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The impedance of a real speaker cab changes slightly with the excursion. The low-frequency resonance decreases and shifts slightly. The inductance changes.
The low-frequency resonance changes because the speaker suspension goes nonlinear and the B * l product changes with displacement.
The inductance changes because the voice coil moves in and out of the magnet gap. The more turns inside the magnet the greater the inductance.
The are papers by Klippel et. al. that quantify the effects. FWIW, our products model this.
However... Jay is 100% correct that the linear differences are far more audible. Even two copies of a speaker in an enclosure will measure differently due to manufacturing variances.
The low-frequency resonance changes because the speaker suspension goes nonlinear and the B * l product changes with displacement.
The inductance changes because the voice coil moves in and out of the magnet gap. The more turns inside the magnet the greater the inductance.
The are papers by Klippel et. al. that quantify the effects. FWIW, our products model this.
However... Jay is 100% correct that the linear differences are far more audible. Even two copies of a speaker in an enclosure will measure differently due to manufacturing variances.