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The Range Equation
+5 XP
Deriving a compact formula for horizontal range on level ground
Fire a cannonball from level ground at 100 m/s. At 30° it lands closer than at 45°; at 60° it also lands closer than at 45° but travels the same distance as the 30° shot. There is a single angle that maximises horizontal range when launch and landing height are equal, and deriving why requires combining the horizontal and vertical motion equations.
Launch Angle Analysis, how angle affects range on level ground.
Derivation
The horizontal velocity is constant (no air resistance):
$v_x = v\cos\theta$
The time of flight is found from vertical motion. On level ground, the projectile returns to its initial vertical position, so $s_y = 0$:
$s_y = v_y t + \tfrac{1}{2}a_y t^2$
$0 = v\sin\theta \cdot t_{\text{flight}} - \tfrac{1}{2}g \cdot t_{\text{flight}}^2$
$t_{\text{flight}} = \dfrac{2v\sin\theta}{g}$
The range is horizontal velocity multiplied by time of flight:
$R = v_x \times t_{\text{flight}} = v\cos\theta \times \dfrac{2v\sin\theta}{g} = \dfrac{v^2(2\sin\theta\cos\theta)}{g}$
Using the double-angle identity $\sin(2\theta) = 2\sin\theta\cos\theta$:
Maximum Range
The maximum value of $\sin(2\theta)$ is 1, which occurs when $2\theta = 90°$, giving $\theta = 45°$.
At $\theta = 45°$:
$R_{\text{max}} = \dfrac{v^2}{g}$
Within these model conditions, the maximum range depends only on launch speed and gravitational acceleration.
Worked example 1
+5 XP on full reveal
Comparing ranges. A point projectile is launched at 15 m/s from and onto level ground. Find its range at 30°, 45° and 60°. Take $g=9.8\ \text{m/s}^2$ and neglect air resistance.
1
Check the formula conditions
Launch height equals landing height; $g$ is uniform; drag is neglected.
These conditions permit the level-ground shortcut $R=v^2\sin(2\theta)/g$.
2
Calculate the 30° range
$R_{30}=\dfrac{15^2\sin60°}{9.8}=\mathbf{19.9\text{ m}}$.
The range equation doubles the launch angle inside the sine function.
3
Calculate the 45° range
$R_{45}=\dfrac{15^2\sin90°}{9.8}=\mathbf{23.0\text{ m}}$.
$\sin90°=1$, the greatest possible value of the sine function.
4
Calculate the 60° range
$R_{60}=\dfrac{15^2\sin120°}{9.8}=\mathbf{19.9\text{ m}}$.
$\sin120°=\sin60°$, so the complementary launches have equal ranges.
5
Compare and conclude
$R_{30}=R_{60}=19.9\text{ m}$; $R_{45}=23.0\text{ m}$ is greatest.
At fixed speed on level ground, 45° maximises range. Equal range does not imply equal flight time.
For a point projectile with equal launch and landing heights, uniform $g$ and negligible drag, $R = v^2\sin(2\theta)/g$; it is maximised at $\theta = 45°$, giving $R_{\text{max}} = v^2/g$. The time of flight is $t_{\text{flight}} = 2v\sin\theta/g$ and is derived by setting $s_y = 0$.
Pause, copy the highlighted range equation and the maximum-range result into your book before moving on.