Friction

Friction resists sliding between surfaces. Learn static and kinetic friction, the coefficient of friction, angle of friction, inclined planes, belt and rope friction, and where engineers want more or less friction.

Without friction you couldn't walk, drive, hold a tool or keep a bolt tight. With too much, machines waste energy and wear out. Engineers constantly design for the right amount: high in brakes and clutches, low in bearings and slides.

The Coulomb friction model — friction force proportional to the normal force — is simple and remarkably useful for everyday design calculations.

An analogy

Microscopically, surfaces are like two brushes pressed together: their bristles (asperities) interlock. Press harder (more normal force) and they interlock more, so it's harder to slide.

Static vs kinetic

Up to a limit, static friction matches whatever force tries to slide the object, so it stays put. Once the applied force exceeds μ_s·N, sliding starts and friction drops to the kinetic value μ_k·N. That's why it's harder to start pushing a heavy box than to keep it moving.

Typical coefficients

Steel on steel (dry) ≈ 0.6–0.8; lubricated ≈ 0.05–0.15; rubber on dry asphalt ≈ 0.7–1.0; wet ≈ 0.4–0.6; PTFE on steel ≈ 0.04. Values vary with surface finish, temperature and contamination, so designs use conservative ranges.

Inclined planes

On a slope of angle θ, weight splits into mg sin θ down the slope and mg cos θ into it. The block slides if tan θ > μ_s. Screws and wedges are inclined planes wrapped or stacked, which is why they can be self-locking.

Belt and rope friction

Friction around a curved surface grows exponentially with wrap angle: T₁/T₂ = e^{μθ}. A few turns of rope on a bollard let a person hold a ship. Belt drives use this to transmit torque; slipping occurs when the ratio exceeds e^{μθ}.

Beyond Coulomb

Real friction depends on sliding speed (Stribeck curve: boundary, mixed and hydrodynamic lubrication), temperature and time (stick-slip causes squeals and chatter). Rolling resistance, tyre slip curves and tribology — the science of friction, wear and lubrication — refine the simple model.

Formulas

Worked example: Force to start a crate moving

Given: m = 50 kg; μ_s = 0.4, μ_k = 0.3

Find: Force to start sliding and to keep it sliding.

Answer: 196 N to start, 147 N to keep moving

Worked example: Block on an incline

Given: m = 20 kg on 30° slope; μ = 0.25

Find: Does it slide? Acceleration?

Answer: Slides at 2.78 m/s²

Common mistakes

Applications

Key takeaways

Going further