Physics · Mechanics · Motion & Energy

Spring–mass natural frequency calculator

Find undamped natural angular frequency, frequency and period from moving mass and spring stiffness. This describes oscillation about equilibrium.

Created v1.0

By Thibaut Grzelak, Mechanical Analysis Engineer

Mechanics · Motion & Energy
01Calculation inputsωₙ = √(k / m)
km
Ideal spring of stiffness k attached to moving mass m; the model uses small oscillations about equilibrium.
02

Results

Natural frequency
—

Number of complete cycles per second.

Period
—

Duration of one complete cycle.

Relation and numerical substitutionωₙ = √(k / m)

—

Ideal undamped linear spring; m,k > 0; oscillations about equilibrium.

01Formulas and symbols

Formulas used

ωₙωₙ = √(k / m)Undamped natural angular frequency in radians per second.
fₙfₙ = ωₙ / (2π)Number of complete cycles per second.
TT = 1 / fₙDuration of one complete cycle.
02Assumptions and limits

Scope of validity

  • Ideal undamped linear spring; m,k > 0; oscillations about equilibrium.
03Validation example

Reference numerical case

  1. m = 2 kg, k = 200 N/m: ωₙ = √(200/2) = 10 rad/s; fₙ = 10/(2π) ≈ 1.59154943 Hz; T ≈ 0.62831853 s.
04References

FAQ

Does gravity change the natural frequency of a vertical spring–mass system?

In the ideal linear one-degree-of-freedom model, gravity shifts the static equilibrium position but does not change ωₙ = √(k/m) for small oscillations about that equilibrium.

What happens to natural frequency if stiffness or mass is doubled?

Because fₙ is proportional to √(k/m), doubling stiffness multiplies the frequency by √2. Doubling the mass divides the frequency by √2.

05How it works

The spring restoring force accelerates the moving mass. Increasing stiffness raises natural frequency; increasing mass lowers it. Quadrupling stiffness doubles frequency, while quadrupling mass halves it. Frequency in Hz counts cycles; angular frequency in rad/s equals 2π times that value.

06Limits of the model

A single translational degree of freedom, linear massless spring, positive moving mass and no damping. Distributed spring mass, damping, multiple coupled masses and nonlinear stiffness need another model. No resonance amplitude or forced-response prediction is made.

07Common mistakes

1 N/mm is 1000 N/m. Use the moving mass, not its weight in newtons. Do not confuse natural angular frequency with cycles per second.