Problem 343
Medium Applications of Derivatives

A body is thrown vertically upward with initial speed

A body is thrown vertically upward with initial speed $v_{0}$. Find (a) its height after $t$ seconds, (b) its velocity and acceleration, (c) the time to reach the greatest height and that height.

Explanation of Method

Integrating a constant acceleration twice.

Step 1: Set up

Measure $s$ upward from the launch point. The only acceleration is gravity, directed downward: $w = \frac{d^{2}s}{dt^{2}} = -g$.

Step 2: Integrate once

With $v(0) = v_{0}$: $v(t) = v_{0}-gt$.

Step 3: Integrate again

With $s(0) = 0$: $s(t) = v_{0}t-\frac{gt^{2}}{2}$.

Step 4: The highest point

The body rises while $v>0$ and falls when $v\lt 0$, so the summit is where $v = 0$: $v_{0}-gt^{*} = 0 \;\Longrightarrow\; t^{*} = \frac{v_{0}}{g}$.

\[ s_{\max} = v_{0}\cdot\frac{v_{0}}{g}-\frac{g}{2}\cdot\frac{v_{0}^{2}}{g^{2}} = \frac{v_{0}^{2}}{g}-\frac{v_{0}^{2}}{2g} = \frac{v_{0}^{2}}{2g}. \]

Step 5: Verification

\[\text{Energy: } \frac{v_{0}^{2}}{2} = g\,s_{\max} \;\Longrightarrow\; s_{\max} = \frac{v_{0}^{2}}{2g} \;\;\checkmark\]

\[s = 0 \text{ again at } t = \frac{2v_{0}}{g} = 2t^{*}, \text{ with } v = -v_{0}: \text{ rise and fall are mirror images} \;\;\checkmark\]

\[v_{0} = 20\ \text{m/s}:\ t^{*} \approx 2.04\ \text{s},\ s_{\max} \approx 20.4\ \text{m} \;\;\checkmark\]


Result

Final answer:

\[\boxed{\,s = v_{0}t-\frac{gt^{2}}{2}, \qquad v = v_{0}-gt, \qquad w = -g, \qquad t^{*} = \frac{v_{0}}{g}, \qquad s_{\max} = \frac{v_{0}^{2}}{2g}\,}\]

Remark

Remark. The acceleration is $-g$ throughout, including at the summit, where the velocity is zero but still changing — a point worth insisting on, since "momentarily at rest" is often confused with "momentarily unaccelerated". The symmetry of the trajectory, equal times up and down and equal speeds at equal heights, is a consequence of $w$ being constant.