9709/42

Mathematics 9709/42October/November 2022

Cambridge A-Level · Mechanics · worked solutions for every part, with the mark scheme

7
questions
50
marks
75
minutes

Topics Kinematics of Motion in a Straight Line · Newton's Laws of Motion · Energy, Work and Power · Forces and Equilibrium · Momentum

Q13MEnergy, Work and PowerFree sample

A cyclist is riding a bicycle along a straight horizontal road ABAB of length 50 m50\text{ m}. The cyclist starts from rest at AA and reaches a speed of 6 m s16\text{ m s}^{-1} at BB. The cyclist produces a constant driving force of magnitude 100 N100\text{ N}. There is a resistance force, and the work done against the resistance force from AA to BB is 3560 J3560\text{ J}.

Find the total mass of the cyclist and bicycle.

DifficultyMedium-Easy
Worked solution

Approach

Use the work–energy principle: the net work done on the cyclist and bicycle (the work done by the driving force minus the work done against the resistance) is equal to the increase in kinetic energy. Because the cyclist starts from rest at AA, the initial kinetic energy is zero.

Working

Work done by the driving force along the 50 m50\text{ m} road:

Wdriving=Fd=100×50=5000 JW_{\text{driving}} = Fd = 100 \times 50 = 5000\text{ J}

Work done against the resistance is given as 3560 J3560\text{ J}, so the net work done is:

Wnet=50003560=1440 JW_{\text{net}} = 5000 - 3560 = 1440\text{ J}

By the work–energy principle, this net work equals the gain in kinetic energy:

12mv2=1440\frac{1}{2}mv^2 = 1440

Substitute v=6v = 6:

12m(62)=1440\frac{1}{2}m(6^2) = 1440 18m=144018m = 1440 m=144018=80 kgm = \frac{1440}{18} = 80\text{ kg}

Answer

m=80 kgm = 80\text{ kg}
Final answer

80 kg

Detailed explanation

Walkthrough

Start by identifying what energy is involved. The road ABAB is horizontal, so the height of the cyclist does not change and there is no change in gravitational potential energy. The only energy change is the increase in kinetic energy, which starts at 00 because the cyclist begins from rest at AA.

First, find the work done by the driving force. The force of 100 N100\text{ N} acts in the same direction as the motion, so the angle between the force and the displacement is 0° and W=Fdcos0°=Fd=100×50=5000 JW = Fd\cos 0° = Fd = 100 \times 50 = 5000\text{ J}. This is the total energy supplied to the system by the cyclist.

Not all of this energy becomes kinetic energy: some of it is spent overcoming the resistance. The question gives the work done against the resistance as 3560 J3560\text{ J}. The net work available to increase speed is therefore:

50003560=1440 J5000 - 3560 = 1440\text{ J}

The work–energy principle states that the net work done on an object equals its change in kinetic energy:

1440=12mv21440 = \frac{1}{2}mv^2

With v=6v = 6:

12m(36)=1440\frac{1}{2}m(36) = 1440 18m=144018m = 1440 m=80 kgm = 80\text{ kg}

As a cross-check, the alternative SUVAT approach gives the same result. Assuming constant acceleration, v2=u2+2asv^2 = u^2 + 2as with u=0u = 0, v=6v = 6, s=50s = 50 yields:

a=36100=0.36 m s2a = \frac{36}{100} = 0.36\text{ m s}^{-2}

The resistance force is 356050=71.2 N\frac{3560}{50} = 71.2\text{ N}. Newton's second law, 10071.2=0.36m100 - 71.2 = 0.36m, gives m=28.80.36=80 kgm = \frac{28.8}{0.36} = 80\text{ kg}, confirming the answer.

Key Takeaways

  • The work–energy principle: net work done on an object equals its change in kinetic energy.
  • Work done by a constant force: W=FdcosθW = Fd\cos\theta; when the force is along the motion, W=FdW = Fd.
  • On a horizontal road there is no change in gravitational potential energy, so all net work becomes kinetic energy.
  • Units used: work and energy in joules (J), mass in kilograms (kg), speed in m s1\text{m s}^{-1}.

Common Mistakes

  • Omission of the resistance term: writing 5000=12mv25000 = \frac{1}{2}mv^2 ignores the 3560 J3560\text{ J} and produces the wrong mass.
  • Sign errors in the energy equation. The mark scheme allows sign errors for the method mark but still needs the three-term equation to be dimensionally correct.
  • Confusing 'work done by the resistance' with 'work done against the resistance'.
  • In the SUVAT alternative, applying Newton's second law without including both the driving force and the resistance.

Things to Be Careful About

  • The force and displacement are both along the road, so cosθ=1\cos\theta = 1 and W=FdW = Fd directly.
  • The speed is squared: the kinetic energy is 12m×62\frac{1}{2}m \times 6^2, not 12m×6\frac{1}{2} m \times 6.
  • Keep all units consistent; the mass must be expressed in kilograms.
  • Show the work done by the cyclist (5000 J5000\text{ J}) explicitly, since the mark scheme awards the first mark for it.
Techniques used
compute the work done by a constant forceapply the work-energy principlesolve for mass from the kinetic energy change

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