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Static Friction

Static friction adjusts up to a maximum to prevent relative motion.
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Derivation

What static friction is

Static friction is the force that prevents two surfaces in contact from sliding relative to each other.

It is a self-adjusting force — it takes whatever value is needed to prevent sliding, up to a maximum limit.

fsμsNf_s \leq \mu_s N

where μs\mu_s is the coefficient of static friction and NN is the normal force between the surfaces.

The self-adjusting nature

This is what makes static friction different from kinetic friction.

Push a heavy box with a small force. The box does not move. Static friction exactly equals your push — it adjusts to match. Push harder. The box still does not move. Friction increases to match your push again.

Push hard enough, and the box finally moves. At that point, static friction has reached its maximum value μsN\mu_s N — called limiting friction — and can no longer increase to prevent sliding.

Where the friction force comes from

At the microscopic level, surfaces are not perfectly smooth. Even surfaces that appear smooth have microscopic asperities — tiny bumps and valleys. When two surfaces are in contact, these asperities interlock.

Static friction arises from:

  • Mechanical interlocking of surface asperities
  • Adhesive forces (molecular attraction) between surface atoms in contact

The normal force NN pushes the surfaces together harder, increasing the real area of contact and thus the total interlocking and adhesion — which is why friction is proportional to NN.

What μs\mu_s depends on

The coefficient of static friction μs\mu_s depends on:

  • The materials of the two surfaces in contact
  • The surface condition (dry, wet, lubricated, rough, polished)

It does not depend on:

  • The area of contact (a surprising result — a large block and a small block of the same material have the same μs\mu_s)
  • The magnitude of the normal force
Surface pairμs\mu_s (approximate)
Rubber on dry concrete0.6 – 0.8
Steel on steel (dry)0.5 – 0.8
Wood on wood0.25 – 0.5
Ice on ice0.03 – 0.1
Teflon on Teflon0.04

Direction of static friction

Static friction acts opposite to the direction of impending motion — the direction the body would move if friction were removed.

It is not always opposite to the applied force. If a force is applied at an angle, the impending motion might be in a different direction, and friction opposes that direction.

Static friction and equilibrium

For a body in static equilibrium on a rough surface:

fs=Fapplied(if body does not move)f_s = F_{applied} \quad \text{(if body does not move)}

The static friction force equals whatever is needed for equilibrium — it is found from the equilibrium condition, not from μsN\mu_s N.

μsN\mu_s N only gives the maximum value. The actual value of static friction is determined by the equilibrium equations.

Note
$f_s \leq \mu_s N$ is an inequality. The friction force is somewhere between 0 and $\mu_s N$. Its exact value comes from the condition that the body is in equilibrium ($\sum F = 0$). Only when the body is on the verge of sliding does $f_s = \mu_s N$.