Scolavo Instrument · Differential Equations
The Impulse Hammer
The bell · x″ + 2ζω₀x′ + ω₀²x = Σ Jₖδ(t−tₖ)
Oscilloscope · displacement x(t)
AT RESTthe bell is quiet
press the stage to strike — you are the impulse
Strikes0
Ring A0.00
Phase @hit—
Period ×—

Field notes

A struck bell is an underdamped oscillator: displace it and it rings, the amplitude fading as friction bleeds the energy away.

A hammer blow is idealised as a Dirac delta — an infinitely brief force that leaves the position unchanged but jumps the velocity. The bell's answer to one unit kick is its impulse response: a single damped sinusoid.

Because the equation is linear, many blows just add their shifted impulse responses (Duhamel's principle). Land them one period apart and they reinforce — resonance by percussion.

Strike once, dead against the swing, with a blow that exactly matches the current velocity, and the sum collapses to zero: position zero, velocity zero, silence. One delta erases the ring.

This lab hit a snag

The instrument fell silent mid-measurement. The lesson continues without it — read on, and the ideas will still be here.