Audited 05 Aug 2026·Last updated 28 Oct 2026·3 citations·Tier 2·0 uses

Particles Velocity Calculator

Find how fast gas molecules move: most probable, mean and root-mean-square Maxwell–Boltzmann speeds in m/s from absolute temperature and molar mass.

Particles Velocity Calculator

K
g/mol
Root-mean-square molecular speed
516.8392
Root-mean-square molecular speed, √(3RT/M), in metres per second: the speed linked directly to the gas's average kinetic energy.
Mean molecular speed
476.1731m/s
Most probable molecular speed
421.9974m/s

Background.

The air in a quiet room is anything but still. At room temperature its nitrogen molecules travel at roughly 500 metres per second — faster than a cruising airliner and faster than sound — and they collide with one another billions of times a second, so no molecule keeps one speed or direction for long. What stays fixed, for a gas held at a steady temperature, is the spread of speeds across the whole population: the Maxwell–Boltzmann distribution.

That distribution has no single speed, so it is summarised three ways. The most probable speed is the peak of the curve, the speed more molecules have than any other. The mean speed is the ordinary average. The root-mean-square speed is the square root of the average squared speed, and it is the one tied directly to kinetic energy and therefore to temperature and pressure. Because the curve has a long tail of fast molecules, the three always come in the same order and ratio: the mean is about 1.128 times the most probable speed, and the rms about 1.225 times.

All three depend on just two things, absolute temperature and molar mass. Speed grows with the square root of temperature, so doubling the kelvin temperature makes molecules about 41% faster. It falls with the square root of molar mass, which is why light gases are so quick: helium at 300 K has an rms speed of about 1,367 m/s, more than two and a half times nitrogen's. That difference is one reason a helium balloon goes soft sooner than one blown up with air.

The figures describe an ideal gas in equilibrium — a vast population of molecules, not any single one of them, and not a directed beam or a plasma out of balance.

What is particles velocity calculator?

Molecular speed here means three statistical measures of how fast the molecules of an ideal gas move at a given temperature: the most probable speed, √(2RT/M); the mean speed, √(8RT/πM); and the root-mean-square speed, √(3RT/M). Each is in metres per second and summarises the whole population of molecules in a gas at equilibrium, whose individual speeds range widely above and below these values.

How to use this calculator.

  1. Enter Absolute temperature in kelvin. Add 273.15 to a Celsius reading: 0 °C is 273.15 K and 27 °C is 300.15 K.
  2. Enter Molar mass in grams per mole. Nitrogen (N₂) is 28.0134, oxygen (O₂) about 32.00, helium 4.0026 and carbon dioxide about 44.01.
  3. For air, entering its average molar mass of about 28.97 g/mol gives a representative figure, but each gas in a mixture has its own distribution, and oxygen molecules run slightly slower than nitrogen ones.
  4. Use the rms speed for anything involving energy or pressure, the mean speed for collision and effusion rates, and the most probable speed to locate the peak of the distribution.

The formula.

vmp=√(2RT/M), vmean=√(8RT/πM), vrms=√(3RT/M)

All three speeds share the form √(c × R × T ÷ M), with c = 2 for the most probable speed, 8/π for the mean and 3 for the root-mean-square. R is the molar gas constant, 8.31446261815324 J/(mol·K), exact since the 2019 redefinition of the SI; T is the temperature in kelvin; M is the molar mass in kilograms per mole, which is why the g/mol figure you enter is divided by 1,000. The rms form comes from setting the average kinetic energy per mole, ½Mv²rms, equal to (3/2)RT. Because each c is fixed, the ratios between the three never change: 1 : 1.128 : 1.225. Temperature and molar mass enter only as the ratio T/M, so quadrupling the temperature has the same effect as switching to a gas one quarter as heavy: both double every speed.

A worked example.

Example

Take nitrogen at 300 K, about 27 °C, with a molar mass of 28.0134 g/mol, or 0.0280134 kg/mol. First, RT = 8.31446261815324 × 300 = 2,494.34 J/mol. For the rms speed, 3RT = 7,483.02; dividing by 0.0280134 gives 267,122.7 m²/s², whose square root is 516.8392 m/s, about 1,861 km/h. The mean speed uses 8RT/πM = 226,740.8, giving 476.1731 m/s, and the most probable speed uses 2RT/M = 178,081.8, giving 421.9974 m/s. Heat the same nitrogen to 600 K and every speed rises by a factor of √2, taking the rms speed to 730.92 m/s. Swap in helium at 4.0026 g/mol and keep 300 K, and the rms speed is 1,367.31 m/s.

molar Mass28.013
temperature300

Frequently asked questions.

How can molecules move faster than sound when sound travels through the gas?
Sound is a pressure wave handed from molecule to molecule by collisions, so it travels at a speed set by the same motion but somewhat below it. For nitrogen at 300 K the speed of sound, √(γRT/M) with γ = 1.4, is about 353 m/s, against an rms molecular speed of 516.84 m/s.
Why do light gases such as helium and hydrogen move so much faster?
At the same temperature every gas has the same average kinetic energy per molecule, so a lighter molecule must move faster to carry it. Speed scales with one over the square root of molar mass: helium, at about a seventh of nitrogen's mass, moves about 2.65 times as fast.
Does compressing the gas change how fast its molecules move?
Not for an ideal gas at a fixed temperature. Squeezing it raises the number of molecules per cubic metre, so they collide more often and push harder on the walls, but their speed distribution depends only on temperature and molar mass. Compression changes speeds only through any heating it causes.
What share of the molecules move faster than these speeds?
Integrating the Maxwell–Boltzmann curve gives about 57% of molecules faster than the most probable speed, about 47% faster than the mean, and about 39% faster than the rms speed. Only about 4.6% exceed twice the most probable speed, but that fast tail drives evaporation and many chemical reactions.
What happens to these speeds near absolute zero?
The formulas send every speed towards zero as temperature falls, but real gases condense into liquids or solids long before that, and at very low temperatures quantum effects replace the classical distribution. The results are reliable for gases well above their boiling points and at ordinary pressures.

How this page was produced

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Quanta Calculator
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Method
vmp=√(2RT/M), vmean=√(8RT/πM), vrms=√(3RT/M)
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