9709/42

Mathematics 9709/42May/June 2017

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

6
questions
50
marks
75
minutes

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

Q13MEnergy, Work and PowerFree sample

One end of a light inextensible string is attached to a block. The string makes an angle of θ\theta^{\circ} with the horizontal. The tension in the string is 20 N20\text{ N}. The string pulls the block along a horizontal surface at a constant speed of 1.5 m s11.5\text{ m s}^{-1} for 12 s12\text{ s}. The work done by the tension in the string is 50 J50\text{ J}. Find θ\theta.

DifficultyMedium-Easy
Worked solution

Approach

Resolve the tension into its horizontal component 20cosθ20\cos\theta, since only this component acts in the direction of motion. Find the distance travelled from speed and time, then use W=FdcosθW = Fd\cos\theta to solve for θ\theta.

Working

The block moves at constant speed for 12 s12\text{ s}, so

d=vt=1.5×12=18 m.d = vt = 1.5 \times 12 = 18\text{ m}.

The horizontal component of the tension is

Fhorizontal=20cosθ.F_{\text{horizontal}} = 20\cos\theta.

Thus the work done by the tension is

W=Fhorizontald=(20cosθ)(18)=360cosθ.W = F_{\text{horizontal}} d = (20\cos\theta)(18) = 360\cos\theta.

Given W=50 JW = 50\text{ J}:

50=360cosθ50 = 360\cos\theta cosθ=50360=536\cos\theta = \frac{50}{360} = \frac{5}{36} θ=cos1(536)=82.0\theta = \cos^{-1}\left(\frac{5}{36}\right) = 82.0^{\circ}

Answer

θ=82.0\theta = 82.0^{\circ}
Final answer

θ = 82.0°

Detailed explanation

Walkthrough

Start by listing what is known: the tension is 20 N20\text{ N}, it acts at angle θ\theta to the horizontal, the block moves at 1.5 m s11.5\text{ m s}^{-1} for 12 s12\text{ s}, and the work done by the tension is 50 J50\text{ J}.

The block moves horizontally, so only the horizontal component of the tension does work. That component is 20cosθ20\cos\theta. The vertical component 20sinθ20\sin\theta is perpendicular to the displacement and does no work.

The distance travelled is

d=vt=1.5×12=18 m.d = vt = 1.5 \times 12 = 18\text{ m}.

Using the work formula for a constant force acting at an angle,

W=Fdcosθ=(20)(18)cosθ=360cosθ.W = Fd\cos\theta = (20)(18)\cos\theta = 360\cos\theta.

Set this equal to the given work:

50=360cosθcosθ=536.50 = 360\cos\theta \quad \Rightarrow \quad \cos\theta = \frac{5}{36}.

Then

θ=cos1(536)=82.0.\theta = \cos^{-1}\left(\frac{5}{36}\right) = 82.0^{\circ}.

An equivalent method uses power. The power supplied by the tension is

P=Wt=5012=256 W.P = \frac{W}{t} = \frac{50}{12} = \frac{25}{6}\text{ W}.

Since P=FvcosθP = Fv\cos\theta,

256=(20)(1.5)cosθ=30cosθ,\frac{25}{6} = (20)(1.5)\cos\theta = 30\cos\theta,

so cosθ=25180=536\cos\theta = \frac{25}{180} = \frac{5}{36}, giving the same answer.

Key Takeaways

  • Work done by a constant force at an angle to the displacement is W=FdcosθW = Fd\cos\theta.
  • Only the component of force in the direction of motion does work.
  • Distance can be found from constant speed and time using d=vtd = vt.
  • Power is the rate of doing work, and for a force at angle θ\theta to the velocity, P=FvcosθP = Fv\cos\theta.
  • Inverse cosine is used to recover an angle from its cosine.

Common Mistakes

  • Using the full 20 N20\text{ N} without multiplying by cosθ\cos\theta.
  • Using the time 12 s12\text{ s} as the distance instead of computing 1.5×12=18 m1.5 \times 12 = 18\text{ m}.
  • Treating 360cosθ360\cos\theta as the answer for work, rather than setting it equal to 50 J50\text{ J}.
  • Having the calculator in radians instead of degrees.
  • Using the vertical component 20sinθ20\sin\theta in the work formula; it does no work here.
  • In the power method, forgetting the cosθ\cos\theta factor in P=FvcosθP = Fv\cos\theta.

Things to Be Careful About

  • The angle is measured to the horizontal, so the horizontal component is 20cosθ20\cos\theta.
  • Keep units consistent: newtons, metres, seconds, joules, watts.
  • Constant speed means zero net work, but the tension itself can still do positive work while friction does negative work.
  • The mark scheme requires the method to be shown: award B1 for W=FdcosθW = Fd\cos\theta (or P=W/tP = W/t), M1 for substituting W=50W=50 and solving, and A1 for θ=82.0\theta = 82.0^{\circ}.
Techniques used
resolve tension into component along direction of motionapply work done formula W = Fd cos θuse distance = speed × timesolve for θ using inverse cosine

The rest of this paper

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