Damping in this visualization
Damping is the loss of energy that makes an oscillation die out. For a mass on a spring with a damper, , written with the natural frequency and the damping ratio . Below 1 the motion is underdamped (it swings), at 1 critically damped, above 1 overdamped (it creeps). For a mass hanging vertically, gravity only moves the rest position down by mg/k; x is measured from there. The page releases the mass from rest at x = 1 and asks whether more damping stops it sooner.
The right of the picture is the root plane. The two roots multiply to , so while the motion swings they lie on the circle of radius ω₀: the real part sets the decay, the imaginary part the frequency, so damping also slows each swing. At ζ = 1 the roots meet at −ω₀. Past it one root runs left and the other creeps back towards 0, about for large ζ. The slowest part of the motion decays like , and this decay rate σ, the distance of the rightmost root from the imaginary axis, is largest exactly at ζ = 1. On x(t) the dashed blue curve shows it: the envelope when underdamped (the curve touches it between its peaks), the slow root's term when overdamped.
“Stops” needs a rule. The page uses , the earliest time after which |x| stays within 1 % of the release for good. Its strip under x(t) magnifies the band. The extrema sit at with , which decides exactly which peaks leave the band; the last return is then found by bisection on the closed-form solution, so the readout is numeric. A smaller ζ gives a slightly later settling time whenever one more peak leaves the band, so the curve of against ζ jumps. Its minimum is not at critical damping but at , where the one overshoot touches −1 % exactly: 0.667 T₀ against 1.057 T₀. Critical damping is the fastest only among motions that never cross x = 0, and only from rest; another band moves ζ* (a 2 % band gives about 0.780).
Things to notice
- Two different “fastest”: the decay rate σ peaks at ζ = 1 exactly; the settling time is shortest at ζ*, a little below. A literal 0.826 is not ζ*: it overshoots by 1.0015 %, and its settling time jumps to 0.896 T₀. The page keeps ζ* exact.
- Doubling a large damping ratio roughly doubles the time to creep back: the slow root's time constant is about c/k.
- x(t) is the exact solution in all three regimes; the regime of a typed ratio is decided on the number as typed, so 0.99999999999999999 is underdamped. The fluid in the cylinder is only a sketch.
Controls
- Push the ζ fader (it catches at 0.1, 1 and 10), type a fraction or decimal, or press ζ = 1 or ζ*. A root can be dragged along its path; at −ω₀ it catches, and only there does it change branch. Drag the red time cursor to move the mass.
- Presentation mode opens a full-screen view: ← → change ζ by a fader step, H hides the decay rate and settling times.
Related
On the trace–determinant map of the phase portrait page, the damped oscillator is the horizontal line Δ = ω₀².
- G04Simple harmonic motion
- G06ResonancePlanned
- G07Phase portraitPlanned
Further reading: Wikipedia: Damping; OpenStax, University Physics Volume 1, 15.5 Damped Oscillations.