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Motion graphs and acceleration (VCE Physics Unit 2)

Syllabus dot point

“Interpret and construct position-time, velocity-time and acceleration-time graphs for one-dimensional motion, including reading slope (instantaneous rates) and area (displacement and change in velocity)”

7 min read

Quick answer

Slope of a position-time graph gives velocity; slope of a velocity-time graph gives acceleration. Area under a velocity-time graph is signed displacement, and area under an acceleration-time graph is the change in velocity, which lets you convert between all three graphs.

Jump to a section
  1. What this dot point is asking
  2. Three motion graphs
  3. Reading between graphs
  4. Sign of area
  5. Worked example
  6. Common traps
  7. In one sentence
  8. Examples in context
  9. Try this
  10. Exam-style questions

What this dot point is asking

VCAA wants you to read motion graphs fluently and to convert between xx-tt, vv-tt and aa-tt using slope and area.

Three motion graphs

Position-time (xx-tt).

  • Slope = instantaneous velocity.
  • Horizontal line = stationary.
  • Straight slope = constant velocity.
  • Curved = changing velocity (acceleration).

Velocity-time (vv-tt).

  • Slope = instantaneous acceleration.
  • Area = displacement (with sign).
  • Horizontal line = constant velocity.
  • Straight slope = constant acceleration.

Acceleration-time (aa-tt).

  • Area = change in velocity Δv\Delta v.

Reading between graphs

  • xx-tt slope →v\to v-tt values.
  • vv-tt slope →a\to a-tt values.
  • aa-tt area →Δv\to \Delta v added to vv-tt.
  • vv-tt area →Δx\to \Delta x added to xx-tt.

For uniformly accelerated motion, xx-tt is parabolic, vv-tt is linear, aa-tt is constant.

Sign of area

Area above the time axis is positive displacement; below is negative. A round-trip object has zero net displacement but positive total distance (sum of absolute areas).

Worked example

A ball thrown straight up at 19.619.6 m s−1^{-1} returns to the launcher.

vv-tt graph: straight line from (0,+19.6)(0, +19.6) with slope −9.8-9.8 m s−2^{-2}. Reaches zero at t=2.0t = 2.0 s (peak). Continues to (4.0,−19.6)(4.0, -19.6) at return.

Displacement: triangle above (area 19.619.6 m, going up) + triangle below (area −19.6-19.6 m, returning) = 00 net.

Distance: 39.239.2 m total.

Common traps

Reading xx-tt slope as displacement
Slope is velocity. Displacement is read off the vertical axis.
Treating area on xx-tt as meaningful
Only vv-tt and aa-tt areas matter.
Ignoring sign
Negative area on vv-tt reduces net displacement.

Confusing straight vv-tt with constant velocity. A straight vv-tt line means constant acceleration (zero acceleration if horizontal).

In one sentence

The slope of xx-tt is velocity, the slope of vv-tt is acceleration, the area under vv-tt is displacement (signed), and the area under aa-tt is Δv\Delta v, which lets you convert between the three motion graphs for any one-dimensional journey.

Examples in context

Example 1. Bathurst 1000 pit-lane deceleration. A Supercars driver entering Bathurst's pit lane at 8080 km h−1^{-1} (22.222.2 m s−1^{-1}) must reach the 4040 km h−1^{-1} (11.111.1 m s−1^{-1}) limit by the timing line. On a velocity-time graph, the slope from 22.222.2 to 11.111.1 m s−1^{-1} over a 2.02.0 s braking interval has slope (acceleration) a=(11.1−22.2)/2.0=−5.55a = (11.1 - 22.2)/2.0 = -5.55 m s−2^{-2}. The area under that segment, 12(22.2+11.1)×2.0=33.3\tfrac{1}{2}(22.2 + 11.1) \times 2.0 = 33.3 m, is the displacement during braking. Position-time graphs of the same event are concave-down because the car covers progressively less distance per second.

Example 2. CityLink approach to Burnley Tunnel. A driver decelerates from 100100 km h−1^{-1} (27.827.8 m s−1^{-1}) to 8080 km h−1^{-1} (22.222.2 m s−1^{-1}) over 3.03.0 s on the descent into Burnley Tunnel, then holds steady speed. On a velocity-time graph, the first segment slopes negatively at a=(22.2−27.8)/3.0=−1.87a = (22.2 - 27.8)/3.0 = -1.87 m s−2^{-2}, then is horizontal. On an acceleration-time graph the same motion appears as a step from −1.87-1.87 to 00 m s−2^{-2}. The displacement during deceleration equals the trapezoidal area 12(27.8+22.2)×3.0=75\tfrac{1}{2}(27.8 + 22.2) \times 3.0 = 75 m, useful for designing the tunnel approach distance to the toll gantry.

Try this

Q1. Define instantaneous acceleration from a velocity-time graph. [2 marks]

  • Cue. Slope of the tangent to the velocity-time curve at a given instant.

Q2. A cyclist travels at 55 m s−1^{-1} for 1010 s, then accelerates at 0.50.5 m s−2^{-2} for 2020 s. Calculate (a) the final velocity, and (b) the total displacement. [4 marks]

  • Cue. (a) v=5+0.5×20=15v = 5 + 0.5 \times 20 = 15 m s−1^{-1}. (b) 5×10+12(5+15)×20=50+200=2505\times 10 + \tfrac{1}{2}(5+15)\times 20 = 50 + 200 = 250 m.

Q3. Refer to the Bathurst pit-lane example. (a) Calculate the deceleration. (b) Determine the braking distance. (c) Sketch the corresponding position-time graph and describe its curvature. [2+2+2 marks]

  • Cue. (a) −5.55-5.55 m s−2^{-2}. (b) 33.333.3 m. (c) Concave-down because slope (velocity) decreases over time.

Exam-style questions

Questions in the style of VCAA exam questions on this dot point, each with a worked answer. They are written by ExamExplained unless tagged "Past paper"; the year shows the paper a question is modelled on.

Year 11 SAC-style4 marks
A cyclist accelerates from rest at 2.02.0 m s−2^{-2} for 4.04.0 s, then maintains constant velocity for 6.06.0 s. Sketch the vv-tt graph and use it to find the total displacement.
Show worked answer →

vv-tt graph: straight line from (0,0)(0, 0) to (4.0,8.0)(4.0, 8.0) m s−1^{-1}, then horizontal from (4.0,8.0)(4.0, 8.0) to (10,8.0)(10, 8.0).

Displacement = area under graph.

Triangle: 12(4.0)(8.0)=16\frac{1}{2}(4.0)(8.0) = 16 m.

Rectangle: (6.0)(8.0)=48(6.0)(8.0) = 48 m.

Total: 6464 m.

Markers reward the labelled sketch, the area decomposition, and units.

Practise this

Sources & how we know this

ExamExplained