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CIE 9231 2024 November Paper 32 Q3

A Level / CIE / FM

CIE 9231 2024 Nov Paper 32 Paper · Question 3

题目

Problem

The diagram shows two identical smooth uniform spheres AA and BB of equal radii and each of mass mm. The two spheres are moving on a smooth horizontal surface when they collide with speeds 2u2u and 3u3u respectively. Immediately before the collision, AA’s direction of motion makes an angle θ\theta with the line of centres and BB’s direction of motion is perpendicular to that of AA. After the collision, BB moves perpendicular to the line of centres. The coefficient of restitution between the spheres is 13\frac13.

(a) Find the value of tan⁡θ\tan\theta.

(3)

(b) Find the total loss of kinetic energy as a result of the collision.

(2)

(c) Find, in degrees, the angle through which the direction of motion of AA is deflected as a result of the collision.

(2)
题目中文翻译

图中所示为两个相同的光滑均匀球 AA 和 BB,它们半径相等,质量均为 mm。两球在光滑水平面上运动,并分别以速率 2u2u 和 3u3u 发生碰撞。碰撞前的瞬间,AA 的运动方向与两球连心线成角 θ\theta,BB 的运动方向垂直于 AA 的运动方向。碰撞后,BB 沿垂直于连心线的方向运动。两球之间的恢复系数为 13\frac13。

(a) 求 tan⁡θ\tan\theta 的值。

(3)

(b) 求此次碰撞造成的总动能损失。

(2)

(c) 求此次碰撞使 AA 的运动方向偏转的角度,以度为单位。

(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

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取 AA 指向 BB 为正。由两球碰前速度互相垂直,从图上得到两球沿球心连线的分量。BB 碰后该分量为零。

答题过程

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Let vv be the signed component of the final velocity of AA along the line from AA to BB. Initially the components of AA and BB on this line are 2ucos⁡θ2u\cos\theta and −3usin⁡θ-3u\sin\theta. After collision the component of BB is zero. Conservation of momentum and restitution give

mv+m(0)= m(2ucos⁡θ)−m(3usin⁡θ),v= 2ucos⁡θ−3usin⁡θ,−v= 13(2ucos⁡θ+3usin⁡θ).\begin{align*} mv+m(0)=&\,m(2u\cos\theta)-m(3u\sin\theta),\\[4mm] v=&\,2u\cos\theta-3u\sin\theta,\\[4mm] -v=&\,\frac13(2u\cos\theta+3u\sin\theta). \end{align*}

Eliminating vv yields 8cos⁡θ=6sin⁡θ8\cos\theta=6\sin\theta, so tan⁡θ=4/3\tan\theta=4/3.

(b)

解法一

思路

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光滑球的碰撞只改变沿球心连线的分量。只比较这些分量对应的碰前、碰后动能。

答题过程

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Since cos⁡θ=3/5\cos\theta=3/5 and sin⁡θ=4/5\sin\theta=4/5, the initial parallel components are 6u/56u/5 and −12u/5-12u/5. The final ones are −6u/5-6u/5 and zero. The perpendicular components are unchanged. Thus the total loss is

Loss= 12m[(6u5)2+(12u5)2 −(6u5)2]= 7225mu2.\begin{align*} \text{Loss}=&\,\frac12m\bigg[\bigg(\frac{6u}{5}\bigg)^2+\bigg(\frac{12u}{5}\bigg)^2\\[4mm] &\,\hspace{2pt}-\bigg(\frac{6u}{5}\bigg)^2\bigg]\\[4mm] =&\,\frac{72}{25}mu^2. \end{align*}

解法二

思路

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也可分别计算碰撞前后的总动能。碰后用平行和垂直分量的平方和求各球速率的平方。

答题过程

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The initial total kinetic energy is 12m((2u)2+(3u)2)=13mu2/2\frac12m((2u)^2+(3u)^2)=13mu^2/2. After collision the perpendicular components have magnitudes 2usin⁡θ=8u/52u\sin\theta=8u/5 for AA and 3ucos⁡θ=9u/53u\cos\theta=9u/5 for BB. The parallel component magnitudes are 6u/56u/5 and zero. Therefore the final total kinetic energy is

Kf= 12m[(6u5)2+(8u5)2 +(9u5)2]= 18150mu2.\begin{align*} K_f=&\,\frac12m\bigg[\bigg(\frac{6u}{5}\bigg)^2+\bigg(\frac{8u}{5}\bigg)^2\\[4mm] &\,\hspace{2pt}+\bigg(\frac{9u}{5}\bigg)^2\bigg]\\[4mm] =&\,\frac{181}{50}mu^2. \end{align*}

Subtracting gives a loss of (132−18150)mu2=7225mu2\big(\frac{13}{2}-\frac{181}{50}\big)mu^2=\frac{72}{25}mu^2.

(c)

解法一

思路

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对 AA,垂直分量不变,而沿球心连线的分量大小不变、方向反转。根据这两个向量的位置求转角。

答题过程

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The initial and final velocities of AA have parallel components 6u/56u/5 and −6u/5-6u/5 and the same perpendicular component. Each makes the acute angle θ\theta with the corresponding horizontal direction along the line of centres. The deflection is therefore

180∘−2θ= 180∘−2arctan⁡(4/3)= 73.7∘.\begin{align*} 180^\circ-2\theta=&\,180^\circ-2\arctan(4/3)\\[4mm] =&\,73.7^\circ. \end{align*}