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CIE 9231 2022 November Paper 13 Q6

A Level / CIE / FP1

CIE 9231 2022 Nov Paper 13 Paper · Question 6

题目

Problem

(a) Show that the curve with Cartesian equation

(x2+y2)2=36(x2−y2)(x^2+y^2)^2=36(x^2-y^2)

has polar equation r2=36cos⁡2θr^2=36\cos2\theta.

(3)

The curve CC has polar equation r2=36cos⁡2θr^2=36\cos2\theta, for −14π≤θ≤14π-\frac14\pi\le\theta\le\frac14\pi.

(b) Sketch CC and state the maximum distance of a point on CC from the pole.

(3)

(c) Find the area of the region enclosed by CC.

(2)

(d) Find the maximum distance of a point on CC from the initial line, giving the answer in exact form.

(6)
题目中文翻译

(a) 证明直角坐标方程为

(x2+y2)2=36(x2−y2)(x^2+y^2)^2=36(x^2-y^2)

的曲线,其极坐标方程为 r2=36cos⁡2θr^2=36\cos2\theta。

(3)

曲线 CC 的极坐标方程为 r2=36cos⁡2θr^2=36\cos2\theta,其中 −14π≤θ≤14π-\frac14\pi\le\theta\le\frac14\pi。

(b) 画出 CC 的草图,并写出 CC 上的点到极点的最大距离。

(3)

(c) 求 CC 所围区域的面积。

(2)

(d) 求 CC 上的点到极轴的最大距离,答案用精确形式表示。

(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

(a)

解法一

思路

展开

代入极坐标并用余弦倍角式;除r平方后另外保留极点。

答题过程

展开

Substituting x=rcos⁡θx=r\cos\theta, y=rsin⁡θy=r\sin\theta gives

r4= 36r2(cos⁡2θ−sin⁡2θ)= 36r2cos⁡2θ.\begin{align*} r^4=&\,36r^2(\cos^2\theta-\sin^2\theta)\\[4mm] =&\,36r^2\cos2\theta. \end{align*}

For r≠0r\ne0, divide by r2r^2 to obtain r2=36cos⁡2θ\boxed{r^2=36\cos2\theta}. The pole is also represented by this polar equation, for example at θ=π/4\theta=\pi/4, so it is retained.

(b)

解法一

思路

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角区间只对应右侧一个环,关于极轴对称。极径在θ=0最大,不画左侧另一个环。

答题过程

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The radius is zero at θ=±π/4\theta=\pm\pi/4 and positive between them. Sketch a single loop to the right of the pole, symmetric about the initial line, passing through (6,0)(6,0) and returning to the pole. Its two tangents at the pole are the lines y=±xy=\pm x.

Since r2⩽36r^2\leqslant36, the greatest distance from the pole is 6\boxed{6}, at θ=0\theta=0.

(c)

解法一

思路

展开

给定角区间完整扫过右环一次,直接积分半个极径平方。

答题过程

展开 A= 12∫−π/4π/436cos⁡2θ dθ= 9[sin⁡2θ]−π/4π/4= 18.\begin{align*} A=&\,\frac12\int_{-\pi/4}^{\pi/4}36\cos2\theta\,\mathrm{d}\theta\\[4mm] =&\,9\big[\sin2\theta\big]_{-\pi/4}^{\pi/4}\\[4mm] =&\,\boxed{18}. \end{align*}

(d)

解法一

思路

展开

利用上下对称,只在上半环找最大纵坐标。对y求导后,分子可化成余弦三倍角,内部唯一最大点再与端点比较。

答题过程

展开

By symmetry, the maximum perpendicular distance from the initial line equals the maximum yy for 0⩽θ⩽π/40\leqslant\theta\leqslant\pi/4, where

y=6cos⁡2θsin⁡θ.y=6\sqrt{\cos2\theta}\sin\theta.

For 0<θ<π/40<\theta<\pi/4,

dydθ= 6cos⁡2θcos⁡θ −6sin⁡2θsin⁡θcos⁡2θ= 6cos⁡3θcos⁡2θ.\begin{align*} \frac{\mathrm{d}y}{\mathrm{d}\theta} =&\,6\sqrt{\cos2\theta}\cos\theta\\[4mm] &\,-\frac{6\sin2\theta\sin\theta}{\sqrt{\cos2\theta}}\\[4mm] =&\,\frac{6\cos3\theta}{\sqrt{\cos2\theta}}. \end{align*}

Thus the only interior stationary point is θ=π/6\theta=\pi/6. The endpoint values are both y=0y=0, whereas at this point

y=6cos⁡(π/3)sin⁡(π/6)=32.y=6\sqrt{\cos(\pi/3)}\sin(\pi/6) =\frac3{\sqrt2}.

Hence the maximum distance is

322.\boxed{\frac{3\sqrt2}{2}}.

It occurs at θ=±π/6\theta=\pm\pi/6, on the upper and lower halves respectively.