The horizontal range is:
\[\frac{u^2 \sin 2\theta}{g},\]
and the maximum height is:
\[\frac{u^2 \sin^2 \theta}{2g}.\]
Equating:
\[\frac{u^2 \sin 2\theta}{g} = \frac{u^2 \sin^2 \theta}{2g}.\]
Simplifying:
\[2 \sin \theta \cos \theta = \frac{\sin^2 \theta}{2}.\]
Substitute \(\sin 2\theta = 2 \sin \theta \cos \theta\):
\[4 \sin \theta \cos \theta = \sin^2 \theta \implies 4 = \tan \theta.\]
Thus:
\[\theta = \tan^{-1}(4).\]
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 \( g = 10 \, \text{m/s}^2 \)]