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M3 2026 June Q6

A Level / Edexcel / M3

IAL 2026 June Paper · Question 6

题目

Problem

6.

Figure 5 shows a smooth track PQRPQR which is part of a circle.

The track is fixed in a vertical plane.

The circle has centre OO and radius OP=1.5 mOP=1.5\,\mathrm{m}.

The highest point of the track is PP and POPO is horizontal.

The lowest point of the track QQ is on horizontal ground.

A small ball BB, of mass 0.2 kg0.2\,\mathrm{kg}, is released from rest at PP and moves on the track until it leaves the track at RR, where angle QOR=60∘\text{angle }QOR=60^\circ

The ball is modelled as a particle.

(a) Find the magnitude of the normal reaction between the ball and the track when the ball is at QQ.

(5)

After leaving the track, the ball moves freely under gravity and first lands on the ground at the point SS.

(b) Find the distance QSQS.

(8)
题目中文翻译

图 5 所示的光滑轨道 PQRPQR 是圆周的一部分。

轨道固定于竖直平面内。

圆心为 OO,半径为 OP=1.5 mOP=1.5\,\mathrm{m}。

轨道的最高点为 PP,且 POPO 水平。

轨道的最低点 QQ 位于水平地面上。

将质量为 0.2 kg0.2\,\mathrm{kg} 的小球 BB 从 PP 由静止释放,小球沿轨道运动至 RR 后离开轨道,其中 ∠QOR=60∘\angle QOR=60^\circ。

将小球视为质点。

(a) 求小球位于 QQ 时与轨道之间的法向反作用力大小。

(5)

离开轨道后,小球仅在重力作用下自由运动,首次落地于 SS 点。

(b) 求距离 QSQS。

(8)

解答

(a)

解法一

思路

展开

从 PP 到 QQ 的下降高度等于半径,先用能量求速率。最低点的向心方向向上,支持力需要同时克服重力并提供向心力。

答题过程

展开

The drop from PP to QQ is 1.5 m1.5\ \mathrm m. The normal reaction does no work, so

12mvQ2=mg(1.5)⟹vQ2=3g.\frac12mv_Q^2=mg(1.5) \quad\Longrightarrow\quad v_Q^2=3g.

At QQ, resolve upwards towards OO. If the normal reaction is NN,

N−mg=mvQ21.5=m(3g)1.5=2mg.N-mg=\frac{mv_Q^2}{1.5} =\frac{m(3g)}{1.5}=2mg.

Therefore

N=3mg=3(0.2)(9.8)=5.88 N.\boxed{N=3mg=3(0.2)(9.8)=5.88\ \mathrm N.}

(b)

解法一

思路

展开

离轨点 RR 的速度沿圆的切线,与水平线成 60∘60^\circ。先求离轨速率、离地高度及相对 QQ 的水平偏移,再做抛体运动;所求 QSQS 还要加上这段初始偏移。

答题过程

展开

The point RR is above the ground by

h=1.5−1.5cos⁡60∘=0.75 m,h=1.5-1.5\cos60^\circ=0.75\ \mathrm m,

and its horizontal distance to the right of QQ is

xR=1.5sin⁡60∘.x_R=1.5\sin60^\circ.

The drop from PP to RR is 1.5cos⁡60∘=0.75 m1.5\cos60^\circ=0.75\ \mathrm m. Energy conservation gives the departure speed uu:

12mu2=mg(0.75)⟹u=1.5g.\frac12mu^2=mg(0.75) \quad\Longrightarrow\quad u=\sqrt{1.5g}.

At RR the velocity is tangential, directed upwards and to the right at 60∘60^\circ to the horizontal. Thus

ux=1.5gcos⁡60∘,uy=1.5gsin⁡60∘.u_x=\sqrt{1.5g}\cos60^\circ,\qquad u_y=\sqrt{1.5g}\sin60^\circ.

Let tt be the flight time from RR to the first ground contact. With upward positive,

−0.75=uyt−12gt2.-0.75=u_y t-\frac12gt^2.

The positive root is

t=uy+uy2+2g(0.75)g=0.85636… s.t=\frac{u_y+\sqrt{u_y^2+2g(0.75)}}{g} =0.85636\ldots\ \mathrm s.

The other root is negative and is outside the flight interval. Horizontal motion gives

QS=xR+uxt=1.5sin⁡60∘+1.5gcos⁡60∘(0.85636…).QS=x_R+u_x t =1.5\sin60^\circ+\sqrt{1.5g}\cos60^\circ(0.85636\ldots).

Using g=9.8g=9.8 without rounding intermediate values,

QS=2.94 m(3 s.f.).\boxed{QS=2.94\ \mathrm m\quad\text{(3 s.f.)}.}