PhysicsGrade 7–11

Uniform and accelerated motion (distance–time and velocity–time graphs)

A car drives at a steady speed or speeds up. The graphs for distance, speed and acceleration are drawn live.

Loading simulation …

What is it about?

A motion is described by the position ss (measured on a tape) at every time tt. Plotting ss against tt gives the position–time graph (s–t graph). The velocity tells you how fast the position changes:

v=ΔsΔt1 ms=3.6 kmhv = \frac{\Delta s}{\Delta t} \qquad 1\,\tfrac{\text{m}}{\text{s}} = 3.6\,\tfrac{\text{km}}{\text{h}}

Uniform motion: The velocity is constant. In equal times the car covers equal distances:

s(t)=s0+v⋅ts(t) = s_0 + v \cdot t

In the s–t graph you get a straight line – its slope is the velocity. In the v–t graph it is a horizontal line. The area under the v–t graph (a rectangle v⋅tv \cdot t) is the displacement Δs\Delta s.

Uniformly accelerated motion: The velocity changes by the same amount in equal times. The acceleration is

a=ΔvΔt,v(t)=v0+a⋅t,s(t)=s0+v0⋅t+12 a⋅t2.a = \frac{\Delta v}{\Delta t}, \qquad v(t) = v_0 + a \cdot t, \qquad s(t) = s_0 + v_0 \cdot t + \tfrac{1}{2}\, a \cdot t^2 .

Now the v–t graph is a sloping straight line with slope aa, and the s–t graph is a parabola. The velocity at an instant is the slope of the tangent to the parabola. If the car starts from rest, the distances in successive equal time intervals are in the ratio 1:3:5:7:…1 : 3 : 5 : 7 : \ldots – the stroboscope shows this.

Braking to a stop: With initial velocity v0v_0 and deceleration ∣a∣|a|, braking takes tB=v0∣a∣t_B = \frac{v_0}{|a|} and the braking distance is sB=v022 ∣a∣s_B = \frac{v_0^2}{2\,|a|}. Twice the speed therefore means four times the braking distance.

Try it

  1. Press Start and watch the stroboscope: for uniform motion the gaps are equal. Compare with the slope triangle in the s–t graph.
  2. Let the car drive backwards. What do the s–t and v–t graphs look like now? Driving backwards
  3. Speed up with a=2 ms2a = 2\,\tfrac{\text{m}}{\text{s}^2}. How do the gaps in the stroboscope grow? Speeding up
  4. Drag the time marker (triangle at the top of the s–t graph) back and forth. Compare the slope of the tangent with the value in the v–t graph.
  5. Choose the schedule and drag the corners of the v–t graph. Watch how the s–t graph changes. Schedule
  6. Switch off “Show the graphs before the trip” and predict what the graphs will look like. Only then start. Prediction

Tasks

Task 1: Distance at constant velocity

A car moves uniformly at 54 kmh54\,\tfrac{\text{km}}{\text{h}}. How far does it travel in 8 s8\,\text{s}? Load task

Show solution

54 kmh=54:3.6 ms=15 ms54\,\tfrac{\text{km}}{\text{h}} = 54 : 3.6\,\tfrac{\text{m}}{\text{s}} = 15\,\tfrac{\text{m}}{\text{s}}, so Δs=v⋅Δt=15 ms⋅8 s=120 m\Delta s = v \cdot \Delta t = 15\,\tfrac{\text{m}}{\text{s}} \cdot 8\,\text{s} = 120\,\text{m}. This is the rectangle under the v–t graph.

Task 2: Reading a graph

Load the task and read from the s–t graph: Where does the car start, how fast does it move, and when does it pass the point s=0s = 0? Load task

Show solution

Starting position s0=−50 ms_0 = -50\,\text{m}. After 12 s12\,\text{s} the car is at 100 m100\,\text{m}, so v=150 m12 s=12.5 msv = \frac{150\,\text{m}}{12\,\text{s}} = 12.5\,\tfrac{\text{m}}{\text{s}}. It is at s=0s = 0 after t=50 m12.5 m/s=4 st = \frac{50\,\text{m}}{12.5\,\text{m/s}} = 4\,\text{s} (where the graph crosses the t-axis).

Task 3: Speeding up

A car starts from rest and speeds up uniformly with a=2.5 ms2a = 2.5\,\tfrac{\text{m}}{\text{s}^2}. How fast is it after 6 s6\,\text{s}, and how far has it travelled by then? How long does it take to reach 100 kmh100\,\tfrac{\text{km}}{\text{h}}? Load task

Show solution

v=a⋅t=2.5⋅6 ms=15 msv = a \cdot t = 2.5 \cdot 6\,\tfrac{\text{m}}{\text{s}} = 15\,\tfrac{\text{m}}{\text{s}} and s=12⋅2.5⋅62 m=45 ms = \tfrac12 \cdot 2.5 \cdot 6^2\,\text{m} = 45\,\text{m} (triangle under the v–t graph). 100 kmh≈27.8 ms100\,\tfrac{\text{km}}{\text{h}} \approx 27.8\,\tfrac{\text{m}}{\text{s}}, so t=27.82.5 s≈11.1 st = \frac{27.8}{2.5}\,\text{s} \approx 11.1\,\text{s}.

Task 4: Braking distance

A car moving at 20 ms20\,\tfrac{\text{m}}{\text{s}} (72 kmh72\,\tfrac{\text{km}}{\text{h}}) brakes with a=−5 ms2a = -5\,\tfrac{\text{m}}{\text{s}^2}. How long is the braking distance? How long would it be at twice the speed? Load task

Show solution

sB=v022 ∣a∣=(20 m/s)22⋅5 m/s2=40 ms_B = \frac{v_0^2}{2\,|a|} = \frac{(20\,\text{m/s})^2}{2 \cdot 5\,\text{m/s}^2} = 40\,\text{m} after tB=4 st_B = 4\,\text{s}. At 40 ms40\,\tfrac{\text{m}}{\text{s}} it is 160 m160\,\text{m} – four times the braking distance. Twice the speed

Task 5: Evaluating a schedule

A car goes from rest to 15 ms15\,\tfrac{\text{m}}{\text{s}} in 5 s5\,\text{s}, then moves uniformly for 10 s10\,\text{s} and brakes to a stop in 5 s5\,\text{s}. Calculate the accelerations, the distances of the sections, the total distance and the average velocity. Load task

Show solution

a1=3 ms2a_1 = 3\,\tfrac{\text{m}}{\text{s}^2}, a2=0a_2 = 0, a3=−3 ms2a_3 = -3\,\tfrac{\text{m}}{\text{s}^2}. Areas under the v–t graph: 37.5 m+150 m+37.5 m=225 m37.5\,\text{m} + 150\,\text{m} + 37.5\,\text{m} = 225\,\text{m}. Average velocity vˉ=225 m20 s=11.25 ms\bar v = \frac{225\,\text{m}}{20\,\text{s}} = 11.25\,\tfrac{\text{m}}{\text{s}}.

Task 6: Distance or displacement?

In the example “There and back” the car ends up at its start again. How large are the displacement and the distance travelled? What is the car’s acceleration at the turning point at t=8 st = 8\,\text{s}? Load task

Show solution

Displacement Δs=0\Delta s = 0 (the areas above and below the t-axis cancel), distance travelled 4⋅16 m=64 m4 \cdot 16\,\text{m} = 64\,\text{m}. At the turning point v=0v = 0, but a=−2 ms2a = -2\,\tfrac{\text{m}}{\text{s}^2} – the car is at rest for just an instant.

Ideas for the classroom

  • Use: Uniform motion, velocity and the s–t graph when starting mechanics (about grades 7/8); uniformly accelerated motion, the v–t graph and braking distance in grades 9/10. The graphs can be switched off individually, e.g. the a–t graph for younger classes.
  • Notation: The simulation calls the position ss; many textbooks write xx and speak of the position–time graph. Displacement Δs\Delta s (with sign) and distance travelled (always positive) are distinguished.
  • Model: The car is treated as a point mass (white marker, dropped line to the tape); it is drawn larger than to scale. When braking it stops at v=0v = 0 and does not reverse by itself. In the schedule the velocity changes uniformly in each section; the jumps in the a–t graph are idealised.
  • Predictions: With “Show the graphs before the trip” switched off and _hide=1, learners can sketch the graphs first and then check them.
  • Common stumbling blocks:
    • The s–t graph is read as a picture of the path (“the car drives uphill”).
    • “High in the v–t graph means far away” – in fact it is the area under the graph that counts.
    • “If v=0v = 0, then a=0a = 0 too” – at the turning point (task 6) this is not true.
    • Slope and value are mixed up: a flat but high s–t graph means slow, not fast.