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Next: Worked example 3.4: Hail Up: Motion in 3 dimensions Previous: Worked example 3.2: Gallileo's

Worked example 3.3: Cannon shot

Question: A cannon placed on a 50m high cliff fires a cannonball over the edge of the cliff at $v=200 {\rm m}/{\rm s}$ making an angle of $\theta = 30^\circ$ to the horizontal. How long is the cannonball in the air? Neglect air resistance.
 
Answer: In order to answer this question we need only consider the cannonball's vertical motion. At $t=0$ (i.e., the time of firing) the cannonball's height off the ground is $z_0=50$m and its velocity component in the vertical direction is $v_0 = v \sin\theta = 200\times\sin 30^\circ = 100 {\rm m}/{\rm s}$. Moreover, the cannonball is accelerating vertically downwards at $g=9.91 {\rm m}/{\rm s}^2$. The equation of vertical motion of the cannonball is written

\begin{displaymath}
z = z_0 + v_0 t - \frac{1}{2} g t^2,
\end{displaymath}

where $z$ is the cannonball's height off the ground at time $t$. The time of flight of the cannonball corresponds to the time $t$ at which $z=0$. In other words, the time of flight is the solution of the quadratic equation

\begin{displaymath}
0 = z_0 + v_0 t - \frac{1}{2} g t^2.
\end{displaymath}

Hence,

\begin{displaymath}
t = \frac{v_0 +\sqrt{v_0^{ 2}+2 g z_0}}{g} = 20.88 {\rm s}.
\end{displaymath}

Here, we have neglected the unphysical negative root of our quadratic equation.


next up previous
Next: Worked example 3.4: Hail Up: Motion in 3 dimensions Previous: Worked example 3.2: Gallileo's
Richard Fitzpatrick 2006-02-02