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CIE 9231 2024 November Paper 11 Q5

A Level / CIE / FP1

CIE 9231 2024 Nov Paper 11 Paper · Question 5

题目

Problem

(a) Show that the curve with Cartesian equation

(x2+y2)2=6xy(x^2+y^2)^2=6xy

has polar equation r2=3sin⁡2θr^2=3\sin2\theta.

(2)

The curve CC has polar equation r2=3sin⁡2θr^2=3\sin2\theta, for 0⩽θ⩽12π0\leqslant\theta\leqslant\frac12\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.

(6)
题目中文翻译

(a) 证明:笛卡尔方程为

(x2+y2)2=6xy(x^2+y^2)^2=6xy

的曲线,其极坐标方程为 r2=3sin⁡2θr^2=3\sin2\theta。

(2)

曲线 CC 的极坐标方程为 r2=3sin⁡2θr^2=3\sin2\theta,其中 0⩽θ⩽12π0\leqslant\theta\leqslant\frac12\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。

(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

代入直角坐标与极坐标的关系,并用正弦倍角公式。除以r平方时要另外说明极点没有丢失。

答题过程

展开

Using x=rcos⁡θx=r\cos\theta, y=rsin⁡θy=r\sin\theta and x2+y2=r2x^2+y^2=r^2, we obtain

r4=6r2sin⁡θcos⁡θ=3r2sin⁡2θ.r^4=6r^2\sin\theta\cos\theta=3r^2\sin2\theta.

For r≠0r\ne0, division by r2r^2 gives

r2=3sin⁡2θ.\boxed{r^2=3\sin2\theta}.

The pole r=0r=0 belongs to the Cartesian curve and is also represented by this polar equation, for example at θ=0\theta=0. Thus it is retained.

(b)

解法一

思路

展开

给定角区间只画第一象限的一个闭环,不画整个双纽线。正弦取最大值时极径最大,环关于四十五度射线对称。

答题过程

展开

At θ=0\theta=0 and θ=π2\theta=\frac\pi2, r=0r=0. For angles between these values, r>0r>0.

Sketch a single loop in the first quadrant, starting and ending at the pole, symmetric about θ=π4\theta=\frac\pi4. The tangents at the pole are the two coordinate axes.

Since sin⁡2θ⩽1\sin2\theta\leqslant1, the maximum radius occurs at θ=π4\theta=\frac\pi4 and is 3\boxed{\sqrt3}.

(c)

解法一

思路

展开

一整个闭环由0至二分之π扫描,直接用极坐标面积积分。

答题过程

展开 A= 12∫0π/23sin⁡2θ dθ= 32[−12cos⁡2θ]0π/2= 32.\begin{align*} A=&\,\frac12\int_0^{\pi/2}3\sin2\theta\,\mathrm{d}\theta\\[4mm] =&\,\frac32\big[-\tfrac12\cos2\theta\big]_0^{\pi/2}\\[4mm] =&\,\boxed{\frac32}. \end{align*}

(d)

解法一

思路

展开

整个环都在第一象限,到极轴的距离就是纵坐标。对纵坐标求导后用三倍角恒等式整理,最后与端点的零距离比较。

答题过程

展开

The distance from the initial line is

y=rsin⁡θ=3 (sin⁡2θ)1/2sin⁡θ.y=r\sin\theta=\sqrt3\,(\sin2\theta)^{1/2}\sin\theta.

For 0<θ<π20<\theta<\frac\pi2,

dydθ= 3(sin⁡2θ)1/2cos⁡θ +3cos⁡2θsin⁡θ(sin⁡2θ)1/2.\begin{align*} \frac{\mathrm{d}y}{\mathrm{d}\theta} =&\,\sqrt3(\sin2\theta)^{1/2}\cos\theta\\[4mm] &\,+\frac{\sqrt3\cos2\theta\sin\theta}{(\sin2\theta)^{1/2}}. \end{align*}

At an interior stationary point, multiplication by the positive factor sin⁡2θ/3\sqrt{\sin2\theta}/\sqrt3 gives

sin⁡2θcos⁡θ+cos⁡2θsin⁡θ=0,\sin2\theta\cos\theta+\cos2\theta\sin\theta=0,

so sin⁡3θ=0\sin3\theta=0. In 0<θ<π20<\theta<\frac\pi2, the only solution is θ=π3\theta=\frac\pi3.

The distance is zero at both endpoints and positive inside, so this unique interior stationary point gives the maximum. Its distance is

ymax⁡= 3sin⁡(2π/3)sin⁡(π/3)= 332 32= 35/422(≈1.40).\begin{align*} y_{\max}=&\,\sqrt{3\sin(2\pi/3)}\sin(\pi/3)\\[4mm] =&\,\sqrt{\frac{3\sqrt3}{2}}\,\frac{\sqrt3}{2}\\[4mm] =&\,\boxed{\frac{3^{5/4}}{2\sqrt2}} \quad(\approx1.40). \end{align*}