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In this question use g = 9.8 m.s^{-2} A boy attempts to move a wooden crate of mass 20 kg along horizontal ground - AQA - A-Level Maths Mechanics - Question 13 - 2018 - Paper 2

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Question 13

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In this question use g = 9.8 m.s^{-2} A boy attempts to move a wooden crate of mass 20 kg along horizontal ground. The coefficient of friction between the crate and... show full transcript

Worked Solution & Example Answer:In this question use g = 9.8 m.s^{-2} A boy attempts to move a wooden crate of mass 20 kg along horizontal ground - AQA - A-Level Maths Mechanics - Question 13 - 2018 - Paper 2

Step 1

13 (a) The boy applies a horizontal force of 150 N. Show that the crate remains stationary.

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Answer

To show that the crate remains stationary, we first need to calculate the maximum static friction force that can act on the crate using the formula:

Fmax=extμmgF_{max} = ext{μmg}

Where:

  • μ (coefficient of friction) = 0.85
  • m (mass of the crate) = 20 kg
  • g (acceleration due to gravity) = 9.8 m/s²

Calculating the maximum friction:

Fmax=0.85×20×9.8=166 NF_{max} = 0.85 \times 20 \times 9.8 = 166 \text{ N}

The horizontal force applied by the boy is 150 N. Since 150 N < 166 N, the static friction is sufficient to keep the crate stationary. Therefore, the crate does not move.

Step 2

13 (b) Instead, the boy uses a handle to pull the crate forward. He exerts a force of 150 N, at an angle of 15° above the horizontal. Determine whether the crate remains stationary.

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Answer

To determine if the crate remains stationary, we resolve the applied force into its horizontal and vertical components:

The horizontal component of the force is:

Fhorizontal=150cos(15)F_{horizontal} = 150 \cos(15^\circ)

And the vertical component is:

Fvertical=150sin(15)F_{vertical} = 150 \sin(15^\circ)

Calculating these:

  1. Horizontal component:

    • Fhorizontal150×0.9659144.89 NF_{horizontal} ≈ 150 \times 0.9659 ≈ 144.89 \text{ N}
  2. Vertical component:

    • Fvertical150×0.258838.82 NF_{vertical} ≈ 150 \times 0.2588 ≈ 38.82 \text{ N}

Next, we calculate the normal force (R). The weight of the crate is:

W=mg=20×9.8=196 NW = mg = 20 \times 9.8 = 196 \text{ N}

Thus, the normal force is:

R=WFvertical=19638.82157.18 NR = W - F_{vertical} = 196 - 38.82 ≈ 157.18 \text{ N}

Now, we calculate the maximum static friction:

Fmax=extμR=0.85×157.18133.6 NF_{max} = ext{μR} = 0.85 \times 157.18 ≈ 133.6 \text{ N}

Finally, we compare the horizontal force with the maximum friction. Since:

144.89>133.6144.89 > 133.6

The crate will begin to move, which suggests that it does not remain stationary. Therefore, the applied force is greater than the maximum static friction, and the crate begins to move.

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