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CIE 9231 2022 June Paper 12 Q6

A Level / CIE / FP1

CIE 9231 2022 June Paper 12 Paper · Question 6

题目

Problem

The curve CC has polar equation r2=tan⁡−1(12θ)r^2=\tan^{-1}\big(\frac12\theta\big), where 0≤θ≤20\le\theta\le2.

(a) Sketch CC and state, in exact form, the greatest distance of a point on CC from the pole.

(3)

(b) Find the exact value of the area of the region bounded by CC and the half-line θ=2\theta=2.

(5)

Now consider the part of CC where 0≤θ≤12π0\le\theta\le\frac12\pi.

(c) Show that, at the point furthest from the half-line θ=12π\theta=\frac12\pi,

(θ2+4)tan⁡−1(12θ)sin⁡θ−cos⁡θ=0(\theta^2+4)\tan^{-1}\big(\tfrac12\theta\big)\sin\theta-\cos\theta=0

and verify that this equation has a root between 0.60.6 and 0.70.7.

(5)
题目中文翻译

曲线 CC 的极坐标方程为 r2=tan⁡−1(12θ)r^2=\tan^{-1}\big(\frac12\theta\big),其中 0≤θ≤20\le\theta\le2。

(a) 画出 CC 的草图,并用精确形式写出 CC 上的点到极点的最大距离。

(3)

(b) 求由 CC 与射线 θ=2\theta=2 所围区域面积的精确值。

(5)

现在考虑 CC 上满足 0≤θ≤12π0\le\theta\le\frac12\pi 的部分。

(c) 证明在距离射线 θ=12π\theta=\frac12\pi 最远的点处,

(θ2+4)tan⁡−1(12θ)sin⁡θ−cos⁡θ=0(\theta^2+4)\tan^{-1}\big(\tfrac12\theta\big)\sin\theta-\cos\theta=0

并验证此方程在 0.60.6 与 0.70.7 之间有一个根。

(5)
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

半径随角度增大而增大,但端点角度是 22 弧度,曲线应伸入第二象限,不能画成第一象限的闭曲线。

答题过程

展开

As θ\theta increases from 00 to 22, tan⁡−1(θ/2)\tan^{-1}(\theta/2) increases from 00 to π/4\pi/4. The curve starts at the pole on the positive initial line, curves anticlockwise through the first quadrant, and ends in the second quadrant on the half-line θ=2\theta=2.

Since r≥0r\ge0, its greatest distance from the pole is

rmax⁡=tan⁡−1(1)=π2.\boxed{r_{\max}=\sqrt{\tan^{-1}(1)}=\frac{\sqrt\pi}{2}}.

Near the pole, r2∼θ/2r^2\sim\theta/2, so x∼θ/2x\sim\sqrt{\theta/2} and y∼θθ/2y\sim\theta\sqrt{\theta/2}, giving y∼2x3y\sim2x^3. Thus the initial tangent is horizontal. For θ>0\theta>0,

dydx= r′sin⁡θ+rcos⁡θr′cos⁡θ−rsin⁡θ,r′= 1r(θ2+4).\begin{align*} \frac{\mathrm{d}y}{\mathrm{d}x} =&\,\frac{r'\sin\theta+r\cos\theta}{r'\cos\theta-r\sin\theta},\\[4mm] r'=&\,\frac1{r(\theta^2+4)}. \end{align*}

At θ=2\theta=2, this gradient is

sin⁡2+2πcos⁡2cos⁡2−2πsin⁡2≈0.278>0.\frac{\sin2+2\pi\cos2}{\cos2-2\pi\sin2}\approx0.278>0.

The endpoint tangent therefore slopes upwards to the right. Label the maximum radius at this endpoint and mark the initial line and the half-line θ=2\theta=2.

(b)

解法一

思路

展开

极坐标面积要积 r2r^2。反正切的积分用分部积分,剩下的一项可直接识别成对数导数。

答题过程

展开

The required area is

A=12∫02tan⁡−1(θ2) dθ.A=\frac12\int_0^2\tan^{-1}\bigg(\frac\theta2\bigg)\,\mathrm{d}\theta.

Integrate by parts, taking u=tan⁡−1(θ/2)u=\tan^{-1}(\theta/2) and dv=dθ\mathrm{d}v=\mathrm{d}\theta. Then

dudθ=2θ2+4,v=θ.\frac{\mathrm{d}u}{\mathrm{d}\theta}=\frac2{\theta^2+4},\qquad v=\theta.

Consequently,

A= 12[θtan⁡−1(θ2)]02 −12∫022θθ2+4 dθ= π4−12[ln⁡(θ2+4)]02= π4−12ln⁡84= π4−12ln⁡2.\begin{align*} A=&\,\frac12\bigg[\theta\tan^{-1}\bigg(\frac\theta2\bigg)\bigg]_0^2\\[4mm] &\,-\frac12\int_0^2\frac{2\theta}{\theta^2+4}\,\mathrm{d}\theta\\[4mm] =&\,\frac\pi4-\frac12[\ln(\theta^2+4)]_0^2\\[4mm] =&\,\frac\pi4-\frac12\ln\frac84\\[4mm] =&\,\boxed{\frac\pi4-\frac12\ln2}. \end{align*}

(c)

解法一

思路

展开

到正 yy 轴射线的距离是横坐标 rcos⁡θr\cos\theta;在指定第一象限内不需要再取绝对值。求导为零后代入极坐标方程。

答题过程

展开

For 0≤θ≤π/20\le\theta\le\pi/2, the perpendicular distance from the half-line θ=π/2\theta=\pi/2 is

x=rcos⁡θ.x=r\cos\theta.

It is zero at both endpoints and positive in between, so its maximum is at an interior stationary point. Differentiating r2=tan⁡−1(θ/2)r^2=\tan^{-1}(\theta/2) gives

2rdrdθ=2θ2+4.2r\frac{\mathrm{d}r}{\mathrm{d}\theta}=\frac2{\theta^2+4}.

At the maximum,

dxdθ=drdθcos⁡θ−rsin⁡θ=0.\frac{\mathrm{d}x}{\mathrm{d}\theta} =\frac{\mathrm{d}r}{\mathrm{d}\theta}\cos\theta-r\sin\theta=0.

Multiplying by r(θ2+4)r(\theta^2+4), which is positive in the interior, gives

cos⁡θ−(θ2+4)r2sin⁡θ=0.\cos\theta-(\theta^2+4)r^2\sin\theta=0.

Substituting for r2r^2 yields

(θ2+4)tan⁡−1(θ2)sin⁡θ−cos⁡θ=0.\boxed{(\theta^2+4)\tan^{-1}\bigg(\frac\theta2\bigg)\sin\theta-\cos\theta=0}.

Let the left-hand side be F(θ)F(\theta). In radians,

F(0.6)≈ −0.107815,F(0.7)≈ 0.209002.\begin{align*} F(0.6)\approx&\,-0.107815,\\[4mm] F(0.7)\approx&\,0.209002. \end{align*}

Since FF is continuous and changes sign, it has a root between 0.60.6 and 0.70.7.