9709/42

Mathematics 9709/42May/June 2015

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

Q1Kinematics of Motion in a Straight LineEnergy, Work and PowerFree sample

One end of a light inextensible string is attached to a block. The string makes an angle of 6060^{\circ} above the horizontal and is used to pull the block in a straight line on a horizontal floor with acceleration 0.5 m s20.5\text{ m s}^{-2}. The tension in the string is 8 N8\text{ N}. The block starts to move with speed 0.3 m s10.3\text{ m s}^{-1}. For the first 5 s5\text{ s} of the block's motion, find

(i)

the distance travelled,

2M
DifficultyMedium-Easy
Worked solution

Approach

Use a constant-acceleration (suvat) formula for displacement. The block moves with initial speed u=0.3 m s1u = 0.3\text{ m s}^{-1}, acceleration a=0.5 m s2a = 0.5\text{ m s}^{-2} and time t=5 st = 5\text{ s}, so substitute these into

s=ut+12at2s = ut + \frac{1}{2}at^2

Working

s=0.3×5+12×0.5×52s = 0.3 \times 5 + \frac{1}{2} \times 0.5 \times 5^2 s=1.5+6.25s = 1.5 + 6.25 s=7.75s = 7.75

Answer

The distance travelled is

7.75 m7.75\text{ m}
Final answer

7.75 m

Detailed explanation

Walkthrough

We are given the initial speed, the constant acceleration, and the time interval. Since the acceleration is constant, the suvat equations apply. The most direct formula for displacement is s=ut+12at2s = ut + \frac{1}{2}at^2. Substitute u=0.3 m s1u = 0.3\text{ m s}^{-1}, a=0.5 m s2a = 0.5\text{ m s}^{-2} and t=5 st = 5\text{ s}. The term 0.3×50.3 \times 5 gives the distance the block would travel at constant speed, while 12×0.5×52\frac{1}{2} \times 0.5 \times 5^2 accounts for the extra distance gained from acceleration. Adding these gives 7.75 m7.75\text{ m}.

Key Takeaways

This part tests the application of the constant acceleration formula for displacement. It is important to recognise which suvat variables are given and to choose the formula containing exactly those variables and the required quantity.

Common Mistakes

A common error is to use v2=u2+2asv^2 = u^2 + 2as immediately without first finding the final velocity, or to use the wrong time exponent in the 12at2\frac{1}{2}at^2 term. Another common mistake is forgetting to halve the at2at^2 term.

Things to Be Careful About

Check that all units are consistent: distances in metres, speed in metres per second, acceleration in metres per second squared and time in seconds. Also note that the tension and angle given in the question are not needed for part (i); the horizontal motion is fully described by the acceleration already provided.

Techniques used
identify known suvat variablesapply constant acceleration formula for displacementevaluate with numerical substitution
(ii)

the work done by the tension in the string.

2M
DifficultyMedium-Easy
Worked solution

Approach

The work done by a constant force is

W=FdcosθW = Fd\cos\theta

where F=8 NF = 8\text{ N} is the tension, d=7.75 md = 7.75\text{ m} is the distance travelled, and θ=60\theta = 60^{\circ} is the angle between the tension and the horizontal displacement.

Working

W=8×7.75×cos60W = 8 \times 7.75 \times \cos 60^{\circ}

Since cos60=0.5\cos 60^{\circ} = 0.5:

W=8×7.75×0.5W = 8 \times 7.75 \times 0.5 W=31W = 31

Answer

The work done by the tension is

31 J31\text{ J}
Final answer

31 J

Detailed explanation

Walkthrough

From part (i), the block travels 7.75 m7.75\text{ m} during the first 5 s5\text{ s}. The pulling force is the tension 8 N8\text{ N}, but the string is inclined at 6060^{\circ} above the horizontal. Therefore not all of the tension does work in the direction of motion; only the horizontal component Tcos60T\cos 60^{\circ} is parallel to the displacement. The work done is

W=Fdcosθ=8×7.75×cos60.W = Fd\cos\theta = 8 \times 7.75 \times \cos 60^{\circ}.

Since cos60=0.5\cos 60^{\circ} = 0.5, this gives 31 J31\text{ J}. The vertical component Tsin60T\sin 60^{\circ} does no work in the horizontal motion, so the formula FdcosθFd\cos\theta automatically picks out only the component in the direction of displacement.

Key Takeaways

Work is a scalar but is calculated using the component of force in the direction of displacement. The formula W=FdcosθW = Fd\cos\theta handles this, where θ\theta is the angle between the force vector and the displacement vector. This part also shows the importance of using the result from part (i) to answer a follow-up question.

Common Mistakes

A common mistake is to use the full 8 N8\text{ N} without multiplying by cos60\cos 60^{\circ}, which would give 62 J62\text{ J} instead of 31 J31\text{ J}. Another common mistake is to use sin60\sin 60^{\circ} or to forget that the angle should be measured between the force and the displacement, which are the diagonal tension and the horizontal motion in this setup.

Things to Be Careful About

The angle 6060^{\circ} is measured above the horizontal, and the displacement is horizontal, so the angle between the tension and the displacement is indeed 6060^{\circ}. Use cos60=0.5\cos 60^{\circ} = 0.5. Work is measured in joules, so the final answer should be stated as 31 J31\text{ J} rather than just 3131.

Techniques used
use displacement from part (i)apply work done formula with the angle between force and displacementevaluate cosine of the given angle

The rest of this paper

6 more questions
  • Q2Energy, Work and Power · Newton's Laws of Motion5M
  • Q3Energy, Work and Power5M
  • Q4Kinematics of Motion in a Straight Line7M
  • Q5Kinematics of Motion in a Straight Line6M
  • Q6Kinematics of Motion in a Straight Line · Newton's Laws of Motion11M
  • Q7Forces and Equilibrium12M
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