9709/43

Mathematics 9709/43May/June 2017

Cambridge AS 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 · Forces and Equilibrium · Energy, Work and Power · Newton's Laws of Motion

Q1Energy, Work and PowerFree sample

A man pushes a wheelbarrow of mass 25 kg25\text{ kg} along a horizontal road with a constant force of magnitude 35 N35\text{ N} at an angle of 2020^{\circ} below the horizontal. There is a constant resistance to motion of 15 N15\text{ N}. The wheelbarrow moves a distance of 12 m12\text{ m} from rest.

(i)

Find the work done by the man.

2M
DifficultyEasy
Worked solution

Approach

The man's force is applied at 2020^\circ below the horizontal, so only its horizontal component does work in the direction of motion. Use

W=FdcosθW = Fd\cos\theta

with F=35 NF = 35\text{ N}, d=12 md = 12\text{ m} and θ=20\theta = 20^\circ.

Working

W=35cos20×12W = 35\cos 20^\circ \times 12 W394.7 JW \approx 394.7\text{ J}

Answer

W395 JW \approx 395\text{ J}
Final answer

395 J (3 s.f.)

Detailed explanation

Walkthrough

The wheelbarrow moves horizontally, but the pushing force is 2020^\circ below the horizontal. Work is done only by the component of the force in the direction of motion, which is 35cos2035\cos 20^\circ. Multiplying by the distance 12 m12\text{ m} 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: W=FdcosθW = Fd\cos\theta. Work is a scalar quantity measured in joules.

Common Mistakes

Using the full 35 N35\text{ N} instead of its horizontal component; using sin20\sin 20^\circ instead of cos20\cos 20^\circ; forgetting to multiply by the distance 12 m12\text{ m}; omitting units.

Things to Be Careful About

The angle is measured between the force and the horizontal displacement, so cos20\cos 20^\circ is correct even though the force is below the horizontal. Give the answer to 3 significant figures as 395 J395\text{ J}.

Techniques used
resolve force into horizontal componentapply work done formula W = Fd cos θ
(ii)

Find the speed attained by the wheelbarrow after 12 m12\text{ m}.

3M
DifficultyMedium
Worked solution

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:

Wman=35cos20×12394.7 JW_{\text{man}} = 35\cos 20^\circ \times 12 \approx 394.7\text{ J}

Work done against resistance:

Wres=15×12=180 JW_{\text{res}} = 15 \times 12 = 180\text{ J}

Net work done on the wheelbarrow:

Wnet=394.7180=214.7 JW_{\text{net}} = 394.7 - 180 = 214.7\text{ J}

By the work-energy principle:

214.7=12(25)v2214.7 = \frac{1}{2}(25)v^2 214.7=12.5v2214.7 = 12.5v^2 v2=214.712.517.18v^2 = \frac{214.7}{12.5} \approx 17.18 v4.14 m s1v \approx 4.14\text{ m s}^{-1}

Answer

v4.14 m s1v \approx 4.14\text{ m s}^{-1}
Final answer

4.14 m s^-1 (3 s.f.)

Detailed explanation

Walkthrough

First calculate the work done by the man in the same way as part (i): 35cos20×12394.7 J35\cos 20^\circ \times 12 \approx 394.7\text{ J}. The resistance of 15 N15\text{ N} acts opposite to the motion over 12 m12\text{ m}, so it removes 15×12=180 J15 \times 12 = 180\text{ J} of energy. The net work done on the wheelbarrow is therefore 394.7180=214.7 J394.7 - 180 = 214.7\text{ J}. 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 12(25)v2=12.5v2\frac{1}{2}(25)v^2 = 12.5v^2. Solving 12.5v2=214.712.5v^2 = 214.7 gives v4.14 m s1v \approx 4.14\text{ m s}^{-1}.

Alternatively, use Newton's second law. The horizontal component of the push is 35cos2032.9 N35\cos 20^\circ \approx 32.9\text{ N}, so the resultant force is 32.915=17.9 N32.9 - 15 = 17.9\text{ N}. Then a=17.9250.716 m s2a = \frac{17.9}{25} \approx 0.716\text{ m s}^{-2}, and v2=2as=2(0.716)(12)17.2v^2 = 2as = 2(0.716)(12) \approx 17.2, giving v4.14 m s1v \approx 4.14\text{ m s}^{-1}.

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 12mv2\frac{1}{2}mv^2.

Common Mistakes

Forgetting to include the work done against resistance; using the full 35 N35\text{ N} force rather than its horizontal component; using mm incorrectly in 12mv2\frac{1}{2}mv^2; 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 v2=u2+2asv^2 = u^2 + 2as applies with u=0u=0. Give final speed to 3 significant figures: 4.14 m s14.14\text{ m s}^{-1}.

Techniques used
calculate work done by applied forcecalculate work done against resistanceapply work-energy principlesolve for speed from kinetic energy

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
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