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A box of mass 5 kg lies on a rough plane inclined at 30° to the horizontal - Edexcel - A-Level Maths Mechanics - Question 3 - 2012 - Paper 1

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A box of mass 5 kg lies on a rough plane inclined at 30° to the horizontal. The box is held in equilibrium by a horizontal force of magnitude 20 N, as shown in Figur... show full transcript

Worked Solution & Example Answer:A box of mass 5 kg lies on a rough plane inclined at 30° to the horizontal - Edexcel - A-Level Maths Mechanics - Question 3 - 2012 - Paper 1

Step 1

(a) the magnitude of the normal reaction of the plane on the box

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Answer

To find the normal reaction force, we need to resolve the forces acting on the box perpendicular to the inclined plane.

  1. Identify the forces acting on the box:

    • The weight of the box, which acts downwards: W=mg=5imes9.81extN=49.05extNW = mg = 5 imes 9.81 ext{ N} = 49.05 ext{ N}.
    • The horizontal force of 20 N.
    • The normal reaction force, RR, acting perpendicular to the inclined surface.
  2. The vertical components of the forces must be balanced since the box is in equilibrium. We can resolve the weight and the horizontal force:

    • The component of the weight perpendicular to the inclined plane: W_ ext{perpendicular} = W imes rac{1}{2} = 49.05 imes rac{ ext{cos}(30^ ext{°})}{ ext{cos}(60^ ext{°})}, where extcos(60ext°)=0.5 ext{cos}(60^ ext{°}) = 0.5.
    • The applied force also has a component that affects the normal reaction.
  3. The equation for vertical equilibrium can be set up as: R=20imesextcos(60ext°)+49.05imesextcos(30ext°)R = 20 imes ext{cos}(60^ ext{°}) + 49.05 imes ext{cos}(30^ ext{°})

  4. Solving this gives: R = 20 imes 0.5 + 49.05 imes rac{ ext{ extsqrt{3}}}{2} R=10+42.43=52.4extNR = 10 + 42.43 = 52.4 ext{ N}

Thus, the magnitude of the normal reaction is approximately 52.4 N.

Step 2

(b) the coefficient of friction between the box and the plane

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Answer

To find the coefficient of friction, we first need to establish the frictional force acting on the box.

  1. The frictional force can be expressed as: Ff=extμRF_f = ext{μ}R where extμ ext{μ} is the coefficient of friction.

  2. In addition to the forces, we also need to resolve the forces parallel to the inclined plane. The equation will be: Ff+20Nextcos(30ext°)=5gextsin(30ext°)F_f + 20N ext{ cos}(30^ ext{°}) = 5g ext{ sin}(30^ ext{°})

  3. The force acting down the inclined plane can be computed as:

    • Weight component down the incline: Wextparallel=mgextsin(30ext°)W_ ext{parallel} = mg ext{ sin}(30^ ext{°}) Wextparallel=49.05imes0.5=24.525extNW_ ext{parallel} = 49.05 imes 0.5 = 24.525 ext{ N}
  4. Now, substituting the values into the equilibrium equation, we get: Ff+20imes0.866=24.525F_f + 20 imes 0.866 = 24.525

  5. Rearranging gives: Ff=24.52517.327.205extNF_f = 24.525 - 17.32 ≈ 7.205 ext{ N}

  6. Now substituting back into the friction equation: 7.205=extμimes52.47.205 = ext{μ} imes 52.4

  7. Solving for extμ ext{μ}, we get: ext{μ} = rac{7.205}{52.4} ≈ 0.137

Therefore, the coefficient of friction between the box and the plane is approximately 0.137.

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