Reduced Mass Calculator

Turn a two-body problem into a one-body problem: reduced mass, the missing mass, the orbital period and the hydrogen atom correction.

⚛️ Reduced Mass Calculator
Massespick the unit, then type both masses
Mass unit
Mass 1
 
Mass 2
Known reduced mass and one bodymu must be smaller than the known mass
Mass unit
Reduced mass mu
 
Known mass m1
Masses of the two bodies
Mass unit
Mass 1
 
Mass 2
Separation (semi-major axis)
Distance unit
Separation a
Nucleuselectron orbiting a nucleus of mass M
Preset
Nuclear mass M (electron masses)
 
Nuclear charge Z
Reduced mass mu
—
mu in kilograms
—
Total mass
—
mu compared with the lighter body
—
Center of mass position
—

Missing mass m2
—
Total mass
—
Ratio m2 / m1
—
m2 in kilograms
—

How mu depends on the mass ratio. When one body is 100 times heavier, mu is within 1 percent of the lighter mass.

Orbital period
—
Period in seconds
—
Reduced mass
—
Total mass
—
Relative circular speed
—
Orbital energy
—
Mass 1 from the center of mass
—
Mass 2 from the center of mass
—

Reduced mass mu
—
mu in kilograms
—
Rydberg constant RM
—
Ionization energy
—
H-alpha (3 to 2) wavelength, vacuum
—
Same line, infinite nuclear mass
—
Shift caused by finite mass
—

The same calculation for five systems. Z is 2 for He+, and all other rows use Z = 1.

⚛️ What is Reduced Mass?

The reduced mass of two bodies is the effective inertial mass that appears when their relative motion is treated as the motion of a single particle: μ = m1 m2 / (m1 + m2). When two bodies attract each other, both move around their common center of mass. The two-body problem looks hard, but the relative position r = r1 − r2 obeys the equation of a single body of mass μ moving in the same force field, while the center of mass simply moves at constant velocity. That simplification, described in the Wikipedia article on reduced mass, is why the quantity appears all over physics and chemistry.

Typical uses cover very different scales. In astronomy, a binary star or a planet and its moon both orbit their shared barycenter, and the reduced mass sets the energy and angular momentum of the relative orbit. In molecular spectroscopy, a diatomic molecule vibrates as if it were one particle of mass μ on a spring, so the vibrational frequency is ω = √(k / μ) and isotope substitution shifts the lines. In atomic physics, the hydrogen atom is a two-body problem whose Bohr energy levels scale with the reduced mass of the electron and proton, which is why deuterium and hydrogen have slightly different spectra. In collisions, the kinetic energy in the center of mass frame is half of μ times the relative speed squared.

A few properties are worth remembering. The reduced mass is always smaller than the lighter of the two bodies, and for a large mass ratio it is almost equal to the lighter body. For equal masses it is exactly half of either one. It is symmetric, so swapping m1 and m2 changes nothing. It is not the quantity that sets gravity: the force still uses both real masses, and the orbital period depends on the total mass m1 + m2. Mixing up the reduced mass and the total mass is the most common error, along with entering the two masses in different units.

This calculator covers four jobs. Reduced mass gives μ and the center of mass position with a chart of μ against the second mass. Missing mass reverses the formula. Orbit gives the period, speed, orbital energy and each body's distance from the center of mass. Hydrogen-like atom gives μ, the Rydberg constant, the ionization energy and the H-alpha line for hydrogen, deuterium, tritium, He+ and positronium. For the underlying gravity see the gravitational force calculator, for orbits around one dominant mass the orbital period and velocity calculator, and for the hydrogen levels the hydrogen atom energy levels calculator.

📐 Formula

μ  =  m1 m2 ÷ (m1 + m2)    T  =  2π √(a³ ÷ (G M))
m1, m2 = the two masses, in any one unit. M = m1 + m2 = total mass. μ comes out in the same unit.
Missing mass: m2 = μ m1 ÷ (m1 − μ), valid only for μ < m1.
Center of mass: it lies m2 / M of the separation from body 1. Body 1 orbits at a m2 / M and body 2 at a m1 / M from it.
Orbit: a = separation (semi-major axis of the relative orbit), G = 6.67430 × 10−11 m³ kg−1 s−2. Relative circular speed v = √(G M / a), orbital energy E = −G m1 m2 / (2a) = −G M μ / (2a).
Atom: μ / me = M / (M + 1) with M in electron masses. RM = R∞ μ / me, with R∞ = 10973731.568 m−1. Ionization energy = Z² × 13.6057 eV × μ / me. H-alpha vacuum wavelength: 1 / λ = RM Z² (1/4 − 1/9).
Example: 1 and 0.5 solar masses give μ = 0.5 ÷ 1.5 = 0.3333 solar masses.

📖 How to Use This Calculator

Steps

1
Choose a mode. Pick Reduced mass for μ, Missing mass to find a body, Orbit for a binary period, or Hydrogen-like atom for an electron and a nucleus.
2
Choose the unit first. Select the mass unit before typing, so both masses are read in the same unit. Changing the unit afterwards never rewrites the numbers you typed.
3
Enter the values. Type the two masses, or μ with one mass, or the masses with the separation, or choose a nucleus preset.
4
Read the result. The results show μ, the total mass, the center of mass position, the period or the spectral line, with a chart of μ against m2 or of period against separation.

💡 Example Calculations

Example 1 — A Binary Star

Two stars of 1 and 0.5 solar masses

1
Total mass M = 1 + 0.5 = 1.5 solar masses.
2
μ = (1 × 0.5) ÷ 1.5 = 0.3333333 solar masses, which is 6.62823 × 1029 kg.
3
μ is 66.67% of the lighter star, and the center of mass is 33.33% of the way from the heavier star.
μ = 0.3333333 solar masses
Try this example →

Example 2 — A Carbon Monoxide Molecule

Carbon-12 at 12 u and oxygen-16 at 15.995 u

1
Total mass = 12 + 15.995 = 27.995 u.
2
μ = (12 × 15.995) ÷ 27.995 = 6.856224 u, or 1.13850 × 10−26 kg.
3
This is 57.1352% of the carbon mass, the lighter atom, and it is the effective mass in the molecule's vibration.
μ = 6.856224 u
Try this example →

Example 3 — The Hydrogen Atom

An electron (1 electron mass) and a proton (1836.15267343 electron masses)

1
Total mass = 1 + 1836.15267343 = 1837.153 electron masses.
2
μ = 1836.15267343 ÷ 1837.15267343 = 0.9994557 electron masses = 9.10443 × 10−31 kg.
3
So μ is 99.9456% of the electron mass, about 0.054 percent less, and the center of mass sits almost on the proton.
μ = 0.9994557 electron masses
Try this example →

Example 4 — Finding a Missing Mass

A system with a reduced mass of 0.3 solar masses containing a 1 solar mass star

1
m2 = μ m1 ÷ (m1 − μ) = 0.3 × 1 ÷ (1 − 0.3).
2
m2 = 0.3 ÷ 0.7 = 0.4285714 solar masses, or 8.52201 × 1029 kg.
3
The total mass is 1.428571 solar masses and the ratio m2 / m1 is 0.428571.
m2 = 0.4285714 solar masses
Try this example →

Example 5 — The Earth and Moon

1 Earth mass and 0.0123 Earth masses, separated by 384400 km

1
M = 1.0123 Earth masses = 6.0457 × 1024 kg and a = 3.844 × 108 m.
2
T = 2π √(a³ ÷ (G M)) = 2,357,384 s = 27.285 days.
3
μ = 0.0121505 Earth masses. The Earth is 4670.7 km from the center of mass, inside the planet, and the Moon is 379,729 km from it.
Period = 27.285 days, energy = −3.8086 × 1028 J
Try this example →

Example 6 — Two Sun-Like Stars at 1 AU

Two 1 solar mass stars separated by 1 AU

1
M = 2 solar masses and μ = 0.5 solar masses.
2
T = 2π √(a³ ÷ (G M)) = 22,314,677 s = 258.27 days, which is 0.7071 years.
3
Each star is 0.5 AU from the center of mass. The relative speed is 42,123 m/s and the orbital energy is −8.8204 × 1038 J.
Period = 258.27 days
Try this example →

Example 7 — Deuterium Against Hydrogen

An electron around a deuteron of 3670.48296788 electron masses, Z = 1

1
μ / me = 3670.48296788 ÷ 3671.48296788 = 0.99972763.
2
RM = 10973731.568 × 0.99972763 = 10970742.66 per metre, and the ionization energy is 13.60199 eV.
3
The vacuum H-alpha wavelength is 656.291 nm, against 656.4696 nm for ordinary hydrogen, so the isotope line is 0.1788 nm shorter.
H-alpha = 656.291 nm, μ = 0.99972763 me
Try this example →

❓ Frequently Asked Questions

What is the formula for reduced mass?+
μ = m1 × m2 ÷ (m1 + m2). It is the product of the two masses divided by their sum. For 2 kg and 3 kg the reduced mass is 6 ÷ 5 = 1.2 kg.
What is reduced mass used for?+
It reduces a two-body problem to a one-body problem. The relative motion of two bodies that attract each other behaves like a single particle of mass μ, which simplifies binary stars, planets and moons, molecular vibrations and the hydrogen atom.
Why is the reduced mass smaller than both masses?+
Because μ = m1 / (1 + m1/m2) and the bracket is greater than 1, μ is always smaller than m1, and by symmetry smaller than m2. It approaches the lighter mass as the heavier one grows.
What is the reduced mass of two equal masses?+
It is half of one mass, μ = m / 2. Two 1 kg masses have a reduced mass of 0.5 kg, and positronium, an electron bound to a positron, has half the electron mass.
What is the reduced mass of the hydrogen atom?+
Using the electron mass me and the proton mass mp, μ = me mp / (me + mp) = 0.99945568 me, or about 9.1044 × 10−31 kg. It is 0.0544 percent smaller than the electron mass, and that is enough to shift hydrogen's spectral lines.
How do I find the reduced mass of a diatomic molecule?+
Use the atomic masses of the two atoms in the same unit. For carbon monoxide with 12 u and 15.995 u it is 6.856 u. The vibrational frequency depends on the reduced mass through ω = √(k / μ).
Does the orbital period depend on the reduced mass?+
The period of a two-body orbit depends on the total mass: T = 2π √(a³ / (G (m1 + m2))). The reduced mass shows up in the energy E = −G m1 m2 / (2a) and in the angular momentum, not in the period.
How do I find a missing mass from the reduced mass?+
Rearrange the formula to m2 = μ m1 / (m1 − μ). It only works when μ is smaller than m1. With μ = 0.3 and m1 = 1 the missing mass is 0.3 / 0.7 = 0.4286.
Where is the center of mass of two bodies?+
It lies on the line joining them, at a distance m2 / (m1 + m2) times the separation from body 1. In the Earth and Moon system it sits about 4671 km from Earth's center, inside the Earth.
What is the difference between reduced mass and total mass?+
Total mass m1 + m2 sets the gravitational pull on the pair and the orbital period. Reduced mass is the effective inertia of the relative motion. For a small planet around a huge star, μ is close to the planet's mass while the total mass is close to the star's.
Why does deuterium have a different spectrum from hydrogen?+
The deuteron is about twice as heavy as the proton, so the reduced mass is slightly larger (0.99972763 me against 0.99945568 me). That raises the Rydberg constant and moves H-alpha from 656.470 nm to 656.291 nm in vacuum.

What is the formula for reduced mass?

mu = m1 x m2 / (m1 + m2). It is the product of the two masses divided by their sum. For 2 kg and 3 kg the reduced mass is 6 / 5 = 1.2 kg.

What is reduced mass used for?

It reduces a two-body problem to a one-body problem. The relative motion of two bodies that attract each other behaves like a single particle of mass mu, which simplifies binary stars, planets and moons, molecular vibrations and the hydrogen atom.

Why is the reduced mass smaller than both masses?

Because mu = m1 / (1 + m1/m2) and the bracket is greater than 1, mu is always smaller than m1, and by symmetry smaller than m2. It approaches the lighter mass as the heavier one grows.

What is the reduced mass of two equal masses?

It is half of one mass, mu = m / 2. Two 1 kg masses have a reduced mass of 0.5 kg, and positronium, an electron bound to a positron, has half the electron mass.

What is the reduced mass of the hydrogen atom?

Using the electron mass me and the proton mass mp, mu = me mp / (me + mp) = 0.99945568 me, or about 9.1044e-31 kg. It is 0.0544 percent smaller than the electron mass, and that is enough to shift hydrogen's spectral lines.

How do I find the reduced mass of a diatomic molecule?

Use the atomic masses of the two atoms in the same unit. For carbon monoxide with 12 u and 15.995 u it is 6.856 u. The vibrational frequency depends on the reduced mass through omega = sqrt(k / mu).

Does the orbital period depend on the reduced mass?

The period of a two-body orbit depends on the total mass: T = 2 pi sqrt(a cubed / (G (m1 + m2))). The reduced mass shows up in the energy E = -G m1 m2 / (2a) and in the angular momentum, not in the period.

How do I find a missing mass from the reduced mass?

Rearrange the formula to m2 = mu m1 / (m1 - mu). It only works when mu is smaller than m1. With mu = 0.3 and m1 = 1 the missing mass is 0.3 / 0.7 = 0.4286.

Where is the center of mass of two bodies?

It lies on the line joining them, at a distance m2 / (m1 + m2) times the separation from body 1. In the Earth and Moon system it sits about 4671 km from Earth's center, inside the Earth.

What is the difference between reduced mass and total mass?

Total mass m1 + m2 sets the gravitational pull on the pair and the orbital period. Reduced mass is the effective inertia of the relative motion. For a small planet around a huge star, mu is close to the planet's mass while the total mass is close to the star's.

Why does deuterium have a different spectrum from hydrogen?

The deuteron is about twice as heavy as the proton, so the reduced mass is slightly larger (0.99972763 me against 0.99945568 me). That raises the Rydberg constant and moves H-alpha from 656.470 nm to 656.291 nm in vacuum.