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In this question use $g = 9.8 \, ext{ms}^{-2}$ - AQA - A-Level Maths Pure - Question 16 - 2017 - Paper 2

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In this question use $g = 9.8 \, ext{ms}^{-2}$. The diagram shows a box, of mass 8.0 kg, being pulled by a string so that the box moves at a constant speed along ... show full transcript

Worked Solution & Example Answer:In this question use $g = 9.8 \, ext{ms}^{-2}$ - AQA - A-Level Maths Pure - Question 16 - 2017 - Paper 2

Step 1

Show that $\mu = 0.83$

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Answer

To determine the coefficient of friction μ\mu, we start with the equation:

F=μRF = \mu R

Where:

  • FF is the frictional force,
  • RR is the normal reaction force.

Step 1: Resolve Forces Vertically
We know the box is moving at a constant speed, hence the net force is zero.
This gives us:

Rmg+Tsin40=0R - mg + T \sin 40^{\circ} = 0

Substituting values:

  • Mass, m=8.0 kgm = 8.0 \text{ kg}
  • Acceleration due to gravity, g=9.8ms2g = 9.8 \, \text{ms}^{-2}
  • Tension, T=50NT = 50 \, \text{N}

R=mgTsin40R = mg - T \sin 40^{\circ}
R=8×9.850×sin40R = 8 \times 9.8 - 50 \times \sin 40^{\circ}

Calculating this yields:

  • R78.1NR \approx 78.1 \, \text{N}.

Step 2: Resolve Forces Horizontally
For constant speed, the horizontal forces also sum to zero:

Tcos40F=0T \cos 40^{\circ} - F = 0

Where FF is the friction force:

F=μRF = \mu R

Therefore:

50cos40=μ×78.150 \cos 40^{\circ} = \mu \times 78.1

Step 3: Substitute known values

oμ=50cos4078.1\mu = \frac{50 \cos 40^{\circ}}{78.1}

After calculating, we find:
μ0.827. (rounded to 2 d.p.) \mu \approx 0.827. \text{ (rounded to 2 d.p.) }
Thus, \mu = 0.83.

Step 2

Draw a diagram to show the forces acting on the box as it moves.

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Answer

The diagram should accurately depict the forces acting on the box, including:

  • Gravitational force, W=mgW = mg directed downwards,
  • Normal force RR acting perpendicular to the surface,
  • Tension force TT acting along the string,
  • Frictional force F=μRF = \mu R opposite the direction of motion.
    Ensure all forces are labeled with arrows indicating their direction.

Step 3

Find the tension in the string as the box accelerates up the slope at 3 m s$^{-2}$.

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Answer

To find the tension, we utilize Newton's second law.
For the inclined board with an angle of 5^{\circ}:

  • The net force is given by:
    F=ma\sum F = ma
    Where a=3ms2a = 3 \, \text{ms}^{-2}, hence we start with:

Step 1: Resolve Forces Parallel to Inclined Plane
The forces acting along the incline include the tension and the component of weight along the incline:

Tmgsin5F=maT - mg \sin 5^{\circ} - F = ma
With F=μRF = \mu R, we substitute our earlier calculated values of RR:

Step 2: Substituting forces
Using the earlier approximation for friction, we set:
T8×9.8sin5μ×78.1=8×3T - 8 \times 9.8 \sin 5^{\circ} - \mu \times 78.1 = 8 \times 3
Rearranging gives us:
T=8×9.8sin5+μ×78.1+24T = 8 \times 9.8 \sin 5^{\circ} + \mu \times 78.1 + 24
Substituting values into this equation yields:
T=24+0.83×78.1+8×9.8sin5T = 24 + 0.83 \times 78.1 + 8 \times 9.8 \sin 5^{\circ}
Calculating this provides:
T73.56N (rounded to 2 d.p.) T \approx 73.56 \, \text{N} \text{ (rounded to 2 d.p.) }
Thus, the tension in the string is approximately 74N74 \, \text{N}.

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