· H2 Physics — Ten-Year Series, worked ← All 7 questions

2022 A-Level · Paper 2 · Question 2

Friction that changes sides, and a collision read off a velocity–time graph

Forces · dynamics 11 marks Friction on a slope Impulse Conservation of momentum

Eleven marks in three short pieces. A definition. An object on a rough slope, sliding down at constant speed and then pulled up at constant speed: the friction is the same size both times, but it switches direction. Then two objects collide in a line, and a velocity–time graph of one of them gives you the impulse, the other's final speed, and a distance. Below is the full solution, and beside it the slope and the collision.

The model, live

Weight componentFrictionP / object XObject Y

Part (a)(i)

1 mark

State what is meant by a vector quantity.

A quantity that has both magnitude and direction.

Part (a)(ii)

1 mark

Name one vector quantity.

Any one of: displacement, velocity, acceleration, force, momentum.

Part (b)(i)

1 mark

An object of weight 16 N16\,\text{N} slides down a rough 35∘35^\circ slope at constant speed. Find the component WW of the weight down the slope.

W=16sin⁡35∘=9.18 NW = 16\sin 35^\circ = 9.18\,\text{N}

W=9.2 NW = 9.2\,\text{N}

Watch

The component along the slope uses sin⁡\sin of the slope angle; the component into the slope uses cos⁡\cos. A quick test: on a flat surface (0∘0^\circ) nothing acts along the slope, and sin⁡0∘=0\sin 0^\circ = 0.

Part (b)(ii)

2 marks

The object is pulled up the slope at constant speed by a force PP parallel to the slope. Find PP.

Approach

Constant speed both times means zero resultant force. Going down, the friction balances the weight component, so it is 9.2 N9.2\,\text{N} up the slope. The normal force has not changed, so the friction is still 9.2 N9.2\,\text{N}; but friction opposes the motion, so going up it acts down the slope, on the same side as the weight component.

P=W+F=9.18+9.18=18.4 NP = W + F = 9.18 + 9.18 = 18.4\,\text{N}

P=18 NP = 18\,\text{N}

Part (c)(i)

2 marks

X (0.22 kg0.22\,\text{kg}) and Y (0.40 kg0.40\,\text{kg}) collide along a line. From the velocity–time graph of X, find the impulse on X.

Approach

Impulse is the change in momentum. Read X's velocity before (2.6 m s−12.6\,\text{m s}^{-1}) and after (3.5 m s−13.5\,\text{m s}^{-1}) the steep section.

impulse=mΔv=(0.22)(3.5−2.6)=0.198 N s\text{impulse} = m\Delta v = (0.22)(3.5 - 2.6) = 0.198\,\text{N s}

impulse =0.20 N s= 0.20\,\text{N s}

Part (c)(ii)

2 marks

Before the collision Y moved at 3.3 m s−13.3\,\text{m s}^{-1}. Find the speed vv of Y after the collision.

Approach

X sped up, so Y pushed it forwards: Y was behind X, moving the same way and faster. By Newton's third law Y receives an equal and opposite impulse, 0.198 N s0.198\,\text{N s} backwards.

v=3.3−0.1980.40=2.8 m s−1v = 3.3 - \frac{0.198}{0.40} = 2.8\,\text{m s}^{-1}

To check your answer:

Total momentum before: (0.22)(2.6)+(0.40)(3.3)=1.89 N s(0.22)(2.6) + (0.40)(3.3) = 1.89\,\text{N s}. After: (0.22)(3.5)+(0.40)(2.8)=1.89 N s(0.22)(3.5) + (0.40)(2.8) = 1.89\,\text{N s}. Conserved, and Y ends up slower than X, so they separate.

v=2.8 m s−1v = 2.8\,\text{m s}^{-1}

Part (c)(iii)

2 marks

Find the distance travelled by X while it is in contact with Y.

Approach

Contact lasts while X's velocity is changing: from 1.8 s1.8\,\text{s} to 2.0 s2.0\,\text{s}. The distance is the area under the graph over that interval, a trapezium.

s=12(2.6+3.5)(2.0−1.8)=0.61 ms = \tfrac12(2.6 + 3.5)(2.0 - 1.8) = 0.61\,\text{m}

distance =0.61 m= 0.61\,\text{m}

What this question was really testing

  1. Resolving on a slope. mgsin⁡θmg\sin\theta along, mgcos⁡θmg\cos\theta into it.
  2. Friction opposes motion. Same size if the normal force is unchanged, opposite direction when the motion reverses.
  3. Impulse = change in momentum, equal and opposite on the two bodies.
  4. Area under v–t is displacement, even over a fraction of a second.

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