← Unit 2: Linear motion and waves

QLDPhysicsSyllabus dot point

Topic 1: Linear motion and force

Recall and apply the equations for uniformly accelerated motion to one-dimensional problems, including problems involving free fall under gravity

A focused answer to the QCE Physics Unit 2 dot point on the equations of uniformly accelerated motion. Lists the four QCAA-formulae-sheet suvat equations, the conditions under which they apply, and works the free-fall standard question that recurs in IA1 and EA Paper 1.

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What this dot point is asking

QCAA wants you to apply the four standard equations of uniformly accelerated motion to one-dimensional problems, including objects in free fall (acceleration g=9.8g = 9.8 m sβˆ’2^{-2} downward). The equations only apply when acceleration is constant. The IA1 and EA both reward fluent identification of the known and unknown quantities and clean substitution.

The four equations

Using uu for initial velocity, vv for final velocity, aa for acceleration, ss for displacement and tt for time:

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s=12(u+v)ts = \tfrac{1}{2}(u + v) t

Each equation has four of the five variables. Identify what you know and what you want, then pick the equation that contains those four.

When the equations apply

  • Motion is along a straight line.
  • Acceleration is constant (including zero or gg).
  • Motion is from t=0t = 0 with the stated initial conditions.

If acceleration changes during the motion, split the journey into segments and apply the equations to each segment separately. Do not use suvat across a segment where the acceleration jumps.

Sign conventions

Pick a positive direction at the start and apply it consistently. Common choices:

  • Horizontal motion: positive in the direction of initial motion.
  • Vertical motion: up positive (then a=βˆ’g=βˆ’9.8a = -g = -9.8 m sβˆ’2^{-2}) or down positive (then a=+g=+9.8a = +g = +9.8 m sβˆ’2^{-2}).

Stick to one convention through the whole problem.

Free fall

Air resistance is ignored unless the problem states otherwise. The acceleration is g=9.8g = 9.8 m sβˆ’2^{-2} directed downward.

For an object dropped from rest, u=0u = 0; for an object thrown upward, uu is positive (up positive) and the velocity becomes negative after the peak.

At the highest point of flight, v=0v = 0. Use this to find time to peak (t=u/gt = u/g) and peak height (s=u2/(2g)s = u^2 / (2g)).

Worked example

A car accelerates uniformly from 5.05.0 m sβˆ’1^{-1} to 2525 m sβˆ’1^{-1} over a distance of 9090 m. Find the acceleration and the time taken.

Knowns: u=5.0u = 5.0, v=25v = 25, s=90s = 90.

Acceleration from v2=u2+2asv^2 = u^2 + 2as:

252=5.02+2a(90)25^2 = 5.0^2 + 2 a (90)

625=25+180a625 = 25 + 180 a

a=600/180=3.33a = 600 / 180 = 3.33 m sβˆ’2^{-2}.

Time from v=u+atv = u + at:

25=5.0+3.33t25 = 5.0 + 3.33 t

t=20/3.33=6.0t = 20 / 3.33 = 6.0 s.

Common traps

Applying suvat across a change in acceleration. If a car accelerates then brakes, you cannot use one equation across both phases. Split the problem.

Mixing sign conventions. Choosing up as positive then writing a=+9.8a = +9.8 in a free-fall problem is the most common QCAA marking deduction.

Using g=10g = 10 when the question says 9.89.8. QCAA writes problems with g=9.8g = 9.8 m sβˆ’2^{-2} unless otherwise stated. Read the question.

Forgetting a negative root. v2=u2+2asv^2 = u^2 + 2as gives two solutions for vv. Pick the physically sensible one (direction of motion).

Try it: Projectile motion calculator handles two-dimensional cases; for one-dimensional motion the same equations apply with ΞΈ=0\theta = 0 or ΞΈ=90Β°\theta = 90Β°.

In one sentence

The four constant-acceleration equations (v=u+atv = u + at, s=ut+12at2s = ut + \frac{1}{2}at^2, v2=u2+2asv^2 = u^2 + 2as, s=12(u+v)ts = \frac{1}{2}(u+v)t) solve any one-dimensional motion (including free fall with a=g=9.8a = g = 9.8 m sβˆ’2^{-2} downward) provided acceleration is constant and a consistent positive direction is chosen.

Past exam questions, worked

Real questions from past QCAA papers on this dot point, with our answer explainer.

Year 11 SAC4 marksA stone is dropped from rest from the top of a tall building and takes $3.2$ s to reach the ground. Ignoring air resistance and using $g = 9.8$ m s$^{-2}$, calculate (a) the height of the building and (b) the speed of the stone when it lands.
Show worked answer β†’

Take down as positive. Initial velocity u=0u = 0, acceleration a=g=9.8a = g = 9.8 m sβˆ’2^{-2}, time t=3.2t = 3.2 s.

(a) Height. Use s=ut+12at2s = ut + \frac{1}{2} a t^2.

s=0+12(9.8)(3.2)2=12(9.8)(10.24)=50.2s = 0 + \frac{1}{2}(9.8)(3.2)^2 = \frac{1}{2}(9.8)(10.24) = 50.2 m.

(b) Landing speed. Use v=u+atv = u + at.

v=0+(9.8)(3.2)=31.4v = 0 + (9.8)(3.2) = 31.4 m sβˆ’1^{-1} downward.

Markers reward the stated sign convention, the explicit identification of uu, aa and tt, and units on both answers.

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