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MIT 8.01 Physics I Classical Mechanics, Fall 1999
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show that time of ascent=time of descent
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a = -g --> v = -gt + v_0. Tada! We just derived the first basic kinematics equation with integration. Now, we see that the time of ascent is equal to (v_0-v)/g and the time of ascent is equal to (v-v_0)/(-g). Same thing. Boom!
the absolut height as a function of time at vertical throw is: \[s(t) = -\frac{ 1 }{ 2 }*g*(t - t _{maximum})^{2} + s _{maximum}\] now, there exist two time-differences between the time at any height and the time of maximum... \[t - t _{maximum} = \pm \sqrt{-2*\frac{ s(t) - s _{maximum} }{ g }}\] ...which's magnitudes are the same, as you can see!
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