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CIE 9231 2025 November Paper 34 Q1

A Level / CIE / FM

CIE 9231 2025 Nov Paper 34 Paper · Question 1

题目

Problem

A light inextensible string of length 12a12a is threaded through a fixed smooth ring RR. One end of the string is attached to a particle AA of mass mm. The other end of the string is attached to a particle BB of mass 0.5m0.5m. Particle AA hangs in equilibrium vertically below the ring. Particle BB moves with constant angular speed ω\omega in a horizontal circle with particle AA at its centre. The angle between ARAR and BRBR is θ\theta (see diagram).

Express ω\omega in terms of gg and aa.

(5)
题目中文翻译

一根长度为 12a12a 的轻质不可伸长细绳穿过一个固定的光滑环 RR。细绳的一端连接质量为 mm 的质点 AA,另一端连接质量为 0.5m0.5m 的质点 BB。质点 AA 在环的正下方竖直悬挂并处于平衡。质点 BB 以恒定角速度 ω\omega 在水平圆周上运动,且该圆以质点 AA 为圆心。ARAR 与 BRBR 的夹角为 θ\theta(见图)。

用 gg 和 aa 表示 ω\omega。

(5)
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.

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

需要重力加速度的数值时,取 g=10 m s−2g=10\,\mathrm{m\,s^{-2}}。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

解法一

思路

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先由 AA 的平衡求绳张力,再用 BB 的竖直平衡求角度。圆的半径来自绳段 BRBR 的水平投影,水平方向张力提供向心力。

答题过程

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The smooth ring makes the tension TT the same on both sides. Since AA is in equilibrium, T=mgT=mg. The vertical acceleration of BB is zero, so Tcos⁡θ=12mgT\cos\theta=\frac12mg, giving cos⁡θ=12\cos\theta=\frac12.

Since AA and BB are at the same height, AR=BRcos⁡θAR=BR\cos\theta. The total length AR+BR=12aAR+BR=12a gives (1+cos⁡θ)BR=12a(1+\cos\theta)BR=12a, hence 32BR=12a\frac32BR=12a and BR=8aBR=8a. The radius of the circle is BRsin⁡θBR\sin\theta. Resolving horizontally toward its centre,

Tsin⁡θ=12mω2(BRsin⁡θ).T\sin\theta=\frac12m\omega^2(BR\sin\theta).

Here θ=60∘\theta=60^\circ, so sin⁡θ≠0\sin\theta\ne0. Cancelling it gives mg=12mω2(8a)=4maω2mg=\frac12m\omega^2(8a)=4ma\omega^2, hence ω2=g/(4a)\omega^2=g/(4a). Hence

ω=12ga.\boxed{\omega=\frac12\sqrt{\frac ga}}.