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CIE 9231 2022 November Paper 21 Q8

A Level / CIE / FP2

CIE 9231 2022 Nov Paper 21 Paper · Question 8

题目

Problem

(a) Use the substitution u=1−(θ−1)2u=1-(\theta-1)^2 to find

∫θ−11−(θ−1)2 dθ.\int\frac{\theta-1}{\sqrt{1-(\theta-1)^2}}\,\mathrm{d}\theta.
(3)

(b) Find the solution of the differential equation

θdydθ−y=θ2sin⁡−1(θ−1),\theta\frac{\mathrm{d}y}{\mathrm{d}\theta}-y=\theta^2\sin^{-1}(\theta-1),

where 0<θ<20<\theta<2, given that y=1y=1 when θ=1\theta=1. Give your answer in the form y=f(θ)y=\mathrm{f}(\theta).

(11)
题目中文翻译

(a) 用代换 u=1−(θ−1)2u=1-(\theta-1)^2 求

∫θ−11−(θ−1)2 dθ.\int\frac{\theta-1}{\sqrt{1-(\theta-1)^2}}\,\mathrm{d}\theta.
(3)

(b) 求微分方程

θdydθ−y=θ2sin⁡−1(θ−1)\theta\frac{\mathrm{d}y}{\mathrm{d}\theta}-y=\theta^2\sin^{-1}(\theta-1)

的解,其中 0<θ<20<\theta<2,且当 θ=1\theta=1 时 y=1y=1。将答案写成 y=f(θ)y=\mathrm{f}(\theta) 的形式。

(11)
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

(a)

解法一

思路

展开

代换后,(θ−1) dθ=−12du(\theta-1)\,\mathrm{d}\theta=-\frac12\mathrm{d}u,被积函数化为 u−1/2u^{-1/2} 的倍数。

答题过程

展开

With u=1−(θ−1)2u=1-(\theta-1)^2, we have du=−2(θ−1) dθ\mathrm{d}u=-2(\theta-1)\,\mathrm{d}\theta. Therefore

∫θ−11−(θ−1)2 dθ= −12∫u−1/2 du= −1−(θ−1)2+C.\begin{align*} \int\frac{\theta-1}{\sqrt{1-(\theta-1)^2}}\,\mathrm{d}\theta =&\,-\frac12\int u^{-1/2}\,\mathrm{d}u\\ =&\,\boxed{-\sqrt{1-(\theta-1)^2}+C}. \end{align*}

(b)

解法一

思路

展开

除以 θ\theta 后,用积分因子 θ−1\theta^{-1}。右边先平移变量,再分部积分,余项可用 (a)。

答题过程

展开

On 0<θ<20<\theta<2, the standard form is

dydθ−yθ=θarcsin⁡(θ−1).\frac{\mathrm{d}y}{\mathrm{d}\theta}-\frac y\theta =\theta\arcsin(\theta-1).

Since θ>0\theta>0, the integrating factor is e∫−θ−1 dθ=e−ln⁡θ=θ−1e^{\int-\theta^{-1}\,\mathrm{d}\theta}=e^{-\ln\theta}=\theta^{-1}. Multiplying by it gives (y/θ)′=arcsin⁡(θ−1)(y/\theta)'=\arcsin(\theta-1). Put s=θ−1s=\theta-1, so ds=dθ\mathrm{d}s=\mathrm{d}\theta. For integration by parts, take u=arcsin⁡su=\arcsin s and dv=ds\mathrm{d}v=\mathrm{d}s, so du=ds/1−s2\mathrm{d}u=\mathrm{d}s/\sqrt{1-s^2} and v=sv=s. The remaining integral is exactly (a) with s=θ−1s=\theta-1. Thus

yθ= ∫arcsin⁡s ds= sarcsin⁡s−∫s1−s2 ds= sarcsin⁡s+1−s2+C.\begin{align*} \frac y\theta =&\,\int\arcsin s\,\mathrm{d}s\\ =&\,s\arcsin s-\int\frac{s}{\sqrt{1-s^2}}\,\mathrm{d}s\\ =&\,s\arcsin s+\sqrt{1-s^2}+C. \end{align*}

At θ=1\theta=1, s=0s=0 and y=1y=1, so C=0C=0. Thus

y=θ[(θ−1)arcsin⁡(θ−1)+1−(θ−1)2].y=\theta\big[(\theta-1)\arcsin(\theta-1)+\sqrt{1-(\theta-1)^2}\big].