2018 A/L Physics Past Paper · Question 16 (English Medium)

Force from a displacement–time graph

A block of mass 2 kg is pushed along a horizontal surface. The variation of the displacement xx, of the block with time tt, is shown in the figure. The values of the resultant force FF acting on the block along the direction of motion during each of the time intervals 0<t<20 < t < 2, 2<t<42 < t < 4 and 4<t<54 < t < 5 do not change. Which of the following correctly represents the magnitude of FF in each of the time intervals?

  1. (1) 0, 0, 0
  2. (2) 0, 1.5, 0
  3. (3) 0, 2, 0
  4. (4) 1, 0, 0
  5. (5) 2, 1.5, 1
Answer and explanation

Answer: (2) 0, 1.5, 0

What the question asks

We want: the resultant force FF in each of the three time parts.

First read the acceleration from the shape of the graph.

Then use F=maF = ma.

Reading the options

Each option gives three forces, one for each time part (in N).

Read the graph first. Then compare.

Relevant theory

gradient = velocity of the body

The rate of change of moments of an object is proportional to the unbalanced (resultant) force which acts on the object.

Required equations

v=ΔxΔtv = \frac{\Delta x}{\Delta t}

a=v2−v1Δta = \frac{v_2 - v_1}{\Delta t}

F=maF = ma

Reasoning and calculation

The flat axis is time tt (s).

The up axis is the displacement xx (m).

One small square is 0.2 s across and 0.2 m up.

Key points: (0, 0), (2, 1), (4, 3), (5, 5).

From 0 to 2 s the line is straight.

From 2 to 4 s it curves.

From 4 to 5 s it is straight again.

0.50.5

v1=1−02−0v_1 = \dfrac{1 - 0}{2 - 0}

22

v2=5−35−4v_2 = \dfrac{5 - 3}{5 - 4}

The slope of the graph is the velocity.

In 0–2 s and 4–5 s the slope does not change. So the velocity does not change.

No change in velocity means no acceleration. So F=0F = 0 there.

In 2–4 s the velocity grows from 0.50.5 to 2 m s−12\ \text{m s}^{-1}. Only here is there a force.

a=v2−v1Δt=2−0.52a = \dfrac{v_2 - v_1}{\Delta t} = \dfrac{2 - 0.5}{2}

0.750.75

a=1.52a = \dfrac{1.5}{2}

1.51.5

F=2×0.75F = 2 \times 0.75

So the three forces are 0, 1.5 N and 0.

That is the row of option (2).

Checks

m∗(v2−v1)/dtm * (v2 - v1) / dt

Check the unit.

kg×m s−1s=N\frac{\text{kg} \times \text{m s}^{-1}}{\text{s}} = \text{N}

The force comes out in newtons, like the table. Good.

A second way: use the distance.

If the acceleration is steady in 2–4 s, then s=ut+12at2s = ut + \tfrac12 at^2 must hold.

The graph says the block moves s=3−1=2s = 3 - 1 = 2 m in that time.

3−1=0.5×2+12×a×223 - 1 = 0.5 \times 2 + \tfrac{1}{2} \times a \times 2^2

2=1+2a2 = 1 + 2a

0.50.5

a=2−12a = \dfrac{2 - 1}{2}

11

F=2×0.5F = 2 \times 0.5

The official answer sheet says: All. Every option was accepted.

Why? The two ways do not agree.

The slope way gives a=0.75 m s−2a = 0.75\ \text{m s}^{-2}, so F=1.5F = 1.5 N.

The distance way gives a=0.5 m s−2a = 0.5\ \text{m s}^{-2}, so F=1F = 1 N.

A steady force must give the same answer both ways. So the graph is drawn wrong, and every option got the mark.

What to remember: on the straight parts the force is zero. Only on the curved part is F=maF = ma. In the exam, (2) from the slopes is the best answer.

Official ruling — all options accepted

Conclusion

From the slopes: F=0F = 0 in 0–2 s, 1.51.5 N in 2–4 s, 00 in 4–5 s.

That is option (2).

The graph does not fit itself, so officially all options were accepted.

Explore

For the first 22 s the block moves at a steady speed; no resultant force pushes it.

From 22 s to 44 s a push speeds it up, from 0.50.5 to 2 m s−12\ \text{m s}^{-1}.

After 44 s the push is gone and it moves at a steady speed again.

So there is a force only in the middle part, where the speed changes: 00, 1.51.5 N, 00.

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