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In this question use $g = 9.8 \, \text{m s}^{-2}$ - AQA - A-Level Maths Mechanics - Question 16 - 2017 - Paper 2

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In-this-question-use-$g-=-9.8-\,-\text{m-s}^{-2}$-AQA-A-Level Maths Mechanics-Question 16-2017-Paper 2.png

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

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

Step 1

Show that $\mu = 0.83$

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Answer

To find the coefficient of friction μ\mu, we start by resolving the forces acting on the box resting on the horizontal board.

  1. Identify Forces:

    • Weight of the box, W=mg=8.0kg×9.8m s2=78.4NW = mg = 8.0 \, \text{kg} \times 9.8 \, \text{m s}^{-2} = 78.4 \, \text{N}.
    • Normal reaction force, RR.
    • Tension in the string, T=50NT = 50 \, \text{N} at an angle of 4040^{\circ}.
  2. Resolve Forces in the Vertical Direction:

    Using the equation for vertical forces: R+Tsin(40)=WR + T \sin(40^{\circ}) = W
    Substituting known values: R+50sin(40)=78.4R=78.450sin(40)R + 50 \sin(40^{\circ}) = 78.4 \Rightarrow R = 78.4 - 50 \sin(40^{\circ})
    Calculating: R78.450×0.6428=78.432.14=46.26NR \approx 78.4 - 50 \times 0.6428 = 78.4 - 32.14 = 46.26 \, \text{N}

  3. Resolve Forces in the Horizontal Direction:

    The horizontal forces must balance since the box is moving at constant speed: Tcos(40)=Ffriction=μRT \cos(40^{\circ}) = F_{friction} = \mu R
    Substituting for tension: 50cos(40)=μ×46.2650 \cos(40^{\circ}) = \mu \times 46.26

  4. Calculate and Solve for μ\mu:

    μ=50cos(40)46.2638.8546.260.8390.83. \mu = \frac{50 \cos(40^{\circ})}{46.26} \approx \frac{38.85}{46.26} \approx 0.839 \approx 0.83.
    Therefore, we have shown that μ=0.83\mu = 0.83.

Step 2

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

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Answer

To draw the forces acting on the box:

  1. Represent the box on an inclined plane.
  2. Draw the weight vector WW acting downward (vertically down).
  3. Draw the normal force RR, perpendicular to the surface of the inclined board.
  4. Draw the tension force TT at an angle of 4040^{\circ} to the board.
  5. Draw the frictional force FfrictionF_{friction} acting down the slope, opposite to the direction of motion.
    Label all forces clearly.

Step 3

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

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Answer

To find the tension TT in the string when the box accelerates up the incline:

  1. Draw a Free Body Diagram (FBD): Include all forces acting on the box as described above.

    • Weight: W=78.4NW = 78.4 \, \text{N}
    • Normal Reaction: RR
    • Tension: TT
    • Friction: Ffriction=μRF_{friction} = \mu R
  2. Resolve Forces:

    In the direction parallel to the incline: TFfrictionWsin(5)=maT - F_{friction} - W \sin(5^{\circ}) = ma Substitute known values: TμR78.4sin(5)=8.0imes3T - \mu R - 78.4 \sin(5^{\circ}) = 8.0 imes 3 where RR needs to be calculated at this incline: R=mgcos(5)=8.0×9.8×cos(5)77.92N R = mg \cos(5^{\circ}) = 8.0 \times 9.8 \times \cos(5^{\circ}) \approx 77.92 \, \text{N} Thus, Ffriction=μR=0.83×77.9264.67N F_{friction} = \mu R = 0.83 \times 77.92 \approx 64.67 \, \text{N}

  3. Plug into the equation:

    T64.6778.4×0.0872=24substituting for acceleration part T - 64.67 - 78.4 \times 0.0872 = 24\rightarrow \text{substituting for acceleration part}

    Calculate:

    • 78.4×0.08726.8478.4 \times 0.0872 \approx 6.84
    • Thus, plugging back:

ightarrow T \approx 95.51 , \text{N}$$ The final computed tension in the string is approximately T95.5NT \approx 95.5 \, \text{N}.

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