Given:
\[t_1 = \frac{u + \sqrt{u^2 + 2gh}}{g}\]
\[t_2 = \frac{-u + \sqrt{u^2 + 2gh}}{g}\]
For the time \( t \) required if the body is dropped (i.e., initial velocity \( u = 0 \)):
\[t = \sqrt{\frac{2gh}{g^2}} = \frac{\sqrt{2gh}}{g}\]
Now, using the equations for \( t_1 \) and \( t_2 \):
\[t_1 t_2 = \frac{(u^2 + 2gh) - u^2}{g^2} = \frac{2gh}{g^2} = t^2\]
Thus:
\[t = \sqrt{t_1 t_2}\]
To solve this problem, we need to apply the equations of motion under gravity for a body projected from the top of a tower. Let's break down the situation:
Consider a body projected vertically from the top of a tower which has a height \( h \). The initial speed of the body when projected upwards or downwards is \( u \), and the acceleration due to gravity is \( g \). We analyze three situations:
We need to find the time \( t \) when the body is dropped from rest.
For the equations of motion under gravity with initial velocity \( u \) directed upwards or downwards:
1. \(h = ut_1 - \frac{1}{2}gt_1^2\) for upward projection.
2. \(h = ut_2 + \frac{1}{2}gt_2^2\) for downward projection.
3. For free fall, \(h = \frac{1}{2}gt^2\).
From equations 1 and 2, set them equal since both are for the same height:
\[ ut_1 - \frac{1}{2}gt_1^2 = ut_2 + \frac{1}{2}gt_2^2 \]
Rearranging gives:
\[ u(t_1 - t_2) = \frac{1}{2}g(t_1^2 + t_2^2) \]
Upon solving these equations step by step, and simplifying them using known physics identities, the relation found is:
\[ t = \sqrt{t_1 t_2} \]
This implies that the time taken for the body to reach the ground when dropped from rest is \(\sqrt{t_1 t_2}\).
Therefore, the correct answer is \(\sqrt{t_1 t_2}\).
A particle is projected at an angle of \( 30^\circ \) from horizontal at a speed of 60 m/s. The height traversed by the particle in the first second is \( h_0 \) and height traversed in the last second, before it reaches the maximum height, is \( h_1 \). The ratio \( \frac{h_0}{h_1} \) is __________. [Take \( g = 10 \, \text{m/s}^2 \)]
