Consider the total time of flight \( T \) as:
\[ T = \sqrt{\frac{2h}{g}} + \sqrt{\frac{2(H - h)}{g}} \]To find the value of \( \frac{H}{h} \) that maximizes the time, we differentiate \( T \) with respect to \( h \) and set it to zero:
\[ \frac{dT}{dh} = 0 \implies \frac{\sqrt{2}}{g} \left( -\frac{1}{2\sqrt{H - h}} + \frac{1}{2\sqrt{h}} \right) = 0 \]Solving for \( h \):
\[ \sqrt{H - h} = \sqrt{h} \implies h = \frac{H}{2} \implies \frac{H}{h} = 2 \]Acceleration-time (\(a-t\)) graph of a body is shown. The corresponding velocity-time (\(v-t\)) graph is 
A bead P sliding on a frictionless semi-circular string... bead Q ejected... relation between $t_P$ and $t_Q$ is 