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CIE 9709 2023 Nov Paper 32 Q5

A Level / CIE / P3

CIE 9709 2023 Nov Paper 32 Paper · Question 5

题目

Problem

Find the exact value of ∫06x(x+1)x2+4 dx\displaystyle\int_0^6\frac{x(x+1)}{x^2+4}\,\mathrm{d}x.

(6)
题目中文翻译

求 ∫06x(x+1)x2+4 dx\displaystyle\int_0^6\frac{x(x+1)}{x^2+4}\,\mathrm{d}x 的精确值。

(6)
原卷通用作答要求

Answer all questions. You should use a calculator where appropriate.

You must show all necessary working clearly; no marks will be given for unsupported answers from a calculator.

Give non-exact numerical answers correct to 3 significant figures, or 1 decimal place for angles in degrees, unless a different level of accuracy is specified in the question.

请回答所有题目。适当时应使用计算器。必须清楚展示所有必要的计算过程;仅给出计算器答案而没有过程,不予评分。除非题目另有精度要求,非精确数值答案保留 3 位有效数字,以度为单位的角度保留 1 位小数。

解答

解法一

思路

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先做多项式除法,把被积函数拆成常数、对数型与反正切型三项。

答题过程

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Rewrite the integrand:

x(x+1)x2+4= 1+x−4x2+4= 1+xx2+4−4x2+4.\begin{align*} \frac{x(x+1)}{x^2+4} =&\,1+\frac{x-4}{x^2+4}\\[4mm] =&\,1+\frac{x}{x^2+4}-\frac4{x^2+4}. \end{align*}

The derivative of x2+4x^2+4 is 2x2x, and d(tan⁡−1(x/2))/dx=2/(x2+4)\mathrm{d}(\tan^{-1}(x/2))/\mathrm{d}x=2/(x^2+4). Therefore

I= [x+12ln⁡(x2+4)−2tan⁡−1x2]06= 6+12ln⁡40−2tan⁡−13−12ln⁡4= 6+12ln⁡10−2tan⁡−13.\begin{align*} I =&\,\bigg[x+\frac12\ln(x^2+4) -2\tan^{-1}\frac x2\bigg]_0^6\\[4mm] =&\,6+\frac12\ln40-2\tan^{-1}3-\frac12\ln4\\[4mm] =&\,\boxed{6+\frac12\ln10-2\tan^{-1}3}. \end{align*}

解法二

思路

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也可作 x=2tan⁡θx=2\tan\theta。代换后分母与微分中的 sec⁡2θ\sec^2\theta 相消,用 tan⁡2θ=sec⁡2θ−1\tan^2\theta=\sec^2\theta-1 积分。

答题过程

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Put x=2tan⁡θx=2\tan\theta. Then

dx= 2sec⁡2θ dθ,x2+4= 4sec⁡2θ.\begin{align*} \mathrm{d}x=&\,2\sec^2\theta\,\mathrm{d}\theta,\\[4mm] x^2+4=&\,4\sec^2\theta. \end{align*}

The limits x=0,6x=0,6 become θ=0,tan⁡−13\theta=0,\tan^{-1}3. Hence

I= ∫0tan⁡−13(2tan⁡2θ+tan⁡θ) dθ= ∫0tan⁡−13(2sec⁡2θ−2+tan⁡θ) dθ= [2tan⁡θ−2θ+ln⁡(sec⁡θ)]0tan⁡−13.\begin{align*} I =&\,\int_0^{\tan^{-1}3} (2\tan^2\theta+\tan\theta)\,\mathrm{d}\theta\\[4mm] =&\,\int_0^{\tan^{-1}3} (2\sec^2\theta-2+\tan\theta)\,\mathrm{d}\theta\\[4mm] =&\,\big[2\tan\theta-2\theta+\ln(\sec\theta)\big]_0^{\tan^{-1}3}. \end{align*}

Here sec⁡θ>0\sec\theta>0 throughout. At the upper limit, sec⁡θ=1+32=10\sec\theta=\sqrt{1+3^2}=\sqrt{10}. Thus

I=6+12ln⁡10−2tan⁡−13.\boxed{I=6+\frac12\ln10-2\tan^{-1}3}.