A cannonball shot from a cannon has an initial velocity of 600 m/sec. The muzzle of the cannon is inclined at an angle of 30°. Ignoring air resistance, determine the path of the cannonball.
A cannonball shot from a cannon has an initial velocity of 600 m/sec. The muzzle of the cannon is inclined at an angle of 30°. Ignoring air resistance, determine the path of the cannonball.
We place the x – and y-axes so that the mouth of the cannon is at the origin (see Figure 6). The velocity vector v can be resolved into its vertical and horizontal components:
v=vxi+vyjA unit vector in the direction of v is
u=(cos30∘)i+(sin30∘)j=23i+21jSo initially,
v=∣v∣u=600u=3003i+300jThe scalar ∣v∣ is called the speed of the cannonball. Thus initially, vx=3003 m/sec (the initial speed in the horizontal direction) and vy=300 m/sec (the initial speed in the vertical direction). Now the vertical acceleration (due to gravity) is
ay=−9.81 m/sec2 and vy=∫aydt=−9.81t+C.
Since, initially, vy(0)=300, we have C=300 and
vy=−9.81t+300Then
y(t)=∫vydt=−29.81t2+300t+C1.
and since y(0)=0 (we start at the origin), we find that
y(t)=−29.81t2+300tTo calculate the x-component of the position vector, we note that, ignoring air resistance, the velocity in the horizontal direction is constant;† that is,
vx=3003 m/secThen x(t)=∫vxdt=3003t+C2, and since x(0)=0, we obtain
x=3003tThus the position vector describing the location of the cannonball is
s(t)=x(t)i+y(t)j=3003ti+(300t−29.81t2)jTo obtain the Cartesian equation of this curve, we start with
x=3003tso that
t=3003xand
y=300(3003x)−29.81(3003)2x2=3x−540,0009.81x2.
This parabola is sketched in Figure 7 .