Audited 31 Jul 2026·Last updated 28 Oct 2026·3 citations·Tier 2·0 uses

Root Mean Square Speed Calculator for Ideal Gas

Root-mean-square speed of ideal-gas molecules, √(3RT/M), from absolute temperature in kelvin and molar mass in kg/mol, with the result in metres per second.

Root Mean Square Speed Calculator for Ideal Gas

K
kg/mol
Root-mean-square molecular speed
516.8392
The square root of the mean squared molecular speed, in metres per second, for a single ideal gas at the temperature entered.
Model scope
Classical ideal-gas Maxwell distribution; nonideal interactions, mixtures, quantum statistics, relativistic speeds, and temperature distributions are outside it.

Background.

Temperature in a gas is molecular motion. In the air of a room at about 27 °C, nitrogen molecules are flying in random directions at around 500 metres per second, faster than sound travels through that same air. No single speed describes them all: the Maxwell–Boltzmann distribution spreads them over a wide range, from almost at rest to more than double the typical value, with most somewhere in between.

The root-mean-square speed is the summary that connects directly to temperature. Square every molecule's speed, average the squares and take the square root. A molecule moving at that speed carries exactly the average translational kinetic energy of the gas, (3/2)kT, so kinetic theory can turn it into a clean formula: v_rms = √(3RT/M).

Two patterns follow. Speed grows only with the square root of absolute temperature, so doubling the kelvin temperature makes the molecules about 41% faster, not twice as fast. And at a given temperature lighter molecules move faster, in proportion to 1/√M. At 300 K hydrogen's rms speed is about 1,927 m/s, about 3.7 times nitrogen's 517 m/s. The same dependence lies behind Graham's law of effusion and is one reason hydrogen and helium leak from the top of Earth's atmosphere into space.

The rms speed is not the most likely speed of a molecule. For any ideal gas the most probable speed, the mean speed and the rms speed stand in the ratio √2 : √(8/π) : √3, about 1.414 : 1.596 : 1.732, so rms is the largest of the three.

The model is the classical ideal gas, a single species of point-like molecules that interact only by colliding. Dense or strongly interacting gases, mixtures and very cold quantum gases need more than this.

What is root mean square speed calculator for ideal gas?

The root-mean-square speed of a gas is the square root of the average of the squared speeds of its molecules. For an ideal gas in thermal equilibrium it depends only on the absolute temperature and the molar mass. It is the speed at which a molecule would carry the gas's average translational kinetic energy of (3/2)kT, which is why it, rather than the simple mean speed, appears in kinetic theory. It is reported in metres per second.

How to use this calculator.

  1. Enter the temperature in kelvin. Add 273.15 to a Celsius reading: 25 °C is 298.15 K.
  2. Enter the molar mass in kilograms per mole, which is the g/mol figure divided by 1,000. Nitrogen's 28.0134 g/mol becomes 0.0280134 kg/mol.
  3. Use one gas at a time. In a mixture every component has its own rms speed at the same temperature, so run each separately.
  4. Read the rms speed in m/s. Multiply it by 0.921 for the mean speed or by 0.816 for the most probable speed of the same gas.

The formula.

v_rms = sqrt(3RT / M)

v_rms = √(3RT ÷ M), where T is the absolute temperature in kelvin, M the molar mass in kg/mol and R the molar gas constant, 8.31446261815324 J/(mol·K). R is exact in the SI, the product of the fixed Boltzmann and Avogadro constants. Per molecule the same result reads √(3kT ÷ m). It comes from kinetic theory: the pressure of molecules bouncing off a wall is P = ⅓ × (N/V) × m × ⟨v²⟩, and setting that equal to the ideal-gas law PV = NkT gives ⟨v²⟩ = 3kT ÷ m. Since a joule is a kg·m²/s², RT ÷ M comes out in m²/s² only when M is in kilograms per mole. Temperature and molar mass both sit under the square root, so quadrupling T or quartering M doubles the speed.

A worked example.

Example

Take nitrogen, N₂, with a molar mass of 0.0280134 kg/mol, at 300 K. First the numerator: 3 × 8.31446 J/(mol·K) × 300 K = 7,483.02 J/mol. Dividing by the molar mass, 7,483.02 ÷ 0.0280134 = 267,122.7 m²/s², the mean of the squared speeds. Its square root is 516.839 m/s, the root-mean-square speed. The other averages of the same distribution are lower: the mean speed is about 476.2 m/s and the most probable speed about 422.0 m/s. Heating the gas to 600 K raises the rms speed to 730.9 m/s, a factor of √2 rather than 2. Oxygen at 300 K, slightly heavier at 0.031998 kg/mol, comes out a little slower at 483.6 m/s.

molar Mass Kg Per Mol0.028
absolute Temperature K300

Frequently asked questions.

Why are the molecules faster than the speed of sound in the same gas?
Sound is passed along by molecular collisions, but molecules move in random directions, so the wave advances more slowly than they do. For an ideal gas the sound speed is √(γRT/M), with γ = 1.4 for nitrogen, which is √(1.4/3) of the rms speed: about 353 m/s at 300 K against 516.8 m/s.
Why use the root-mean-square speed instead of the ordinary average?
Because temperature measures kinetic energy, and kinetic energy goes with the square of speed. Averaging the squared speeds ties the result directly to (3/2)kT. The plain mean speed, √(8RT/πM), is about 7.9% lower, roughly 476 m/s for nitrogen at 300 K.
My answer for nitrogen came out around 16 m/s. What went wrong?
The molar mass was almost certainly entered in grams per mole, as 28.0134, instead of 0.0280134 kg/mol. That makes M a thousand times too large and the speed √1,000 ≈ 31.6 times too small: 16.3 m/s instead of 516.8 m/s.
Does squeezing a gas to a higher pressure change the rms speed?
Not for an ideal gas held at the same temperature. Pressure does not appear in √(3RT/M); compressing the gas packs the molecules closer so they collide with the walls and with each other more often, but at the same speeds. Only temperature and molar mass move the result.
How small is the speed difference between two isotopes?
Tiny, because speed goes as 1/√M. Uranium hexafluoride made with uranium-235 has a molar mass of about 349.03 g/mol, against about 352.04 g/mol with uranium-238. Their rms speeds differ by a factor of √(352.04/349.03) ≈ 1.0043, which is why gaseous-diffusion enrichment needed long cascades of stages.
When does the ideal-gas answer stop being reliable?
At high pressures or close to condensation, where molecular attractions and size matter; for light gases such as helium at a few kelvin, where quantum effects take over; and at speeds approaching that of light. The formula will still produce a number in those regimes, but it no longer describes the gas.

How this page was produced

Published by
Quanta Calculator
Primary sources
3 cited below
Method
v_rms = sqrt(3RT / M)
Published
Last verified

Built with AI assistance and verified by automated tests against the cited sources — every worked example on this page is computed by the same code that runs the calculator. How we build and check calculators.

In this category

Embed

Quanta Pro

Paid features are coming later.

  • All 1560 calculators remain free
  • No billing is enabled
Coming soon