Mathematics 9709/42 — October/November 2022
Cambridge A-Level · Mechanics · worked solutions for every part, with the mark scheme
Topics Kinematics of Motion in a Straight Line · Newton's Laws of Motion · Energy, Work and Power · Forces and Equilibrium · Momentum
A cyclist is riding a bicycle along a straight horizontal road of length . The cyclist starts from rest at and reaches a speed of at . The cyclist produces a constant driving force of magnitude . There is a resistance force, and the work done against the resistance force from to is .
Find the total mass of the cyclist and bicycle.
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 , the initial kinetic energy is zero.
Working
Work done by the driving force along the road:
Work done against the resistance is given as , so the net work done is:
By the work–energy principle, this net work equals the gain in kinetic energy:
Substitute :
Answer
80 kg
Walkthrough
Start by identifying what energy is involved. The road 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 because the cyclist begins from rest at .
First, find the work done by the driving force. The force of acts in the same direction as the motion, so the angle between the force and the displacement is and . 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 . The net work available to increase speed is therefore:
The work–energy principle states that the net work done on an object equals its change in kinetic energy:
With :
As a cross-check, the alternative SUVAT approach gives the same result. Assuming constant acceleration, with , , yields:
The resistance force is . Newton's second law, , gives , 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: ; when the force is along the motion, .
- 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 .
Common Mistakes
- Omission of the resistance term: writing ignores the 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 and directly.
- The speed is squared: the kinetic energy is , not .
- Keep all units consistent; the mass must be expressed in kilograms.
- Show the work done by the cyclist () explicitly, since the mark scheme awards the first mark for it.
The rest of this paper
6 more questions- Q2Forces and Equilibrium · Newton's Laws of Motion · Kinematics of Motion in a Straight Line7M
- Q3Forces and Equilibrium6M
- Q4Energy, Work and Power · Newton's Laws of Motion6M
- Q5Newton's Laws of Motion · Kinematics of Motion in a Straight Line7M
- Q6Momentum · Kinematics of Motion in a Straight Line9M
- Q7Kinematics of Motion in a Straight Line12M