Height, Range and Time of Flight: MDCAT Physics notes
Height, Range and Time of Flight notes for MDCAT: formulas for H, R and T, maximum range at 45°, complementary angles and H–R ratio problems.
The three results
For a projectile launched with speed $v_i$ at angle $\theta$ above the horizontal, landing back on the same level (air resistance neglected), three quantities are asked again and again.
Maximum height H
At the top $v_y = 0$. Using $v_y^2 = v_{iy}^2 - 2gH$:
$$H = \frac{v_i^2\sin^2\theta}{2g}$$
Time of flight T
Time to reach the top is $v_i\sin\theta/g$; the fall takes the same time, so
$$T = \frac{2v_i\sin\theta}{g}$$
Example: $v_i = 5\ \text{m s}^{-1}$ at $45^\circ$ gives $T = 2(5)(0.707)/9.8 \approx 0.72\ \text{s}$.
Horizontal range R
Range = horizontal velocity × time of flight $= v_i\cos\theta \times 2v_i\sin\theta/g$. Using $2\sin\theta\cos\theta = \sin2\theta$:
$$R = \frac{v_i^2\sin2\theta}{g}$$
The range is measured horizontally.
Maximum and minimum range
- $R$ is maximum when $\sin2\theta = 1$, i.e. $2\theta = 90^\circ$, so $\theta = 45^\circ$. Then $R_{max} = v_i^2/g$.
- $R$ is zero (minimum) when $\sin2\theta = 0$: at $\theta = 0^\circ$ or $\theta = 90^\circ$ (thrown straight up, it comes straight down).
- Half the maximum range: $\sin2\theta = \tfrac12$, so $2\theta = 30^\circ$ and $\theta = 15^\circ$ (or $75^\circ$).
- Since $R \propto v_i^2$, doubling the speed makes the range four times; $H$ also becomes four times, and $T$ doubles.
Complementary angles give equal range
Because $\sin2\theta = \sin(180^\circ - 2\theta) = \sin 2(90^\circ - \theta)$, angles $\theta$ and $(90^\circ - \theta)$ give the same range at the same speed. Pairs such as $15^\circ$ & $75^\circ$, $30^\circ$ & $60^\circ$, $40^\circ$ & $50^\circ$ and $(45^\circ+\alpha)$ & $(45^\circ-\alpha)$ have equal ranges (ratio 1). The larger angle goes higher and stays in the air longer, but lands at the same point.
For a fixed speed, increasing the angle beyond $45^\circ$ increases the height but decreases the range.
Ratio of height to range
Dividing $H$ by $R$:
$$\frac{H}{R} = \frac{\tan\theta}{4}$$
| Condition | $\tan\theta$ | $\theta$ |
|---|---|---|
| $H = R$ | 4 | about $76^\circ$ |
| $H = R/2$ | 2 | about $63^\circ$ |
| $H = R/4$ | 1 | $45^\circ$ |
| $R = 4\sqrt3\,H$ | $1/\sqrt3$ | $30^\circ$ |
Key formulas
- $H = \dfrac{v_i^2\sin^2\theta}{2g}$
- $T = \dfrac{2v_i\sin\theta}{g}$
- $R = \dfrac{v_i^2\sin2\theta}{g}$, $\quad R_{max} = \dfrac{v_i^2}{g}$ at $45^\circ$
- $\dfrac{H}{R} = \dfrac{\tan\theta}{4}$; at $45^\circ$, $H_{max\ range} = R_{max}/4$
Common MDCAT traps
- Maximum range needs $\sin2\theta = 1$, not $\sin\theta = 1$.
- Equal ranges come from angles that add to $90^\circ$, not angles that differ by a fixed amount.
- Half of maximum range is at $15^\circ$ (or $75^\circ$), not $22.5^\circ$.
- Range depends on $v_i^2$: doubling speed gives $4R$, not $2R$.
- At $90^\circ$ height is maximum but range is zero.
Quick revision
- Maximum range at $45^\circ$.
- $\theta$ and $90^\circ-\theta$: same range, different heights and times.
- $H/R = \tan\theta/4$.
- Time of flight is twice the time to reach the top.
- Above $45^\circ$: more height, less range.