Mathematics 9709/43 — May/June 2017
Cambridge AS Level · Mechanics · worked solutions for every part, with the mark scheme
Topics Kinematics of Motion in a Straight Line · Forces and Equilibrium · Energy, Work and Power · Newton's Laws of Motion
A man pushes a wheelbarrow of mass along a horizontal road with a constant force of magnitude at an angle of below the horizontal. There is a constant resistance to motion of . The wheelbarrow moves a distance of from rest.
Find the work done by the man.
Approach
The man's force is applied at below the horizontal, so only its horizontal component does work in the direction of motion. Use
with , and .
Working
Answer
395 J (3 s.f.)
Walkthrough
The wheelbarrow moves horizontally, but the pushing force is below the horizontal. Work is done only by the component of the force in the direction of motion, which is . Multiplying by the distance gives the work done by the man. The vertical component of the push does no work because there is no vertical displacement.
Key Takeaways
Work done by a constant force is the product of the component of force along the displacement and the distance moved: . Work is a scalar quantity measured in joules.
Common Mistakes
Using the full instead of its horizontal component; using instead of ; forgetting to multiply by the distance ; omitting units.
Things to Be Careful About
The angle is measured between the force and the horizontal displacement, so is correct even though the force is below the horizontal. Give the answer to 3 significant figures as .
Find the speed attained by the wheelbarrow after .
Approach
Use the work-energy principle: the total work done on the wheelbarrow equals its increase in kinetic energy. The man does positive work, while the resistance does negative work. Since the wheelbarrow starts from rest, its initial kinetic energy is zero.
Working
Work done by the man:
Work done against resistance:
Net work done on the wheelbarrow:
By the work-energy principle:
Answer
4.14 m s^-1 (3 s.f.)
Walkthrough
First calculate the work done by the man in the same way as part (i): . The resistance of acts opposite to the motion over , so it removes of energy. The net work done on the wheelbarrow is therefore . By the work-energy principle, this net work equals the gain in kinetic energy. Since the wheelbarrow starts from rest, its final kinetic energy is . Solving gives .
Alternatively, use Newton's second law. The horizontal component of the push is , so the resultant force is . Then , and , giving .
Key Takeaways
The work-energy principle states that the total work done by all forces equals the change in kinetic energy. Work done against a resistance is energy removed from the system. Kinetic energy is .
Common Mistakes
Forgetting to include the work done against resistance; using the full force rather than its horizontal component; using incorrectly in ; forgetting that the wheelbarrow starts from rest so initial KE is zero.
Things to Be Careful About
Work done by the man is positive, while work done by the resistance is negative; the net work equals the KE gain. In the alternative Newton's law method, use the horizontal component of the push and remember the acceleration is constant, so applies with . Give final speed to 3 significant figures: .
The rest of this paper
6 more questions- Q2Forces and Equilibrium5M
- Q3Kinematics of Motion in a Straight Line6M
- Q4Kinematics of Motion in a Straight Line6M
- Q5Kinematics of Motion in a Straight Line6M
- Q6Energy, Work and Power · Forces and Equilibrium · Newton's Laws of Motion8M
- Q7Forces and Equilibrium · Newton's Laws of Motion · Kinematics of Motion in a Straight Line14M