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CIE 9231 2024 June Paper 13 Q7

A Level / CIE / FP1

CIE 9231 2024 June Paper 13 Paper · Question 7

题目

Problem

The curve CC has polar equation r2=sin⁡2θcos⁡θr^2=\sin2\theta\cos\theta, for 0⩽θ⩽π0\leqslant\theta\leqslant\pi.

(a) Sketch CC and state the equation of the line of symmetry.

(3)

(b) Find a Cartesian equation for CC.

(3)

(c) Find the total area enclosed by CC.

(4)

(d) Find the greatest distance of a point on CC from the pole.

(6)
题目中文翻译

曲线 CC 的极坐标方程为 r2=sin⁡2θcos⁡θr^2=\sin2\theta\cos\theta,其中 0⩽θ⩽π0\leqslant\theta\leqslant\pi。

(a) 画出 CC 的草图,并写出对称轴的方程。

(3)

(b) 求 CC 的一个笛卡尔方程。

(3)

(c) 求 CC 所围区域的总面积。

(4)

(d) 求 CC 上的点到极点的最大距离。

(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

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将极径平方写成2sinθ乘cos平方,整段角区间都非负。零点把曲线分成第一、第二象限的两个环,关于纵轴对称。

答题过程

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Write

r2= sin⁡2θcos⁡θ= 2sin⁡θcos⁡2θ⩾0.\begin{align*} r^2=&\,\sin2\theta\cos\theta\\[4mm] =&\,2\sin\theta\cos^2\theta\geqslant0. \end{align*}

Here 0⩽θ⩽π0\leqslant\theta\leqslant\pi. The radius is zero at θ=0,π2,π\theta=0,\frac\pi2,\pi, and positive between these angles. Sketch one loop in the first quadrant for 0<θ<π20<\theta<\frac\pi2 and its mirror image in the second quadrant for π2<θ<π\frac\pi2<\theta<\pi, meeting at the pole. At the pole, each loop has one tangent along the initial line and one along the vertical axis.

Since replacing θ\theta by π−θ\pi-\theta leaves r2r^2 unchanged, the line of symmetry is

θ=π2(the y-axis).\boxed{\theta=\frac\pi2}\qquad\text{(the $y$-axis)}.

(b)

解法一

思路

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先用倍角式,再乘r三次方,右边恰好化成两个横坐标与一个纵坐标的乘积。保留二分之五次幂形式,不平方增加下半平面的额外分支。

答题过程

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Using r2=2sin⁡θcos⁡2θr^2=2\sin\theta\cos^2\theta, multiply by r3r^3:

r5=2(rsin⁡θ)(rcos⁡θ)2=2yx2.r^5=2(r\sin\theta)(r\cos\theta)^2=2yx^2.

Since r=x2+y2r=\sqrt{x^2+y^2}, a Cartesian equation is

(x2+y2)5/2=2x2y.\boxed{(x^2+y^2)^{5/2}=2x^2y}.

This equation retains the upper-half-plane condition of the polar curve; it also includes the pole.

(c)

解法一

思路

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整个角区间恰好扫过两个环各一次,可直接积分;把正弦倍角展开后,余弦立方的导数立即出现。

答题过程

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The total area is

A= 12∫0πsin⁡2θcos⁡θ dθ= ∫0πsin⁡θcos⁡2θ dθ= [−13cos⁡3θ]0π= 23.\begin{align*} A=&\,\frac12\int_0^\pi\sin2\theta\cos\theta\,\mathrm{d}\theta\\[4mm] =&\,\int_0^\pi\sin\theta\cos^2\theta\,\mathrm{d}\theta\\[4mm] =&\,\big[-\tfrac13\cos^3\theta\big]_0^\pi\\[4mm] =&\,\boxed{\frac23}. \end{align*}

(d)

解法一

思路

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对极径平方求导,比直接对根式求导简洁。先检查三个极径为零的角,再找两个环内部的最大点。

答题过程

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Since r⩾0r\geqslant0, maximising rr is equivalent to maximising r2=2sin⁡θcos⁡2θr^2=2\sin\theta\cos^2\theta.

Differentiating,

d(r2)dθ= 2cos⁡3θ−4sin⁡2θcos⁡θ= 2cos⁡θ(cos⁡2θ−2sin⁡2θ)= 2cos⁡θ(3cos⁡2θ−2).\begin{align*} \frac{\mathrm{d}(r^2)}{\mathrm{d}\theta} =&\,2\cos^3\theta-4\sin^2\theta\cos\theta\\[4mm] =&\,2\cos\theta\big(\cos^2\theta-2\sin^2\theta\big)\\[4mm] =&\,2\cos\theta(3\cos^2\theta-2). \end{align*}

The value at θ=0,π2,π\theta=0,\frac\pi2,\pi is r=0r=0. The remaining stationary candidates satisfy

cos⁡2θ=23,sin⁡θ=13,\cos^2\theta=\frac23,\qquad \sin\theta=\frac1{\sqrt3},

with one angle in each loop. At either point,

r2=2(13)23=433.r^2=2\bigg(\frac1{\sqrt3}\bigg)\frac23 =\frac4{3\sqrt3}.

These positive values exceed those at all endpoints, so the greatest distance is

rmax⁡=433(≈0.877).\boxed{r_{\max}=\sqrt{\frac4{3\sqrt3}}} \quad(\approx0.877).