Skip to content
CalcGospel 國際數學圖譜
返回

CIE 9231 2024 November Paper 33 Q3

A Level / CIE / FM

CIE 9231 2024 Nov Paper 33 Paper · Question 3

题目

Problem

A particle PP of mass m kgm\text{ kg} is attached to one end of a light elastic string of natural length 2 m2\text{ m} and modulus of elasticity 2mg N2mg\text{ N}. The other end of the string is attached to a fixed point OO. The particle PP hangs in equilibrium vertically below OO. The particle PP is pulled down vertically a distance d md\text{ m} below its equilibrium position and released from rest.

(a) Given that the particle just reaches OO in the subsequent motion, find the value of dd.

(6)

(b) Hence find the speed of PP when it is 2 m2\text{ m} below OO.

(2)
题目中文翻译

质量为 m kgm\text{ kg} 的质点 PP 连接在一根原长为 2 m2\text{ m}、弹性模量为 2mg N2mg\text{ N} 的轻弹性绳的一端。绳的另一端连接在固定点 OO。质点 PP 悬挂在 OO 的正下方并处于平衡状态。将质点 PP 从平衡位置竖直向下拉动 d md\text{ m},然后由静止释放。

(a) 已知质点在随后的运动中恰好到达 OO,求 dd 的值。

(6)

(b) 由此求 PP 在 OO 下方 2 m2\text{ m} 处时的速率。

(2)
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

先用悬挂平衡求弹性绳的伸长。释放时有弹性势能,恰好到达 OO 时绳已松弛且速率为零。

答题过程

展开

If the equilibrium extension is ee, Hooke’s law gives (2mg/2)e=mg(2mg/2)e=mg, so e=1 me=1\,\mathrm{m}. At release the extension is 1+d1+d and the distance below OO is 3+d3+d, in metres. At OO both the elastic potential energy and kinetic energy are zero. Equating the initial elastic energy to the gain in gravitational potential energy gives

12mg(1+d)2=mg(3+d).\frac12mg(1+d)^2=mg(3+d).

Cancelling mgmg and multiplying by 22 gives 1+2d+d2=6+2d1+2d+d^2=6+2d, so d2=5d^2=5. The downward pull distance is positive, so d=5d=\sqrt5.

(b)

解法一

思路

展开

从释放位置到 OO 下方 2 m2\,\mathrm{m} 使用能量守恒。这个位置恰为绳长等于自然长度的位置。

答题过程

展开

At 2 m2\,\mathrm{m} below OO the string has no elastic potential energy. The particle has risen 1+d1+d metres from release. Hence, if its speed is VV,

12mV2= 12mg(1+d)2−mg(1+d)= 12mg((1+2d+d2)−2(1+d))= 12mg(d2−1).\begin{align*} \frac12mV^2=&\,\frac12mg(1+d)^2-mg(1+d)\\[4mm] =&\,\frac12mg\bigl((1+2d+d^2)-2(1+d)\bigr)\\[4mm] =&\,\frac12mg(d^2-1). \end{align*}

With d2=5d^2=5 and g=10g=10, we get V2=40V^2=40 and V=210 m s−1V=2\sqrt{10}\,\mathrm{m\,s^{-1}}.

解法二

思路

展开

也可从绳刚松弛的位置推到最高点。绳松弛后,质点只受重力,继续上升 2 m2\,\mathrm{m} 后停下。

答题过程

展开

From the point 2 m2\,\mathrm{m} below OO to OO, the tension is zero and the particle moves freely under gravity. Its kinetic energy at the start of this interval is the gain in gravitational potential energy:

12mV2=mg(2).\frac12mV^2=mg(2).

Thus V=210 m s−1V=2\sqrt{10}\,\mathrm{m\,s^{-1}}.