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CIE 9231 2026 June Paper 33 Q2

A Level / CIE / FM

CIE 9231 2026 June Paper 33 Paper · Question 2

题目

Problem

A particle PP of mass mm is moving in a straight horizontal line towards a fixed point AA on the line. The particle is subject to a resistive force that is inversely proportional to the square of the distance between PP and AA. Initially, the distance between PP and AA is dd and the speed of PP is uu. When the distance between PP and AA is 12d\frac12d, the particle has lost 34\frac34 of its kinetic energy.

Find, in terms of dd, the minimum distance of PP from AA.

(6)
题目中文翻译

质量为 mm 的质点 PP 沿一条水平直线朝该直线上的固定点 AA 运动。质点受到的阻力与 PP 和 AA 之间距离的平方成反比。初始时,PP 和 AA 之间的距离为 dd,PP 的速率为 uu。当 PP 和 AA 之间的距离为 12d\frac12d 时,质点已损失其动能的 34\frac34。

求 PP 到 AA 的最小距离,用 dd 表示。

(6)
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

解法一

思路

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以到 AA 的距离为坐标,把阻力方向和速度方向分清。对速度的微分方程积分,用已知的动能损失确定比例常数。

答题过程

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Let rr be the distance from AA, and let v=−dr/dtv=-\mathrm{d}r/\mathrm{d}t be the speed towards AA while PP is moving. Write the magnitude of the resistance as k/r2k/r^2, with k>0k>0. Taking the direction towards AA as positive in Newton’s second law gives

mdvdt= −kr2,mvdvdr= kr2.\begin{align*} m\frac{\mathrm{d}v}{\mathrm{d}t}=&\,-\frac{k}{r^2},\\[4mm] mv\frac{\mathrm{d}v}{\mathrm{d}r}=&\,\frac{k}{r^2}. \end{align*}

Using dr/dt=−v\mathrm{d}r/\mathrm{d}t=-v accounts for the sign in the second equation. Integrating from the initial state gives

∫uvmw dw= ∫drks2 ds,12m(v2−u2)= [−ks]dr= −k(1r−1d).\begin{align*} \int_u^v mw\,\mathrm{d}w=&\,\int_d^r\frac{k}{s^2}\,\mathrm{d}s,\\[4mm] \frac12m(v^2-u^2)=&\,\bigg[-\frac{k}{s}\bigg]_d^r\\[4mm] =&\,-k\bigg(\frac1r-\frac1d\bigg). \end{align*}

Hence

12mv2=12mu2−k(1r−1d).\frac12 mv^2=\frac12mu^2-k\bigg(\frac1r-\frac1d\bigg).

At r=d/2r=d/2, the loss is 34⋅12mu2\frac34\cdot\frac12mu^2, so

kd=38mu2,k=38mdu2.\frac{k}{d}=\frac38mu^2,\qquad k=\frac38mdu^2.

The kinetic energy decreases as rr decreases. It first reaches zero when

1r−1d=12mu238mdu2=43d.\frac1r-\frac1d=\frac{\frac12mu^2}{\frac38mdu^2}=\frac4{3d}.

Thus 1/r=1/d+4/(3d)=7/(3d)1/r=1/d+4/(3d)=7/(3d), so the minimum distance is 37d\boxed{\frac37d}.

解法二

思路

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也可以从起点沿运动方向量距离。此时若质点已走了 xx,它到 AA 的距离就是 d−xd-x。

答题过程

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Let xx be the distance travelled from the initial point. Newton’s second law gives

mvdvdx=−k(d−x)2.mv\frac{\mathrm{d}v}{\mathrm{d}x}=-\frac{k}{(d-x)^2}.

Since ∫(d−x)−2 dx=(d−x)−1\int(d-x)^{-2}\,\mathrm{d}x=(d-x)^{-1}, integrating gives 12mv2=C−kd−x\frac12mv^2=C-\frac{k}{d-x}. At x=0x=0 and x=d/2x=d/2, respectively,

12mu2= C−kd,18mu2= C−2kd.\begin{align*} \frac12mu^2=&\,C-\frac{k}{d},\\[4mm] \frac18mu^2=&\,C-\frac{2k}{d}. \end{align*}

Subtracting gives 3mu2/8=k/d3mu^2/8=k/d, so k=38mdu2k=\frac38mdu^2. Then C=mu2/2+k/d=78mu2C=mu^2/2+k/d=\frac78mu^2. At the first stop, v=0v=0, so

d−x=kC=37d.d-x=\frac{k}{C}=\frac37d.