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CIE 9709 2024 November Paper 43 Q7

A Level / CIE / M1

CIE 9709 2024 Nov Paper 43 Paper · Question 7

题目

Problem

Two particles, AA and BB, of masses 3 kg3\,\mathrm{kg} and 5 kg5\,\mathrm{kg} respectively, are connected by a light inextensible string that passes over a fixed smooth pulley. The particles are held with the string taut and its straight parts vertical. Particle AA is 1 m1\,\mathrm{m} above a horizontal plane, and particle BB is 2 m2\,\mathrm{m} above the plane (see diagram).

The particles are released from rest. In the subsequent motion, AA does not reach the pulley, and after BB reaches the plane it remains in contact with the plane.

(a) Find the tension in the string and the time taken for BB to reach the plane.

(6)

(b) Find the time for which AA is at least 3.25 m3.25\,\mathrm{m} above the plane.

(4)

题目中文翻译

两个质点 AA 和 BB 的质量分别为 3 kg3\,\mathrm{kg} 和 5 kg5\,\mathrm{kg},由一根绕过固定光滑滑轮的轻且不可伸长的绳连接。两质点被保持在绳绷紧且绳的直线部分竖直的位置。质点 AA 位于一个水平面上方 1 m1\,\mathrm{m} 处,质点 BB 位于该平面上方 2 m2\,\mathrm{m} 处(见图)。

两质点从静止释放。在随后的运动中,AA 不会到达滑轮,且 BB 到达平面后保持与平面接触。

(a) 求绳中的张力和 BB 到达平面所需的时间。

(6)

(b) 求 AA 位于该平面上方至少 3.25 m3.25\,\mathrm{m} 处的持续时间。

(4)

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

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重者B下落、A上升,分别列牛顿第二定律求张力与加速度,再用B下降2米求时间。

答题过程

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Let aa be the common acceleration magnitude and TT the tension. Newton’s second law gives

T−30=3a,50−T=5a.T-30=3a,\qquad50-T=5a.

Adding gives 20=8a20=8a, so a=2.5 m s−2a=2.5\,\mathrm{m\,s^{-2}}. Thus

T=30+3(2.5)=37.5 N.\boxed{T=30+3(2.5)=37.5\,\mathrm{N}}.

If tt is the time for BB to fall 2 m2\,\mathrm{m} from rest,

2=12(2.5)t2,t=1.6 s≈1.26 s.2=\frac12(2.5)t^2, \qquad \boxed{t=\sqrt{1.6}\,\mathrm{s}\approx1.26\,\mathrm{s}}.

解法二

思路

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也可先由两粒子系统的机械能守恒求落地速度,再用匀加速平均速率求用时。张力仍由牛顿第二定律求。

答题过程

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When BB falls 2 m2\,\mathrm{m}, AA rises 2 m2\,\mathrm{m}. The net loss of potential energy equals the total gain in kinetic energy:

5(10)(2)−3(10)(2)=12(3+5)v2.5(10)(2)-3(10)(2)=\frac12(3+5)v^2.

Thus v2=10v^2=10, so v=10 m s−1v=\sqrt{10}\,\mathrm{m\,s^{-1}}. The acceleration is constant because all forces are constant. Using the average speed,

2=0+102t,t=410 s≈1.26 s.2=\frac{0+\sqrt{10}}{2}t, \qquad \boxed{t=\frac4{\sqrt{10}}\,\mathrm{s}\approx1.26\,\mathrm{s}}.

Also

a=v22(2)=2.5,T=30+3a=37.5 N.a=\frac{v^2}{2(2)}=2.5, \qquad \boxed{T=30+3a=37.5\,\mathrm{N}}.

(b)

解法一

思路

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B落地时A高3米,此后绳松弛,A自由上抛。求高度3.25米的上行、下行两个时刻,相减得到持续时间。

答题过程

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When BB reaches the plane, AA is at height 3 m3\,\mathrm{m} and its upward speed satisfies

u2=2(2.5)(2)=10.u^2=2(2.5)(2)=10.

Afterwards the string is slack. Let τ\tau be the time after BB reaches the plane. The height of AA is

h=3+10 τ−5τ2.h=3+\sqrt{10}\,\tau-5\tau^2.

Setting h=3.25h=3.25 gives

5τ2−10 τ+14=0,5\tau^2-\sqrt{10}\,\tau+\frac14=0,

with roots

τ1= 10−510,τ2= 10+510.\begin{align*} \tau_1=&\,\frac{\sqrt{10}-\sqrt5}{10},\\[4mm] \tau_2=&\,\frac{\sqrt{10}+\sqrt5}{10}. \end{align*}

Before this free flight AA is below 3.25 m3.25\,\mathrm{m}. During free flight the downward-opening height parabola is at least 3.253.25 between these roots. The required duration is

τ2−τ1=55 s≈0.447 s.\tau_2-\tau_1=\boxed{\frac{\sqrt5}{5}\,\mathrm{s}} \approx0.447\,\mathrm{s}.

解法二

思路

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利用最高点两侧运动对称。先求最高高度3.5米,再求从3.25米到最高点的时间,乘二。

答题过程

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When the string becomes slack, AA is at height 3 m3\,\mathrm{m} and has upward speed 10 m s−1\sqrt{10}\,\mathrm{m\,s^{-1}}. Its further rise to the highest point is

0=10−20H,H=0.5 m.0=10-20H,\qquad H=0.5\,\mathrm{m}.

Thus the greatest height is 3.5 m3.5\,\mathrm{m}. The level 3.25 m3.25\,\mathrm{m} is 0.25 m0.25\,\mathrm{m} below this. Starting from rest at the highest point, the time to fall that distance satisfies

0.25=12(10)τ2,τ=510.0.25=\frac12(10)\tau^2, \qquad \tau=\frac{\sqrt5}{10}.

The ascent and descent times over this height interval are equal. Hence the duration is

2τ=55 s≈0.447 s.2\tau=\boxed{\frac{\sqrt5}{5}\,\mathrm{s}} \approx0.447\,\mathrm{s}.

解法三

思路

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还可以先求3.25米处的速度大小,再求从该速度减到零的时间,利用最高点两侧对称乘二。

答题过程

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The speed when the string becomes slack at height 3 m3\,\mathrm{m} satisfies u2=2(2.5)(2)=10u^2=2(2.5)(2)=10. At height 3.25 m3.25\,\mathrm{m}, the upward speed ww satisfies

w2=10−2(10)(0.25)=5.w^2=10-2(10)(0.25)=5.

The time from this level to the highest point is

0=5−10τ,τ=510.0=\sqrt5-10\tau, \qquad \tau=\frac{\sqrt5}{10}.

By symmetry about the highest point, the total time above or at this level is

2τ=55 s≈0.447 s.2\tau=\boxed{\frac{\sqrt5}{5}\,\mathrm{s}} \approx0.447\,\mathrm{s}.

解法四

思路

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用能量计算两个关键高度的速率,再通过重力作用下的匀减速求时间,与前面的动力学方法相互校验。

答题过程

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Before BB reaches the plane, conservation of mechanical energy for the system gives

5(10)(2)−3(10)(2)=12(3+5)u2.5(10)(2)-3(10)(2)=\frac12(3+5)u^2. u2=10.u^2=10.

The string then becomes slack at height 3 m3\,\mathrm{m}. As AA rises another 0.25 m0.25\,\mathrm{m}, its loss in kinetic energy equals its gain in potential energy:

12(3)(10−w2)=3(10)(0.25).\frac12(3)(10-w^2)=3(10)(0.25).

Thus w2=5w^2=5. The time from the upward crossing of 3.25 m3.25\,\mathrm{m} to the highest point is 5/10\sqrt5/10. The downward part is symmetric, so the duration is

2(510)=55 s≈0.447 s.\boxed{2\bigg(\frac{\sqrt5}{10}\bigg) =\frac{\sqrt5}{5}\,\mathrm{s}\approx0.447\,\mathrm{s}}.