It will take me more than 1 post to say what I think of Ashley James's statement.
Starting with his claim that "Damping is a miserly 300 times worse" in a passive system than an active one.
That statement is based on which amplifier, speaker and cables? He doesn't say.
Let's see if his statement applies to speakers, amp and cables that I am highly familiar with and where we all have easy access to the technical info.
Starting with what is damping? https://en.wikipedia.org/wiki/Damping_factor
http://www.crownaudio.com/media/pdf/amps/damping_factor.pdf
Wikipedia says:
"The voltage generated by the moving voice coil forces current through three resistances:
- the resistance of the voice coil itself;
- the resistance of the interconnecting cable; and
- the output resistance of the amplifier."
For my example I will use my Bozak Symphony speakers, JBL 6290 power amplifier and 10 metres of my 752 strand speaker cable.
In passive mode there's actually a 4th resistance / reactance not mentioned in Wikipedia: that of the inductor in my passive crossover.
In the circuit between my power amp and speakers in passive mode we have:
Amp: 0.04 ohms output impedance (source: amplifiers owners manual)
10 metres speaker cable with an impedance of approx 0.1 ohm (source: amplifiers owners manual)
The L1 inductor which has a value of 1.58mH (source Bozak Yahoo group crossover ref document)
The speaker coils themselves in the bass drivers with a nominal impedance of 8 ohms. In reality it'll vary between just under 6 ohms and 14 ohms depending on frequency. I'll assume near worst case (rounded off) in terms of passive crossover impact and use 6 ohms for my calculations.
To find the effect of the L1 inductor we can use this calculator: http://www.electronics2000.co.uk/calc/reactance-calculator.php
Where we find that the L1 inductive reactance depends on the frequency (and so it should. That's what it's there for). So that at 400 hz - the crossover frequency of my speakers, L1 is giving us a reactance of 4 ohms. Which makes a lot of sense as at that frequency we want the signal equally split between the 8 ohm bass drivers and the 8 ohm midrange unit.
At 100 hz L1 gives us 1 ohm reactance.
At 60 hz (the approx resonant frequency of the bass drivers) L1 gives us 0.6 ohms.
So in passive mode, the total impedance / reactance of our circuit is the total of the impedance of the cables (0.1 ohms), plus the reactance of the passive crossover (4 ohms at 400 hz down to 0.6 ohms at 60 hz), the impedance of the speaker voice coils (6 ohms), plus the impedance of the amplifier (0.04 ohms)
At 400 hz, adding these all together gives us a total of 10.14 ohms. This is the load through which the electricity generated by the voicecoils has to dissipate.
But, and it's a big but, 400 hz is quite a long way above the resonant frequency of my speaker drivers.
If we add all the numbers up for our 60 hz resonant frequency we get a total of 6.74 ohms through which the electricity generated by the voicecoils has to dissipate.
If we go active and hypothetically move our amp into the speaker cabinet we can get rid of the L1 inductor and the speaker cables from our circuit. This would give us 6.04 ohms at 400 hz and 60hz through which our voicecoil electrity has to dissipate.
You need to bear in mind that at 400hz my bass drivers will have more mechanical damping than they will at 60hz. Also they will have less movement and therefore generate less electricity at 400 hz for a given volume than they will at 60hz.
So, active to passive we're taling about a difference of 6.04 to 10.14 ohms (at 400hz). Or 6.04 to 6.74 ohms (at 60hz).
That is nowhere near a 300 times difference.
Therefore, IT IS TOTALLY MISLEADING FOR ANYONE TO SAY THAT DAMPING IS 300 TIMES WORSE IN A PASSIVE SYSTEM.
You can all, of course, do your own calculations on your own speakers, crossovers and cables to see what figures you come up with.