speaker excursion..."mo power"..and bass..Sean


I'd be interested in everyone's thoughts, but hopefully Sean will chime in...

Some reading I've been doing & the "is 22 watts enough" discussion has raised a question in my mind. I'll use the Linkwitz Orions as the example, but the real questions will (should?) apply to powering most any driver.

I've been reading Linkwitz's site on the Orions, some of the theory, what it takes to build them, suggested power..etc...and I remember some post that I read in the A-gon or AA archives stating that the 60 watts Siegfred suggests isn't enough to give significant bass. I read on the SL site that he likes the 60 watts as the amp will clip just before the speaker can reach full excursion & thereby the driver will not sustain damage. He continues to state that the higher power amp he suggests (a larger ATI) will result in the driver reaching full excursion prior to the amp bottoming out & thus driver damage may result.

>Proponents of "lower is plenty" might be, at least conceptually, in line with the needed power to reach a driver's maximum excursion (almost by defintion) being all the power necessary.

>Then comes the "more power, preferrably gobs more clean power" crowd that says more power is the best in most applications.

So my question(s):

>Is the difference between these two camps just "time"(instantaneous versus continuous power)? i.e Lots of mostly unused power sitting "idle" as a reserve for the couple millisecond demand of those dynamic peaks?

>From what I've read the SL Orions do very, to exceptionally, well on bass even with the 60 watts. How would 200 watts instead of his 60 improve the bass if the drivers bottom out at a little over 60 watts? Is it again just the millisecond peak demand for power that would be available or is there another reason?
fishboat
Capacitors DO lose power. This is called "dielectric absorption". ESR is also a term used to describe the series resistance or "internal losses" of a capacitor. If the power loss is severe, the cap "cooks" itself from the inside out and doesn't last very long or changes value to the point that normal circuit operation becomes harder and harder to achieve.

Inductors DO lose power i.e. it is called series resistance. Besides that, some of the energy is dissipated in the magnetic field that the inductor creates and / or through inductive coupling to other nearby parts of the circuit that they shouldn't be in. This is why proper crossover layout is important. I've seen "high end" crossover circuits that had a tremendous amount of crosstalk taking place due to this coupling. The end result is that tweeters and midranges end up being fed energy that should have gone to the woofer. Why did this take place? The inductors are too close together, placed in the same horizontal or vertical plane, etc... Due to their close proximity, the coils become inductively coupled via the previously mentioned magnetic field. By simply changing the horizontal and / or vertical planes of the inductors, without even moving them further apart, crosstalk can be reduced by at least -40 dB's. Not only does this result in less loss in the circuit, but better sound due to less smearing. Power handling is also improved due to having a more effective frequency dividing network with less stray coupling.

The use of a Zobel network that is tuned to operate within the audible pass-band WILL attenuate energy. The capacitor selects what frequency the Zobel comes into play and the value of the resistor dictates how much energy it will consume. If one does not use a resistor of high enough power handling and / or the value is poorly chosen, you WILL burn up the resistor in the Zobel when "cranking" the volume way up on a steady-state basis.

All of these parts DO rise in temperature as they are used and this is part of what "component settling" is all about. If the average power that they are passing is high enough, you would feel the heat that they were dissipating. Since most music is very low in average power consumption and very high in peak power, the energy lost / heat generated within these parts isn't very high and / or consistent. It is these very short duration, high intensity peaks that get "eaten up" in a passive crossover, hence the increase in dynamics and increased detail that one encounters from going active. All of the aforementioned losses in the passive circuit end up costing resolution while increasing the levels of inductive and capacitive reactance that the amp tries to load into.

"Thus, the practical increase in effective power is more like 2X, as that 1975 article you refer to showed".

Doubling the power ( X2 ) is a 100% increase. Losing half the power ( /2 ) is a 50% loss. We've said the same thing using different wording looking at things from opposite points of view.

As far as the 30 / 60 wpc actively crossed amps clipping at the same appr output level as that of the 175 wpc passively crossed amplifier, i can't help you out there. I referenced this from Vance Dickason's Loudspeaker Design Cookbook and do not have access to the original article. Your own response seems to confirm these figures rather than contradict them.

The comments about the active crossovers increasing the gain of the signal have little to nothing to do with amplifier capacity. The amplifier can only put out so much power prior to clipping regardless of whether it has to amplify itself is providing the gain or whether the drive levels are increased. If anything, increasing the drive levels via the active crossover would have driven the amplifier into clipping sooner and more consistently. This is because the amplifier functions at a constant rate of gain, so long as it is linear in operation. More drive means more clipping.

Damping factor is a hoax and is completely taken out of context. I've explained this in the past several times. Couple this with the fact that your .1 ohm output of the SS amplifier is typically fed into 40 - 120 ohm speaker cable to get to your 4 - 12 ohm speakers and you should begin to understand why i rant about using "properly designed" low impedance speaker cables as much as i do. You guys are missing the boat on this one in tall fashion.

Reflected EMF is a reality that the amps have to deal with. If it were not, microphones would not work or produce voltage and we couldn't use them to capture acoustic signals to make recordings with. Now take the microphones that produce EMF and increase their capture area ( cone size ) and motor structure by a few dozen times and tell me that they don't generate voltages, especially when their excursions are made in great amplitude and speed. Just as feeding voltage into a coil in a magnetic field causes the cone to move, moving the cone that has the coil attached to it that is placed within the magnetic field generates voltage. This is an action / reaction that is unavoidable. Obviously, one has to "out muscle" the other opposing source of voltage / current, otherwise the two would cancel each other out as heat and there would be no acoustic output what so ever.

"The externally mounted 3.5mH inductors of my MG1.6 are 10 AWG air core coils with dc resistance of 0.2 ohms, which is about the same as the original equipment iron core inductors. Since the driver is 4 ohms, 0.2/4 which is 5 percent of the power will end up as heat in the inductor".

Bombaywall, El just answered your "Thermal losses in a capacitor & coil????? Physics does not allow this!" comment. On top of that, he was talking about a 5% thermal loss using a 10 gauge conductor, which has very low series resistance. How much more loss is there in an inductor that is wound using a 16 - 20 gauge conductor as found in most commercially produced loudspeakers?

"It is dangerous to run a tweeter directly from a power amp. Turnon and turnoff can be accompanied by "thumps" that the tweeter won't like, and a loose interconnect can be an instant disaster."

If you look at some of the old Stereo Review, Audio and even Stereophile reviews of speakers, i think that you'll find that many tweeters will easily cope with transient bursts into the 100's if not 1000+ watt range, so long as they are limited in duration. I've seen tests were the tweeters handled more power than the woofers did, so long as they were bandwidth limited. Other than that, the easy way to get around "turn on surges" is not to turn your gear off.

"I think that it was on the Adair Audio website that I read that VCs are only about 1-2% efficient! I was shocked to read such a low number - I knew that they were largely inefficient but wasn't expecting 1-2%! If that's true, it's easy to see why "Duration" would fry a tweeter."

Pretty efficient horn designs only come up around 4% - 5% or so. Almost all of the power generated within an amplifier is dissipated as thermal losses in a loudspeaker. As such, removing even several tenths of one percentage point via getting rid of "lossy" passive components between the amplifier and driver can make a sizeable difference. Increasing power transfer via proper impedance matching can also improve system efficiency AND improve transient characteristics.

Sorry if this jumps around quite a bit, but i'm limited on time. Due to my increased work load ( busiest time of the year ) and changes in my personal schedule due to family health problems, i can't hang out here as much as i'd like. Hope this at least clarifies a few things. Sean
>
Hey Sean,

Neither Eldartford nor I totally denied that L & C do lose power.
Eldarford: "Passive crossovers do not absorb power to the degree that you suggest." &
I wrote: "Inductors will dissipate some heat as a coil of wire will have some resistance. If one is using a low ESR capacitor, very little heat gets generated in a capacitor."

However, I think that you are mistaken as to just how much gets dissipated in these Ls & Cs on average.
Optimizing the losses in a reactive component is NOT the way biamping achieves its perceived increase in power. Separation of power amplification into multiple chassis & the constructive addition of the music signal is what gives biamping its perceived increase in power.

"The comments about the active crossovers increasing the gain of the signal have little to nothing to do with amplifier capacity."
True! However an amplified signal fed into an amp needs less amplification to the speaker => more headroom for dynamics. Such a setup would have more air/the music would flow easier/more transparent.
The comparison is between passive & active xover cases.

"Couple this with the fact that your .1 ohm output of the SS amplifier is typically fed into 40 - 120 ohm speaker cable"
What???? Who in their right mind would use a 40-120 Ohm speaker cable?? Does a speaker cable with 40-120 Ohms even exist? I think that you would ripe for catching much flack for this one, Sean! :-)
I think it's a typo. You really meant milli-Ohm, right??

"Reflected EMF is a reality that the amps have to deal with."
Oh, it certainly is. No question about & I never denied it in my post. However, not to the degree that you mentioned in your original post. There IS the reverse isolation of the xover & their IS the output impedance of the amplifier/damping factor as only an active circuit can get rid of the back-EMF

"Damping factor is a hoax and is completely taken out of context."
No it certainly is not! Without a damping factor, which is really a glorified name for amplifier output impedance there'd be no "out muscling" the woofer.
We can agree to disagree here, which is just fine w/ me.
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Anyway, I, too, am in the more power, the better camp as long as the user is careful to not overdrive the speaker. If there are transients, then they should be shorter in duration (than being longer) & if one doesn't know then it's better to listen with a slightly lower level to be conservative. Case-in-point: Last summer I fried my Green Mountain floor stander tweeter after trying to break-in the woofer by playing music too loud for 14 hrs at a stretch! What Roy Johnson told me was that tweeter can handle way more than its 100W RMS rating if I play loud music for about 3-4 minutes (1 track) every 20 minutes or so. He says that he does that all shows regularly & the tweeter survives each time. So, now I know.......
More power results in the music flowing better, more air, more transparency, more lower level details.
Drivers can handle many more watts of peak power even tho they are rated for lower RMS power. (Usually, the driver ratings are RMS power, which is average program power).
So, yes, Fishboat, its reserve power mostly.
Additionally, a large amp has more current capacity even at lower power levels, which what gives the music is ease of flow. To get that driver moving, you need current in the voice coil.

I think the damping factor issue is directly related to the speaker in question, which may very likely have a very low moving mass and very high magnetic field and very short excursion length(such as my speakers), and thus have a very significant amount of its own internal damping ability.

In cases such as this, high numerical "damping factors" may actually inhibit transient response, and may not be an advantage at all.

As long as the relationship between the amp's output impedance and the speaker's relative impedance at any given frequency(damping factor) remains enough to control the speaker(>5), then it is sufficient in that circumstance. It is when the speakers have poor internal damping characteristics(ie high moving mass/low magnetic field strength/very long excursion length) where problems are more likely to be "fixed" by high electrical damping factor numbers.

Regarding high power being "better" than low power, we all know I'm in the "low power" camp. I think(and I'm pretty sure Sean agrees) that you are much better off to have higher efficiency speakers than to try to overcome low efficiency speakers with brute force, because of the exponential curve of power needed to add a few db to the output.

Also, it has been my experience that high power amps seem to be less "delicate" in nuances and details, due to the beefy construction needed to handle all that power. And in addition, to have power like that, you simply have to go out of Class A operation, which I don't like to do.

And, when you have low efficiency speakers, you have a higher "low-level detail threshold" because it simply takes more power to make the speaker move at all, so that some very low level stuff never even makes it out of the speakers, unless you have it turned up alot.

If the speakers are high efficiency, you can still get pretty loud SPL, with great low level detail, with very low power amps. I do realize that this normally sacrifices some of the very low bass. I think it is not a bad trade-off.
I do realize that this (very low power amps -high efficiency spkrs) normally sacrifices some of the very low bass
As you note, "normally". You can add active subwoofs for very little outlay and resolve the issue (if issue there is).
Whoa!

This thread had a great technical edge and now its tumbling out of control.

Passive crossovers are "voltage dividers", this is where the power goes, to ground especially in 2nd order and filters with notch filter etc. There are small losses in the components but the passive filter itself is a loss as it is addressing the fully amplified signal.

Drew/Bombay & Sean your original long posts were about 75% correct but this second group is getting into the land of speculation. Again good posts but now you guys are down to about 50% correct.

Sorry,I don't have time to correct the errors point for point.