✓ Sources checked · 10 September 2026 · View verification
Critical damping is the boundary between oscillatory and nonoscillatory free response in a linear mass–spring–damper system: bc = 2√(mk), or damping ratio ζ = 1.
By Matan · Updated
What “fastest” assumes
For mx″ + bx′ + kx = 0, the critical solution is x = (A + Bt)e^(−ω₀t), with ω₀ = √(k/m). For release from rest at displacement x₀, x = x₀(1 + ω₀t)e^(−ω₀t): it approaches equilibrium without crossing it. “Fastest nonoscillatory return” refers to this standard comparison, not every possible initial velocity or control objective. [1]
Worked damping coefficient
With m = 2 kg and k = 50 N/m, ω₀ = 5 rad/s and bc = 20 N·s/m. Released from rest at x₀ = 0.10 m, after 0.40 s the displacement is 0.10 × 3 × e⁻² = 0.0406 m.
Real products are not automatically critical
A car damper alone does not determine a suspension’s damping ratio, and a real vehicle has multiple vibration modes. Critical damping is a model condition, not a universal optimum for comfort or isolation. Zero repeated oscillation also does not mean exact rest is reached in finite time.
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How this article was checked
Sources checked; calculations checked where shown. The definitions, model assumptions and main explanatory claims were cross-checked against the sources below. Worked-example arithmetic and units were checked separately. These examples are illustrative calculations, not experimental measurements.
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Sources and further reading
- OpenStax: Damping regimes — Damping regimes.
Cite this article
Matan. “Critical damping.” Your Physicist. Originally published 2023-03-17; updated 2026-09-10. https://your-physicist.com/critical-damping/
Revision history
: Added the critical coefficient and a checked response; qualified the fastest-return and car-suspension claims. Added linked sources and a transparent verification record.