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Coefficient of Friction Simplified Revision Notes

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3.3.2 Coefficient of Friction

Concept:

  • In A-Level Maths, friction is modelled as being proportional to the normal contact force between objects.

Mathematical Representation:

infoNote
FRF \propto R
  • FF is the frictional force.
  • RR is the normal contact force.

Equation:

infoNote
FμRF \leq \mu R
  • μ\mu is the coefficient of friction and measures how rough the contact between two objects is.

Diagram:

image
  • The frictional force opposes the driving force, and mg is the gravitational force acting on the object.

Nature of Friction:

  • Friction "fights" and resists any driving force up to a limit Fmax=μRF_{\text{max}} = \mu R.
  • When an object is on the point of slipping, it is said to be in "limiting equilibrium." At this point, the frictional force is at its maximum value FmaxF_{\text{max}}.

Example 1: Finding the Maximum Force without Causing Motion (Limiting Equilibrium)

Problem Statement:

infoNote
  • A mass of 8 kg rests on a rough horizontal plane.
  • The coefficient of friction between the mass and the plane is 0.5.
  • Find the magnitude of the maximum force P that can act on this mass without causing it to move if:
  1. The force P is horizontal.
  2. The force P acts at an angle of 6060^\circ above the horizontal.

Part (a): Force P is Horizontal

  1. Given:
  • Coefficient of friction μ=0.5\mu = 0.5
  • Weight mg=8gmg = 8g
  1. Equilibrium in the vertical direction:
  • The normal reaction force R=8gR = 8g
  1. Frictional force at the point of slipping:
Fmax=μR=0.5×8g=4gF_{\text{max}} = \mu R = 0.5 \times 8g = 4g image
  1. Maximum force PP:
P=Fmax=4gNP = F_{\text{max}} = 4g \, \text{N}

Answer (a): P=4gNP = 4g \, \text{N}


Part (b): Force P Acts at an Angle of 6060^\circ above the Horizontal

  1. Resolve the force PP:
  • Horizontal component: Pcos60P \cos 60^\circ
  • Vertical component: Psin60P \sin 60^\circ
  1. Vertical equilibrium:
R+Psin60=8gR=8g32PR + P \sin 60^\circ = 8g \quad \Rightarrow \quad R = 8g - \frac{\sqrt{3}}{2} P image
  1. Frictional force at the point of slipping:
Fmax=μR=0.5×(8g32P)F_{\text{max}} = \mu R = 0.5 \times \left(8g - \frac{\sqrt{3}}{2} P\right)
  1. Horizontal equilibrium:
Pcos60=Fmax=0.5×(8g32P)P \cos 60^\circ = F_{\text{max}} = 0.5 \times \left(8g - \frac{\sqrt{3}}{2} P\right)

Simplifying:

12P=4g34P\frac{1}{2} P = 4g - \frac{\sqrt{3}}{4} P 12P+34P=4g\frac{1}{2} P + \frac{\sqrt{3}}{4} P = 4g P(12+34)=4gP\left(\frac{1}{2} + \frac{\sqrt{3}}{4}\right) = 4g
  1. Solve for PP:
P=4g12+3442.01NP = \frac{4g}{\frac{1}{2} + \frac{\sqrt{3}}{4}} \approx 42.01 \, \text{N}

Answer (b): P42.01NP \approx 42.01 \, \text{N}


Tips:

infoNote
  1. Understand the formula: The frictional force FfrictionF_{\text{friction}} is given by Ffriction=μFnormalF_{\text{friction}} = \mu F_{\text{normal}}, where μ\mu is the coefficient of friction and FnormalF_{\text{normal}} is the normal reaction force. Ensure you calculate FnormalF_{\text{normal}} accurately, especially on inclined planes.
  2. Distinguish between static and kinetic friction: Static friction prevents motion, and FfrictionμsFnormalF_{\text{friction}} \leq \mu_s F_{\text{normal}} (maximum value before slipping). Kinetic friction applies once the object is moving, and Ffriction=μkFnormal F_{\text{friction}} = \mu_k F_{\text{normal}}.
  3. Consider all forces: Don't forget to account for other forces acting on the object, such as applied forces or weight components on an inclined plane. Use F=maF = ma to find acceleration or tension when needed.
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