Skip to main content
ScotlandMathematics of MechanicsSyllabus dot point

How do you model a projectile moving under gravity, and how do you find its range, maximum height, time of flight and path?

Model projectile motion under gravity by treating horizontal and vertical motion independently; find time of flight, range, maximum height, velocity at any time, and the equation of the parabolic path.

A focused answer to the SQA Advanced Higher Mathematics of Mechanics content on projectiles, resolving the initial velocity into horizontal and vertical parts, applying the constant-acceleration equations independently in each direction, and deriving time of flight, range, maximum height and the equation of the trajectory.

Generated by Claude Opus 4.813 min answer

Reviewed by: AI editorial process; not yet individually human-reviewed

Have a quick question? Jump to the Q&A page

Jump to a section
  1. What this dot point is asking
  2. Resolving and separating the motion
  3. Maximum height, time of flight and range
  4. The equation of the path
  5. Try this

What this dot point is asking

A projectile is anything moving freely under gravity once it has been launched, with air resistance ignored. The SQA wants you to model it by splitting the motion into two independent parts: horizontal motion at constant velocity, and vertical motion with constant downward acceleration gg. From that split come all the standard results - time of flight, range, maximum height, the velocity at any instant, and the parabolic equation of the path.

Resolving and separating the motion

The key modelling idea is that gravity acts only downward, so it changes only the vertical velocity. The horizontal velocity stays constant throughout the flight.

Because the two sets of equations share only the time tt, the time is the bridge between them: solve a vertical condition for tt, then feed that tt into the horizontal equation (or vice versa).

Maximum height, time of flight and range

These standard results all come from applying the right condition to the vertical motion.

The maximum height comes from vy2=uy22gHv_y^2 = u_y^2 - 2gH with vy=0v_y = 0, giving H=uy22gH = \dfrac{u_y^2}{2g}. The time of flight on level ground comes from setting the vertical displacement back to zero, t=2uygt = \dfrac{2u_y}{g}. The range is then the horizontal distance covered in that time, R=uxt=2uxuygR = u_x t = \dfrac{2u_x u_y}{g}, which (using 2sinθcosθ=sin2θ2\sin\theta\cos\theta = \sin 2\theta) equals V2sin2θg\dfrac{V^2\sin 2\theta}{g} and is greatest at θ=45\theta = 45^\circ.

The equation of the path

Eliminating the time between the horizontal and vertical equations gives yy as a function of xx. The result is a downward parabola, which is why projectile motion is described as parabolic.

y=xtanθgx22V2cos2θ.y = x\tan\theta - \frac{gx^2}{2V^2\cos^2\theta}.

This form is useful for "does it clear the wall" problems: substitute the wall's horizontal distance for xx and compare the resulting yy with the wall's height.

Try this

Q1. A ball is kicked at 1414 m s1^{-1} at 4545^\circ. Find its range on level ground (g=9.8g = 9.8). [3 marks]

  • Cue. R=V2sin2θg=196sin909.8=20R = \dfrac{V^2\sin 2\theta}{g} = \dfrac{196\sin 90^\circ}{9.8} = 20 m.

Q2. A projectile launched at 2525^\circ has initial vertical velocity 1010 m s1^{-1}. Find its greatest height (g=9.8g = 9.8). [2 marks]

  • Cue. H=uy22g=10019.65.1H = \dfrac{u_y^2}{2g} = \dfrac{100}{19.6} \approx 5.1 m.

Exam-style practice questions

Practice questions written in the style of SQA exam questions on this dot point, with worked answer explainers. The year tag is the paper they imitate, not the source.

AH style: range and height6 marksA ball is projected from ground level at 2020 m s1^{-1} at 3030^\circ above the horizontal. Taking g=9.8g = 9.8 m s2^{-2}, find the time of flight, the horizontal range, and the greatest height reached.
Show worked answer →

Resolve: ux=20cos30=103u_x = 20\cos 30^\circ = 10\sqrt{3}, uy=20sin30=10u_y = 20\sin 30^\circ = 10 m s1^{-1} (1 mark).

Time of flight: vertical displacement returns to zero, 0=uyt12gt20 = u_y t - \tfrac{1}{2}gt^2, so t=2uyg=209.82.04t = \dfrac{2u_y}{g} = \dfrac{20}{9.8} \approx 2.04 s (2 marks).

Range: R=uxt=103×2.0435.3R = u_x t = 10\sqrt{3}\times 2.04 \approx 35.3 m (1 mark).

Greatest height: at the top vy=0v_y = 0, so vy2=uy22gHv_y^2 = u_y^2 - 2gH gives H=uy22g=10019.65.10H = \dfrac{u_y^2}{2g} = \dfrac{100}{19.6} \approx 5.10 m (2 marks). Markers reward resolving the velocity, treating the two directions independently, and using vy=0v_y = 0 at the highest point.

AH style: trajectory equation5 marksA projectile is launched from the origin with speed VV at angle θ\theta. Show that its path has equation y=xtanθgx22V2cos2θy = x\tan\theta - \dfrac{gx^2}{2V^2\cos^2\theta}.
Show worked answer →

Horizontal: x=Vcosθtx = V\cos\theta\, t, so t=xVcosθt = \dfrac{x}{V\cos\theta} (1 mark).

Vertical: y=Vsinθt12gt2y = V\sin\theta\, t - \tfrac{1}{2}gt^2 (1 mark).

Substitute for tt: y=VsinθxVcosθ12g(xVcosθ)2y = V\sin\theta\cdot\dfrac{x}{V\cos\theta} - \tfrac{1}{2}g\left(\dfrac{x}{V\cos\theta}\right)^2 (2 marks).

Simplify: the first term is xtanθx\tan\theta and the second is gx22V2cos2θ\dfrac{gx^2}{2V^2\cos^2\theta}, giving y=xtanθgx22V2cos2θy = x\tan\theta - \dfrac{gx^2}{2V^2\cos^2\theta} (1 mark). Markers reward eliminating tt between the two component equations and the correct simplification, recognising the path is a parabola in xx.

Related dot points

Sources & how we know this