Bozak Midrange: B-800 / B-800A vs B-209B / B-209Bc / B-209C

Here is what I previously wrote, four years ago (on October 2016), about midrange polarity, phase shifts at the band's center versus the band's ends:

https://www.audiokarma.org/forums/i...m-built-3-ways-any-good.740219/#post-10030241

First, the rationale from Bob Betts, Rudy Bozak's right-hand man and the co-designer of the famed Bozak 909/919 preamp and 929/939 amps among others:
www.bobsamerica.com/bozak-xoveranalysis.html
After much analysis, testing, and evaluation we made the decision to accept the phase shifts at the center of the midrange band, rather than at both ends of the midrange band. We then sat back and waited for the fireworks to begin. Oddly enough, there were amazingly few! This is surprising, since customers are usually very quick to express a complaint, but remain conspicuously quiet when content. The feedback from our dealers, reps and end-users was almost unanimously complimentary. One Sunday morning I received a phone call from Benny Goodman asking when I was going to come to his studio and "...make the new repairs that I heard at the factory?"This is not a "yes" or "no" or good or bad decision. It is a gray area of engineering that is associated with the subjectivity of how we listen, what we listen for, our personal tastes, our ear-to-brain calibration from live vs. reproduced experiences (or lack thereof), and the intuitive thought process. The condition (and dilemma) of where to place the phase incoherency is a trade off - neither is technically correct when applied to a passive crossover, but quite often, the intuitive thoughts of a semi-technical evaluator will weigh in favor of the in-phase condition, only because "it seems to make sense." Oddly enough, Bozak Inc. was one of the last manufacturers to effect the midrange phase reversal. At that time, according to our research of currently available 3-way speaker products, about 85% to 90% of the speaker industry had already made the "correction" changeover.

Tobin's commentary:
forums.stevehoffman.tv/threads/tobin-mods-to-bozak-302a-urban-speakers-definitely-worth-it.75950/page-2
The early Bozaks ('50s) were never an easy first sale. I worked as the repair tech in a prominent stereo store in the '50s (yes, I was barely out of diapers) and saw this first hand: In A-B comparisons in the listening room, most first-time buyers would opt for a competing system that had more flash bang in the sound. The Bozaks are just too true, while the competing iron jumped at you. Bozak was under a lot of pressure from the dealer network to make the Bozaks sound more like the inferior competition which was selling better. Most first-time buyers, after learning how little they liked hearing the same flash and bang in everything they played, would come back to the store in a few months and say, "Uh...could I hear those Bozaks again?" But this was little consolation to the dealers, who wanted Bozak to compete for first-time sales.

The early Bozak systems were perfectly balanced - woofer to midrange to tweeters - and everything in phase. So in the early '60s, when the aluminum-coned B-209A/B midrange and B-200Y tweets came on stream, Bozak really fouled up the xovers. For starters, the polarity of the midrange was reversed. This resulted in a mid sound that was incredibly prominent without actually being louder. With the mid reversed in polarity compared with the woofs and tweets, the xover regions were cancellation notches. This 'isolated' the midrange in a manner similar to a picture which is surrounded by a wide, plain matte - it makes the subject more prominent. But the down sides were degraded overall smoothness and seriously degraded stereo imaging. Without any doubt, the reversed polarity on all Bozak N-10102A xovers should be corrected. (It is not crossed on the N-10102 xover, used with the early paper-coned B-209 midrange and B-200X tweets.

The other issue was the Y tweets. They are about 9 dB hotter (louder) than the woofer and midrange (and the previous paper-coned X tweets). Presumably this was to enable inclusion of a Brightness control which could reduce tweeter level or make it higher than flat. Only a very few systems actually had the Brightness control, mainly the early Symphonies and a few B-302A systems. After just a year or so, the Brightness control pots were eliminated. A simple network consisting of a 25 ohm resistor paralleled by a 2.0 uF capacitor was put in series with the Y tweets. The results, by today's standards, are pretty awful. It results in a big hump in the mid highs, 5.0 kHz to 10.0 klHz, allowing the natural rolloff of the Y tweet above 10 kHz to go unaided. Can you say, "Disco?"

It is not my job to help Bozak sell speakers in a tough '60s and '70s market. What I am doing is re-engineering the xovers to remove the strange tweaks and allow the world-class drivers to sing in their full, true voices, unhampered by the craziness of the '60s and '70s. To that end I designed a much better circuit to drive the Y tweeters. It is more complex than the bozak one, and works much better. It reduces the extra 9 dB level to match that of the woofs and midrange, flat, without the hump. Then, with 9 dB of 'extra' level to play with, it is used to extend the extreme high range, boosting from 10 kHz up to the tweeter's normal limit of about 16 kHz. The result is highs that are very smooth; no peaks, no dips, and a smoothly extended upper range.

Betts also has an observation about transient response:
www.bobsamerica.com/bozak-xoveranalysis.html
If a speaker sounds like the sound is coming from inside the box, then it probably has poor transient capability, and if it sounds dull and lifeless, then the damping qualities are probably not very good. Here’s a standard test that engineers have used over the years: Play a known (to you), small jazz combo of acoustical (not electronic) instruments and listen to the bass drum and string bass. Are they separate and distinct? Or is the woofer just flopping around in rhythm to the beat? Bass is bass, but what is it that makes up the bass—can you tell by listening? So this is basically why two loudspeakers with similar “published” specifications can sound so vastly different. It would seem that no one ever offers specifications on IM, harmonic, and phase distortions. In my 40-plus years as an audio products design engineer, it has never ceased to amaze me how audio manufacturers perpetuate the virtues of “flatness”—linearity—without even so much as a mention of other physics characteristics. Over the years, amplifier producers have been forced, by public demand, to publish such numbers as intermodulation distortion, harmonic distortion, damping factor, etc. But remember that these figures are gleaned, gathered and garnered on a test bench using sine waves as audio signals and resistors, not loudspeakers, as loads. Seldom will you hear any discussions concerning “dynamic stability” or “transient reproduction.” Likewise, the loudspeaker industry suffers similar, if not worse, negative virtues.
 
I had an instinctive negative reaction to the idea of dumping substantial low frequency energy into a midrange (the B800A, without capacitor). Just intuitively, it seems wrong to dump all that power into a speaker that cannot convert it into sound. The energy has to go somewhere; it can't just disappear. First law of thermodynamics, you know. So where does it go? Either it has to be given off as heat, perhaps heating up the voice coil, or being radiated as heat via the aluminum cone; or else it is reflected back to the amplifier as a circulating line current. Like a power factor issue. So in theory, it sounds messy.

On the other hand. The sound. As described by Dr. Biggles (and I believe some others), the B800A merits adjectives like "smooth," "creamy," "wide" "clarity" and "depth." Wow.

So it's like many other hi-fi issues. It depends on personal preference! No one can tell me which driver I will like better. Got it. I think I'm in for some experimenting!

Retrovert, thanks for taking the trouble to dig up those references. Very informative!
 
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I had an instinctive negative reaction to the idea of dumping substantial low frequency energy into a midrange. Just intuitively, it seems wrong to dump all that power into a speaker that cannot convert it into sound. The energy has to go somewhere; it can't just disappear. First law of thermodynamics, you know. So where does it go? Either it has to be given off as heat, perhaps heating up the voice coil, or being radiated as heat via the aluminum cone; or else it is reflected back to the amplifier as a circulating line current. Like a power factor issue. So in theory, it sounds messy.

Not exactly. This is not the First Law of Thermodynamic, it is Joule's First Law.

The current through a voice coil, like any inductor, always, as necessity, returns to the amplifier, as a complete circuit is required for current flow. Electrons do not evaporate into the aether, they move in a circuit from negative to positive. What happens during this process is that the current (electrons) passing through the resistance of the voice coil results in ohmic heating, as the voltage (energy) is converted into heat. The technical name for this process is "Joule Heating", as Joule was the first to observe that passing a current through a conductor produces heat and formulate a law. Lenz had independently observed resistive heating in conductors, but had not worked out as much as Joule. The phenomenon is consequently known either as Joule's First Law, or sometimes as the Joule-Lenz Law to acknowledge Lenz's work. Regardless of the name, the law states that P = I^2 × R.

In practice the ohmic heating it far from a theoretical issue, and is significantly messier, and more expensive, than you might think, as the midrange driver blows up: the voice coil melts or burns, the cone fragments, and the cone assembly may jump out of the normal path and be damaged. This is a good way to destroy a perfectly good midrange, resulting in replacement accompanied by the ka-ching! of the cash register.

The issue is not that the cone is damaged because it cannot convert current into magnetic field, for it can and does. Even if the cone is not moving because the cone will not vibrate at that frequency current is still flowing through the voice coil and heat is still generated. Current flow does not cease even if cone movement ceases. Here's a simple way to prove that. Wire up a coil as an electromagnet with an ammeter. The coil still heats up even when the magnetic is not near any steel, and current still flows. Wrap wire around a steel bolt as a core and you'll see how it works.

The issue, instead, is that the voice coil of a woofer contains greater mass (thicker wire) for greater power handling, and is therefore far more robust than the voice coil in a midrange which must be lighter to faster move. The increased mass of the woofer's voice coil, however, creates inertia, i.e. an opposition to change in motion, which thus slows down the cone movement, thereby limiting the highest frequencies which may be reproduced. Beyond that, the woofer reproduces longer waves which require higher power levels and the cone thus has greater excursion than the midrange, and must be differently designed to be more robust. A midrange cone must be light and fast to reproduce higher frequencies, and it is consequently vulnerable to excursion damage, a physical damage to the entire assembly.

The speaker gods giveth and the speaker gods taketh away.

Cooling drivers is complex; aluminum bobbins conduct heat, the dust cap is used to perform cooling, ferrofluid conducts heat, over-hung voice coils are used to both prevent excursion damage and increase cooling.

On the other hand. The sound. As described by Dr. Biggles (and I believe some others), the B800A merits adjectives like "smooth," "creamy," "wide" "clarity" and "depth." Wow. So it's like many other hi-fi issues. It depends on personal preference! No one can tell me which driver I will like better. Got it. I think I'm in for some experimenting!

It is not clear to me that the clarity will deleteriously suffer in the midrange if a conventional high-pass filter is constructed using polypropylene capacitors (or PTFE if one has the money) constructed with suitable by-passing as I have elsewhere outlines. Disclaimer: I have not done the A/B comparison, but I have a reasonable amount of knowledge in this area.

I caution you that a midrange may not be operated at any reasonable volume without a high-pass filter or it will melt or the lightweight cone will be ruptured. The thin aluminum cone is unable to reproduce those low frequencies at significant power output without suffering catastrophic damage.

I further caution you that beyond blowing up the midrange, should you remove the high-pass filter on the midrange you are now running the woofer and midrange in parallel, thereby halving (more or less, as the two drivers do not have matching impedance curves) the impedance of the two drivers (parallel resistors reduce impedance, unlike parallel capacitors which are additive) and thereby altering the crossover point for the low-pass component. This is why woofers in series for a 2.5 way have a different low-pass filter (inductor), as the drivers, of necessity, are either wired in parallel or series. The impedance change will not matter for solid-state, provided the overall impedance does not dip low enough to blow the output devices, but because of reflected impedance through the output transformer will consequently alter the load-line seen by the output tube, resulting in distortion.

What you are pursuing is impossible to realize without a modified driver.

Biggles and I had long ago discussed this as a gedanken experiment, where I proposed stiffening the surround of a non-A suffix B-800, thereby raising Fs, by coating it to make it into an A-suffix driver, but this would require a number of sacrificial drivers to achieve success. It also is not clear to me that the mechanical limitation will not roll off into the low end of the driver's frequency response, as the mechanical limitation is not a brick wall. I still see no value in performing this experiment, and any results would be ad hoc. I would not suggest making such a modification to the B-209. Even though the mechanical limitation will prevent destruction, the drivers are still in parallel to some degree, altering the impedance. Increasing cone mass also impedes high-frequency response, and, as a related issue, a cone which is too stiff will have ringing. This is why the B-209A required a damping ring, until the surround could be redesigned for the B-209B and its variants Tinkering with the surround stiffness may raise Fs, but as a by-product create ringing which degrades the sound.

This is a complex issue and I do not think it will be easily applied to make a crossover-free Bozak driver to which one would want to listen.

The speaker gods giveth and the speaker gods taketh away.
 
There's only one way to settle this. I just pulled the trigger on a pair of B-800A. Most likely at some point I will pick up a pair of the six inch mids to try out as well. But first I will see about getting some B200YA tweeters. Soon I will want to talk about crossovers.
I lurked through all the other Bozak threads and didn't see anything on alternative cabinet ideas. I want to start one about my ideas for my Bozak Symphony # 1/2.

Thanks for the help, all. You are the go-to guys!
 
Retrovert, I agree with everything you said. I taught electronics for years, and I'm familiar with the principles you mentioned. I would just add that the first law of thermodynamics comes into the matter from the standpoint that the low-frequency energy still has to be accounted for, even if the cone doesn't move. Just as you said, it can't just disappear. It turns to heat. Entropy. As the second and third laws of thermodynamics explain. As far as returning to the generator, I'm not talking about electron flow. Of course there is a complete circuit. But in AC circuits where reactance is present, there is an effect of "power factor" which means that not all of the current delivered does useful work, but rather circulates as reflected line current. I'm only speculating about whether that might apply to a speaker circuit in which the electric energy is not allowed to move the voice coil. It's probably WAY not relevant for me to throw that in!

Now, as to the other thing, I think I might have given the impression that I wanted to run a B-209A without a capacitor. I don't! But I believe it's OK with the B-800A, is it not?
 
Retrovert, I agree with everything you said. I taught electronics for years, and I'm familiar with the principles you mentioned. I would just add that the first law of thermodynamics comes into the matter from the standpoint that the low-frequency energy still has to be accounted for, even if the cone doesn't move. Just as you said, it can't just disappear. It turns to heat. Entropy. As the second and third laws of thermodynamics explain. As far as returning to the generator, I'm not talking about electron flow. Of course there is a complete circuit. But in AC circuits where reactance is present, there is an effect of "power factor" which means that not all of the current delivered does useful work, but rather circulates as reflected line current. I'm only speculating about whether that might apply to a speaker circuit in which the electric energy is not allowed to move the voice coil. It's probably WAY not relevant for me to throw that in!

Uh, not really. The core issue is not thermodynamics. The energy need not "be accounted for" as if it would otherwise evaporate into the aether. The issue is what frequency bands move through the voice coil of each driver. That's why we use multiple filters to divide current depending upon driver characteristics. Remove one of those filters and out-of-band signal now passes through the driver.

I think you may be confusing heating and thermo because Joule's First Law and Thermodynamics First Law had a similar-sounding name. Yes, energy is neither created nor destroyed, but that's not the core issue before us. The energy moving through the voice coil, which is a function of current moving through the midrange's filter — either a band-pass (traditional surround) or a low-pass (mechanically limited surround) — but the current always makes a complete circuit from ground through one side of the output stage. The lack of a high-pass filter forces the midrange to continually pass current from lower frequencies normally segregated and sent to the woofer, but not make any sound from it. This requires a more robust voice coil or power limiting. I don't see how the surround not moving alters the current through the voice coil.

Remember, the wire heating occurs regardless of whether or not the cone moves. The ΔT is higher when the cone isn't moving air past the voice coil.

Tweeters heat up and burn out, which is why ferrofluid and heatsinks are used for cooling, along with pumping air through the assembly by the mechanical cone movement. A tweeter cannot properly reproduce low-frequency sound, being mechanically limited, so by your argument no tweeter high-pass filter is needed: just run it full range and it won't reproduce lower signal. Nuh-uh. Not unless the tweeter is intended to go to Valhalla.

The issue is ohmic heating of the wire as explained by Joule's First Law. Current flow and voltage drop.

The strength of an magnetic field generated by a coil varies by ampere-turns per meter, neglecting as constant the wire gauge (for this example) F ≈ I^2 × N^2. So number of turns and current are clearly related, if gauge is held constant. We could rewrite that to be F ≈ (I × N)^2. So one may see that if current is constant and the gauge is constant, the number of turns, controls both field strength and cone inertia. Resistance controls current so voltage becomes an issue. We may also rewrite magnetic strength in terms of voltage because the wire resistance will control current as per Ohm's Law. If we want to move the same current through a higher resistance the voltage must increase.

Now, as to the other thing, I think I might have given the impression that I wanted to run a B-209A without a capacitor. I don't! But I believe it's OK with the B-800A, is it not?

Yeah, not so much for the reasons I have outlined.

It is physically and electrically impossible for the surround to mechanically function as a brick-wall, i.e. blocking everything below, say, 100 Hz and nothing above it. Impossible!

Even if it did, and it does not, consider what would happen with various drivers. The B-800B variant has an Fs of 37 Hz, specifically lowered from the 50 Hz delivered by the straight 800, and was intended to be more suitable for a coaxial system with the B-800B as a full-range driver and a separate tweeter. It thus functions as a woofer and midrange. The B-800A is limited to 100 Hz.

So if the B-800A is mechnically limited purely to 100 Hz to prevent damage, and the woofer is running to 400 Hz as it normally does, you have overlapping drivers from 100 Hz to 400 Hz! That's just a fact. Why are you adding driver overlap between the B-199 and the B-800? What possible good outcome can arise from that? Yeah, ok, the B-800A has a rolloff, so it likely limits at something like 6 dB / Octave and thus gently rolls off to maybe 300 to 400 Hz, so the overlap is smaller. Plus it sort of acts as a bass boost, but the B-199 in a B-302 is producing enough on its own in the desired region. In the Concert Grand the four are production plenty of bass. But the fact remains that overlap does exist, and out-of-band signal is passing through the driver which may cause other issues beyond the impedance drop. Plus the boost may make the region overlapping with the woofer more prominent. That might require attenuation in that region.

The fact is that most humans who are not musicians do not hear particularly inaccuracies well below 400 Hz, and the ginormous size of the Concert Grand is creating all manner of convergence issues amongst the woofers, so the overlap from the fifth woofer is likely not heard at all, as it acts like another woofer. But it's still there!

While not entire dispositive on its own right for obvious reasons, the technique of mechanically limiting drivers is not generally used and for good reason: it causes distortion from cone breakup. Woofers in coaxials are typically run this way to save money by eliminating the crossover. Yeah, it eliminates some phase shift, but humans generally poorly hear that. Many fine speakers were built with first-order crossovers instead of using the surround as a crossover.

Edit: clarified a few thoughts.
 
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"Remember, the wire heating occurs regardless of whether or not the cone moves. The ΔT is higher when the cone isn't moving air past the voice coil."

--Yes. And also because the stationary motor with current going through it, isn't generating any back-EMF.

"Tweeters heat up and burn out, which is why ferrofluid and heatsinks are used for cooling, along with pumping air through the assembly by the mechanical cone movement. A tweeter cannot properly reproduce low-frequency sound, being mechanically limited, so by your argument no tweeter high-pass filter is needed: just run it full range and it won't reproduce lower signal. Nuh-uh. Not unless the tweeter is intended to go to Valhalla."

--Sure. But somehow the B-800A is apparently designed to withstand that thermal stress.

"The issue is ohmic heating of the wire as explained by Joule's First Law. Current flow and voltage drop."

--I have no problem with that!

"It is physically and electrically impossible for the surround to mechanically function as a brick-wall, i.e. blocking everything below, say, 100 Hz and nothing above it. Impossible!"

--Yes I think the rolloff idea you mention below is more realistic.

"So if the B-800A is mechnically limited purely to 100 Hz to prevent damage, and the woofer is running to 400 Hz as it normally does, you have overlapping drivers from 100 Hz to 400 Hz! That's just a fact. Why are you adding driver overlap between the B-199 and the B-800? What possible good outcome can arise from that?"

--I have no idea. I guess the overlap was more of a by-product of eliminating the phase shift, rather than a goal.

"Yeah, ok, the B-800A has a rolloff, so it likely limits at something like 6 dB / Octave and thus gently rolls off to maybe 300 to 400 Hz . . ."

--I read this ten times, and I don't get the part about rolling off to 300 to 400Hz. Unless you mean the LF rolloff begins at maybe 300 or 400Hz, rolling off below that point and moving towards 100Hz. That would certainly be a real-world scenario, much more realistic than the "brick wall" thing (which I agree is impossible).

" . . . so the overlap is smaller. Plus it sort of acts as a bass boost, but the B-199 in a B-302 is producing enough on its own . . ."

--Yes I thought about how the overlap might augment the bass. But the augmentation would be in a band where the B-199 needs no help, which I know is your point also. Again, I think the overlap is just there, a by-product of eliminating the capacitor, and not the reason for eliminating the capacitor. I imagine it colors the sound, maybe not in a good way.

"But the fact remains that overlap does exist, and out-of-band signal is passing through the driver which may cause other issues beyond the impedance drop. Plus the boost may make the region overlapping with the woofer more prominent. That might require attenuation in that region."

--Yep. Again, I think we agree on that.

" . . . and the ginormous size of the Concert Grand is creating all manner of convergence issues amongst the woofers . . ."

--You used the term "convergence" before. What is that, in speaker terms? Is it about phase cancellations? I haven't seen this term used before.

"Woofers in coaxials are typically run this way to save money by eliminating the crossover."

--At the high end of the woofer's range, you mean? To eliminate the need for an inductor.

So. Your point is that while eliminating the phase shift is a good idea in itself, it isn't worth doing if it's going to cause so many other complications. Got it. These would all be reasons why it might make more sense to use the B-209, then. Still, that "smooth and creamy" sound of the B-800A seems seductive. I'll probably wind up with a stash of Bozak drivers before I get this sorted!

Thank you.
 
Dude, you so totally need to put in the time to cut-and-paste the quote/end-quote tags to make it readable. Word.

And also because the stationary motor with current going through it, isn't generating any back-EMF.

It's not perfectly stationary so the back-EMF is not zero. The cone still moves, but the waves are heavily damped and not radiated. The surround muffles the sound.

But damping of back-EMF is an amplifier issue, not a crossover issue.

But somehow the B-800A is apparently designed to withstand that thermal stress.

Well, this is an energy spectrum issue. Most of the energy in music is going to be at the woofer. The question is how much additional energy is flowing into the midrange from roughly 100 Hz to 400 Hz.

I wrote:
Yeah, ok, the B-800A has a rolloff, so it likely limits at something like 6 dB / Octave and thus gently rolls off to maybe 300 to 400 Hz . . .

I read this ten times, and I don't get the part about rolling off to 300 to 400Hz. Unless you mean the LF rolloff begins at maybe 300 or 400Hz, rolling off below that point and moving towards 100Hz. That would certainly be a real-world scenario, much more realistic than the "brick wall" thing (which I agree is impossible).

I was observing that the mechanical limitation of the surround begins removing sound above 100 Hz at (speculation) 6 dB / Octave. So while Fc is 100 Hz, not much signal is around until 300 to 400 Hz, so it's not adding a huge amount of overlap with the woofer. Someone should measure this. It's probably 12 dB / octave to make this work.

Making a brick-wall filter using real-world components, including inductors and capacitors but also surrounds, is tricky. Even ceramic filters have a few hundred Hz to several kilo Hz of rolloff. Plus ringing. Analog is messy.

Yes I thought about how the overlap might augment the bass. But the augmentation would be in a band where the B-199 needs no help, which I know is your point also. Again, I think the overlap is just there, a by-product of eliminating the capacitor, and not the reason for eliminating the capacitor. I imagine it colors the sound, maybe not in a good way.

Not my point at all. The overlap is an undesirable and unintended artifact which cannot be removed using a mechanical filter, but this may not much matter in practice. That was my point.

I wrote:
. . . and the ginormous size of the Concert Grand is creating all manner of convergence issues amongst the woofers . . ."

You used the term "convergence" before. What is that, in speaker terms? Is it about phase cancellations? I haven't seen this term used before.

The sound to blend together instead of being perceived as originating from separate point sources. The desirability of a point-source explains why full-range drivers and coaxial/triaxial drivers are preferred.

Large speakers with separated drivers do not sound good until one is far back. This is why the larger Bozaks do not work in smaller rooms. Just a fact of life. Biggles sold off his Symphony project for exactly this reason. In a small room the dual woofer, with its separated drivers, sounded exactly like separate drivers. I have seen Concert Grand owners with too-small rooms, such that listening decomposes to near field, but the owners apparently don't care. No accounting for taste.

Again, witness the preference for a full-range drivers with point-source characteristics.

I wrote:
Woofers in coaxials are typically run this way to save money by eliminating the crossover.

At the high end of the woofer's range, you mean? To eliminate the need for an inductor.

Yes. Inductors are expensive, even iron-core ones, particularly in high-volume situations.

The coaxial speaker uses only a tweeter inductor because the tweeter would otherwise burn out from the out-of-band energy. Plus it would sound, really, really bad.

So. Your point is that while eliminating the phase shift is a good idea in itself, it isn't worth doing if it's going to cause so many other complications. Got it. These would all be reasons why it might make more sense to use the B-209, then. Still, that "smooth and creamy" sound of the B-800A seems seductive. I'll probably wind up with a stash of Bozak drivers before I get this sorted!

Much of that description may be for the B-800 as a full-range driver. It's a wonderful speaker. I'll need to ask Biggles. I just don't think the upper end is going be as clean as the smaller 6" cone of the B-209. Measurements are required.

Anyway, the point is we may not be able to hear that phase shift so the elimination is a non-starter. I would argue that first-order phase shift is not so terrible that it ruins the sound. We have many wonderful speakers with first-order crossovers. Reproduction of sound is an approximation, we do what we can and accept the limitations of the world because we must.

Rule 5 of Bozak Cult: Loudspeakers are competing forms of millenarism seeking to immanentize the audio eschaton, so experimentation upon Bozaks is not merely encouraged, but respected, even when it fails, as true knowledge must be painfully acquired.

The B-800 has advantages in that it can be lower run which would permit the B-199 to be offloaded at a lower point. This is why I will someday build a five-way using the B-800 running from somewhere like 200 to 300 Hz to 600 Hz. Take the crossover hits where humans (at least other than Bud Fried) do not particularly well hear.
 
Retovert, it looks like you were earlier thinking that woofer/midrange overlap could be a good thing, but later apparently changed your mind. At first, you seem in favor of the idea:

Assuming the B-800 / B-800A would work in the same frequency band, another option is running the B-800 down to 100Hz and overlapping the B-199 woofer to improve the lower frequency response. This would essentially be a woofer and midwoofer. The disadvantage of running the midrange lower (provided it can, of course, act as a midwoofer without damage, which a B-800 / B-800A can do) is lower efficiency, but I'm not concerned as I listen at low volumes . . .

So a second woofer-class driver would, presumably, substantially boost the bass.
Still running the B-199 to 400 Hz as per Tobin? So the overlap is only between the B-800 and B-199 from 200 to 400Hz? Why not go lower?

And here, you found reasons to question it:

So if the B-800A is mechnically limited purely to 100 Hz to prevent damage, and the woofer is running to 400 Hz as it normally does, you have overlapping drivers from 100 Hz to 400 Hz! That's just a fact. Why are you adding driver overlap between the B-199 and the B-800? What possible good outcome can arise from that? Yeah, ok, the B-800A has a rolloff, so it likely limits at something like 6 dB / Octave and thus gently rolls off to maybe 300 to 400 Hz, so the overlap is smaller. Plus it sort of acts as a bass boost, but the B-199 in a B-302 is producing enough on its own in the desired region. In the Concert Grand the four are production plenty of bass. But the fact remains that overlap does exist, and out-of-band signal is passing through the driver which may cause other issues beyond the impedance drop. Plus the boost may make the region overlapping with the woofer more prominent. That might require attenuation in that region.

I wanted to clarify if you think the overlap is a bad idea:

A. Mainly for the B-800;
B. Mainly for the B-800A;
C. A bad idea period.

For one thing, you concluded the additional boost is probably not needed.
But also, you refer to the out-of-band signal passing through the driver possibly causing other issues beyond the impedance drop.
Questions about that:

A. Does the "other issues" refer to the B-800A cone breakup you discussed earlier in the below 100Hz band? And/or possibly even occurring above 100Hz? Or something else?
B. How does impedance drop come into the picture? Is that an artifact of the cone being immobilized below 100Hz? Apparently though a reduction of back-EMF? That's what I'm reading into it, that the impedance drop occurs at or below 100Hz?

Also, I believe in order to add bass boost with the midrange driver, it probably needs not to be under a salad bowl in order to be working into adequate volume. But to provide the best sound, isolated from the B-199A, it needs to be under the salad bowl. Something of a paradox. That would seem to argue against overlap.

Your thoughts?
 
Time-Alignment , Group Delay, and Distortion

Like any 8" driver, the B-800 does not well reproduce lower frequencies. So the issue becomes how much distortion accrues. The driver's position is likely within 1/4 wavelength, so the comb artifacts are not a significant problem.

The time-alignment — which varies with frequency — between the B-199 and B-800 will be different because the acoustical center for the two drivers is different.

How well can humans hear that? Well, I'd point to the Dahlquist DQ-10 and other time-aligned drivers.

Linear power distribution requires that the area of the radiating surface match the wavelength lengths being reproduced. This is why woofers cannot reproduce high frequencies, and small drivers cannot properly reproduce low frequencies.

Bass-Boost Unnecessary

For one thing, you concluded the additional boost is probably not needed.

Correct.

First, the B-199 clearly requires no bass boost; that is gilding the lily.

Second, the 8" B-800's output is going to be far smaller than a 12" woofer, just look at the cone area: Area is proportional to the square of the diameter, to 64 vs 144 (note, the actually area has π in it, but since that is constant for the two we can neglect that) a factor of 2.4 difference in the area.

Impedance Shift from Parallel Drivers

But also, you refer to the out-of-band signal passing through the driver possibly causing other issues beyond the impedance drop. Questions about that:
A. Does the "other issues" refer to the B-800A cone breakup you discussed earlier in the below 100Hz band? And/or possibly even occurring above 100Hz? Or something else?
B. How does impedance drop come into the picture? Is that an artifact of the cone being immobilized below 100Hz? Apparently though a reduction of back-EMF? That's what I'm reading into it, that the impedance drop occurs at or below 100Hz?​

Not quite. Back-EMF has no bearing on this situation. That does not alter the overall speaker's (aggregate) impedance.

Back-EMF arises because, as Faraday observed, moving a wire coil in a magnetic field induces current flow through that wire. Mechanical energy converted to electrical energy. A motor in reverse. Basis for alternator and generators. So as the cone returns to the rest position a current through the voice coil is generated, aka back-EMF. This back-EMF is absorbed by the amplifier. Smaller drivers have smaller voice coils and smaller excursion, thus generating smaller amounts of current. The core issue here has nothing to do with the surround damping out the lower frequencies and cone movement. Think, instead, about current flow through the voice coil, because that's all that matters from the standpoint of impedance.

Without any filter for the midrange the current flowing between the amplifier terminals, i.e. flowing from one side to the other (it's AC so we can't say from – to +, only from terminal to terminal) therefore simultaneously passes through the voice coils in both drivers at the frequencies where the drivers overlap. The drivers, therefore, are in parallel, which is now half the impedance for the overlapped region, which will shift the loadline for a tube amplifier, but does not matter for solid state, provided, of course, that the impedance does not too low drop.

Remember, the B-199 has an inductor so current only flows through its voice coil, again subject to rolloff, below 400 Hz. The B-800A used as a midrange has no high-pass filter, so current flows all the way down to 100 Hz and below that down to DC. The cone's lack of movement does not stop current flow through the voice coil.

The crossover electrically isolates the different drivers which is why the impedance remains constant even though three drivers are present. Subject to overlap from rolloff, of course, but as one driver is rising the other is falling so the impedance curve remains flat. (Yeah, not exactly, because driver impedance is a convenient fiction, but you get the idea.)

Midrange Enclosure Now Necessary

Also, I believe in order to add bass boost with the midrange driver, it probably needs not to be under a salad bowl in order to be working into adequate volume. But to provide the best sound, isolated from the B-199A, it needs to be under the salad bowl. Something of a paradox. That would seem to argue against overlap.

Yes, the cover is too small for linear bass response, i.e. below the normal midrange band which would occur using the high-pass filter, and the backwave would likely cause some distortion.

The question, again, is what is the driver rolloff between 100 Hz and 400 Hz? If the B-800 tends to not properly reproduce those frequencies the overlap is small and the B-199 dominates. Since the Concert Grand has four B-199s, it stands to reason that the contribution of the B-800, and any ensuing distortion, is small. But small enough to be invisible? Probably not if one had the A/B comparison. The B-800 system may simply have better dispersion of the midrange by way of the larger cone, so the perception may be that of a louder midrange, which is where humans best hear, and this increase in volume may be perceived as desirable, much like an inverted bathtub curve on an equalizer. Look at the purported benefits of the inverted polarity midrange for those who cannot hear absolute polarity.

Removing the cover would cause the very cross-modulation, i.e. between woofer and midrange, we now prevent with the flower-pot cover. That cover, again, was not put into the smaller Bozak cabinets to reduce manufacturing costs. Or so I would assume. I can see not benefit to the sound for omitting it, and we see the benefits of using the flower pot. Seems to be purely an economic issue.

So the B-800 would require an internal cabinet suitable for 100 Hz, basically the same type of cabinet one would use for a B-800 operated as a full-range driver as in the Sonata 1 or the B-801. The small B-800 models — LS-200 and DMS 2500 — are both ported cabinets. The ported versions produce less, but more accurate, bass with the port plugged, but the 1 to 2 cu ft cabinets are a bit too small for the driver used as a woofer. Any substantial cabinet will rob volume from the B-199. Less critical in the large Concert Grand, more critical in the smaller B-302.

Speculation that Economics, Not Sonics, Was the Reason for Elimination of Midrange's High-Pass Filter

The whole concept of the capacitor-less filter for the midrange may, in fact, be based purely upon the high expense of PIO capacitors of 1950s and 1960s, not merely the low performance which was not particularly good, even when new. Our polypropylene capacitors are light-years beyond the 1960s PIO.

I expect the goal was eliminating the expense of a large bank of capacitors necessary for the midrange. The cost for a 50 µF capacitor in those days would have been high. In 1963, Lafayette lists an oil-filled metalized capacitor of 8 µF at $1.19, so figure $6 for the full bank, but Bozak would have paid about 1/3 of that wholesale, so about $2. That's still expensive: about $40 in today's income. (The B-800 cost $50 at the same time, so the capacitor would have been 5% of the cost of adding the midrange, plus, of course, the expense of the inductor.)

Remember, inflation has been terrible. In 1960 the median family income was $5,620 (I looked it up) or $107 per week, and that was pre-taxes. So figure that median family kept about $75 after federal and state. Housing was less than one third of what it was, in constant dollars. For purposes of ready comparison, a skilled factory workers made somewhere around $2 per hour (pre-tax) and the minimum wave was $1.25 per hour (pre-tax).

A non-polar electrolytic would have been less expensive, of course, but would have had a terrible sound. So that was the Hobson's Choice which Bozak was attempting to circumvent.

TL/DR

Retovert, it looks like you were earlier thinking that woofer/midrange overlap could be a good thing, but later apparently changed your mind. At first, you seem in favor of the idea:

Mmmm, not so much. I never was in favor of it, just observing that it might not be entirely as bad as I initially thought.

I wanted to clarify if you think the overlap is a bad idea:
A. Mainly for the B-800;
B. Mainly for the B-800A;
C. A bad idea period.​

Yes, Yes, and Yes! Three chances to win, and you hit all three! Woo-hoo!

I think this is enough to kill the idea that running the midrange as a full-range driver to eliminate the capacitor is a poor choice, both for the economy of eliminating the high-pass filter (capacitor) and foolhardy from the perspective of sonics. I think this was done purely to save money, not because of the sonics. Remember, a modified B-209 could have been generated if this was such a great idea.

You could, of course, try the B-800 both with and without a polypropylene capacitor, use a switch for proper A/B testing, and see what happens. I'd be surprised if the no-capacitor version sounded better.
 
My reason for bringing back-EMF into it was that when an electric motor is in overload, and draws too much current, or is seized up and draws still more current, and consequently either trips a breaker or burns up, the reason is that when it's running normally, the back-EMF opposes the current to an extent, thereby mitigating the current draw. But when it stalls or freezes, there is no back-EMF, the current exceeds design limits, and the motor burns up. Now, a dynamic loudspeaker, being basically an electric motor, ought to do the same thing. So I reasoned that if the cone is restricted from moving much in response to the low frequency energy, then it might be drawing more current, which would be another way of describing an "impedance drop." Just sticking my neck out a bit in order to understand your post.
 
I had B 4000 contemporarys that I helped built the enclosures from kits, assemble and I had the B-800's and changed to the 800 A. It mated better with my B-199's. and 200 Y's. A very pleasant balance and easy to listen to in all environments. The Symphonies with the B-209 BC could get hard and penetrating real fast in bright environments. I have B-4005's now and B-410's. The 410's have the older Alnico 209B the 4005 and the 313's have the bc. But in my case I now use parametric EQ's and the Symphonies are bi amped crossing at 250 HZ at 12 db per octave, and the Grands tri amped with super tweeters and crossed at 250 HZ and 10,000 HZ using the steeper crossover rate. The N-107 crosses the mid/tweeters with the original balance and out of phase relation ship. With some minor 1 to 3 db changes the 209/ 200y and Yc blend very gracefully. the 313s are stock. So I have had to attenuate the 209 in the crossover and use further electronic equalization to make them flat enough for HT side channel use. When my Grands were new fresh out of the box I was startled how hard sounding they were compared to my 4000 Symphonies. I padded down my room as best I could adding heavier drapes etc and thick carpet. I decided then and there to bi-amp as the idea was just being introduced to tame the mids a bit. When I changed to direct couple amps to improve the bass over tube amps I had to further tame the mids. Today I'm very happy after I finally got things the way I wanted them in 2008. Changing amps even though the frequency response stayed the same made for a much more pleasant experience. But watch out the 209s want to take the lead and you have to be mind-full or they will conquer the entire system, Something my B-800 A's never did. The top EQ was for the speaker touch up. The bottom a program EQ. Image7-68.jpeg9.jpeg
 
Twiiii, this is making me feel really good about selecting the B-800A for my project!

I love that top photo! My favorite style of the Symphony #1, and the McIntosh tube amps. I don't think I could have given any of that up!

I wonder what the center amp was for.

The bookcases look like they were built to match the style of the Symphonies!
 
I had B 4000 contemporarys that I helped built the enclosures from kits, assemble and I had the B-800's and changed to the 800 A. I have B-4005's now and B-410's.

Twiiii, do you find that the B4005, with the B310 type tweeter array, images as well as the column array of the B4000?
 
I had B 4000 contemporarys that I helped built the enclosures from kits, assemble and I had the B-800's and changed to the 800 A. It mated better with my B-199's. and 200 Y's. A very pleasant balance and easy to listen to in all environments. The Symphonies with the B-209 BC could get hard and penetrating real fast in bright environments. I have B-4005's now and B-410's. The 410's have the older Alnico 209B the 4005 and the 313's have the bc. But in my case I now use parametric EQ's and the Symphonies are bi amped crossing at 250 HZ at 12 db per octave, and the Grands tri amped with super tweeters and crossed at 250 HZ and 10,000 HZ using the steeper crossover rate. The N-107 crosses the mid/tweeters with the original balance and out of phase relation ship. With some minor 1 to 3 db changes the 209/ 200y and Yc blend very gracefully. the 313s are stock. So I have had to attenuate the 209 in the crossover and use further electronic equalization to make them flat enough for HT side channel use. When my Grands were new fresh out of the box I was startled how hard sounding they were compared to my 4000 Symphonies. I padded down my room as best I could adding heavier drapes etc and thick carpet. I decided then and there to bi-amp as the idea was just being introduced to tame the mids a bit. When I changed to direct couple amps to improve the bass over tube amps I had to further tame the mids. Today I'm very happy after I finally got things the way I wanted them in 2008. Changing amps even though the frequency response stayed the same made for a much more pleasant experience. But watch out the 209s want to take the lead and you have to be mind-full or they will conquer the entire system, Something my B-800 A's never did. The top EQ was for the speaker touch up. The bottom a program EQ. View attachment 1831623View attachment 1831624

When is the color photo from, and what was the MC60 on the TV for? Those photos are an amazing time capsule, looks to me like you had a lot of fun.
 
because there is a Bozak B-207 and a B-209b mounted in the TV acting as a center channel. There a switch that selects the input for the MC 60, either the TV or the C-22. The picture was taken around 64 or 5. The Picture of the Grands about 74. There was a MR-77 and a C-28 with A Thorens TD 125, and my Ampex F-4460 in the top of the cabinet. There were a few changes over the years. In 76 the Bottom SAE was replaced by a Crown EQ2, which I still have today. The Pioneer Crossover was replaced by a Urei. So much better. The C-28 nd MR 77 were replaced with. a C-29 and a MR-78 and then a few years later a MR-80. The F-4460 was pulled out in the early 80's and the space left vacant to this day where often used manuals and headphones reside. The Thorens is still there but cartridges have come and gone over the years. I guess I had the Stanton 881 and 981 Hzl the longest. But I have been a Dynavector owner now for 12 years. 3 different ones for the Thorens. 10 x4, a gift then the 10 X5 and after the 20X. For the past 10 or so years I wanted to up grade my Thorens, but couldn't find anything I was thrilled with for the small space. Well I finally decided I didn't need the Cassette machine and S- vis player of the Sony SL-1800 super beta machines. So I reorganized thing s and my New TT was installed Monday, with a Dynavector 20 X 2. It feeds the HT processor.
 
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My reason for bringing back-EMF into it was that when an electric motor is in overload, and draws too much current, or is seized up and draws still more current, and consequently either trips a breaker or burns up, the reason is that when it's running normally, the back-EMF opposes the current to an extent, thereby mitigating the current draw. But when it stalls or freezes, there is no back-EMF, the current exceeds design limits, and the motor burns up. Now, a dynamic loudspeaker, being basically an electric motor, ought to do the same thing. So I reasoned that if the cone is restricted from moving much in response to the low frequency energy, then it might be drawing more current, which would be another way of describing an "impedance drop." Just sticking my neck out a bit in order to understand your post.

Ummm, no, not so much. This is not what happens.

I suggest not speculating, filling your head with incorrect models, and then asking others to laboriously explain and correct the errors.

Why not, instead, seek out primary sources for this information? You'll find many detailed and accurate explanations with diagrams. Continually speculating, developing incorrect models, and then requesting a from-scratch reproduction of information to correct the misapprehension is highly time consuming, and the approximations and summaries are never worth the fighting and quibbling which ensue, nor the wasteland of a locked thread. Certainly not when numerous definitive explanations, embodying many tens of thousands of hours of work by widely respected authors and commentators, exist.

I instead suggest turning to any of the standard learned tomes, as these will adequately explain the issues in gory detail, with meticulously created text and diagrams.

Even Wikipedia would be better than speculating and filling your head with incorrect information which only requires self-debunking.

A basic book on speakers will explain the issues. I suggest Loudspeaker Design Cookbook 7th Edition by Vance Dickason.
 
because there is a Bozak B-207 and a B-209b mounted in the TV acting as a center channel. There a switch that selects the input for the MC 60, either the TV or the C-22. The .

That's got to be the most hot-rodded black and white TV ever seen! What a cool setup you had.
 
For the Moon landing I bought a Sony Trinitron that sat on top for the next 9 years, till I moved to my own home. Now a 4005 Symphony sits under the Pioneer 151 plasma. And the B-4000 were updated to B410s in 1970.
 
I would again observe that Bozak could have trivially produced a similarly damped B-209 to eliminate the need for a high-pass filter in the midrange crossover.

Yet it did not. That is telling.

The fact is that throughout the Bozak's entire lifespan — both the company and Rudy — the B-209 was the most widely used midrange, appearing in every single Bozak model except for the mid-1970s low-cost budget units, which were notably ported, which instead used the B-450 to save money. That upgrade could easily have been performed if removing the crossover either (a) delivered superior sonics or (b) eliminated the expense of a crossover capacitor without impacting sonics. I further note that If the B-450 would have been able to eliminate the crossover capacitor via a surround upgrade that it, too, would have been done to save money on the line. Yet the B-450 was not modified.

We do not commonly see this type of modification made on midranges from other manufacturers, and for good reason. As I explained, placing a midrange in parallel with the woofer will:
(a) create distortion on a tube amplifier because the impedance is now halved for the region where the woofer and midrange overlap, so two different impedances exist —overlapping woofer and midrange region until the woofer's low-pass stops the overlap, and non-overlapping midrange and tweeter — and the reflected impedance is now mismatched for the tube, as an incorrect tap on the output transformer is always being used, either for the woofer-midrange region (4 Ω) or for the midrange-tweeter region (8 Ω);

(b) likely blow up a transistor amplifier without output over-current protection if the impedance falls below a few ohms, a potential problem with low-frequency reproduction;

(c) create distortion or damage with high volume:
(i) creating distortion in the midrange for the low-frequency regions not well reproduced by the cone and voice coil.

(ii) damaging the voice coil when its mechanical limits are exceeded because of excessive woofer signal.

(iii) creating voice coil heating which may alter the impedance or characteristics in the desired midrange region.​

Removing the low-pass filter (capacitor) from the midrange band-pass (capacitor plus inductor) is thus not the solution to eliminating distortion in the midrange region. It may even exacerbate it and create a worse sound than using the appropriate B-209 driver.

Edit: fixed typo.
 
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