Thoughts on an Amplifier Damping Factor and Transient Response of Speaker
Some say that an amplifier's damping factor is irrelevant for all purposes. I beg to disagree.
An amplifier's output impedance, that is damping factor, can have an effect on how a speaker's moving mass responds faithfully to the program material fed to it. Please bear in mind that, at 4 ohms, the damping factor is also divided by two as compared to the published specification which is usually based on an 8 ohm speaker load. The amplifier's damping factor is obtained by dividing the speaker impedance by the internal output impedance of the amplifier.
The transient response of a speaker cone depends on several factors. These are:
- The Qts of the speaker: This is affected mainly by the ratio of the coercivity of the magnet to the moving mass of the transducer. With a set moving mass, the stronger the magnet, the lower is the Qts figure, and this situation favors an excellent transient response. In a closed enclosure, this figure is not as important as in a vented one, because of the entrapped air pressure which acts as a damper.
But if you drive a speaker with a high moving mass to magnet coercivity ratio in a bass-reflex enclosure, with a tube amplifier, or even a McIntosh solid state amplifier designed with an output transformer (added resistance), those amplifiers having a high output impedance, you risk obtaining a very poor transient response.
2. Use of an inductance in series with the speaker in a passive crossover. The resistance of the inductor is added to the internal resistance of the amplifier and there goes most of the original damping factor. The use of two power amplifiers, one for the woofer and one for the high frequency drivers preserves a good part of the low resistance of the amplifier, provided that the cable connected between that amplifier and the woofer has a low resistance. This configuration is called bi-amping and an active crossover is required between the preamplifier and the two power amplifiers to divide the frequencies among the transducers. Another advantage of the bi- amplification is that you have a more efficient woofer (less resistance in series).
3. Resistance of the speaker cable. This factor depends of course on the size of the wire (AWG 14 as an example) and the length. For serious audiophile listening, one should use no smaller than gauge 14 and preferably use a bigger wire, at least gauge 10, when driving a 4 ohm woofer, because of the higher currents necessary to drive such driver.
NOTE: IMHO, THERE IS NOT MUCH POINT IN BI-WIRING SPEAKERS. Should you suspect a poor transient response, you would get quite better results by just attaching both cables together in parallel and connecting them to only one speaker terminal. That way, you might get a noticeable advantage with half the cable resistance, more so since your speakers use passive crossovers.