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CIE 9231 2024 June Paper 31 Q2

A Level / CIE / FM

CIE 9231 2024 June Paper 31 Paper · Question 2

题目

Problem

The points AA and BB are at the same horizontal level a distance 4a4a apart. The ends of a light elastic string, of natural length 4a4a and modulus of elasticity λ\lambda, are attached to AA and BB. A particle PP of mass mm is attached to the midpoint of the string. The system is in equilibrium with PP at a distance 32a\frac32a below MM, the midpoint of ABAB.

(a) Find λ\lambda in terms of mm and gg.

(3)

The particle PP is pulled down vertically and released from rest at a distance 83a\frac83a below MM.

(b) Find, in terms of aa and gg, the speed of PP as it passes through MM in the subsequent motion.

(4)
题目中文翻译

点 AA 和 BB 位于同一水平高度,相距 4a4a。一根原长为 4a4a、弹性模量为 λ\lambda 的轻弹性绳的两端分别连接在 AA 和 BB。质量为 mm 的质点 PP 连接在绳的中点。系统处于平衡状态,此时 PP 位于 ABAB 的中点 MM 下方 32a\frac32a 处。

(a) 用 mm 和 gg 表示 λ\lambda。

(3)

将质点 PP 竖直向下拉动,在 MM 下方 83a\frac83a 处由静止释放。

(b) 用 aa 和 gg 表示 PP 在随后的运动中经过 MM 时的速率。

(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。

Where a numerical value for the acceleration due to gravity (gg) is needed, use 10 m s−210\,\mathrm{m\,s^{-2}}.

需要使用重力加速度 gg 的数值时,取 10 m s−210\,\mathrm{m\,s^{-2}}。

解答

(a)

解法一

思路

展开

平衡时两半段绳对称。由直角三角形求每段的长度与张力的竖直分量,再用胡克定律。

答题过程

展开

Each half of the string has natural length 2a2a. At equilibrium each half has length

(2a)2+(3a/2)2=52a,\sqrt{(2a)^2+(3a/2)^2}=\frac52a,

so its extension is a/2a/2 and its tension is λ(a/2)/(2a)=λ/4\lambda(a/2)/(2a)=\lambda/4. The vertical component of each tension is its magnitude multiplied by (3a/2)/(5a/2)=3/5(3a/2)/(5a/2)=3/5. Thus

2λ435= mg,3λ10= mg,λ= 103mg.\begin{align*} 2\frac{\lambda}{4}\frac35=&\,mg,\\[4mm] \frac{3\lambda}{10}=&\,mg,\\[4mm] \lambda=&\,\frac{10}{3}mg. \end{align*}

(b)

解法一

思路

展开

释放时先由几何求两段绳的伸长。在 MM,两段恰好恢复自然长度,用弹性势能的减少量减去重力势能的增加量。

答题过程

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At release each half has length

(2a)2+(8a/3)2=103a\sqrt{(2a)^2+(8a/3)^2}=\frac{10}{3}a

and extension 4a/34a/3. The total initial elastic potential energy is

E= 2λ2(2a)(43a)2= 89λa= 89⋅103mga=8027mga.\begin{align*} E=&\,2\frac{\lambda}{2(2a)}\bigg(\frac43a\bigg)^2\\[4mm] =&\,\frac89\lambda a\\[4mm] =&\,\frac89\cdot\frac{10}{3}mga=\frac{80}{27}mga. \end{align*}

At MM the string is at its natural length and the particle has risen by 8a/38a/3. Conservation of energy gives

12mv2= 8027mga−83mga= 80−7227mga=827mga,v2= 1627ag.\begin{align*} \frac12mv^2=&\,\frac{80}{27}mga-\frac83mga\\[4mm] =&\,\frac{80-72}{27}mga=\frac8{27}mga,\\[4mm] v^2=&\,\frac{16}{27}ag. \end{align*}

Therefore v=433agv=\frac{4}{3\sqrt3}\sqrt{ag}.