Application-1 :
If a body projected horizontally with velocity u from the top of a tower strikes the ground at an angle of 45°
\(
\begin{gathered}
v_y = v_x ,gt = u \hfill \\
\therefore t = \frac{u}
{g} \hfill \\
\end{gathered}
\)
Application-2
A body is projected horizontally from the top of a tower. The line joining the point of projection and the striking point make an angle of 45° with the ground. Then
h = u.
\(
\begin{gathered}
\frac{1}
{2}gt^2 = ut \hfill \\
t = \frac{{2u}}
{g} \hfill \\
\end{gathered}
\)
Application-3:
A body is projected horizontally from the top of a tower. The line joining the point of projection and the striking point make an angle of 45° with the ground. Then, the displacement=
\(\sqrt 2h\) or \(\sqrt 2x\)
From the figure tan 45° =1=\(
\frac{h}
{X} \Rightarrow h = X
\)
.. displacement AC =\(
\sqrt {\left( {AB} \right)^2 + \left( {BC} \right)^2 }
\)
= \(
\sqrt {h^2 + H^2 } = \sqrt 2 h
\) (or)
\(
\sqrt 2 X
\) (since h = X)
Application-4:
Two towers having heights and are separated by a distance 'd'. A person throws a ball horizontally with a velocity u from the top of the 1st tower to the top
of the 2nd tower, then Time taken,t=\(
\sqrt {\frac{{2(h_1 - h_2 )}}
{g}}
\)
Distance between the towers
d = ut=u\(
\sqrt {\frac{{2(h_1 - h_2 )}}
{g}}
\)
Application-5
An aeroplane flies horizontally with a velocity 'u'. If a bomb is dropped by the pilot when the plane is at a height 'h' then
a) the path of such as body is a vertical straight line as seen by the pilot and
b) The path is a parabola as seen by an observer on the ground
c) the body will strike the ground at a certain horizontal distance. This distance is equal to the range given by
x = ut = u\(
\sqrt {\frac{{2u}}
{g}}
\)
Application-6
A ball rolls off the top of a staircase with a horizontal velocity u. If each step has height h and width b, then the ball will just hit the nth step if n equals to
sol: nb=ut and nh=\(
\frac{1}
{2}gt^2 \Rightarrow n = \frac{{2hu^2 }}
{{gb^2 }}
\)
Application-7
From the top of a tower, one stone is thrown towards east with velocity u, and another is thrown towards north with velocity u,. The distance be- tween then after striking the ground.
\(
d = t\sqrt {u_1^2 + u_2^2 }
\)
Application-8:
Two bodies are thrown horizontally with velocities u1,u2 in mutually opposite directions from the same height. (or)
A bomb at rest explodes into two fragments at a height 'h' and moves horizontally in opposite di- rections with velocities u1 and u2 respectively. Then
a) time after which velocity vectors are perpendicular is
\(
t = \frac{{\sqrt {u_1 u_2 } }}
{g}
\)
For velocity vectors to be perpendicular after a time t, their dot product must be zero.
\(
\therefore \overline {v_1 } .\overline {v_2 } = 0
\)
\(
\left( {u_1 \hat{i} - gt\hat{j}} \right).( - u_2 \hat{i} - gt\hat{j}) = 0
\)
\(
\therefore t = \frac{{\sqrt {u_1 u_2 } }}
{g}
\)
b) Separation between them when velocity vectors are perpendicular is
X=(\(
u_1 + u_2
\))\(
t = \frac{{(u_1 + u_2 )\sqrt {u_1 u_2 } }}
{g}
\)
c) Time after which their displacement vectors are perpendicular is \(
t = \frac{{2\sqrt {u_1 u_2 } }}
{g}
\)