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Further Calculus -- Diagnostic Tests

flowchart TD
A[Diag Further Calculus] --> B[Key Concepts]
A --> C[Core Principles]
A --> D[Practical Applications]
B --> E[Fundamental definitions]
C --> F[Design patterns]
D --> G[Real-world usage]

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

Question: (a) Evaluate ∫1∞1x2 dx\int_1^{\infty} \frac{1}{x^2}\,dx. (b) Determine whether ∫1∞1x dx\int_1^{\infty} \frac{1}{x}\,dx converges or diverges. (c) Evaluate ∫011x dx\int_0^1 \frac{1}{\sqrt{x}}\,dx. (d) Explain the difference between a convergent and divergent improper integral.

Solution:

(a) ∫1∞1x2 dx=lim⁡b→∞[−1x]1b=lim⁡b→∞(−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) ∫1∞1x dx=lim⁡b→∞[ln⁡x]1b=lim⁡b→∞(ln⁡b−0)=∞\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) ∫011x dx=lim⁡a→0+[2x]a1=lim⁡a→0+(2−2a)=2−0=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 y≥0y \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=2π∫abxy dxV = 2\pi\int_a^b xy\,dx.

Solution:

(a) V=π∫04y2 dx=π∫04x dx=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=π∫02x2 dy=π∫02y4 dy=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=2π∫01x⋅x2 dx=2π∫01x3 dx=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=t3−ty = 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=3t2−1\frac{dy}{dt} = 3t^2 - 1. dydx=3t2−12t\frac{dy}{dx} = \frac{3t^2 - 1}{2t}.

(b) Stationary points: dydx=0\frac{dy}{dx} = 0 So 3t2−1=03t^2 - 1 = 0, t=±13t = \pm\frac{1}{\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}}. 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(3t2−12t)/dxdt=6t⋅2t−(3t2−1)⋅24t2/2t=12t2−6t2+24t2⋅12t=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=12−14=114\frac{dy}{dx} = \frac{12-1}{4} = \frac{11}{4}.

Normal gradient =−411= -\frac{4}{11}. Equation: y−6=−411(x−5)y - 6 = -\frac{4}{11}(x - 5) I.e., 11y−66=−4x+2011y - 66 = -4x + 20 So 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(1000−P)\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(1000−P)=0.001 dt\frac{dP}{P(1000-P)} = 0.001\,dt. Using partial fractions: 1P(1000−P)=1/1000P+1/10001000−P\frac{1}{P(1000-P)} = \frac{1/1000}{P} + \frac{1/1000}{1000-P}.

11000ln⁡∣P1000−P∣=0.001t+C\frac{1}{1000}\ln\left|\frac{P}{1000-P}\right| = 0.001t + C. ln⁡∣P1000−P∣=t+C"\ln\left|\frac{P}{1000-P}\right| = t + C".

P1000−P=Aet\frac{P}{1000-P} = Ae^t. At t=0t = 0: 100900=A\frac{100}{900} = A So A=1/9A = 1/9.

P1000−P=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 t→∞t \to \infty: P→1000P \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/2xsin⁡x dx\int_0^{\pi/2} x\sin x\,dx using integration by parts. (b) Use the Maclaurin series for exe^x to evaluate ∫00.1e−x2 dx\int_0^{0.1} e^{-x^2}\,dx correct to 4 decimal places. (c) Evaluate ∫1x2−9 dx\int \frac{1}{x^2 - 9}\,dx using partial fractions. (d) Evaluate ∫0∞xe−x dx\int_0^{\infty} xe^{-x}\,dx.

Solution:

(a) u = x$$dv = \sin x\,dx. du = dx$$v = -\cos x. ∫0π/2xsin⁡x dx=[−xcos⁡x]0π/2+∫0π/2cos⁡x dx=0+[sin⁡x]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) e−x2=1−x2+x42−x66+⋯e^{-x^2} = 1 - x^2 + \frac{x^4}{2} - \frac{x^6}{6} + \cdots ∫00.1e−x2 dx=[x−x33+x510−x742]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} =0.1−0.0013+0.0000110−0.000000142= 0.1 - \frac{0.001}{3} + \frac{0.00001}{10} - \frac{0.0000001}{42} =0.1−0.000333+0.000001−0.0000000024=0.099668≈0.0997= 0.1 - 0.000333 + 0.000001 - 0.0000000024 = 0.099668 \approx 0.0997.

(c) 1x2−9=1(x−3)(x+3)=1/6x−3−1/6x+3\frac{1}{x^2 - 9} = \frac{1}{(x-3)(x+3)} = \frac{1/6}{x-3} - \frac{1/6}{x+3}. ∫=16ln⁡∣x−3∣−16ln⁡∣x+3∣+C=16ln⁡∣x−3x+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}. ∫0∞xe−x dx=[−xe−x]0∞+∫0∞e−x dx=0+[−e−x]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 (0≤θ≤2π0 \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)2 dxs = \int_a^b \sqrt{1 + \left(\frac{dy}{dx}\right)^2}\,dx. dydx=x1/2\frac{dy}{dx} = x^{1/2}. s=∫031+x dx=[23(1+x)3/2]03=23(8−1)=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 =2π∫03y1+(dydx)2 dx=2π∫0323x3/21+x dx= 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: =4π3∫14(u−1)3/2u1/2 du= \frac{4\pi}{3}\int_1^4 (u-1)^{3/2}u^{1/2}\,du.

This integral requires expanding (u−1)3/2=u3/2−3u1/2+3u−1/2−u−3/2(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.

=4π3∫14(u2−3u+3−u−1) du=4π3[u33−3u22+3u−ln⁡u]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[(643−24+12−ln⁡4)−(13−32+3−0)]=4π3(633−12+9−32−ln⁡4)= \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(21−12+9−1.5−1.386)=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. (−2sin⁡θ)2+(2cos⁡θ)2=4=2\sqrt{(-2\sin\theta)^2 + (2\cos\theta)^2} = \sqrt{4} = 2. s=∫02π2 dθ=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 Δx→0\Delta x \to 0: ds=1+(dy/dx)2 dxds = \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)2 dx\int \sqrt{1 + (dy/dx)^2}\,dx, not ∫y dx\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 2π∫y1+(dy/dx)2 dx2\pi\int y\sqrt{1+(dy/dx)^2}\,dx. Students often write π∫y1+(dy/dx)2 dx\pi\int y\sqrt{1+(dy/dx)^2}\,dx (confusing it with the volume formula π∫y2 dx\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=2cos⁡θx = 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).