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M3 2020 Oct Q7

A Level / Edexcel / M3

IAL 2020 Oct Paper · Question 7

题目

Problem

7.

A particle of mass mm is attached to one end of a light inextensible string of length 8a8a. The other end of the string is fixed to the point OO on the smooth horizontal surface of a desk. The point EE is on the edge of the desk, where OE=5aOE=5a and OEOE is perpendicular to the edge of the desk. The particle is held at the point AA, vertically above OO, with the string taut.

The particle is projected horizontally from AA with speed 8ag\sqrt{8ag} in the direction OEOE, as shown in Figure 5.

When the particle is above the level of OEOE the particle is moving in a vertical circle with radius 8a8a.

Given that, when the string makes an angle θ\theta with the upward vertical through OO, the tension in the string is TT,

(a) show that T=3mg(1−cos⁡θ)T=3mg(1-\cos\theta)

(7)

At the instant when the string is horizontal, the particle passes through the point BB.

(b) Find the instantaneous change in the tension in the string as the particle passes through BB.

(3)

The particle hits the vertical side EFEF of the desk and rebounds. As a result of the impact, the particle loses one third of the kinetic energy it had immediately before the impact.

In the subsequent motion the string becomes slack when it makes an angle α\alpha with the upward vertical through OO.

(c) Show that cos⁡α=712\cos\alpha=\dfrac7{12}

(7)
题目中文翻译

一个质量为 mm 的质点连接于一根长为 8a8a 的不可伸长轻绳的一端,另一端固定于桌子光滑水平桌面上的 OO 点。EE 点位于桌边,OE=5aOE=5a,且 OEOE 垂直于桌边。将质点保持在 OO 正上方的 AA 点,绳绷紧。

如图 5 所示,将质点从 AA 沿 OEOE 方向以速率 8ag\sqrt{8ag} 水平发射。

质点位于 OEOE 所在水平面上方时,沿半径为 8a8a 的竖直圆周运动。

已知绳与过 OO 的竖直向上方向成 θ\theta 角时,绳中的张力为 TT,

(a) 证明 T=3mg(1−cos⁡θ)T=3mg(1-\cos\theta)。

(7)

绳水平的瞬间,质点经过 BB 点。

(b) 求质点经过 BB 时绳中张力的瞬时变化。

(3)

质点撞向桌子的竖直侧面 EFEF 后反弹。碰撞使质点损失碰撞前瞬间动能的三分之一。

在随后的运动中,绳与过 OO 的竖直向上方向成 α\alpha 角时开始松弛。

(c) 证明 cos⁡α=712\cos\alpha=\dfrac7{12}。

(7)

解答

(a)

解法一

思路

展开

先从 A 到一般位置用能量求速率,再沿指向 O 的径向写牛顿第二定律。角度从竖直向上量起,因此重力指向圆心的分量为 mg cosθ。

答题过程

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Take the level of OO as the zero of gravitational potential energy. At AA the height is 8a8a, and at angle θ\theta it is 8acos⁡θ8a\cos\theta. Conservation of mechanical energy gives

12m(8ag)+mg(8a)=12mv2+mg(8acos⁡θ).\frac12m(8ag)+mg(8a)=\frac12mv^2+mg(8a\cos\theta).

Hence

v2=24ag−16agcos⁡θ.v^2=24ag-16ag\cos\theta.

Resolving towards OO along the radius,

T+mgcos⁡θ=mv28a.T+mg\cos\theta=\frac{mv^2}{8a}.

Substituting the energy result,

T+mgcos⁡θ=3mg−2mgcos⁡θ,T+mg\cos\theta=3mg-2mg\cos\theta, T=3mg(1−cos⁡θ).\boxed{T=3mg(1-\cos\theta)}.

(b)

解法一

思路

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通过 B 时绳开始绕桌边 E 弯折,有效圆心改为 E,半径从 8a 变为 3a。瞬时速率连续,但所需向心力改变,所以张力跃增。

答题过程

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At BB, θ=π/2\theta=\pi/2, so the speed immediately before passing BB satisfies

vB2=24ag.v_B^2=24ag.

Immediately before BB, the radius is 8a8a. Since weight has no radial component there,

T−=m(24ag)8a=3mg.T_-=\frac{m(24ag)}{8a}=3mg.

As the string bends round the edge at EE, the free length becomes

EB=8a−OE=8a−5a=3a.EB=8a-OE=8a-5a=3a.

The speed is continuous at BB, but the radius immediately afterwards is 3a3a. Therefore

T+=m(24ag)3a=8mg.T_+=\frac{m(24ag)}{3a}=8mg.

Thus the instantaneous change is

T+−T−=5mg, an increase.\boxed{T_+-T_-=5mg\text{, an increase}}.

(c)

解法一

思路

展开

先算绕 E 下落到竖直桌边时的速率,再将动能乘 2/3 得反弹后的速率。返回桌面上方后,圆心又是 O、半径为 8a;松绳时张力为零。

答题过程

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Below the desk level the particle moves on a circle of radius 3a3a about EE. It strikes the wall vertically below EE, at height −3a-3a relative to OO. Let its speeds immediately before and after the impact be v1v_1 and v2v_2. The total fall from AA to the impact point is 11a11a, so conservation of energy before impact gives

12mv12=12m(8ag)+mg(11a),\frac12mv_1^2=\frac12m(8ag)+mg(11a), v12=30ag.v_1^2=30ag.

The collision removes one third of the kinetic energy, leaving two thirds. Hence

12mv22=23(12mv12),v22=20ag.\frac12mv_2^2=\frac23\left(\frac12mv_1^2\right),\qquad v_2^2=20ag.

After rebounding the particle rises, and above the desk level the string again describes a circle of radius 8a8a about OO. When the string makes angle α\alpha with the upward vertical, let the speed be vv. Energy from immediately after impact gives

12m(20ag)−mg(3a)=12mv2+mg(8acos⁡α).\frac12m(20ag)-mg(3a)=\frac12mv^2+mg(8a\cos\alpha).

Therefore

v2=14ag−16agcos⁡α.v^2=14ag-16ag\cos\alpha.

At the instant the string becomes slack, T=0T=0. The inward radial equation for the circle about OO is consequently

mgcos⁡α=mv28a.mg\cos\alpha=\frac{mv^2}{8a}.

Substituting,

mgcos⁡α=74mg−2mgcos⁡α,mg\cos\alpha=\frac74mg-2mg\cos\alpha, 3cos⁡α=74,cos⁡α=712.3\cos\alpha=\frac74,\qquad \boxed{\cos\alpha=\frac7{12}}.