· H2 Mathematics — Ten-Year Series, worked ← All 10 questions

2016 A-Level · Paper 2 · Question 2

2016 H2 Maths Paper 2, Question 2

Integration 10 marks by parts · definite integrals
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Part (a)(i)

3 marks

Approach

x2cos⁡nxx^{2}\cos nx is a product of a polynomial and a trigonometric function, so we integrate by parts, choosing x2x^{2} as the part that differentiates to something simpler and applying the process twice.

Let u=x2u = x^{2} and dvdx=cos⁡nx\frac{dv}{dx} = \cos nx, so dudx=2x\frac{du}{dx} = 2x and v=1nsin⁡nxv = \frac{1}{n}\sin nx.

∫x2cos⁡nx dx\int x^{2}\cos nx\, dx
=x2nsin⁡nx−∫2xnsin⁡nx dx= \frac{x^{2}}{n}\sin nx - \int\frac{2x}{n}\sin nx\, dx

For ∫xsin⁡nx dx\int x\sin nx\, dx, integrate by parts again with u=xu = x, dvdx=sin⁡nx\frac{dv}{dx} = \sin nx, so dudx=1\frac{du}{dx} = 1, v=−1ncos⁡nxv = - \frac{1}{n}\cos nx:

∫xsin⁡nx dx\int x\sin nx\, dx
=−xncos⁡nx+∫1ncos⁡nx dx= - \frac{x}{n}\cos nx + \int\frac{1}{n}\cos nx\, dx
=−xncos⁡nx+1n2sin⁡nx= - \frac{x}{n}\cos nx + \frac{1}{n^{2}}\sin nx

Substituting back:

∫x2cos⁡nx dx\int x^{2}\cos nx\, dx
=x2nsin⁡nx−2n(−xncos⁡nx+1n2sin⁡nx)+C= \frac{x^{2}}{n}\sin nx - \frac{2}{n}\left( - \frac{x}{n}\cos nx + \frac{1}{n^{2}}\sin nx \right) + C
=x2nsin⁡nx+2xn2cos⁡nx−2n3sin⁡nx+C= \frac{x^{2}}{n}\sin nx + \frac{2x}{n^{2}}\cos nx - \frac{2}{n^{3}}\sin nx + C

∴∫x2cos⁡nx dx=x2nsin⁡nx+2xn2cos⁡nx−2n3sin⁡nx+C\therefore\int x^{2}\cos nx\, dx = \frac{x^{2}}{n}\sin nx + \frac{2x}{n^{2}}\cos nx - \frac{2}{n^{3}}\sin nx + C.

Part (a)(ii)

2 marks

Approach

We evaluate the antiderivative from (i) at x=2πx = 2\pi and x=πx = \pi. Since nn is an integer, sin⁡nπ=sin⁡2nπ=0\sin n\pi = \sin 2n\pi = 0 for every nn, so only the cos⁡nx\cos nx term survives; but cos⁡2nπ=1\cos 2n\pi = 1 always, while cos⁡nπ=(−1)n\cos n\pi = ( - 1)^{n} depends on the parity of nn, so the two cases must be treated separately.

Using the result of (i):

∫π2πx2cos⁡nx dx=[x2nsin⁡nx+2xn2cos⁡nx−2n3sin⁡nx]π2π\int_{\pi}^{2\pi}x^{2}\cos nx\, dx = \left\lbrack \frac{x^{2}}{n}\sin nx + \frac{2x}{n^{2}}\cos nx - \frac{2}{n^{3}}\sin nx \right\rbrack_{\pi}^{2\pi}

Since nn is an integer, sin⁡2nπ=sin⁡nπ=0\sin 2n\pi = \sin n\pi = 0, so this reduces to

∫π2πx2cos⁡nx dx=4πn2cos⁡2nπ−2πn2cos⁡nπ\int_{\pi}^{2\pi}x^{2}\cos nx\, dx = \frac{4\pi}{n^{2}}\cos 2n\pi - \frac{2\pi}{n^{2}}\cos n\pi
=4πn2−2πn2cos⁡nπ= \frac{4\pi}{n^{2}} - \frac{2\pi}{n^{2}}\cos n\pi

Note: cos⁡nπ=(−1)n\cos n\pi = ( - 1)^{n}, which is 11 when nn is even and −1- 1 when nn is odd.

If nn is even:

∫π2πx2cos⁡nx dx=4πn2−2πn2=2πn2\int_{\pi}^{2\pi}x^{2}\cos nx\, dx = \frac{4\pi}{n^{2}} - \frac{2\pi}{n^{2}} = \frac{2\pi}{n^{2}}

If nn is odd:

∫π2πx2cos⁡nx dx=4πn2+2πn2=6πn2\int_{\pi}^{2\pi}x^{2}\cos nx\, dx = \frac{4\pi}{n^{2}} + \frac{2\pi}{n^{2}} = \frac{6\pi}{n^{2}}

∴∫π2πx2cos⁡nx dx=aπn2\therefore\int_{\pi}^{2\pi}x^{2}\cos nx\, dx = a\frac{\pi}{n^{2}}, where a=2a = 2 if nn is even, and a=6a = 6 if nn is odd.

Part (b)

5 marks

Approach

We need ∫02πy2 dx=π∫02x3(9−x2)2 dx\int_{0}^{2}\pi y^{2}\, dx = \pi\int_{0}^{2}\frac{x^{3}}{\left( 9 - x^{2} \right)^{2}}\, dx. The given substitution u=9−x2u = 9 - x^{2} turns 9−x29 - x^{2} into uu and, since du=−2x dxdu = - 2x\, dx, turns the leftover x2⋅x dxx^{2} \cdot x\, dx into (9−u)(9 - u) times a constant times dudu — this is why the substitution is chosen: it clears the awkward x2x^{2} inside the bracket as well as supplying the x dxx\, dx.

Let y=xx9−x2y = \frac{x\sqrt{x}}{9 - x^{2}}, so y2=x3(9−x2)2y^{2} = \frac{x^{3}}{\left( 9 - x^{2} \right)^{2}}.

Volume =π∫02y2 dx=π∫02x3(9−x2)2 dx\text{=}\pi\int_{0}^{2}y^{2}\, dx = \pi\int_{0}^{2}\frac{x^{3}}{\left( 9 - x^{2} \right)^{2}}\, dx.

Let u=9−x2u = 9 - x^{2}. Then dudx=−2x\frac{du}{dx} = - 2x, so x dx=−12 dux\, dx = - \frac{1}{2}\, du, and x2=9−ux^{2} = 9 - u.

When x=0x = 0, u=9u = 9; when x=2x = 2, u=5u = 5.

∫02x3(9−x2)2 dx=∫02x2(9−x2)2⋅x dx\int_{0}^{2}\frac{x^{3}}{\left( 9 - x^{2} \right)^{2}}\, dx = \int_{0}^{2}\frac{x^{2}}{\left( 9 - x^{2} \right)^{2}} \cdot x\, dx
=∫959−uu2(−12)du= \int_{9}^{5}\frac{9 - u}{u^{2}}\left( - \frac{1}{2} \right)du
=12∫59(9u2−1u)du= \frac{1}{2}\int_{5}^{9}\left( \frac{9}{u^{2}} - \frac{1}{u} \right)du
=12[−9u−ln⁡u]59= \frac{1}{2}\left\lbrack - \frac{9}{u} - \ln u \right\rbrack_{5}^{9}

Evaluating:

12[−9u−ln⁡u]59\frac{1}{2}\left\lbrack - \frac{9}{u} - \ln u \right\rbrack_{5}^{9}
=12[(−1−ln⁡9)−(−95−ln⁡5)]= \frac{1}{2}\left\lbrack \left( - 1 - \ln 9 \right) - \left( - \frac{9}{5} - \ln 5 \right) \right\rbrack
=12[45+ln⁡5−ln⁡9]= \frac{1}{2}\left\lbrack \frac{4}{5} + \ln 5 - \ln 9 \right\rbrack
=12(45+ln⁡59)= \frac{1}{2}\left( \frac{4}{5} + \ln\frac{5}{9} \right)
=25−12ln⁡95= \frac{2}{5} - \frac{1}{2}\ln\frac{9}{5}

So Volume =π(25−12ln⁡95)\text{=}\pi\left( \frac{2}{5} - \frac{1}{2}\ln\frac{9}{5} \right).

To check your answer: numerically this is π(0.4−0.2939…)=π(0.1061…)≈0.333\pi(0.4 - 0.2939\ldots) = \pi(0.1061\ldots) \approx 0.333, which is positive and small, consistent with a thin sliver of solid swept from a curve with y(0)=0y(0) = 0 and y(2)=225≈0.566y(2) = \frac{2\sqrt{2}}{5} \approx 0.566. ✓

∴\therefore the exact volume is π(25−12ln⁡95) units3\pi\left( \frac{2}{5} - \frac{1}{2}\ln\frac{9}{5} \right)\ \text{units}^{3}.

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