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CIE 9709 2025 November Paper 41 Q7

A Level / CIE / M1

CIE 9709 2025 Nov Paper 41 Paper · Question 7

题目

Problem

A particle PP starts from a point OO and moves in a straight line. The velocity v m s−1v\,\mathrm{m\,s^{-1}} of PP, at time t st\,\mathrm{s} after leaving OO, is given by v=13(2t−3)(t−4)v=\frac13(2t-3)(t-4).

(a) Find the acceleration of PP when t=2t=2.

(2)

(b) Find the total distance travelled by PP in the first 33 seconds of its motion.

(5)

(c) Determine whether PP returns to OO.

(2)
题目中文翻译

质点 PP 从点 OO 出发,沿直线运动。离开 OO 后 t st\,\mathrm{s} 时,PP 的速度 v m s−1v\,\mathrm{m\,s^{-1}} 由 v=13(2t−3)(t−4)v=\frac13(2t-3)(t-4) 给出。

(a) 求 PP 在 t=2t=2 时的加速度。

(2)

(b) 求 PP 在运动的前 33 秒内运动的总路程。

(5)

(c) 判断 PP 是否返回 OO。

(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

展开

展开速度后求导,再代入2。

答题过程

展开 v= 13(2t2−11t+12),a= dvdt=13(4t−11).\begin{align*} v=&\,\frac13(2t^2-11t+12),\\[4mm] a=&\,\frac{\mathrm{d}v}{\mathrm{d}t}=\frac13(4t-11). \end{align*}

At t=2t=2,

a=13(8−11)=−1 m s−2.a=\frac13(8-11)=\boxed{-1\text{ m s}^{-2}}.

(b)

解法一

思路

展开

前3秒内只有1.5秒反向,把两个区间位移的大小相加。

答题过程

展开

The velocity is zero at t=1.5t=1.5 and t=4t=4. It is positive for 0≤t<1.50\leq t<1.5 and negative for 1.5<t≤31.5<t\leq3.

Since PP starts at OO, its displacement is

s(t)=∫0tv dt=29t3−116t2+4t.s(t)=\int_0^t v\,\mathrm{d}t =\frac29t^3-\frac{11}{6}t^2+4t.

In particular,

s(0)= 0,s(1.5)= 218=2.625,s(3)= 32=1.5.\begin{align*} s(0)=&\,0,\\[4mm] s(1.5)=&\,\frac{21}{8}=2.625,\\[4mm] s(3)=&\,\frac32=1.5. \end{align*}

Thus the total distance is

d= [s(1.5)−s(0)]+[s(1.5)−s(3)]= 2.625+(2.625−1.5)=3.75 m.\begin{align*} d=&\,\bigl[s(1.5)-s(0)\bigr]+\bigl[s(1.5)-s(3)\bigr]\\[4mm] =&\,2.625+(2.625-1.5)=\boxed{3.75\text{ m}}. \end{align*}

(c)

解法一

思路

展开

在4秒后速度恢复为正;返回O的最后机会在4秒之前,检查转向点位移仍为正。

答题过程

展开

After first moving away from OO, PP moves back towards it only during 1.5<t<41.5<t<4. At the end of that interval,

s(4)=29(4)3−116(4)2+4(4)=89 m>0.s(4)=\frac29(4)^3-\frac{11}{6}(4)^2+4(4)=\frac89\text{ m}>0.

For t>4t>4, v>0v>0 and the displacement increases again. Thus PP does not return to OO.

解法二

思路

展开

也可令位移为零,除去出发时刻t=0后用判别式排除其余实根。

答题过程

展开

For a return to OO at t>0t>0,

0=s(t)=t18(4t2−33t+72).0=s(t)=\frac{t}{18}(4t^2-33t+72).

Hence 4t2−33t+72=04t^2-33t+72=0 would be required. Its discriminant is

(−33)2−4(4)(72)=−63<0.(-33)^2-4(4)(72)=-63<0.

There is no real solution, so PP never returns to OO after departure.