topic explores fundamental concepts that shape our understanding of the world.

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 011xdx\int_0^1 \frac{1}{\sqrt{x}}\,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) 011xdx=lima0+[2x]a1=lima0+(22a)=20=2\int_0^1 \frac{1}{\sqrt{x}}\,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.

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 = 0And 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=32π5V = \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{32\pi}{5}.

(c) V=2π01xx2dx=2π01x3dx=2π[x44]01=2π×14=π2V = 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{\pi}{2}.

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} = 0So 3t21=03t^2 - 1 = 0, t=±13t = \pm\frac{1}{\sqrt{3}}.

t=13t = \frac{1}{\sqrt{3}}: x=43x = \frac{4}{3}, y=13313=233y = \frac{1}{3\sqrt{3}} - \frac{1}{\sqrt{3}} = -\frac{2}{3\sqrt{3}}. t=13t = -\frac{1}{\sqrt{3}}: x=43x = \frac{4}{3}, y=133+13=233y = -\frac{1}{3\sqrt{3}} + \frac{1}{\sqrt{3}} = \frac{2}{3\sqrt{3}}.

(c) d2ydx2=ddt(3t212t)/dxdt=6t2t(3t21)24t2/2t=12t26t2+24t212t=6t2+28t3\frac{d^2y}{dx^2} = \frac{d}{dt}\left(\frac{3t^2-1}{2t}\right) \Big/ \frac{dx}{dt} = \frac{6t \cdot 2t - (3t^2-1) \cdot 2}{4t^2} \Big/ 2t = \frac{12t^2 - 6t^2 + 2}{4t^2} \cdot \frac{1}{2t} = \frac{6t^2 + 2}{8t^3}.

At t=13t = \frac{1}{\sqrt{3}}: d2ydx2=6/3+28/(33)=48/(33)=1238=332>0\frac{d^2y}{dx^2} = \frac{6/3 + 2}{8/(3\sqrt{3})} = \frac{4}{8/(3\sqrt{3})} = \frac{12\sqrt{3}}{8} = \frac{3\sqrt{3}}{2} \gt 0: minimum.

At t=13t = -\frac{1}{\sqrt{3}}: d2ydx2=6/3+28/(33)=332<0\frac{d^2y}{dx^2} = \frac{6/3 + 2}{8/(-3\sqrt{3})} = -\frac{3\sqrt{3}}{2} \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 + 20So 4x+11y=864x + 11y = 86.


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

Section titled “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} = ASo 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)

Section titled “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 = x$$dv = \sin x\,dx. du = dx$$v = -\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 = x$$dv = e^{-x}\,dx. du = dx$$v = -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)

Section titled “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 = 2\cos\theta$$y = 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 1+(dydx)2\sqrt{1 + \left(\frac{dy}{dx}\right)^2}.

Solution:

(a) Arc length s=ab1+(dydx)2dxs = \int_a^b \sqrt{1 + \left(\frac{dy}{dx}\right)^2}\,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 =2π03y1+(dydx)2dx=2π0323x3/21+xdx= 2\pi\int_0^3 y\sqrt{1 + \left(\frac{dy}{dx}\right)^2}\,dx = 2\pi\int_0^3 \frac{2}{3}x^{3/2}\sqrt{1+x}\,dx.

Let u = 1 + x$$du = dx$$x = u - 1: =4π314(u1)3/2u1/2du= \frac{4\pi}{3}\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.

=4π314(u23u+3u1)du=4π3[u333u22+3ulnu]14= \frac{4\pi}{3}\int_1^4 (u^2 - 3u + 3 - u^{-1})\,du = \frac{4\pi}{3}\left[\frac{u^3}{3} - \frac{3u^2}{2} + 3u - \ln u\right]_1^4

=4π3[(64324+12ln4)(1332+30)]=4π3(63312+932ln4)= \frac{4\pi}{3}\left[\left(\frac{64}{3} - 24 + 12 - \ln 4\right) - \left(\frac{1}{3} - \frac{3}{2} + 3 - 0\right)\right] = \frac{4\pi}{3}\left(\frac{63}{3} - 12 + 9 - \frac{3}{2} - \ln 4\right)

=4π3(2112+91.51.386)=4π3(15.114)=63.3= \frac{4\pi}{3}(21 - 12 + 9 - 1.5 - 1.386) = \frac{4\pi}{3}(15.114) = 63.3.

(c) \frac{dx}{d\theta} = -2\sin\theta$$\frac{dy}{d\theta} = 2\cos\theta. (2sinθ)2+(2cosθ)2=4=2\sqrt{(-2\sin\theta)^2 + (2\cos\theta)^2} = \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=(Δx)2+(Δy)2\Delta s = \sqrt{(\Delta x)^2 + (\Delta y)^2}. Dividing by Δx\Delta x: Δs=1+(ΔyΔx)2Δx\Delta s = \sqrt{1 + \left(\frac{\Delta y}{\Delta x}\right)^2}\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.

Confusing the arc length formula with the area under a curve: Arc length uses 1+(dy/dx)2dx\int \sqrt{1 + (dy/dx)^2}\,dx, not ydx\int y\,dx. The square root and the squared derivative are essential — omitting them gives the area, not the length. This is one of the most common errors in further calculus.

Forgetting the 2π2\pi in surface of revolution formulas: When rotating a curve about the xx-axis, the surface area formula is 2πy1+(dy/dx)2dx2\pi\int y\sqrt{1+(dy/dx)^2}\,dx. Students often write πy1+(dy/dx)2dx\pi\int y\sqrt{1+(dy/dx)^2}\,dx (confusing it with the volume formula πy2dx\pi\int y^2\,dx). The 2π2\pi comes from the circumference of the circle traced by each point.

Misidentifying the limits of integration for parametric curves: When given a curve parametrically, convert the limits to the parameter values, not the Cartesian coordinates. If x=2cosθx = 2\cos\theta and the Cartesian limits are x=0x = 0 to x=2x = 2, the parameter limits are θ=π/2\theta = \pi/2 to θ=0\theta = 0 (not the other way around without justification).