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CIE 9231 2021 November Paper 21 Q8

A Level / CIE / FP2

CIE 9231 2021 Nov Paper 21 Paper · Question 8

题目

Problem

(a) Starting from the definition of cosh in terms of exponentials, prove that

2cosh⁡2A=cosh⁡2A+1.2\cosh^2A=\cosh 2A+1.
[3]

The curve CC has parametric equations

x= 2cosh⁡2t+3t,y= 32cosh⁡2t−4t,−12≤t≤12.\begin{align*} x=&\,2\cosh 2t+3t,\\ y=&\,\frac{3}{2}\cosh 2t-4t,\qquad -\frac{1}{2}\le t\le\frac{1}{2}. \end{align*}

The area of the surface generated when CC is rotated through 2π2\pi radians about the yy-axis is denoted by AA.

(b) (i) Show that

A=10π∫−1212(2cosh⁡2t+3t)cosh⁡2t dt.A=10\pi\int_{-\frac{1}{2}}^{\frac{1}{2}}\big(2\cosh 2t+3t\big)\cosh 2t\,\mathrm{d}t.
[4]

(ii) Hence find AA in terms of π\pi and ee.

[7]
题目中文翻译

(a) 从用指数表示的 cosh⁡\cosh 定义出发,证明

2cosh⁡2A=cosh⁡2A+12\cosh^2A=\cosh 2A+1
(3)

曲线 CC 的参数方程为

x= 2cosh⁡2t+3t,y= 32cosh⁡2t−4t,−12≤t≤12.\begin{align*} x=&\,2\cosh 2t+3t,\\ y=&\,\frac{3}{2}\cosh 2t-4t,\qquad -\frac{1}{2}\le t\le\frac{1}{2}. \end{align*}

将曲线 CC 绕 yy 轴旋转 2π2\pi 弧度后生成的曲面面积记为 AA。

(b) (i) 证明

A=10π∫−1212(2cosh⁡2t+3t)cosh⁡2t dtA=10\pi\int_{-\frac{1}{2}}^{\frac{1}{2}}\big(2\cosh 2t+3t\big)\cosh 2t\,\mathrm{d}t
(4)

(ii) 由此求出用 π\pi 和 ee 表示的 AA。

(7)
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

把 cosh⁡A\cosh A 写成两个指数之和。平方展开后,首尾两项组成 cosh⁡2A\cosh2A。

答题过程

展开

The exponential definition is cosh⁡A=(eA+e−A)/2\cosh A=(e^A+e^{-A})/2. Hence

2cosh⁡2A= 12(eA+e−A)2= 12(e2A+2+e−2A)= cosh⁡2A+1.\begin{align*} 2\cosh^2A=&\,\frac12(e^A+e^{-A})^2\\ =&\,\frac12(e^{2A}+2+e^{-2A})\\ =&\,\cosh2A+1. \end{align*}

(b)(i)

解法一

思路

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绕 yy 轴旋转的半径是 xx。两个参数导数平方相加后,交叉项抵消,弧长因子化为 5cosh⁡2t5\cosh 2t。

答题过程

展开

The derivatives are x′=4sinh⁡2t+3x'=4\sinh2t+3 and y′=3sinh⁡2t−4y'=3\sinh2t-4. Thus

(x′)2+(y′)2= 16sinh⁡22t+24sinh⁡2t+9 +9sinh⁡22t−24sinh⁡2t+16= 25(sinh⁡22t+1)= 25cosh⁡22t.\begin{align*} (x')^2+(y')^2=&\,16\sinh^22t+24\sinh2t+9\\ &\,\hspace{2pt}+9\sinh^22t-24\sinh2t+16\\ =&\,25(\sinh^22t+1)\\ =&\,25\cosh^22t. \end{align*}

The speed is 5cosh⁡2t5\cosh2t. Also x=2cosh⁡2t+3t≥2−32>0x=2\cosh2t+3t\ge2-\frac32>0 on the given interval. Rotating about the yy-axis therefore gives

A= 2π∫−1/21/2x(x′)2+(y′)2 dt= 10π∫−1/21/2(2cosh⁡2t+3t)cosh⁡2t dt.\begin{align*} A=&\,2\pi\int_{-1/2}^{1/2}x\sqrt{(x')^2+(y')^2}\,\mathrm{d}t\\ =&\,10\pi\int_{-1/2}^{1/2}(2\cosh2t+3t)\cosh2t\,\mathrm{d}t. \end{align*}

(b)(ii)

解法一

思路

展开

展开被积函数。tcosh⁡2tt\cosh2t 是奇函数,在对称区间上的积分为零。其余部分用 (a) 的倍角恒等式积分。

答题过程

展开

Since tcosh⁡2tt\cosh2t is odd and the interval is symmetric, its integral is zero. Applying (a) with argument 2t2t gives

A= 10π∫−1/21/22cosh⁡22t dt= 10π∫−1/21/2(cosh⁡4t+1) dt= 10π[14sinh⁡4t+t]−1/21/2= 10π(1+12sinh⁡2)= 10π(1+e2−e−24).\begin{align*} A=&\,10\pi\int_{-1/2}^{1/2}2\cosh^2 2t\,\mathrm{d}t\\ =&\,10\pi\int_{-1/2}^{1/2}(\cosh4t+1)\,\mathrm{d}t\\ =&\,10\pi\bigg[\frac14\sinh4t+t\bigg]_{-1/2}^{1/2}\\ =&\,10\pi\bigg(1+\frac12\sinh2\bigg)\\ =&\,\boxed{10\pi\bigg(1+\frac{e^2-e^{-2}}4\bigg)}. \end{align*}

解法二

思路

展开

也可直接对乘积做分部积分,把积分中的 cosh⁡2t\cosh2t 先积分为 12sinh⁡2t\frac12\sinh2t。余下的平方项用双曲正弦的倍角恒等式。

答题过程

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For integration by parts take u=2cosh⁡2t+3tu=2\cosh2t+3t and dv=cosh⁡2t dt\mathrm{d}v=\cosh2t\,\mathrm{d}t. Then u′=4sinh⁡2t+3u'=4\sinh2t+3 and v=12sinh⁡2tv=\frac12\sinh2t, giving

A10π= [(cosh⁡2t+32t)sinh⁡2t]−1/21/2 −∫−1/21/2(2sinh⁡22t+32sinh⁡2t) dt.\begin{align*} \frac{A}{10\pi} =&\,\bigg[\bigg(\cosh2t+\frac32t\bigg)\sinh2t\bigg]_{-1/2}^{1/2}\\ &\,\hspace{2pt}-\int_{-1/2}^{1/2}\bigg(2\sinh^2 2t+\frac32\sinh2t\bigg)\,\mathrm{d}t. \end{align*}

The boundary term from tsinh⁡2tt\sinh2t cancels because it is even, and the integral of sinh⁡2t\sinh2t is zero because it is odd. The remaining boundary term is sinh⁡2\sinh2, and 2sinh⁡22t=cosh⁡4t−12\sinh^2 2t=\cosh4t-1. Hence

A10π= sinh⁡2−[14sinh⁡4t−t]−1/21/2= 1+12sinh⁡2= 1+e2−e−24.\begin{align*} \frac A{10\pi}=&\,\sinh2-\bigg[\frac14\sinh4t-t\bigg]_{-1/2}^{1/2}\\ =&\,1+\frac12\sinh2\\ =&\,1+\frac{e^2-e^{-2}}4. \end{align*}