I'll get into it with Andre one more time as I tire his cheap
uniformed shots at audio engineers. As usual, part of what Andre
writes (here and on his website) is slightly correct, but much of it
misleading and uninformed half truths. He is a self appointed expert
without the benefit of an audio engineering education and is more
often wrong than right. Every forum needs a clown to keep it
entertaining, and Andre without his vitriol would fit the bill
nicely.
A couple of caveats: Andre and I have got into it before and I've
endured his personal attacks which don't bother me. He knows my
qualifications and hopefully won't waste time questioning them
again. Only one of us is a member of the AES, SMPTE, and ASA.
I've also been a big Quad fan my entire adult life, which means I've
owned and (and repaired) Quads since 1976, including 57's, 63', 988's,
989's. I've also listened to the new 9805's for roughly eight hours
of listening time. Toured the Huntington factory three times (twice
with Peter Walker, once with Ross) before it closed. I am listening
to a Kate Bush CD on 988's as I write this...
The traditional calculation of damping factor is a ratio of the total
impedance of the speaker divided by the total impedance to the speaker
system being driven. Both vary with frequency, especially the speaker
complex impedance. Assuming a given amplifier with a fixed impedance
of 0.1 ohm across its power output (a huge assumption, especially with
tube equipment), we only have to deal with the three other impedances
associated with the speaker: acoustic, electrical, and mechanical of
the speaker cable, speaker, and listening environment. The last two
vary across the entire listening spectrum rather radically. Most
audio engineers don't waste time calculating damping factor anymore as
the number is somewhat meaningless from a comparative standpoint.
Just the static electrical/mechanical impedance of a Quad 57 can be
seen on this website:
http://www.quadesl.com/quad_main.shtml. You
tell me how to provide a single number based on that impedance graph,
let alone with the acoustic impedance of the room added. The simple
answer is you can't. Calculating these three impedances is
impossible, although it can be measured fairly easily with B&K, TEF,
MLSSA, and other commerically available machines in a given acoustic
space with a given speaker. I suspect Andre has never seen, owned, or
operated one of these devices based on my previous experiences with
his writing.
The "lowest frequency in a room" calculation stumping most audio
engineers is an even more specious argument, because it stumps all of
them! You can only estimate it, even after having all of the
dimensions and materials entered into you auralization program (like
EASE or Bose's). Again, you have to measure it with computer driven
analytic tools to really know what's going on.
The acoustic size of a room (not the mechanical size) varies with
frequency. In smaller rooms (like the one you're probably in right
now) you have dramatic differences in energy densities with time,
which argues against the traditional homogenous, statistically
reverberant sound field calculations. The acoustic juncture between
of a small room can fall as high as 500 Hz, where it is typically
below 30 Hz in a small room. The frequency dependency of the
pressure zone, modal zone, the diffusion zone, and specular reflection
zones will alter with room treatments. In other words, the low
frequency cutoff changes constantly as you play your music.
I suspect the same is true of your listening acuity as well, which
further complicates the issue.