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|    Message 41,584 of 41,683    |
|    dpierce.cartchunk.org@gmail.com to All    |
|    Re: Damping Factor in drivers    |
|    03 Jul 18 07:27:59    |
      september.org> 69fd7f17       On Monday, July 2, 2018 at 1:41:13 PM UTC-4, G wrote:       > I understand effects of electrical damping of woofers. I'm wondering how It       > may affect midranges and tweeters. Is it the same, or does it dimish at       > higher frequencies. Remove any crossover components for direct feed to amp.       > Tone bursts should Show any difference in DF. Without testing, I'm       > guessing.              To cut to the chase: forget about "damping factor." It's essentially       a made-up "spec" that indicates very little about the performance of       loudspeaker drivers. Really. The important number, if you're worried about       how well a driver is controlled at its resonance, is it's total Q       factor: in the case of the driver itself, it's the Qts of the driver.              The Q of any resonant system is a measure, essentially, of the       ratio of the amount of energy stored in the resonance to the amount       of energy dissipated. In the case of a driver, you have essentially       three ways by which that energy is dissipated, or lost or, if you prefer,       how it is removed from the system. These are:              1. Electrical losses, which, for most drivers, is the largest        loss mechanism (and is usually specific Qes),              2. Mechanical losses, which, for most drivers, is secondary        to the electrical losses (designated as Qms),              3. Acoustical losses, i.e., the sound that is actually radiated        into the room which, for almost all drivers, is an insignificant        loss mechanism (this is why speakers are so inefficient).              Now, #1 might seem contradictory to me declaration that damping       factor is essentially useless, since we are (I assume) talking       about electrical damping, but it becomes clearer once you realize       the fact that it's the total resistance in the circuit that's       responsible for the electrical Q. That not only includes the output       resistance of the amplifier (which is where the "damping factor"       spec comes from), it not only includes the electrical resistance       in the crossover (not impedance, not inductance, but resistance),       it also includes the DC resistance of the voice coil.              The problem is, far and away, the single largest resistance in that       collection is the DC resistance of the voice coil. That resistance       dominates all others, and attempting to reduce the other resistances       (crossover, speaker wire, amplifier) won't make a hill of beans       difference in the damping of the system.              Le's take a typical 8-ohm woofer, with an equally typical DC       resistance of about 6.5 ohms. Let's assume the mechanical Q       of the driver is 4, the electrical Q is 0.85, and the resulting       total Qts is about 0.701 (Qts = Qes*Qms/(Qes+Qts). How is this       going to perform with an amplifier whose damping fact is, say,       1000 vs one whose damping factor is 50. One might be inclined       to say that there will be a factor of 20 difference in the       damping of in each case (1000/50=20), but it turns out not to       be so.              Whatever with a damping factor of 1000, our "highly-damped"       amplifier has an output resistance of 0.008 ohms, while our       "not-so-well-damped" amplifier has an output resistance of `0.16       ohms.              The amplifier output resistance will increase the electrical       Qes: in the case of the first amplifier, it will increase it from       0.85 to 0.851 (Qes' = Qes * (Re+Rg)/Re. In the second case, it       will increase it from 0.85 to 0.87. NOt much.              But it's the TOTAL Qts that we're interested in. In the first case,       it will change from 0.701 to 0.702. In the second case, it will change       from 0.701 to 0.714. In both cases, the actual damping of the system       changes by less than 2%. This is less than the typical variation in       these kinds of parameters one finds from one sample of a driver       to another.              The situation with midranges and, especially, tweeters is even       more the case where these external resistances have little       effect, because in these cases, the total Qts is more heavily       dominated by the mechanical losses, and thus changes in the       electrical Q have even less of an effect. Further, in many systems,       the principle resonance is designed outside of the operating       bandwidth of the driver by the crossover, so it has even LESS       of an effect.              > Tone bursts should Show any difference in DF.              Tone bursts are very likely to tell you nothing useful at all.       They're not a terribly useful test in and off themselves and,       given the very small changes you're likely to encounter in       the changes you're proposing, a tone burst is not going to       reveal anything. Further, tone bursts are very hard to measure.       Bump your microphone a little bit, change its position, and       you'll measure a different tone burst              --- SoupGate-Win32 v1.05        * Origin: you cannot sedate... all the things you hate (1:229/2)    |
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