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M2 2021 June Q8

A Level / Edexcel / M2

IAL 2021 June Paper · Question 8

题目

Problem

8.

Particles AA, BB and CC, of masses 2m2m, mm and 3m3m respectively, lie at rest in a straight line on a smooth horizontal plane with BB between AA and CC. Particle AA is projected towards particle BB with speed 2u2u and collides directly with BB.

The coefficient of restitution between each pair of particles is ee.

(a) (i) Show that the speed of BB immediately after the collision with AA is 43u(1+e)\frac43u(1+e)

(ii) Find the speed of AA immediately after the collision with BB.

(7)

At the instant when AA collides with BB, particle CC is projected with speed uu towards BB so that BB and CC collide directly.

(b) Show that there will be a second collision between AA and BB.

(6)
题目中文翻译

质点 AA、BB 和 CC 的质量分别为 2m2m、mm 和 3m3m,沿同一直线静止在光滑水平面上,BB 位于 AA 和 CC 之间。质点 AA 以速率 2u2u 向质点 BB 投射,并与 BB 发生正碰。

每对质点之间的恢复系数均为 ee。

(a) (i) 证明 BB 与 AA 碰撞后瞬间的速率为 43u(1+e)\frac43u(1+e)。

(ii) 求 AA 与 BB 碰撞后瞬间的速率。

(7)

当 AA 与 BB 碰撞的瞬间,质点 CC 以速率 uu 向 BB 投射,使 BB 和 CC 发生正碰。

(b) 证明 AA 和 BB 将发生第二次碰撞。

(6)

解答

(a)(i)

解法一

思路

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统一取从 AA 指向 CC 的方向为正。先写动量守恒和恢复系数方程,再联立消元;恢复系数使用分离速率除以接近速率。

答题过程

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Take the direction from AA towards CC as positive. Let the velocities of AA and BB immediately after their first collision be vv and ww respectively.

Conservation of momentum gives

2m(2u)=2mv+mw,4u=2v+w.2m(2u)=2mv+mw,\qquad4u=2v+w.

Newton’s law of restitution gives

w−v=e(2u−0)=2eu.w-v=e(2u-0)=2eu.

Thus v=w−2euv=w-2eu, and substitution gives

4u=2(w−2eu)+w.4u=2(w-2eu)+w.

Therefore

w=43u(1+e),\boxed{w=\frac43u(1+e)},

which is positive and is therefore the speed of BB.

(a)(ii)

解法一

思路

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把上一问的 BB 速度代回恢复系数方程。还要检查所得有符号速度为正,才可以直接把它写成速率。

答题过程

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Using v=w−2euv=w-2eu,

v=43u(1+e)−2eu=23u(2−e).v=\frac43u(1+e)-2eu=\frac23u(2-e).

Since 0≤e≤10\le e\le1, this is positive. Thus the speed of AA is

23u(2−e).\boxed{\frac23u(2-e)}.

(b)

解法一

思路

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CC 在第二次碰撞前向左运动,因此初速度为 −u-u。求出 BB 碰后有符号速度为负,再结合 AA 仍在其左方并向右运动,才能说明两者必定再次碰撞。

答题过程

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Before the collision between BB and CC, their velocities are

w=43u(1+e),−u.w=\frac43u(1+e),\qquad -u.

Let their velocities afterwards be xx and yy, respectively, using the same positive direction as before.

Conservation of momentum gives

w−3u=x+3y,w-3u=x+3y,

so

x+3y=u3(4e−5).x+3y=\frac{u}{3}(4e-5).

The restitution equation is

y−x=e(w+u)=eu3(7+4e).y-x=e(w+u)=\frac{eu}{3}(7+4e).

Subtracting three times the restitution equation from the momentum equation,

4x=u3(4e−5)−eu(7+4e).4x=\frac{u}{3}(4e-5)-eu(7+4e).

Therefore

x=−u12(12e2+17e+5).x=-\frac{u}{12}(12e^2+17e+5).

Since u>0u>0 and 0≤e≤10\le e\le1, x<0x<0: BB moves back towards AA.

Meanwhile, AA is still moving to the right with positive velocity

v=23u(2−e).v=\frac23u(2-e).

At the collision between BB and CC, AA is to the left of BB. Afterwards they move towards each other, with closing speed v−x>0v-x>0. Hence there will be a second collision between AA and BB.