Interesting! This just shows the electrical properties of the coil - I would imagine the acoustic output of the speaker probably has quite a few more resonances
Yes, but generally the acoustical resonances will have some effect upon the impedance, as the voice coil impedance consists of both a static element and a back EMF from motion of the coil. Hence the acoustic impedance alters the back EMF to some degree by changing the motional loading of the coil and hence the measured |Z| and/or phase angle.
The attached plot shows the electrical impedance of a speaker with two mountings. Both demonstrate a strong resonance around 400 Hz, which is due, in my opinion, to acoustical resonance of the speaker and (in the second case) resonance of the combined speaker and mounting plate. The possibility of this being an LC resonance due to distributed capacitance can be discarded rather easily with a quick calculation of the required capacitance value.
One is the speaker frame resting on my measurement bench, and the second is the same speaker mounted in its normal mounting plate. The speaker is the internal device normally supplied with an Elecraft K2 ham radio transceiver and is attached to an L shaped metal plate that forms the top enclosure of the transceiver cabinet. The second measurement is the speaker mounted on the L panel but the panel is not installed in the transceiver (won't fit - my K2 has an optional 100 watt amplifier module where the speaker normally mounts) but is resting on the bench.
Even though the changes between the two mounting arrangements are not great, there's enough change in acoustic loading to be seen in the impedance measurement. I would expect a greater change in electrical impedance and resonant frequency if the speaker were mounted in the normal arrangement.