Knudsen Number Calculator

Enter gas temperature, pressure, and molecular diameter to compute the mean free path, then compare it with a characteristic length to get the Knudsen number (Kn = λ/L) and its flow regime.

Quick Facts

Definition
Kn = λ / L
Ratio of the gas molecules' mean free path to the flow's characteristic length.
Mean free path
λ = kB·T / (√2·π·d²·P)
From kinetic theory of gases; kB = 1.380649×10⁻²³ J/K.
Flow regimes
Kn<0.01 continuum · 0.01-0.1 slip · 0.1-10 transition · >10 free-molecular
Standard classification used in rarefied gas dynamics.
Typical case
Air at 20°C, 1 atm
Mean free path ≈ 66-68 nm — matters once L shrinks below a few microns.

Your Results

Calculated
Mean Free Path (λ)
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Average distance between molecular collisions
Knudsen Number (Kn)
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Kn = λ / L (dimensionless)
Flow Regime
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Based on standard Kn thresholds
Modeling Guidance
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Recommended governing equations

Ready

Enter gas conditions and a characteristic length, then press Calculate.

Formula and Method for the Knudsen Number

The Knudsen number is a dimensionless quantity used in fluid mechanics and rarefied gas dynamics to determine whether a gas can be treated as a continuum or must be modeled molecule by molecule. It is defined as Kn = λ / L, where λ (lambda) is the mean free path of the gas molecules — the average distance a molecule travels between collisions — and L is a characteristic length scale of the flow, such as a pipe diameter, a gap width, or a particle size. This calculator first computes λ from kinetic theory, then divides it by your chosen L to get Kn and reports the resulting flow regime.

How the calculation works

From the kinetic theory of gases, the mean free path of a molecule in an ideal gas is λ = kB·T / (√2·π·d²·P), where kB is the Boltzmann constant (1.380649×10⁻²³ J/K), T is the absolute temperature, d is the effective collision diameter of the gas molecule, and P is the pressure. The √2 factor accounts for the relative motion of all the gas molecules, not just one molecule moving through stationary neighbors. Once λ is known, the Knudsen number follows directly from Kn = λ / L. Because λ shrinks as pressure or molecular size increases and grows as temperature increases, Kn is highly sensitive to operating conditions — the same geometry can be continuum flow at atmospheric pressure and free-molecular flow inside a vacuum chamber.

Common mistakes

  • Mixing temperature scales: the mean free path formula needs an absolute temperature (Kelvin) — plugging in Celsius or Fahrenheit directly gives a wrong, sometimes negative, result. This calculator converts for you, but hand calculations must convert first.
  • Wrong characteristic length: L should represent the smallest relevant flow dimension — a channel height, a pore diameter, a particle radius — not an unrelated large-scale dimension, which would make Kn artificially small and hide real rarefaction effects.
  • Guessing the molecular diameter: effective collision diameters vary by gas (about 0.37 nm for air/N₂, 0.36 nm for O₂, 0.26 nm for He) — using the wrong value can shift the mean free path, and therefore Kn, by 30% or more.

Flow regimes and when they apply

  • Kn < 0.01 — Continuum flow: the Navier–Stokes equations with standard no-slip boundary conditions are accurate. This covers most everyday aerodynamics and pipe flow.
  • 0.01 ≤ Kn < 0.1 — Slip flow: Navier–Stokes still applies, but boundary conditions need velocity-slip and temperature-jump corrections. Common in microfluidic channels and MEMS devices.
  • 0.1 ≤ Kn < 10 — Transition flow: continuum equations break down; models need the Burnett equations or particle-based methods such as direct simulation Monte Carlo (DSMC).
  • Kn ≥ 10 — Free-molecular flow: molecule–surface collisions dominate over molecule–molecule collisions; this regime governs high-vacuum systems and spacecraft in low Earth orbit or the upper atmosphere.

Frequently Asked Questions

What is the Knudsen number used for?
The Knudsen number tells you whether a gas flow can be treated as a continuous fluid or must be modeled as individual molecules. It is essential in vacuum system design, microfluidics, MEMS devices, aerosol science, and high-altitude or rarefied aerodynamics, where the flow passage can become comparable to or smaller than the distance molecules travel between collisions.
How do I find the mean free path of a gas?
Use the kinetic theory formula λ = kB·T / (√2·π·d²·P), with temperature in Kelvin, pressure in pascals, and the molecular collision diameter in meters. For air at 20°C (293.15 K) and 1 atm (101,325 Pa) with d ≈ 0.37 nm, this gives a mean free path of about 66-68 nanometers.
What Knudsen number counts as continuum flow?
By convention, Kn below 0.01 is continuum flow, where the Navier-Stokes equations with no-slip walls hold. Between 0.01 and 0.1 is slip flow, 0.1 to 10 is transition flow, and above 10 is free-molecular flow, each needing a different modeling approach.
Does pressure or temperature matter more for the Knudsen number?
Pressure usually dominates: mean free path is inversely proportional to pressure, so dropping from 1 atm to a rough vacuum increases the mean free path (and Kn) by the same large factor. Temperature enters only to the first power, so pressure changes are almost always the bigger lever.