202010130604 Example 1, Chapter 1.1, Methods in Physics II (2015-2016 Lectures)

Find the trajectory of a cannon ball fired by a cannoneer at 45^\circ above his eye level with an initial speed v.


Ans.

Imagine you are in his place, like the picture below:

Then, suppose you are opening fire at such positive \textrm{(+ve)\enspace }x-axis direction as that follows along the meridian. In addition, assume that the earth is to be lying flat beneath the cannon ball during its flight, that every pole (z-axis) upheld would be so much right-angled (/normal /perpendicular) to the ground as parallel (-transported) anywhere.

We neglect air friction.

1. Along the x-direction, the speed is kept v\cos 45^\circ.

2. Along the z-direction, the speed is initially v\sin 45^\circ. By the laws of gravity, the cannon ball will experience a net force m\mathbf{g} due to gravitational pull by the Earth. If upward direction is taken the positive sign, an equation of motion due to the Galilean transformation (i.e., v=u+at) will depict that v_z(t)=v\sin 45^\circ -gt.

3. One another equation s(t)=ut+\displaystyle{\frac{1}{2}}at^2 depicts how distance s (i.e., the magnitude of displacement \mathbf{s}) varies with time t during linear motion in constant acceleration a.

One might have already noticed I am setting the original question aside, as it were. Let’s pinpoint the answer now.

The trajectory should be obtained in the form:

\mathbf{s}(t)=s_x(t)\,\hat{\mathbf{i}} + s_z(t)\,\hat{\mathbf{k}}.

where

\begin{aligned} s_x(t) & = u_x t+\frac{1}{2}a_xt^2 \\ & = (v\cos 45^\circ )\, t + \frac{1}{2}(0)(t^2) \\ & = (v\cos 45^\circ )\, t \\ \end{aligned}

and

\begin{aligned} s_z(t) & = u_zt + \frac{1}{2}a_zt^2 \\ & = (v\sin 45^\circ )\, t + \frac{1}{2}(-g)(t^2) \\ \end{aligned}

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