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Coefficient of Kinetic Friction Formula

Force and laws of motion formulasDimensionlessClass 11Updated 1 Nov 2026

μk=fkN\mu_k = \frac{f_k}{N}
SI unit
no unit (dimensionless)
Dimensions
[M⁰ L⁰ T⁰]
where
  • μk coefficient of kinetic (sliding) friction
  • fk kinetic friction force N
  • N normal force N

The coefficient of kinetic friction formula is μk=fkN\mu_k = \frac{f_k}{N}: divide the friction force on a sliding object by the normal force between the surfaces. A 25 kg box dragged across a floor at steady speed by a 70 N horizontal rope has μk=70245≈0.29\mu_k = \frac{70}{245} \approx 0.29.

Kinetic friction, also called sliding or dynamic friction, acts only once surfaces are moving relative to each other. Its coefficient is usually a bit lower than the static one for the same pair, which is why it is easier to keep a heavy box moving than to start it. This page shows three ways to find μk, all built on the friction force formula and the laws of motion.

Quick facts

  • Formula

    μk=fkN\mu_k = \frac{f_k}{N}
  • From braking on level ground

    μk=ag\mu_k = \frac{a}{g}
  • Steady slide down a slope

    μk=tan⁡θ\mu_k = \tan\theta
  • Accelerating down a slope

    μk=tan⁡θ−agcos⁡θ\mu_k = \tan\theta - \frac{a}{g\cos\theta}
  • Unit

    None
  • Compared with static

    Usually μk<μs\mu_k < \mu_s

Kinetic coefficient of friction formula and its parts

Terms in μk = fk / N
SymbolMeaningUnit
μk\mu_kCoefficient of kinetic frictionnone
fkf_kFriction while slidingN
NNPerpendicular contact forceN

Once sliding starts, fk=μkNf_k = \mu_k N stays roughly constant for ordinary speeds. That makes kinetic friction easy to handle: it is a fixed backward force, so the acceleration it causes is constant and the equations of motion apply.

Three ways to apply the coefficient of kinetic friction formula

  1. Steady pull. Drag the object at constant velocity. The pull then equals friction, so μk=FpullN\mu_k = \frac{F_{\text{pull}}}{N}.
  2. Sliding to a stop. Give the object a push on a level surface and let it slide. Friction is the only horizontal force, so μkmg=ma\mu_k mg = ma and μk=ag\mu_k = \frac{a}{g}. Find a from v2=u2−2asv^2 = u^2 - 2as.
  3. Incline. Tilt a ramp until a nudged block slides down at constant speed. Then mgsin⁡θ=μkmgcos⁡θmg\sin\theta = \mu_k mg\cos\theta, so μk=tan⁡θ\mu_k = \tan\theta. If the block speeds up with acceleration a, use μk=tan⁡θ−agcos⁡θ\mu_k = \tan\theta - \frac{a}{g\cos\theta}.

Worked examples for the formula for coefficient of kinetic friction

Example 1: steady drag

A 25 kg box is dragged steadily over a level floor by a 70 N horizontal force. Find μk (g = 9.8 m/s²).

N = 25 × 9.8 = 245 N. At constant speed, fk = 70 N.

μk=70245=0.286≈0.29\mu_k = \frac{70}{245} = 0.286 \approx 0.29

Example 2: a puck sliding to rest

An ice hockey puck leaves a stick at 6.0 m/s and slides 30 m before stopping. Find μk.

Deceleration: a=u22s=6.022×30=3660=0.60 m/s2a = \frac{u^2}{2s} = \frac{6.0^2}{2 \times 30} = \frac{36}{60} = 0.60\ \text{m/s}^2.

μk=ag=0.609.8=0.061\mu_k = \frac{a}{g} = \frac{0.60}{9.8} = 0.061

The mass of the puck is not needed, because it cancels.

Example 3: a block speeding up on a 35° ramp

A block slides down a 35° ramp with an acceleration of 3.0 m/s². Find μk.

tan⁡35∘=0.700\tan 35^\circ = 0.700 and gcos⁡35∘=9.8×0.819=8.03 m/s2g\cos 35^\circ = 9.8 \times 0.819 = 8.03\ \text{m/s}^2.

μk=0.700−3.08.03=0.700−0.374=0.326≈0.33\mu_k = 0.700 - \frac{3.0}{8.03} = 0.700 - 0.374 = 0.326 \approx 0.33

Why kinetic friction is usually smaller

At the microscopic level, surfaces touch only at tiny high points. When they sit still, those contact points settle and bond more firmly. Once sliding, they break and remake contact constantly and never get as firm a hold. The result is that, for most pairs, μk\mu_k is noticeably smaller than μs\mu_s, though the size of the gap depends on the materials. The coefficient of static friction formula page covers the gripping case, and the general coefficient of friction formula page compares both.

Energy view of sliding friction

The work done by kinetic friction over a sliding distance d is W=−μkNdW = -\mu_k N d. On level ground with no other horizontal force, all the starting kinetic energy is used up: 12mu2=μkmgd\frac{1}{2}mu^2 = \mu_k mg d, so d=u22μkgd = \frac{u^2}{2\mu_k g}. Check with Example 2: 362×0.061×9.8≈30 m\frac{36}{2 \times 0.061 \times 9.8} \approx 30\ \text{m}. The work done by friction page develops this method.

Mistakes with μk

  • Using an accelerating pull as if it equalled friction. Only a constant velocity pull does.
  • Forgetting that N = mg cos θ on a slope.
  • Quoting μk with a unit.
  • Swapping μk and μs, so the moving case seems to have more grip.
If μk comes out negative on an incline, the block must be accelerating faster than a frictionless slope allows. Recheck the angle or the acceleration.

Frequently asked questions

What is the formula for coefficient of kinetic friction?

μk = fk / N: sliding friction over the normal reaction. On level ground with only friction slowing an object, it also equals a / g.

Does the coefficient of kinetic friction have a unit?

No. Newtons on top and newtons underneath cancel, leaving a pure number.

Is μk always less than μs?

For nearly all ordinary pairs of surfaces, yes. A few special materials have the two nearly equal, but μk is never meant to exceed μs in school problems.

Does kinetic friction depend on speed?

For dry surfaces at everyday speeds it is nearly constant, which is the assumption used in exams. At very high speeds or with lubricants it can change.