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3.3.5 Coefficient of Friction - Harder Problems

infoNote

In harder coefficient of friction problems, multiple forces and varying conditions come into play. Here's a summary of the approach:

  1. Identify all forces: Draw a free body diagram, showing forces like weight, normal reaction, friction, applied forces, and tension (if present).
  2. Resolve forces into components: On inclined planes, break forces into parallel and perpendicular components. Use mgsin(θ)mg \sin(\theta) and mgcos(θ)mg \cos(\theta) for weight components.
  3. Apply friction formulas:
  • Static friction: FfrictionμsFnormalF_{\text{friction}} \leq \mu_s F_{\text{normal}} (when preventing motion).
  • Kinetic friction: Ffriction=μkFnormalF_{\text{friction}} = \mu_k F_{\text{normal}} (when the object is moving).
  1. Use F=maF = ma: Apply Newton's second law to solve for unknowns like acceleration, tension, or friction. Consider equilibrium conditions if the object is stationary. These problems require careful force resolution, consistent sign convention, and correct use of friction formulas.
infoNote

Example: Force on a Rough Inclined Plane

Problem Statement:

  • A box of mass 10 kg rests in limiting equilibrium on a rough plane inclined at 20° above the horizontal.
  • A horizontal force of magnitude P is applied to the box.
  • Given that the box remains in equilibrium, find:
  1. The coefficient of friction between the box and the plane.
  2. The maximum possible value of P.

Part (a): Find the Coefficient of Friction

  1. Forces acting:
  • Gravitational force component along the slope: 10gsin20°10g \sin 20°
  • Normal reaction force: R=10gcos20°R = 10g \cos 20°
  • Frictional force Fmax=μRF_{\text{max}} = \mu R (acting up the slope). image
  1. Equations of equilibrium:
  • Along the plane:
Fmax=10gsin20°=μRF_{\text{max}} = 10g \sin 20° = \mu R
  • Perpendicular to the plane:
R=10gcos20°R = 10g \cos 20°
  1. Solve for μ\mu:
μ=10gsin20°10gcos20°=33.51892.08990.3640\mu = \frac{10g \sin 20°}{10g \cos 20°} = \frac{33.518}{92.0899} \approx 0.3640

Answer (a): The coefficient of friction μ0.3640\mu \approx 0.3640.


Part (b): Find the Maximum Possible Value of PP

image
  1. Forces acting:
  • The force P is horizontal and can be resolved into components parallel and perpendicular to the slope:
  • Parallel: Pcos20°P \cos 20°
  • Perpendicular: Psin20°P \sin 20°
  1. Equations of equilibrium:
  • Along the slope:
Fmax+Pcos20°10gsin20°=0-F_{\text{max}} + P \cos 20° - 10g \sin 20° = 0
  • Perpendicular to the slope:
R=Psin20°+10gcos20°R = P \sin 20° + 10g \cos 20°
  1. Substitute and solve for PP:
μ(Psin20°+10gcos20°)+Pcos20°10gsin20°=0\mu (P \sin 20° + 10g \cos 20°) + P \cos 20° - 10g \sin 20° = 0 0.3640(Psin20°+92.0899)+Pcos20°=33.5180.3640(P \sin 20° + 92.0899) + P \cos 20° = 33.518 0.8159P=67.03870.8159P = 67.0387 P82.24NP \approx 82.24 \, \text{N}

Answer (b): The maximum possible value of P is approximately 82.24 N.

:::


Tips:

infoNote
  1. Resolve forces correctly: Always resolve forces into horizontal and vertical components (or parallel/perpendicular to an inclined plane). Pay special attention to the normal force, as it may not always equal mgmg if other forces are acting at angles.
  2. Check motion status: Determine whether static or kinetic friction applies. If the object is on the verge of moving, use the maximum static friction Ffriction=μsFnormalF_{\text{friction}} = \mu_s F_{\text{normal}}. If it's already moving, apply kinetic friction.
  3. Solve systematically: Use F=maF = ma in both horizontal and vertical directions to set up equations for unknowns. Make sure to account for all forces, including tension, applied forces, and weight components, for precise solutions.
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