Year 12 Physics Module 5 ⏱ ~45 min 5 MC · 3 Short Answer Lesson 2 of 18

Launch Angle Analysis

Why can two launches follow very different paths yet land at the same horizontal position? Derive the level-ground range relationship, compare complementary angles, then test how unequal heights and real-world limitations change the result.

Today's hook: At the same launch speed on level ground, 30° and 60° reach the same range, but the 60° projectile stays airborne longer. By the end, you will be able to prove both claims and state exactly when the shortcut is valid.
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Orient and predict

Warm up first

Three quick questions from earlier lessons. Pulling old material back to mind before you learn something new makes the new material stick better, so this is not busywork.

Worksheets

Practise this lesson

Four printable worksheets that build from the foundations up to exam-style questions, start at whatever level suits you.

Before you read, estimate

Estimate the range of a soccer penalty kick struck at 25 m/s, 20° above horizontal. Show your reasoning.

Write your estimate before working through the lesson, you will revisit it at the end.

Warm-up, for a projectile on level ground, what determines the time of flight?

2

Set the scope and language

Learning Intentions
goals

Know, Range Equation

  • Derive and use the range equation for projectile motion on level ground

Understand, Maximum Range

  • Explain why 45° gives maximum range on level ground using the sine double-angle identity

Can Do, Height Effects

  • Analyse how different launch and landing heights affect the optimal launch angle
Scan these before reading
vocab
RangeTotal horizontal displacement from launch to landing.
Complementary anglesTwo angles that sum to 90°; give identical ranges on level ground.
Double-angle identity$\sin(2\theta) = 2\sin\theta\cos\theta$, used to derive the range equation.
Optimal angleThe launch angle that maximises range for given conditions.
Cross-lesson links: L01 established the component method for projectile motion. L02 combines those components to derive the conditional range relationship; L03 will apply the same reasoning to multi-step projectile problems.
What is assessable in this lesson?
Core: assessable

Derive and apply the level-ground range equation, explain complementary-angle range and flight-time differences, and solve unequal-height problems from the component equations.

Useful extension

You do not need to derive a general closed-form expression for the exact optimum angle at unequal heights. You do need to compare calculated ranges and explain why the optimum shifts.

Model and reference convention

Work in an inertial ground frame with $+x$ in the launch direction and $+y$ upward. Treat the projectile as a point particle, take $a_x=0$ and $a_y=-g=-9.8\ \text{m/s}^2$, assume uniform $g$, and neglect air resistance and Earth curvature. The shortcut $R=v^2\sin(2\theta)/g$ additionally requires the launch and landing heights to be equal.

Misconceptions to fix
45° always gives maximum range.
Only for equal launch and landing heights under the ideal model. When launch is above landing, the extra fall time shifts the optimum below 45°.
A steeper angle always means a shorter range.
On level ground at fixed speed, range rises to its 45° maximum and then falls. Complementary angles have equal ranges.
Mass appears in the ideal range equation.
Mass cancels from the ideal point-particle model. In real flight, size, shape and drag can make unlike objects follow different paths.
3

Derive the level-ground range

1
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

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 $\sin(2\theta) = 2\sin\theta\cos\theta$:

Range Equation (Level Ground)

$R = \dfrac{v^2\sin(2\theta)}{g}$

Valid for a point projectile with equal launch and landing heights, uniform $g$ and negligible air resistance in an inertial ground frame.

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.

A ball is kicked on level ground at 20 m/s. What is the maximum possible range? ($g = 9.8\ \text{m/s}^2$)

4

Compare complementary angles

2
Complementary Angles
+5 XP

Two different launch angles that produce exactly the same range

We just saw that the range equation contains $\sin(2\theta)$, which peaks at 45°. That raises a question: are there other angles that give the same range as each other? This card answers it → complementary angles (summing to 90°) produce identical ranges.

A powerful symmetry in the range equation reveals that two different launch angles can produce exactly the same range.

Recall the identity: $\sin(180° - \phi) = \sin(\phi)$. If we set $\phi = 2\theta$, then:

$\sin(2\theta) = \sin(180° - 2\theta) = \sin\bigl(2(90° - \theta)\bigr)$

This means launching at angle $\theta$ gives the same range as launching at angle $(90° - \theta)$. These angles are called complementary angles (they sum to 90°).

Key insight

30° and 60° give the same range because $\sin(60°) = \sin(120°)$. The steeper trajectory (60°) goes higher and flies for longer; the shallower trajectory (30°) stays lower and lands sooner. The horizontal distance is identical under the level-ground, no-drag model.

Worked example 2 +5 XP on full reveal

Complementary angles. A point projectile is launched at 25 m/s from and onto level ground. Show that 25° and 65° give the same range. Take $g=9.8\ \text{m/s}^2$ and neglect air resistance.

1
Identify the relationship
$25°+65°=90°$, so the launch angles are complementary.
For the level-ground model, complementary angles produce equal values of $\sin(2\theta)$.
2
Calculate at 25°
$R_{25}=\dfrac{25^2\sin50°}{9.8}=\mathbf{48.9\text{ m}}$.
Use the same initial speed and gravitational acceleration for both launches.
3
Calculate at 65°
$R_{65}=\dfrac{25^2\sin130°}{9.8}=\mathbf{48.9\text{ m}}$.
$\sin130°=\sin50°=0.766$ to three significant figures.
4
Compare the flight times
$t=2v\sin\theta/g$, so $t_{65}>t_{25}$.
The 65° launch has the larger vertical component and remains airborne longer.
5
State the conclusion precisely
Both ranges are $\mathbf{48.9\text{ m}}$, but their trajectories and flight times differ.
Equal horizontal displacement does not mean the two motions are identical.

Complementary angles $\theta$ and $(90° - \theta)$ produce identical ranges on level ground because $\sin(2\theta) = \sin(180° - 2\theta)$; for example, 30° and 60° always give the same range at any launch speed.

Add the highlighted complementary-angle rule to your notes before the check below.

30° and 60° launch angles produce the same range on level ground at any given speed.

Complementary angles are any two angles that give different ranges.

A 25° and 65° launch at the same speed produce the same range because $\sin(50°) = \sin(130°)$.

At the same launch speed on level ground, 30° and 60° give equal ranges. Which launch remains airborne longer?

5

Model unequal launch and landing heights

3
Launch Height Not Equal to Landing Height
+5 XP

How height difference shifts the optimal launch angle away from 45°

We just saw that 45° maximises range on level ground and complementary angles give equal ranges. That raises a question: does 45° stay optimal when launch and landing heights differ? This card answers it → height difference shifts the optimal angle below 45° (from a cliff) or above 45° (uphill).

So far we have assumed launch and landing at the same height. In many real situations this is not true, a projectile may be launched from a cliff, a ramp, or a building, or may land on a slope.

Time of Flight from Height

When a projectile is launched from height $h$ above the landing point, the vertical displacement is $s_y = -h$ (downward). Using the quadratic formula on $s_y = v_y t + \tfrac{1}{2}a_y t^2$:

$-h = v\sin\theta \cdot t - \tfrac{1}{2}g \cdot t^2$

$\tfrac{1}{2}gt^2 - v\sin\theta \cdot t - h = 0$

Solving this quadratic for the positive root:

$t_{\text{flight}} = \dfrac{v\sin\theta + \sqrt{v^2\sin^2\theta + 2gh}}{g}$

The extra term $+2gh$ under the square root increases the flight time compared to level ground. The range is then $R = v\cos\theta \times t_{\text{flight}}$.

Why the Optimal Angle Changes

Launch above landing (cliff, ramp)

The projectile has extra time to fall. A shallower angle (less than 45°) lets the horizontal velocity component carry it further during this extended flight. Optimal angle is less than 45°.

Launch below landing (uphill slope)

The projectile lands sooner. A steeper angle (greater than 45°) gives more vertical velocity to reach the higher landing point. Optimal angle is greater than 45°.

Worked example 3 +5 XP on full reveal

Launching above the landing point. A point projectile is launched from a 30 m cliff at 20 m/s. Compare its range at 30°, 45° and 60°. Take $g=9.8\ \text{m/s}^2$ and neglect air resistance.

1
Select the unequal-height method
$t=\dfrac{v\sin\theta+\sqrt{v^2\sin^2\theta+2gh}}{g}$, then $R=v\cos\theta\,t$.
The level-ground range shortcut is invalid because the vertical displacement is $s_y=-30\text{ m}$.
2
Calculate at 30°
$t=\dfrac{10.0+\sqrt{100+588}}{9.8}=3.70\text{ s}$
$R=20\cos30°(3.70)=\mathbf{64.0\text{ m}}$.
Use the positive root because elapsed time after launch must be positive.
3
Calculate at 45°
$t=\dfrac{14.14+\sqrt{200+588}}{9.8}=4.31\text{ s}$
$R=20\cos45°(4.31)=\mathbf{60.9\text{ m}}$.
Retaining extra figures during working prevents premature-rounding error.
4
Calculate at 60°
$t=\dfrac{17.32+\sqrt{300+588}}{9.8}=4.81\text{ s}$
$R=20\cos60°(4.81)=\mathbf{48.1\text{ m}}$.
The longer flight time does not compensate for the much smaller horizontal component.
5
Compare without overclaiming
Of the three sampled angles, 30° gives the greatest range. The continuous-model optimum is about $32.5°$.
The calculation supports an optimum below 45°; testing three angles alone does not prove the exact optimum is 30°.

When launched from height $h$, flight time is $t = (v\sin\theta + \sqrt{v^2\sin^2\theta + 2gh})/g$; launching above landing makes the optimal angle less than 45°, and launching below landing (uphill) makes it greater than 45°.

Pause, write the highlighted cliff-launch formula and the two height-effect rules into your book.

Three of these statements about a projectile launched from a cliff are correct. Pick the odd one out.

Key Formulas, Launch Angle Analysis

Range (level ground): $R = \dfrac{v^2\sin(2\theta)}{g}$, only for equal launch and landing heights, uniform $g$, a point projectile and negligible drag.

Time of flight (level ground): $t_{\text{flight}} = \dfrac{2v\sin\theta}{g}$

Time of flight from height $h$: $t_{\text{flight}} = \dfrac{v\sin\theta + \sqrt{v^2\sin^2\theta + 2gh}}{g}$

Maximum range (level ground): $R_{\text{max}} = \dfrac{v^2}{g}$ at $\theta = 45°$

Fill the gap. For a projectile launched from a cliff of height $h$, the flight time formula has an extra term under the square root: $t = (v\sin\theta + \sqrt{v^2\sin^2\theta + \_\_\_gh})/g$. The missing coefficient is _____.

4
Drive It: The Cliff Question the Range Equation Gets Wrong
+XP for exploring

Component independence and the height effect, measured by experiment instead of asserted

Interactive · Projectile motion explorer

Try this: launch, then drag the time scrubber to the apex and read the two velocity components. The teal horizontal arrow never changes length; the plum vertical one passes through zero while the gravity indicator stays on. Then run the Drop test race, fire Complementary angles from level ground, and build the range-versus-angle chart one launch at a time.

Predict then reveal+8 XP
1 · Predict
2 · Reveal
3 · Compare

A ball is launched at 25 m/s from a platform 20 m above the ground. Predict: of 30°, 38° and 45°, will 45° still give the greatest range, and if not, which wins?

50%

Use the simulator. Set speed 25 m/s and launch height 20 m, then launch at 30°, 38° and 45° and read the range after each flight. Which angle gives the greatest range, and roughly what is it?

Use the simulator's Drop test. Two balls leave the same platform edge at the same instant, one dropped and one thrown sideways at the set speed. Run the probe, read both flight times, then answer:

The dropped ball lands first, because the thrown ball has further to travel.

Both land at the same instant, because time of flight is set by the vertical motion alone.

6

Evaluate real contexts and compare data

Real world, Soccer Penalty Kick

As an idealised comparison, take a penalty kick from 11 m away at 25 m/s. The level-ground model predicts a range of about 32 m at 15°, whereas 45° would predict about 64 m.

This does not make 15° a universal sporting optimum. A real kick is chosen for placement, arrival time and height at the goal; launch speed also changes with technique, and the ball experiences drag and spin. The example shows why maximum theoretical range is not the same objective as successful performance.

Why do soccer players use a low launch angle (around 15°) for penalty kicks rather than 45°?

Activity 1, Angle Comparison Table
ApplyBand 3

Complete the table for a projectile launched at $v = 20\ \text{m/s}$ on level ground. Take $g = 9.8\ \text{m/s}^2$.

Launch Angle $\theta$ $\sin(2\theta)$ Range $R$ (m) $t_{\text{flight}}$ (s)
15° 0.500 ________ ________
30° 0.866 ________ ________
45° 1.000 ________ ________
60° 0.866 ________ ________
75° 0.500 ________ ________

Questions:

  1. Which angle gives the maximum range? By how much does it exceed the range at 15°?
  2. Which pairs of angles give identical ranges? Explain why using the complementary angle property.
  3. As the angle increases from 15° to 45°, does the time of flight increase or decrease? Explain.
Check the table and reasoning

Ranges: 15°: 20.4 m; 30°: 35.3 m; 45°: 40.8 m; 60°: 35.3 m; 75°: 20.4 m.

Flight times: 15°: 1.06 s; 30°: 2.04 s; 45°: 2.89 s; 60°: 3.53 s; 75°: 3.94 s.

45° exceeds the 15° range by 20.4 m. The complementary pairs 15°/75° and 30°/60° have equal ranges, while flight time increases as the initial vertical component increases.

In the angle-comparison table, which pair of angles gives the same range?

7

Investigate and consolidate

Activity 2, Optimal Angle Investigation
ApplyBand 5

A point projectile is launched from the top of a 50 m cliff at 18 m/s. Calculate the range at each sampled angle and determine which sample gives the greatest range. Take $g = 9.8\ \text{m/s}^2$ and neglect air resistance.

Use the formula: $t_{\text{flight}} = \dfrac{v\sin\theta + \sqrt{v^2\sin^2\theta + 2gh}}{g}$, then $R = v\cos\theta \times t_{\text{flight}}$.

Angle $\theta$ $v_y = v\sin\theta$ (m/s) $\sqrt{v_y^2 + 2gh}$ (m/s) $t_{\text{flight}}$ (s) $v_x = v\cos\theta$ (m/s) Range $R$ (m)
20° ________ ________ ________ ________ ________
35° ________ ________ ________ ________ ________
45° ________ ________ ________ ________ ________
55° ________ ________ ________ ________ ________

Conclusion: Which sampled angle gives the greatest range? What can you infer about the true optimum relative to 45°? Explain using horizontal velocity and flight time.

Check the table and conclusion

20°: $v_y=6.16\text{ m/s}$, square-root term $31.90\text{ m/s}$, $t=3.884\text{ s}$, $v_x=16.91\text{ m/s}$, $R=65.69\text{ m}$.

35°: $v_y=10.32\text{ m/s}$, square-root term $32.96\text{ m/s}$, $t=4.417\text{ s}$, $v_x=14.74\text{ m/s}$, $R=65.13\text{ m}$.

45°: $R=60.42\text{ m}$. 55°: $R=51.99\text{ m}$.

Of the listed angles, 20° gives the greatest range. The data support a true optimum below 45°; for this continuous ideal model it is about 26.5°, between the sampled values.

Wrap-up, Misconceptions & Summary

Misconceptions, final check

45° always gives maximum range.
Only for equal launch and landing heights under the ideal model. A launch above landing shifts the optimum below 45°.
A steeper angle always means a shorter range.
At fixed speed on level ground, range rises to 45° and then falls; complementary angles have equal ranges.
Mass appears in the ideal range equation.
Mass cancels from the ideal point-particle model. Real objects can still differ because drag depends on their size, shape and motion through air.

Copy into your books

θ range

Range Equation

  • $R = v^2\sin(2\theta)/g$ (level ground only)
  • $R_{\text{max}} = v^2/g$ at $\theta = 45°$
  • Requires equal launch and landing heights, uniform $g$, a point projectile and negligible drag

Complementary Angles

  • $\theta$ and $(90° - \theta)$ give same range
  • Example: 30° = 60°, 25° = 65°
  • Proof: $\sin(2\theta) = \sin(180° - 2\theta)$

Height Effects

  • Launch above landing → optimal angle < 45°
  • Launch below landing → optimal angle > 45°

Cliff Formula

  • $t = (v\sin\theta + \sqrt{v^2\sin^2\theta + 2gh})/g$
  • Then $R = v\cos\theta \times t_{\text{flight}}$

A projectile is launched from the top of a tall building. The angle for maximum range will be:

Independent practice

Quick recall, launch angle analysis
+5 XP

A fresh five-question set drawn from this lesson's bank, feedback shown immediately. +5 XP per correct · +25 XP all correct

Pick your answer, then rate your confidence, that tells the system what to drill next.

Short Answer, 10 marks
+5 XP

AnalyseBand 4(3 marks) 1. Derive the range equation $R = v^2\sin(2\theta)/g$ starting from the equations of motion. State all assumptions.

1 mark: time of flight $t = 2v\sin\theta/g$ with working · 1 mark: substitution into horizontal equation · 1 mark: use of double-angle identity and assumptions stated

ApplyBand 4(3 marks) 2. A projectile is launched at 25 m/s on level ground. Calculate the range for launch angles of (a) 25°, (b) 45°, (c) 65°. Comment on your results. ($g = 9.8\ \text{m/s}^2$)

1 mark each for (a) and (b) with working · 1 mark for comment on complementary angles

EvaluateBand 6(4 marks) 3. Assess the claim that "a 45° launch angle is always optimal for maximum range in sporting contexts." Use contextual examples to support your evaluation.

1 mark: identifies ideal-model conditions · 1 mark: explains a launch/landing-height effect · 1 mark: uses two contextual sporting factors or examples without treating one angle as universal · 1 mark: reasoned conclusion

Show all answers

Multiple choice

MC answers and full explanations are shown inline as you complete each question. Use the retry button to attempt a fresh set drawn from the lesson bank.

Short Answer, Model Answers

Q1, Derivation (3 marks):
Start with horizontal motion: $s_x = v_x t = v\cos\theta \cdot t$.
For vertical motion on level ground, set $s_y = 0$:
$0 = v\sin\theta \cdot t_{\text{flight}} - \tfrac{1}{2}g \cdot t_{\text{flight}}^2$
Solving: $t_{\text{flight}} = 2v\sin\theta/g$ (1 mark)
Substitute into horizontal equation:
$R = v\cos\theta \times 2v\sin\theta/g = v^2(2\sin\theta\cos\theta)/g$ (1 mark)
Using $\sin(2\theta) = 2\sin\theta\cos\theta$: $R = v^2\sin(2\theta)/g$ (1 mark)
Assumptions: level ground (same launch and landing height), no air resistance, constant $g = 9.8\ \text{m/s}^2$, point projectile.

Q2, Range at Different Angles (3 marks):
(a) At 25°: $R = (25)^2 \times \sin(50°)/9.8 = 625 \times 0.766/9.8 = \mathbf{48.9\ \text{m}}$ (1 mark)
(b) At 45°: $R = 625 \times \sin(90°)/9.8 = 625/9.8 = \mathbf{63.8\ \text{m}}$ (1 mark)
(c) At 65°: $R = 625 \times \sin(130°)/9.8 = 625 \times 0.766/9.8 = \mathbf{48.9\ \text{m}}$
25° and 65° give the same range because they are complementary angles ($25° + 65° = 90°$). 45° gives the maximum range on level ground. (1 mark for comment)

Q3, Assessment of 45° in Sport (4 marks):
The claim is incorrect. A 45° launch angle is only optimal under idealised conditions (level ground, no air resistance, point projectile).
Launch and landing heights differ: In most sports, the projectile is launched from above ground level and lands at ground level. This makes the optimal angle less than 45°, as the extra fall time benefits a shallower trajectory. (1 mark)
Launch speed varies with angle: Athletes cannot achieve the same launch speed at all angles. For example, in the long jump, the optimal takeoff angle is approximately 20° because the athlete's horizontal speed from the run-up is dominant, attempting a steeper angle would drastically reduce horizontal velocity. (1 mark)
Contextual examples:
Elite long-jump takeoff angles are commonly around 20°, because preserving run-up speed matters and the landing point is below the centre of mass at takeoff. Shot-put release angles are often in the high 30s, but vary with release height, athlete strength and technique. Javelin release choices also vary with wind, implement attitude and aerodynamics. These observed values are contextual, not universal constants. (1 mark for two relevant factors or examples)
Conclusion: While 45° is a useful theoretical reference for level-ground projectile motion, it is rarely the optimal angle in sporting contexts due to differing launch/landing heights, biomechanical speed limitations, and aerodynamic effects. (1 mark for reasoned conclusion)

Retrieve and reflect

Check what actually stuck
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How did your thinking change?

At the start you estimated the range of a kick at 25 m/s and 20° above horizontal.

Under the level-ground ideal model, $R=25^2\sin40°/9.8=\mathbf{41.0\text{ m}}$ to three significant figures. That value assumes equal launch and landing heights, a point projectile, uniform $g$ and negligible drag. A real football experiences drag and spin, so the calculation is a model prediction rather than a guaranteed match result.

Compare the calculated value with your estimate. Which assumption or calculation step most changed your reasoning?