Skip to content
CalcGospel 國際數學圖譜
返回

CIE 9709 2023 June Paper 33 Q6

A Level / CIE / P3

CIE 9709 2023 June Paper 33 Paper · Question 6

题目

Problem

(a) Express 3cos⁡x+2cos⁡(x−60∘)3\cos x+2\cos(x-60^\circ) in the form Rcos⁡(x−α)R\cos(x-\alpha), where R>0R>0 and 0∘<α<90∘0^\circ<\alpha<90^\circ. State the exact value of RR and give α\alpha correct to 22 decimal places.

(4)

(b) Hence solve the equation

3cos⁡2θ+2cos⁡(2θ−60∘)=2.53\cos2\theta+2\cos(2\theta-60^\circ)=2.5

for 0∘<θ<180∘0^\circ<\theta<180^\circ.

(4)
题目中文翻译

(a) 将 3cos⁡x+2cos⁡(x−60∘)3\cos x+2\cos(x-60^\circ) 表示为 Rcos⁡(x−α)R\cos(x-\alpha) 的形式,其中 R>0R>0 且 0∘<α<90∘0^\circ<\alpha<90^\circ。写出 RR 的精确值,并求 α\alpha,结果保留 22 位小数。

(4)

(b) 由此解方程

3cos⁡2θ+2cos⁡(2θ−60∘)=2.5,3\cos2\theta+2\cos(2\theta-60^\circ)=2.5,

其中 0∘<θ<180∘0^\circ<\theta<180^\circ。

(4)
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

先展开 cos⁡(x−60∘)\cos(x-60^\circ),再比较 Rcos⁡(x−α)R\cos(x-\alpha) 的余弦与正弦系数。

答题过程

展开

Using the addition formula,

 3cos⁡x+2cos⁡(x−60∘)= 3cos⁡x +2(12cos⁡x+32sin⁡x)= 4cos⁡x+3sin⁡x.\begin{align*} &\,3\cos x+2\cos(x-60^\circ)\\[4mm] =&\,3\cos x\\[4mm] &\,\hspace{2pt}+2\bigg(\frac12\cos x+\frac{\sqrt3}{2}\sin x\bigg)\\[4mm] =&\,4\cos x+\sqrt3\sin x. \end{align*}

Also,

Rcos⁡(x−α)=Rcos⁡αcos⁡x+Rsin⁡αsin⁡x.R\cos(x-\alpha)=R\cos\alpha\cos x+R\sin\alpha\sin x.

Thus

Rcos⁡α= 4,Rsin⁡α= 3.\begin{align*} R\cos\alpha=&\,4,\\[4mm] R\sin\alpha=&\,\sqrt3. \end{align*}

Hence

R= 16+3=19,α= tan⁡−134= 23.413224…∘.\begin{align*} R=&\,\sqrt{16+3}=\sqrt{19},\\[4mm] \alpha=&\,\tan^{-1}\frac{\sqrt3}{4}\\[4mm] =&\,23.413224\ldots^\circ. \end{align*}

Therefore

R=19,α≈23.41∘.R=\boxed{\sqrt{19}},\quad\alpha\approx\boxed{23.41^\circ}.

(b)

解法一

思路

展开

把(a)中的 xx 换成 2θ2\theta。先求移相后的两个余弦角,再加回相位角,最后除以 22。

答题过程

展开

Using part (a), with the unrounded value of α\alpha,

19cos⁡(2θ−α)=2.5.\sqrt{19}\cos(2\theta-\alpha)=2.5.

Let

β=cos⁡−12.519=55.002595…∘.\beta=\cos^{-1}\frac{2.5}{\sqrt{19}} =55.002595\ldots^\circ.

Since 0∘<2θ<360∘0^\circ<2\theta<360^\circ, the two possible values are

2θ= α+βor2θ= α+360∘−β.\begin{align*} 2\theta=&\,\alpha+\beta\\[4mm] \text{or}\quad2\theta=&\,\alpha+360^\circ-\beta. \end{align*}

Therefore

θ=39.2∘or164.2∘.\boxed{\theta=39.2^\circ\quad\text{or}\quad164.2^\circ}.