1990 Paper 1 Q11

Year: 1990
Paper: 1
Question Number: 11

Course: LFM Pure and Mechanics
Section: Projectiles

Difficulty: 1500.0 Banger: 1484.0

Problem

A shell of mass \(m\) is fired at elevation \(\pi/3\) and speed \(v\). Superman, of mass \(2m\), catches the shell at the top of its flight, by gliding up behind it in the same horizontal direction with speed \(3v\). As soon as Superman catches the shell, he instantaneously clasps it in his cloak, and immediately pushes it vertically downwards, without further changing its horizontal component of velocity, but giving it a downward vertical component of velocity of magnitude \(3v/2\). Calculate the total time of flight of the shell in terms of \(v\) and \(g\). Calculate also, to the nearest degree, the angle Superman's flight trajectory initially makes with the horizontal after releasing the shell, as he soars upwards like a bird. {[}Superman and the shell may be regarded as particles.{]}

Solution

The particle has initial velocity \(\displaystyle \binom{v \cos \frac{\pi}{3}}{v \sin \frac{\pi}{3}}\) and acceleration \(\displaystyle \binom{0}{-g}\). It will have zero vertical speed (ie be at the top of its trajectory) when \(t = \frac{\sqrt{3}v}{2g}\). Since \(0 = v^2-u^2 + 2as\) the height achieved will be \(\frac{3v^2}{8g}\) At this point it will need to travel the same distance again, but this time the initial speed is \(\frac{3v}{2}\) so: \begin{align*} && \frac{3v^2}{8g} &= \frac{3v}{2} t + \frac12 g t^2 \\ \Rightarrow && 0 &= 4g^2t^2+12vgt - 3v^2 \\ \Rightarrow && t &= \l \frac{-3+2\sqrt{3}}{2} \r \frac{v}{g} \end{align*} Therefore the total time is: \begin{align*} \l \frac{\sqrt{3}}{2} - \frac32 + \sqrt{3} \r \frac{v}{g} &= \frac{3\sqrt{3}-3}{2}\frac{v}{g} \end{align*} \begin{align*} COM(\uparrow): && 0 &= 2m v_y - m \frac{3}{2}v \\ \Rightarrow &&v_y &= \frac34 v \\ COM(\rightarrow): && 3mV &= 2m (3v) +m \frac{v}{2} \\ \Rightarrow && V &= \frac{13}6\\ \end{align*} Therefore superman is now travelling at a vector of \(\displaystyle \binom{\frac{13}6}{\frac34}v\) ie an angle of \(\tan^{-1} \frac 9{26}\) to the horizontal, approximately \(19^\circ\)
Rating Information

Difficulty Rating: 1500.0

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Banger Rating: 1484.0

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Problem source
A shell of mass $m$ is fired at elevation $\pi/3$ and speed $v$. Superman, of mass $2m$, catches the shell at the top of its flight, by gliding up behind it in the same horizontal direction with speed $3v$. As soon as Superman catches the shell, he instantaneously clasps it in his cloak, and immediately pushes it vertically downwards, without further changing its horizontal component of velocity, but giving it a downward vertical component of velocity of magnitude $3v/2$. 
Calculate the total time of flight of the shell in terms of $v$ and $g$. Calculate also, to the nearest degree, the angle Superman's flight trajectory initially makes with the horizontal after releasing the shell, as he soars upwards like a bird. 
{[}Superman and the shell may be regarded as particles.{]}
Solution source
The particle has initial velocity $\displaystyle \binom{v \cos \frac{\pi}{3}}{v \sin \frac{\pi}{3}}$ and acceleration $\displaystyle \binom{0}{-g}$. It will have zero vertical speed (ie be at the top of its trajectory) when $t = \frac{\sqrt{3}v}{2g}$.

Since $0 = v^2-u^2 + 2as$ the height achieved will be $\frac{3v^2}{8g}$

At this point it will need to travel the same distance again, but this time the initial speed is $\frac{3v}{2}$ so:

\begin{align*}
&& \frac{3v^2}{8g} &= \frac{3v}{2} t + \frac12 g t^2 \\
\Rightarrow && 0 &= 4g^2t^2+12vgt - 3v^2 \\
\Rightarrow && t &= \l \frac{-3+2\sqrt{3}}{2} \r \frac{v}{g}
\end{align*}

Therefore the total time is:

\begin{align*}
\l \frac{\sqrt{3}}{2} - \frac32 + \sqrt{3} \r \frac{v}{g} &= \frac{3\sqrt{3}-3}{2}\frac{v}{g}
\end{align*}

\begin{align*}
COM(\uparrow): && 0 &= 2m v_y - m \frac{3}{2}v \\
\Rightarrow &&v_y &= \frac34 v \\
COM(\rightarrow): && 3mV &= 2m (3v) +m \frac{v}{2} \\
\Rightarrow && V &= \frac{13}6\\
\end{align*}

Therefore superman is now travelling at a vector of $\displaystyle \binom{\frac{13}6}{\frac34}v$ ie an angle of $\tan^{-1} \frac 9{26}$ to the horizontal, approximately $19^\circ$