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How is motion in one dimension described using displacement, velocity and acceleration?

Kinematics of motion in one dimension: displacement, velocity, acceleration, the equations of uniformly accelerated motion (suvat), and graphical analysis

A focused answer to the VCE Physics Unit 2 key knowledge point on one-dimensional kinematics. Position vs displacement, velocity vs speed, average vs instantaneous quantities, the suvat equations for uniformly accelerated motion, and graphical analysis (slope and area under graphs).

Generated by Claude Opus 4.810 min answer

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

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  1. What this dot point is asking
  2. Definitions
  3. SUVAT equations (uniformly accelerated motion)
  4. Free fall
  5. Graphical analysis
  6. Examples in context
  7. Try this

What this dot point is asking

VCAA wants you to describe motion in one dimension using displacement, velocity and acceleration, apply the suvat (constant-acceleration) equations to motion problems, and interpret motion graphically.

Definitions

Position xx
Location of an object along the chosen axis. Vector quantity in higher dimensions but scalar (positive or negative) in one dimension.
Displacement Δx\Delta x
Change in position. Vector. Different from distance (a scalar).
Velocity vv
Rate of change of displacement: v=Δx/Δtv = \Delta x / \Delta t. Vector. Sign indicates direction.
Speed v|v|
Magnitude of velocity. Always non-negative.
Acceleration aa
Rate of change of velocity: a=Δv/Δta = \Delta v / \Delta t.
Average vs instantaneous
Average is over a finite time interval. Instantaneous is the limit as Δt0\Delta t \to 0 (the derivative).

SUVAT equations (uniformly accelerated motion)

For constant acceleration:

  • v=u+atv = u + at
  • s=ut+12at2s = ut + \frac{1}{2} a t^2
  • v2=u2+2asv^2 = u^2 + 2 a s
  • s=12(u+v)ts = \frac{1}{2}(u + v) t
  • s=vt12at2s = vt - \frac{1}{2} a t^2

Where uu = initial velocity, vv = final velocity, aa = acceleration, ss = displacement, tt = time.

Choose the equation that contains the four known variables (and the one unknown).

Free fall

An object in free fall near Earth's surface has a=g9.8a = g \approx 9.8 m s2^{-2} directed downward. (Ignoring air resistance.)

Apply suvat with a=ga = -g (taking up as positive) or a=+ga = +g (taking down as positive). Sign consistency is essential.

Graphical analysis

Position-time graph
Slope = instantaneous velocity at that moment.
Velocity-time graph
Slope = instantaneous acceleration. Area under the curve = displacement.
Acceleration-time graph
Area under the curve = change in velocity.

A horizontal line on a velocity-time graph means constant velocity (zero acceleration). A straight line with constant positive slope means constant positive acceleration.

Examples in context

Example 1. Tullamarine Airport runway take-off roll. A Qantas A330 (230000230\,000 kg) accelerates from rest along Tullamarine's runway 16/34 (length 36573657 m) and lifts off at 8080 m s1^{-1}. Assuming uniform acceleration, v2=u2+2asv^2 = u^2 + 2as gives a=v2/(2s)=6400/(2×1600)=2.0a = v^2/(2s) = 6400/(2 \times 1600) = 2.0 m s2^{-2} over the 16001600 m to rotation, with t=v/a=40t = v/a = 40 s. The remaining 20002000 m of runway is safety overrun. Pilots cross-check this acceleration with V1_1 (decision speed) and VR_R (rotation speed) markers; if acceleration is less than expected, the pilot aborts before V1_1.

Example 2. Free fall test of an FMG drill core at Mt Stromlo. A geophysics lab at Mt Stromlo drops a 0.50.5 m rock core into a vacuum tube to time-of-flight test gravimeter calibration. Free fall from rest gives s=12gt2s = \tfrac{1}{2}gt^2. For s=1.0s = 1.0 m and g=9.80g = 9.80 m s2^{-2}, t=2s/g=2/9.80=0.452t = \sqrt{2s/g} = \sqrt{2/9.80} = 0.452 s and final velocity v=gt=4.43v = gt = 4.43 m s1^{-1}. Photogate timing to four decimal places lets the lab resolve gg to ±0.001\pm 0.001 m s2^{-2}, sufficient to detect Earth-tide variations and to calibrate field gravimeters used in iron-ore exploration.

Try this

Q1. Define uniform acceleration and state the units of acceleration. [2 marks]

  • Cue. Constant rate of change of velocity with time; m s2^{-2}.

Q2. A car starting from rest reaches 3030 m s1^{-1} over 150150 m. Calculate (a) the acceleration, and (b) the time taken. [4 marks]

  • Cue. (a) v2=2asv^2 = 2as, a=900/300=3.0a = 900/300 = 3.0 m s2^{-2}. (b) t=v/a=10t = v/a = 10 s.

Q3. Refer to the Tullamarine A330 example. (a) Calculate the rotation acceleration. (b) Determine the time to lift-off. (c) Explain why airlines require excess runway beyond rotation distance. [2+2+2 marks]

  • Cue. (a) 2.02.0 m s2^{-2}. (b) 4040 s. (c) Engine-out safety: aircraft must accelerate, abort and stop within runway length even if one engine fails.

Exam-style practice questions

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

Year 11 SAC4 marksA car accelerates from rest at 3.03.0 m s2^{-2} for 8.08.0 s. (a) Find the final velocity. (b) Find the distance travelled.
Show worked answer →

(a) Final velocity. v=u+at=0+3.0×8.0=24v = u + at = 0 + 3.0 \times 8.0 = 24 m s1^{-1}.

(b) Distance. s=ut+12at2=0+12×3.0×64=96s = ut + \frac{1}{2} a t^2 = 0 + \frac{1}{2} \times 3.0 \times 64 = 96 m.

Or use s=12(u+v)t=12(0+24)×8=96s = \frac{1}{2}(u + v) t = \frac{1}{2}(0 + 24) \times 8 = 96 m.

Markers reward the choice of correct suvat equation and the substitution.

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