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Home/Engineering/Jeffcott Rotor Critical Speed

Jeffcott Rotor Critical Speed

Single disk on a flexible shaft: ω_n = √(k/m), unbalance response, whirl orbit, phase lag, and critical-speed crossing.

Rotor and shaft

18 kg
850 kN/m
0.06

Unbalance and speed

0.25 mm
1800 rpm

The Jeffcott rotor is a linear single-disk model. Real machines add bearings, gyroscopic effects, multiple modes, anisotropic stiffness, rubs, and nonlinear seals.

Measured values

Critical speed2075rpm
Speed ratio Ω/ωn0.87
Orbit amplitude X0.70mm
Phase lag22.8°
Unbalance force159.9N

The response peaks near the first critical speed. In practice rotors are balanced, accelerated through critical speeds with care, and checked against bearing loads, mode shapes, and vibration limits.

Live graphs

About this model

The Jeffcott rotor is the classic first model of rotor dynamics: a rigid disk of mass m mounted on a massless flexible shaft with lateral stiffness k and damping ratio ζ. Its first critical speed is ω_n = sqrt(k/m). A small mass eccentricity e creates a rotating unbalance force m e Ω²; the steady orbit amplitude follows X/e = r² / sqrt((1−r²)² + (2ζr)²), where r = Ω/ω_n. This simulator animates the disk whirl, plots amplification versus speed ratio, and highlights the passage through the first critical speed. It is a teaching model only: real rotors include bearings, gyroscopic effects, shaft distributed mass, anisotropic stiffness, multiple modes, seals, rubs, thermal bow, and nonlinear supports.

Who it's for: Rotor dynamics, machine vibration, turbomachinery, pumps, motors, and mechanical design introductions.

Key terms

  • Jeffcott rotor
  • Critical speed
  • Unbalance response
  • Whirl orbit
  • Damping ratio

How it works

Jeffcott rotor critical-speed simulator: disk on a flexible shaft with unbalance force, resonance amplification, whirl orbit, phase lag, and critical speed crossing.

Key equations

ω_n = sqrt(k/m), r = Ω/ω_n
X/e = r² / sqrt((1−r²)² + (2ζr)²)

Frequently asked questions

Why does vibration peak near critical speed?
At r = Ω/ω_n near 1, the forcing frequency from imbalance matches the lateral natural frequency of the rotor. Damping limits the peak but does not remove the resonance.
Is it always unsafe to run above a critical speed?
Not necessarily. Many machines pass through a critical speed during startup and operate supercritically. The design question is whether the crossing and operating range satisfy vibration and bearing-load limits.