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CIE 9231 2023 November Paper 32 Q6

A Level / CIE / FM

CIE 9231 2023 Nov Paper 32 Paper · Question 6

题目

Problem

A particle PP is projected with speed uu at an angle α\alpha above the horizontal from a point OO on a horizontal plane and moves freely under gravity. The horizontal and vertical displacements of PP from OO at a subsequent time tt are denoted by xx and yy respectively.

(a) Derive the equation of the trajectory of PP in the form

y=xtan⁡α−gx22u2sec⁡2α.y=x\tan\alpha-\frac{gx^2}{2u^2}\sec^2\alpha.
(3)

During its flight, PP must clear an obstacle of height h mh\text{ m} that is at a horizontal distance of 32 m32\text{ m} from the point of projection. When u=402 m s−1u=40\sqrt2\text{ m s}^{-1}, PP just clears the obstacle. When u=40 m s−1u=40\text{ m s}^{-1}, PP only achieves 80%80\% of the height required to clear the obstacle.

(b) Find the two possible values of hh.

(6)
题目中文翻译

一个质点 PP 从水平面上的点 OO 以速率 uu、与水平方向成仰角 α\alpha 抛出,此后仅在重力作用下自由运动。此后时刻 tt,PP 相对于 OO 的水平位移和竖直位移分别记为 xx 和 yy。

(a) 推导 PP 的轨迹方程,并写成以下形式:

y=xtan⁡α−gx22u2sec⁡2α.y=x\tan\alpha-\frac{gx^2}{2u^2}\sec^2\alpha.
(3)

在飞行过程中,PP 必须越过一个高度为 h mh\text{ m}、与抛出点的水平距离为 32 m32\text{ m} 的障碍物。当 u=402 m s−1u=40\sqrt2\text{ m s}^{-1} 时,PP 恰好越过障碍物。当 u=40 m s−1u=40\text{ m s}^{-1} 时,PP 仅达到越过障碍物所需高度的 80%80\%。

(b) 求 hh 的两个可能值。

(6)
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

分别写水平和竖直位移。水平运动匀速,可用水平式消去时间。

答题过程

展开

The horizontal and vertical displacement equations are

x= utcos⁡α,y= utsin⁡α−12gt2.\begin{align*} x=&\,ut\cos\alpha,\\[4mm] y=&\,ut\sin\alpha-\frac12gt^2. \end{align*}

The first equation gives t=x/(ucos⁡α)t=x/(u\cos\alpha). Substituting into the second gives

y= usin⁡αxucos⁡α−g2(xucos⁡α)2= xtan⁡α−gx22u2sec⁡2α,\begin{align*} y=&\,u\sin\alpha\frac{x}{u\cos\alpha} -\frac g2\bigg(\frac{x}{u\cos\alpha}\bigg)^2\\[4mm] =&\,x\tan\alpha-\frac{gx^2}{2u^2}\sec^2\alpha, \end{align*}

as required.

(b)

解法一

思路

展开

在相同横坐标处写出两种初速对应的高度。用较小初速的高度等于 0.8h0.8h 消去 hh,再分别代入求障碍物高度。

答题过程

展开

Let z=tan⁡αz=\tan\alpha and use sec⁡2α=1+z2\sec^2\alpha=1+z^2. At x=32x=32 with g=10g=10, the two trajectories give

h= 32z−85(1+z2),45h= 32z−165(1+z2).\begin{align*} h=&\,32z-\frac85(1+z^2),\\[4mm] \frac45h=&\,32z-\frac{16}{5}(1+z^2). \end{align*}

Multiplying the first equation by 4/54/5 and equating the expressions for 4h/54h/5 gives

1285z−3225(1+z2)= 32z−165(1+z2),325z= 4825(1+z2),10z= 3(1+z2),3z2−10z+3= 0,(3z−1)(z−3)= 0.\begin{align*} \frac{128}{5}z-\frac{32}{25}(1+z^2) =&\,32z-\frac{16}{5}(1+z^2),\\[4mm] \frac{32}{5}z=&\,\frac{48}{25}(1+z^2),\\[4mm] 10z=&\,3(1+z^2),\\[4mm] 3z^2-10z+3=&\,0,\\[4mm] (3z-1)(z-3)=&\,0. \end{align*}

Thus z=1/3z=1/3 or z=3z=3. Substituting into the first height equation gives

z=13:h= 323−85109=809 m,z=3:h= 96−85×10=80 m.\begin{align*} z=\frac13:\quad h=&\,\frac{32}{3}-\frac85\frac{10}{9} =\frac{80}{9}\,\mathrm{m},\\[4mm] z=3:\quad h=&\,96-\frac85\times10=80\,\mathrm{m}. \end{align*}