thxgoon said:
Could you explain this? Thanks.
Sure, I can try. Power factor is defined as the Cosine of the phase angle between the voltage phasor (a.k.a. vector in the old days) and the current phasor.
For an inductive load, such as a voice coil, the current will be lagging behind the voltage. For a capacitive load, the current will be leading. You can see the phase relationship between the voltage and current phasors if you display their waveforms on an oscilloscope. For a purely inductive load (i.e. with negligible resistance), the current is 90 deg lagging the voltage. Cosine 90 deg is 0, so you can only develop reactive power (unit is VAR, not Watt) into a pure inductive load such as an inductive coil. The real power dissipation (watt), is 0. I believe a conventional loudspeaker circuit is a complex load that has all 3 components of resistance, inductance and capacitance. The overall impedance has the same unit as resistance, i.e. ohms. However, the amplifier that drives the loudspeaker will see a complex load, and the current driven into this complex load will generally be lagging the voltage by an angle, say 40 deg (just an example). That will give a power factor=Cosine 40 deg=approx 0.766. I suspect different speakers will have different power factors and the p.f. will likely varies with frequencies. In any case, it will be less than 1, may be in the range of 0.7 to 0.9 except at 0 (d.c.) frequency.
I mentioned the p.f. thing because like efficiency, it has to be in the equation for any a.c. power calculations, unless the load is purely resistive.
Sorry if I failed to explain it clearly. Hopefully others can do a better job.