Oscillations & Simple Harmonic Motion

damped oscillation

Damped oscillation is what real oscillations actually do: they gradually die away. A plucked guitar string fades to silence, a child on a swing slows and stops if nobody keeps pushing, and a car settles after bouncing over a bump. It answers the honest question that ideal SHM sets aside: what happens when friction or drag steadily drains the energy out?

Precisely, a resistive force, such as air drag or friction, often roughly proportional to speed, F = -b v, where b is a damping coefficient, removes a bit of energy every cycle. The amplitude then shrinks exponentially over time, roughly A(t) = A_0 e^(-(b/2m) t). There are three regimes: underdamped, where the system oscillates while slowly fading; critically damped, where it returns to rest in the shortest time without overshooting; and overdamped, where it creeps back so sluggishly that it never oscillates at all.

Damping is often exactly what engineers want. Car shock absorbers and self-closing doors are designed near critical damping so they settle fast without bouncing. One subtle but honest detail: damping also lowers the oscillation frequency a little compared with the undamped natural frequency, because the drag slightly slows each cycle.

A car's suspension is tuned close to critical damping: after you drive over a pothole, the body dips once and settles, rather than bouncing up and down (underdamped) or sagging back slowly (overdamped).

Critical damping returns a system to rest fastest without overshoot, ideal for shock absorbers.

Damping not only shrinks the amplitude over time but also slightly lowers the oscillation frequency compared with the undamped case.

Also called
dampingdamped harmonic motion阻尼振動