Skip to content
CalcGospel 國際數學圖譜
返回

CIE 9231 2023 November Paper 31 Q4

A Level / CIE / FM

CIE 9231 2023 Nov Paper 31 Paper · Question 4

题目

Problem

A light elastic string has natural length 8a8a and modulus of elasticity 5mg5mg. A particle PP of mass mm is attached to the midpoint of the string. The ends of the string are attached to points AA and BB which are a distance 12a12a apart on a smooth horizontal table. The particle PP is held on the table so that AP=BP=LAP=BP=L (see diagram). The particle PP is released from rest. When PP is at the midpoint of ABAB it has speed 80ag\sqrt{80ag}.

(a) Find LL in terms of aa.

(5)

(b) Find the initial acceleration of PP in terms of gg.

(3)
题目中文翻译

一根轻弹性绳的自然长度为 8a8a,弹性模量为 5mg5mg。一个质量为 mm 的质点 PP 连接在绳的中点。绳的两端分别连接在光滑水平桌面上相距 12a12a 的点 AA 和 BB 处。将质点 PP 保持在桌面上,使得 AP=BP=LAP=BP=L(见图)。质点 PP 从静止释放。当 PP 位于 ABAB 的中点时,其速率为 80ag\sqrt{80ag}。

(a) 用 aa 表示 LL。

(5)

(b) 用 gg 表示 PP 的初始加速度。

(3)
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

桌面光滑且水平,动能的增加完全来自绳的弹性势能减少。注意到达 ABAB 中点时绳仍有伸长。

答题过程

展开

At release the whole string has extension 2L−8a2L-8a. At the midpoint of ABAB, the total length is 12a12a, giving extension 4a4a. Since AP=BPAP=BP throughout this motion, both halves have equal extension and the total elastic energy is given by the whole-string expression. Conservation of energy gives

12m(80ag)=5mg16a[(2L−8a)2−(4a)2].\frac12m(80ag) =\frac{5mg}{16a}\bigg[(2L-8a)^2-(4a)^2\bigg].

Cancelling mgmg and multiplying by 16a/516a/5 gives

128a2= (2L−8a)2−16a2,(2L−8a)2= 144a2.\begin{align*} 128a^2=&\,(2L-8a)^2-16a^2,\\[4mm] (2L-8a)^2=&\,144a^2. \end{align*}

Since L≥6aL\ge6a, we have 2L−8a>02L-8a>0, so 2L−8a=12a2L-8a=12a and L=10aL=10a.

(b)

解法一

思路

展开

释放时两段张力相同,垂直于对称轴的分量互相抵消。由 6a6a、10a10a 构成的直角三角形求沿对称轴的分量。

答题过程

展开

The initial tension is 5mg(2L−8a)/(8a)=15mg/25mg(2L-8a)/(8a)=15mg/2. If MM is the midpoint of ABAB, then

PM=(10a)2−(6a)2=8a.PM=\sqrt{(10a)^2-(6a)^2}=8a.

Each tension has a component T(8a/10a)=4T/5T(8a/10a)=4T/5 towards MM. If the initial acceleration has magnitude A0A_0, Newton’s second law gives

mA0= 2T⋅45= 2⋅15mg2⋅45=12mg.\begin{align*} mA_0=&\,2T\cdot\frac45\\[4mm] =&\,2\cdot\frac{15mg}{2}\cdot\frac45=12mg. \end{align*}

Thus A0=12gA_0=12g towards MM.