Skip to content
CalcGospel 國際數學圖譜
返回

CIE 9231 2026 June Paper 12 Q7

A Level / CIE / FP1

CIE 9231 2026 June Paper 12 Paper · Question 7

题目

Problem

The curve CC has polar equation r2=a1+tan⁡2θr^2=\dfrac{a}{1+\tan2\theta} for 0⩽θ<14π0\leqslant\theta<\frac{1}{4}\pi, where aa is a positive constant.

(a) Show that, at the point on CC furthest from the initial line,

cos⁡θ−sin⁡θcos⁡2θ(sin⁡2θ+cos⁡2θ)=0\cos\theta-\frac{\sin\theta}{\cos2\theta(\sin2\theta+\cos2\theta)}=0

and verify that this equation has a root between 0.50.5 and 0.60.6.

(6)

(b) Sketch CC.

(2)

(c) Use the substitution v=tan⁡2θv=\tan2\theta to show that the area enclosed by CC and the initial line is

14a∫0∞1(1+v)(1+v2) dv\frac{1}{4}a\int_0^{\infty}\frac{1}{(1+v)(1+v^2)}\,\mathrm{d}v

and find the exact value of this area.

(9)

题目中文翻译

曲线 CC 的极坐标方程为 r2=a1+tan⁡2θr^2=\dfrac{a}{1+\tan2\theta},其中 0⩽θ<14π0\leqslant\theta<\frac{1}{4}\pi,aa 为正常数。

(a) 证明:在 CC 上距离极轴最远的点处,

cos⁡θ−sin⁡θcos⁡2θ(sin⁡2θ+cos⁡2θ)=0\cos\theta-\frac{\sin\theta}{\cos2\theta(\sin2\theta+\cos2\theta)}=0

并验证此方程在 0.50.5 与 0.60.6 之间有一个根。

(6)

(b) 画出 CC 的草图。

(2)

(c) 使用代换 v=tan⁡2θv=\tan2\theta,证明 CC 与极轴所围成的面积为

14a∫0∞1(1+v)(1+v2) dv\frac{1}{4}a\int_0^{\infty}\frac{1}{(1+v)(1+v^2)}\,\mathrm{d}v

并求此面积的精确值。

(9)

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

离初始线最远是让纵坐标y=r sinθ最大。对纵坐标求导,提出正因子后可化成指定式。

答题过程

展开

The perpendicular distance from the initial line is

y=rsin⁡θ=a (1+tan⁡2θ)−1/2sin⁡θ.y=r\sin\theta =\sqrt a\,(1+\tan2\theta)^{-1/2}\sin\theta.

It is positive for 0<θ<π/40<\theta<\pi/4 and tends to zero at the two ends. At an interior maximum, dy/dθ=0\mathrm{d}y/\mathrm{d}\theta=0.

By the product and chain rules,

dydθ= a(1+tan⁡2θ)−1/2cos⁡θ −asin⁡θ(1+tan⁡2θ)−3/2sec⁡22θ= r(cos⁡θ−sin⁡θsec⁡22θ1+tan⁡2θ).\begin{align*} \frac{\mathrm{d}y}{\mathrm{d}\theta} =&\,\sqrt a(1+\tan2\theta)^{-1/2}\cos\theta \\[4mm] &\,\hspace{2pt}-\sqrt a\sin\theta(1+\tan2\theta)^{-3/2}\sec^22\theta \\[4mm] =&\,r\bigg(\cos\theta- \frac{\sin\theta\sec^22\theta}{1+\tan2\theta}\bigg). \end{align*}

Since r>0r>0 at the maximum, division by rr is valid. Also

sec⁡22θ1+tan⁡2θ=1cos⁡2θ(sin⁡2θ+cos⁡2θ).\frac{\sec^22\theta}{1+\tan2\theta} =\frac1{\cos2\theta(\sin2\theta+\cos2\theta)}.

Thus the maximum satisfies

cos⁡θ−sin⁡θcos⁡2θ(sin⁡2θ+cos⁡2θ)=0,\boxed{\cos\theta- \frac{\sin\theta}{\cos2\theta(\sin2\theta+\cos2\theta)}=0},

as required.

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

f(0.5)= 0.2354162034…>0,f(0.6)= −0.3785037476…<0.\begin{align*} f(0.5)=&\,0.2354162034\ldots>0,\\[4mm] f(0.6)=&\,-0.3785037476\ldots<0. \end{align*}

The denominator is non-zero and ff is continuous on [0.5,0.6][0.5,0.6]. Hence there is a root between 0.50.5 and 0.60.6.

解法二

思路

展开

也可对距离平方求导,因为纵坐标为正,内部最大值对应距离平方的驻点。

答题过程

展开

The squared distance from the initial line is

y2=asin⁡2θ1+tan⁡2θ.y^2=\frac{a\sin^2\theta}{1+\tan2\theta}.

It vanishes at the two ends in the limiting sense and is positive in between. At an interior maximum of yy, differentiating gives

2ydydθ= 2asin⁡θcos⁡θ1+tan⁡2θ −2asin⁡2θsec⁡22θ(1+tan⁡2θ)2=0.\begin{align*} 2y\frac{\mathrm{d}y}{\mathrm{d}\theta} =&\,\frac{2a\sin\theta\cos\theta}{1+\tan2\theta} \\[4mm] &\,\hspace{2pt}-\frac{2a\sin^2\theta\sec^22\theta}{(1+\tan2\theta)^2}=0. \end{align*}

Divide by 2asin⁡θ/(1+tan⁡2θ)>02a\sin\theta/(1+\tan2\theta)>0:

cos⁡θ−sin⁡θsec⁡22θ1+tan⁡2θ=0.\cos\theta-\frac{\sin\theta\sec^22\theta}{1+\tan2\theta}=0.

Using sec⁡22θ/(1+tan⁡2θ)=1/[cos⁡2θ(sin⁡2θ+cos⁡2θ)]\sec^22\theta/(1+\tan2\theta)=1/[\cos2\theta(\sin2\theta+\cos2\theta)] gives the required equation. Its left-hand side has values 0.2354162034…0.2354162034\ldots and −0.3785037476…-0.3785037476\ldots at 0.50.5 and 0.60.6, respectively, and is continuous between them. Thus a root lies in (0.5,0.6)(0.5,0.6).

(b)

解法一

思路

展开

曲线在第一象限,从初始线上的半径√a处出发,再向极点靠近;画出单一拱形及其水平最高点。

答题过程

展开

At θ=0\theta=0, r=ar=\sqrt a, giving (a,0)(\sqrt a,0). As θ→π/4−\theta\to\pi/4^-, r→0r\to0, so the curve approaches the pole.

Sketch a single smooth arch in the first quadrant joining (a,0)(\sqrt a,0) towards OO, above the initial line. Mark the initial line and pole clearly, with a horizontal tangent at the highest point identified in (a). The tangent at (a,0)(\sqrt a,0) has gradient −1-1; near the pole the tangent approaches gradient 11.

(c)

解法一

思路

展开

先用极坐标面积公式,再完整处理题目指定的代换和无穷上限。分式分解后积分,对数项先合并再取极限。

答题过程

展开

The area is

A= 12∫0π/4r2 dθ= a2∫0π/411+tan⁡2θ dθ.\begin{align*} A=&\,\frac12\int_0^{\pi/4}r^2\,\mathrm{d}\theta\\[4mm] =&\,\frac a2\int_0^{\pi/4}\frac1{1+\tan2\theta}\,\mathrm{d}\theta. \end{align*}

Set v=tan⁡2θv=\tan2\theta. Then

dvdθ=2sec⁡22θ=2(1+v2).\frac{\mathrm{d}v}{\mathrm{d}\theta}=2\sec^22\theta=2(1+v^2).

Therefore

dθ=dv2(1+v2).\mathrm{d}\theta=\frac{\mathrm{d}v}{2(1+v^2)}.

When θ=0\theta=0, v=0v=0; as θ→π/4−\theta\to\pi/4^-, v→∞v\to\infty. Hence

A=a4∫0∞1(1+v)(1+v2) dv,\boxed{A=\frac a4\int_0^\infty\frac1{(1+v)(1+v^2)}\,\mathrm{d}v},

as required.

For partial fractions, write

1(1+v)(1+v2)=C1+v+Dv+E1+v2.\frac1{(1+v)(1+v^2)} =\frac{C}{1+v}+\frac{Dv+E}{1+v^2}.

Equating coefficients in

1=C(1+v2)+(Dv+E)(1+v)1=C(1+v^2)+(Dv+E)(1+v)

gives C+D=0C+D=0, D+E=0D+E=0, C+E=1C+E=1, so C=E=1/2C=E=1/2 and D=−1/2D=-1/2. Thus

1(1+v)(1+v2)=12(11+v−v1+v2+11+v2).\frac1{(1+v)(1+v^2)} =\frac12\bigg(\frac1{1+v}-\frac v{1+v^2}+\frac1{1+v^2}\bigg).

Therefore

A=a8lim⁡R→∞[ln⁡(1+v)−12ln⁡(1+v2)+tan⁡−1v]0R.A=\frac a8\lim_{R\to\infty} \bigg[\ln(1+v)-\frac12\ln(1+v^2)+\tan^{-1}v\bigg]_0^R.

Combine the logarithms before taking the limit:

ln⁡(1+R)−12ln⁡(1+R2)=ln⁡1+R1+R2⟶ln⁡1=0.\ln(1+R)-\frac12\ln(1+R^2) =\ln\frac{1+R}{\sqrt{1+R^2}} \longrightarrow\ln1=0.

Since tan⁡−1R→π/2\tan^{-1}R\to\pi/2 and the lower endpoint contributes zero,

A=a8π2=πa16.A=\frac a8\frac\pi2=\boxed{\frac{\pi a}{16}}.