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CIE 9709 2022 March Paper 42 Q7

A Level / CIE / M1

CIE 9709 2022 March Paper 42 Paper · Question 7

题目

Problem

A bead, AA, of mass 0.1 kg0.1\,\mathrm{kg} is threaded on a long straight rigid wire which is inclined at sin⁡−1(725)\sin^{-1}\big(\frac7{25}\big) to the horizontal. AA is released from rest and moves down the wire. The coefficient of friction between AA and the wire is μ\mu. When AA has travelled 0.45 m0.45\,\mathrm{m} down the wire, its speed is 0.6 m s−10.6\,\mathrm{m\,s^{-1}}.

(a) Show that μ=0.25\mu=0.25.

(6)

Another bead, BB, of mass 0.5 kg0.5\,\mathrm{kg} is also threaded on the wire. At the point where AA has travelled 0.45 m0.45\,\mathrm{m} down the wire, it hits BB which is instantaneously at rest on the wire. AA is brought to instantaneous rest in the collision. The coefficient of friction between BB and the wire is 0.2750.275.

(b) Find the time from when the collision occurs until AA collides with BB again.

(6)

题目中文翻译

一颗质量为 0.1 kg0.1\,\mathrm{kg} 的珠子 AA 穿在一根长直刚性金属丝上,金属丝与水平面的夹角为 sin⁡−1(725)\sin^{-1}\big(\frac7{25}\big)。AA 从静止释放并沿金属丝向下运动。AA 与金属丝之间的摩擦系数为 μ\mu。当 AA 沿金属丝向下移动 0.45 m0.45\,\mathrm{m} 时,其速率为 0.6 m s−10.6\,\mathrm{m\,s^{-1}}。

(a) 证明 μ=0.25\mu=0.25。

(6)

另一颗质量为 0.5 kg0.5\,\mathrm{kg} 的珠子 BB 也穿在该金属丝上。AA 沿金属丝向下移动 0.45 m0.45\,\mathrm{m} 时,撞到在金属丝上瞬时静止的 BB。碰撞使 AA 瞬时静止。BB 与金属丝之间的摩擦系数为 0.2750.275。

(b) 求从此次碰撞发生起,直到 AA 再次与 BB 碰撞为止的时间。

(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

(a)

解法一

思路

展开

先由位移和末速求恒加速度,再用沿线方向的牛顿第二定律求摩擦力及摩擦系数。

答题过程

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Let the inclination be θ\theta. Since sin⁡θ=7/25\sin\theta=7/25 and the wire slopes above the horizontal,

cos⁡θ=1−(7/25)2=2425.\cos\theta=\sqrt{1-(7/25)^2}=\frac{24}{25}.

The acceleration of AA is constant. Using v2=u2+2asv^2=u^2+2as,

0.62=0+2a(0.45),a=0.4 m s−2.0.6^2=0+2a(0.45), \qquad a=0.4\,\mathrm{m\,s^{-2}}.

The normal reaction is

R=0.1(10)2425=0.96 N.R=0.1(10)\frac{24}{25}=0.96\,\mathrm{N}.

Resolving down the wire,

0.1(10)725−μ(0.96)=0.1(0.4).0.1(10)\frac7{25}-\mu(0.96)=0.1(0.4).

Thus 0.96μ=0.28−0.04=0.240.96\mu=0.28-0.04=0.24, giving μ=0.25\boxed{\mu=0.25}, as required.

解法二

思路

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也可用功—能法,把重力势能减少量分为动能增加与克服摩擦的功。

答题过程

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As AA moves 0.45 m0.45\,\mathrm{m} down the wire, the loss of gravitational potential energy and gain in kinetic energy are

ΔEP= 0.1(10)(0.45)725=0.126 J,ΔEK= 12(0.1)(0.6)2=0.018 J.\begin{align*} \Delta E_P=&\,0.1(10)(0.45)\frac7{25}=0.126\,\mathrm{J}, \\[4mm] \Delta E_K=&\,\frac12(0.1)(0.6)^2=0.018\,\mathrm{J}. \end{align*}

The normal reaction is R=0.1(10)(24/25)=0.96 NR=0.1(10)(24/25)=0.96\,\mathrm{N}. Hence the work-energy equation gives

0.126=0.018+(0.96μ)(0.45).0.126=0.018+(0.96\mu)(0.45).

Thus 0.432μ=0.1080.432\mu=0.108, so μ=0.25\boxed{\mu=0.25}, as required.

(b)

解法一

思路

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碰撞时沿线方向动量守恒求B的初速。碰后A重新由静止下滑,两者加速度不同;从碰撞点写位移并令其相等。

答题过程

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Taking down the wire as positive, conservation of momentum at the first collision gives

0.1(0.6)+0.5(0)=0.1(0)+0.5uB.0.1(0.6)+0.5(0)=0.1(0)+0.5u_B.

Hence uB=0.12 m s−1u_B=0.12\,\mathrm{m\,s^{-1}}.

After the collision, AA again accelerates down the wire at

aA=10(725−0.252425)=0.4 m s−2.a_A=10\bigg(\frac7{25}-0.25\frac{24}{25}\bigg) =0.4\,\mathrm{m\,s^{-2}}.

For BB, Newton’s second law gives

 0.5(10)725 −0.275(0.5)(10)2425=0.5aB,\begin{align*} &\,0.5(10)\frac7{25}\\[4mm] &\,-0.275(0.5)(10)\frac{24}{25}=0.5a_B, \end{align*}

so aB=0.16 m s−2a_B=0.16\,\mathrm{m\,s^{-2}}.

Let tt be the time since the collision, with displacement measured down the wire from the collision point. Then

sA= 12(0.4)t2=0.2t2,sB= 0.12t+12(0.16)t2.\begin{align*} s_A=&\,\frac12(0.4)t^2=0.2t^2,\\[4mm] s_B=&\,0.12t+\frac12(0.16)t^2. \end{align*}

For the next collision,

0.2t2= 0.12t+0.08t2,0.12t(t−1)= 0.\begin{align*} 0.2t^2=&\,0.12t+0.08t^2, \\[4mm] 0.12t(t-1)=&\,0. \end{align*}

The root t=0t=0 is the first collision, so the required elapsed time is 1 s\boxed{1\,\mathrm{s}}.