solderdude
Grand Contributor
As a result of this ratio, the speaker is unable to move the amplifier around by way of its back EMF, since a relatively high Z speaker is trying to push a near dead short around.
The damping factor is merely another way of describing output impedance. A parlor trick so manufacturers could state huge numbers and use it as a marketing tool.
You might remember the DF race with Sigma drive reaching numbers of 10000 and tales of 'control' or 'grip' on the drivers.
Consider a speaker with a resistance of 8 ohm and it is externally 'moved' up an down.
It generates a voltage (coil in a magnetic field).
When you load that voltage source (with an 8ohm resistance) with a short (D.F. infinite) the motion of the speaker is generating a current (Vvoicecoil/Rvoicecoil) so the current that 'damps' is U/8. Lets make the voicecoil voltage 8V (open coil voltage) this means the damping current is 1A.
When the output R is not 0ohm but say 0.2ohm the damping current is 8/8.2 = 0.975A so basically the same.
The fact that there is no voltage that can be measured with a 0ohm output R does not mean the driver cannot move. It just means you cannot measure a voltage when a current is applied.
A relatively high output R (opposite the driver) can noticeably reduce the actual 'damping current'.
This is not what is the actual problem though. What is audible is a simple voltage division issue (frequency dependent) which changes the FR of the signal arriving at the speaker terminals (R out + R speaker cable).