Friction is a contact force that acts parallel to the common surface and always opposes impending or actual relative motion between the surfaces.
Pause & think: Could you walk if friction suddenly vanished?
Static friction \(f_s\) rises from zero up to its maximum value \((f_s)_{\text{max}}=\mu_s N\) to keep the body at rest.
After motion starts, kinetic friction \(f_k=\mu_k N\) acts; it stays nearly constant and is smaller than \((f_s)_{\text{max}}\).
Dimensionless ratio of limiting friction to the normal reaction between two surfaces.
Dry wood on wood: \( \mu_s \approx 0.4 \), \( \mu_k \approx 0.3 \).
Block on inclined plane showing weight components and friction
A block of mass \(m\) rests on a rough incline at angle \(\theta\).
Its weight splits into \(mg\cos\theta\) (normal) and \(mg\sin\theta\) (down-slope).
In the static region, friction \(f_s\) equals the applied force, giving a straight 45° line.
At \((f_s)_{\text{max}}\) the object slips; friction drops to the lower, nearly constant kinetic value \(f_k\).
A 5 kg box stays at rest when a 12 N horizontal force pushes it. Which statement is true?
Since the box is at rest, think about static friction matching the applied force up to its limit.
Static friction balances the 12 N push while the box remains still, so its value is 12 N opposite the applied force.
Because the box is not moving, kinetic friction cannot act. Static friction must equal the 12 N push to keep it at rest.
Friction is a parallel contact force opposing imminent or actual sliding.
Magnitude \(F = \mu N\); μ reflects material pair, surface finish, temperature, and contaminants.
Static friction rises to \( (\!f_s)_{\max} = \mu_s N\); once moving, \(f_k = \mu_k N\) stays lower.
Curve climbs linearly, peaks, then drops abruptly to a nearly constant kinetic level.
Lubricants, bearings, brakes, and tyre treads let engineers reduce or exploit friction as needed.