Academy

Kinetic Friction

Friction force on a body already in motion. Always less than limiting friction.
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Derivation

What kinetic friction is

Once a body begins to slide on a surface, the friction force changes character. It is no longer self-adjusting — it becomes a fixed value:

fk=μkNf_k = \mu_k N

This is kinetic friction (also called sliding friction or dynamic friction). It acts on a body that is already moving relative to the surface.

Key properties

It is constant — unlike static friction which adjusts, kinetic friction has a fixed value μkN\mu_k N regardless of the applied force. Whether you push harder or softer, fkf_k stays the same (as long as the body keeps sliding).

It is less than limiting friction — always:

μk<μs\mu_k < \mu_s

This means it takes more force to start sliding than to keep sliding. Once you overcome static friction and get the body moving, less force is needed to maintain motion.

It opposes relative motion — kinetic friction always acts opposite to the direction of sliding. It acts on each surface in the direction that opposes its motion relative to the other surface.

It is independent of speed — to a good approximation, fkf_k does not depend on how fast the surfaces slide past each other. (At very high speeds this breaks down, but for typical problems it holds.)

It is independent of contact area — same as static friction.

Kinetic friction and deceleration

When kinetic friction is the only horizontal force acting on a sliding body:

Fnet=fk=μkN=μkmgF_{net} = -f_k = -\mu_k N = -\mu_k mg

a=μkga = -\mu_k g

The body decelerates at μkg\mu_k g until it stops (or until the applied force changes the situation).

Example: A block slides on a floor with μk=0.4\mu_k = 0.4. Deceleration:

a=μkg=0.4×10=4 m/s2a = -\mu_k g = -0.4 \times 10 = -4 \text{ m/s}^2

The friction vs applied force graph

A clear picture of how friction changes with applied force:

  • From F=0F = 0 to F=μsNF = \mu_s N: friction =F= F (static, self-adjusting, linear increase)
  • At F=μsNF = \mu_s N: friction =μsN= \mu_s N (limiting — peak of graph)
  • For F>μsNF > \mu_s N: friction drops to μkN\mu_k N and stays constant (kinetic)

The drop from μsN\mu_s N to μkN\mu_k N at the onset of motion is a real, observable effect.

Heat generation

Kinetic friction converts kinetic energy into heat. The rate of heat generation:

P=fkv=μkNvP = f_k \cdot v = \mu_k N v

where vv is the sliding speed. This is why brakes get hot, why your hands warm up when rubbed together, and why meteors glow as they enter the atmosphere.

Note
In problems, once you establish that a body is moving (applied force exceeded limiting friction), switch from $\mu_s$ to $\mu_k$ for the friction force. Using $\mu_s$ for a moving body is a common error.