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2017 A-Level · Paper 1 · Question 7

2017 H2 Maths Paper 1, Question 7

Integration 8 marks products of sines
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Part (i)

3 marks

Approach

A product of two sines has no elementary antiderivative on its own; we first rewrite it as a sum using the factor formula sin⁡Asin⁡B=12[cos⁡(A−B)−cos⁡(A+B)]\sin A\sin B = \frac{1}{2}\left\lbrack \cos(A - B) - \cos(A + B) \right\rbrack, which is easy to integrate term by term.

Using the factor formula with A=2mxA = 2mx, B=2nxB = 2nx:

sin⁡2mxsin⁡2nx=12[cos⁡(2(m−n)x)−cos⁡(2(m+n)x)]\sin 2mx\sin 2nx = \frac{1}{2}\left\lbrack \cos\left( 2(m - n)x \right) - \cos\left( 2(m + n)x \right) \right\rbrack

Since m≠nm \neq n, both m−nm - n and m+nm + n are non-zero, so we may integrate term by term:

∫sin⁡2mxsin⁡2nx dx\int\sin 2mx\sin 2nx\, dx
=12∫[cos⁡(2(m−n)x)−cos⁡(2(m+n)x)]dx= \frac{1}{2}\int\left\lbrack \cos\left( 2(m - n)x \right) - \cos\left( 2(m + n)x \right) \right\rbrack dx
=sin⁡(2(m−n)x)4(m−n)−sin⁡(2(m+n)x)4(m+n)+C= \frac{\sin\left( 2(m - n)x \right)}{4(m - n)} - \frac{\sin\left( 2(m + n)x \right)}{4(m + n)} + C

∴ ∫sin⁡2mxsin⁡2nx dx=sin⁡(2(m−n)x)4(m−n)−sin⁡(2(m+n)x)4(m+n)+C\therefore\ \int\sin 2mx\sin 2nx\, dx = \frac{\sin\left( 2(m - n)x \right)}{4(m - n)} - \frac{\sin\left( 2(m + n)x \right)}{4(m + n)} + C

Part (ii)

5 marks

Approach

Expanding (f(x))2\left( f(x) \right)^{2} gives two squared-sine terms and a cross term proportional to sin⁡2mxsin⁡2nx\sin 2mx\sin 2nx, which part (i) already handles. Each squared-sine term is dealt with by the double-angle identity sin⁡2θ=12(1−cos⁡2θ)\sin^{2}\theta = \frac{1}{2}\left( 1 - \cos 2\theta \right).

(f(x))2=sin⁡22mx+2sin⁡2mxsin⁡2nx+sin⁡22nx\left( f(x) \right)^{2} = \sin^{2}2mx + 2\sin 2mx\sin 2nx + \sin^{2}2nx

So

∫0π(f(x))2 dx=∫0πsin⁡22mx dx+2∫0πsin⁡2mxsin⁡2nx dx+∫0πsin⁡22nx dx\int_{0}^{\pi}\left( f(x) \right)^{2}\, dx = \int_{0}^{\pi}\sin^{2}2mx\, dx + 2\int_{0}^{\pi}\sin 2mx\sin 2nx\, dx + \int_{0}^{\pi}\sin^{2}2nx\, dx

We first find ∫0πsin⁡22mx dx\int_{0}^{\pi}\sin^{2}2mx\, dx. Using sin⁡22mx=12(1−cos⁡4mx)\sin^{2}2mx = \frac{1}{2}\left( 1 - \cos 4mx \right):

∫0πsin⁡22mx dx\int_{0}^{\pi}\sin^{2}2mx\, dx
=12[x−sin⁡4mx4m]0π= \frac{1}{2}\left\lbrack x - \frac{\sin 4mx}{4m} \right\rbrack_{0}^{\pi}
=12(π−sin⁡4mπ4m)= \frac{1}{2}\left( \pi - \frac{\sin 4m\pi}{4m} \right)

Since mm is a positive integer, sin⁡4mπ=0\sin 4m\pi = 0, so

∫0πsin⁡22mx dx=π2\int_{0}^{\pi}\sin^{2}2mx\, dx = \frac{\pi}{2}

By the same working with nn in place of mm (and sin⁡4nπ=0\sin 4n\pi = 0 since nn is a positive integer),

∫0πsin⁡22nx dx=π2\int_{0}^{\pi}\sin^{2}2nx\, dx = \frac{\pi}{2}

Now the cross term, using the result of (i):

∫0πsin⁡2mxsin⁡2nx dx\int_{0}^{\pi}\sin 2mx\sin 2nx\, dx
=[sin⁡(2(m−n)x)4(m−n)−sin⁡(2(m+n)x)4(m+n)]0π= \left\lbrack \frac{\sin\left( 2(m - n)x \right)}{4(m - n)} - \frac{\sin\left( 2(m + n)x \right)}{4(m + n)} \right\rbrack_{0}^{\pi}

Since m−nm - n and m+nm + n are non-zero integers, sin⁡(2(m−n)π)=0\sin\left( 2(m - n)\pi \right) = 0 and sin⁡(2(m+n)π)=0\sin\left( 2(m + n)\pi \right) = 0, and both terms vanish at x=0x = 0 too, so

∫0πsin⁡2mxsin⁡2nx dx=0\int_{0}^{\pi}\sin 2mx\sin 2nx\, dx = 0

Combining the three results:

∫0π(f(x))2 dx=π2+2(0)+π2\int_{0}^{\pi}\left( f(x) \right)^{2}\, dx = \frac{\pi}{2} + 2(0) + \frac{\pi}{2}
To check your answer: taking m=1m = 1, n=2n = 2 as a concrete case and evaluating ∫0π(sin⁡2x+sin⁡4x)2 dx\int_{0}^{\pi}\left( \sin 2x + \sin 4x \right)^{2}\, dx by GC gives π\pi, which matches. ✓

∴ ∫0π(f(x))2 dx=π\therefore\ \int_{0}^{\pi}\left( f(x) \right)^{2}\, dx = \pi

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