Beyond the Ariel

Graham Maynard said:
For open baffle, I don't think that lightness of cone, and minimal voice coil inductance should be overlooked.

Did Fostex make a larger driver along these lines, which is then unsuitable for 'normal' cabinetted usage ?

Cheers ......... Graham.


This depends on the freq..

If the driver is limited to the bass region (<70 Hz), then its OK.

Beyond obtaining a suitable driver Fs - you actually want more mass as freq.s decrease (..otherwise the sound becomes "lightweight").

Here is a more suitable 21" driver:

http://www.shredmuzic.com/product_p/813-008.htm

Note that such a driver will place SERIOUS demands on the driver's support structure (..which should NOT be "hard" connected to other portions of the speaker).
 
ScottG said:

Beyond obtaining a suitable driver Fs - you actually want more mass as freq.s decrease (..otherwise the sound becomes "lightweight").

Here is a more suitable 21" driver:

http://www.shredmuzic.com/product_p/813-008.htm

Note that such a driver will place SERIOUS demands on the driver's support structure (..which should NOT be "hard" connected to other portions of the speaker).

Certainly cheap enough, at $169. Nothing wrong with a Qts=1.0 at 31 Hz and a (claimed) linear Xmax of 0.75" either.

The required passband is the same as the triplet of 12" drivers - 80 Hz to 220 Hz, where it is intended to overlap with the 12" WR driver. No FR curve, so it's difficult to tell if it's going to need an aggressive lowpass filter or not.

The 338 gram cone gives food for thought. That's a lot of mass to swing back and forth in the 80 to 220 Hz range. The magnet will obviously have to have its own support strut, going to a rigid baseplate, and a pair of sand-filled buckets on either side of the baseplate would be a very good idea. Maybe even put some lead shot in the bottom of the buckets while you're at it.

The difference in cone masses is the most obvious difference between the 3 x 12 and the single 21". Typical masses for the 3 x 12 is around 120 grams, while typical values for 21" drivers seems to be in the 300~340 gram range. That's not a small difference - and all of that is transmitted as reaction forces to the rest of the OB structure. The rear strut, which bears the magnet weights, is going to have to be well-engineered - strong, resonance-free, and low emissive area.
 
Administrator
Joined 2004
Paid Member
ScottG said:
...you actually want more mass as freq.s decrease (..otherwise the sound becomes "lightweight").

I've often read and been told that, but why?
Does the large mass of the cone move the air "better?"
Is the extra inertia needed to give the bass more subjective "weight?"

The moving mass of the 21" Madison would be the equivalent of about 270L of air. Or 9.5 cubic feet.

Is that mass needed to launch a good, solid wave? Would a lighter cone not do as well? Is the higher energy in the heaver cone thus imparted to the air?
 
Hi

Each of us pursuing individual goals just zooms in a portion of the picture. But some still have the veteran character control not to forget that the goal must be the total picture (music) and not specific technical perfection. Its a twist. We don't seek music many times when making stuff. We seek technical achievement. We get to like the sound of 'technique'. Real danger is that we may get to feel that it is the real thing, and become addicted. We are perverts many times. Its part of the game, but at a point we can get over it. And we have a powerful tool for waking up. Boredom! Non natural may succeed feeling even great, but at a point we get sick. Its like eating in fast food chains only, for too long.



salas,
I agree 100% - especially the point with boredom as a cure for us technophile addicted made me laugh out loud – really great frame!




There is one XTA DP 226 for $1400 on e-bay right now.

Seen on a bigger scale, the revolutionary thing about the DCX is its price. This was the very first DSP device that told us that sophisticated XO audio processing can be really cheap.
Copy the concept - throw in caps that do their job - a power supply that works – use less hot melt glue but ribbon wire connectors that don't fail - and set the auto router to "audiophile mode" – and Behringer could launch a smashing next generation DSP-XO unit for around € 50.- € 100.- more expensive than the old one. This is what I would like to see also from other companies like DBX, XTA...






fiacono,
an other candidate for your list ? :

http://www.precisiondevices.co.uk/asps/uploads/super/17.pdf
"http://www.precisiondevices.co.uk/asps/uploads/super/17.pdf"

maybe it would give an additional insight to also look at the division of moving mass against force factor ( B*L / Mms ) . This gives a clue about the limitation of acceleration.





just to set the record straight -

MBL,
sorry that I got you wrong, thanks for correction and also for the links!

I would have been happy to have the Griesinger paper at hand, when I installed a low cost LARS "equivalent" system in a cinema several years ago.
Cinema acoustic is dictated by the needs of artificial control of room perception – in other words: relative highly damped room with relative short RT60 and lots of surround speakers to achieve any acoustic ambience at the movie art directors will.

This works great for movies and in fact is one of the biggest benefits of the THX "standardisation" but does NOT work well for lecture or live music for silent movies.

Reverberation of the main mic's in such cases is OK but not really sufficient. You still HEAR the dead room giving a feeling of isolation.

What worked great is to mount a boundary mic into each side wall and play their reverb signal through the surround speakers. It is not that complicated to balanced towards a concert hall sound by ear, while preserving really good intelligibility.
Apparent source width ASW increases dramatically that way.

All what was needed were two low noise mic's (AKG C 562 CM ), an additional - fairly good - reverb ( TC M-ONE ) and a mixer to change room acoustic with the push of a button.


Greetings
Michael
 
panomaniac said:


I've often read and been told that, but why?
Does the large mass of the cone move the air "better?"
Is the extra inertia needed to give the bass more subjective "weight?"

Is that mass needed to launch a good, solid wave? Would a lighter cone not do as well? Is the higher energy in the heaver cone thus imparted to the air?

I'm not sure why this is.. chalk it up to one more of those "voodoo" things that makes loudspeaker construction as much an art as a science.

I believe Freddyi (who infrequently posts here, and more on the Hi Eff. board of the Audio Asylum) has either this woofer or one similar to it. In fact on the Hi Eff. forum he had (at one time) posted a measurement of the driver in an open baffle configuration.

IMO its strictly a "helper" woofer to reinforce (as an open baffle dipole) the bass freq.s. It WILL require a LOT from the pairing amplifier (current-wise), so in effect - do NOT consider it unless you are going "active".

I doubt the driver will ever be distributed (as a component) in Europe. When I purchased my Knight 10's from them they didn't even offer shipping outside the US, perhaps thats changed now?

Personally, I'd stick to the Rythmik Audio subs (..in an aperiodic enclosure OR a vented config. similar to what I recommended earlier on.. but NOT a sealed design). Its already "active", it goes lower at higher spl's, and there is no real compelling reason for a dipole at lower freq.s.

Looking at the spec.s of drivers - my OB midbass driver of choice (preferably 2X16 ohm drivers connected in parallel), is still the Jensen Neo 15-150. Its simply MUCH more efficient than other offerings EXACTLY WHERE ITS NEEDED, while having extraordinarily low mms for its sd (..for details and delicacy with the right amplifier - i.e. like the kind Lynn has). It also has its fs in the right place for such a design when considering its use in open baffle and its Qts. It does however need an appropriate low pass filter.

When I factor in cost and other attributes this is what I'd propose:

Esthetically similar to the Ascendo System M:

http://www.ascendo.de/english/frameSW.htm

Top down:

Top Module:

OB 175 mm's wide, 750-800 mms "tall" (height dependent on tweeter size).

4 PR170MO's in a vertical line.

..immediately below that:

A High eff. tweeter of choice (the Audax "line" gives you some options here because you can either cross at a lower freq. OR at a higher freq.). Though more costly, I'd choose the Aurum Cantus G1 at a lower freq. (close to 2 kHz). There are however MANY options available - including the recently mentioned Beyma Heil driver OR even the Hi Vi RT8-II that Gary Pimm uses (..as a low cost, yet low crossover capable driver).

Bottom Module:

OB 425 mm's wide, 850 mm's "tall".

2 16 ohm Jensen Neo 15-150's in parallel vertically mounted.

The surrounding "box" for this bottom module could be a cloth or perforated (yet dampened) metal panel(s) or a metal mesh.

Crossover design to suit the drivers (..Lynn's specialty, not mine. ;) .)

Not a "small" loudspeaker.. and there is still the lower freq. to contend with. On the other hand it should be exceptionally "clear/transparent" with a very low compression character, while still being stunningly "dynamic".

Oh well, just my current thoughts - which are always subject to change.. :D
 
panomaniac said:


I've often read and been told that, but why?
Does the large mass of the cone move the air "better?"
Is the extra inertia needed to give the bass more subjective "weight?"

The moving mass of the 21" Madison would be the equivalent of about 270L of air. Or 9.5 cubic feet.

Is that mass needed to launch a good, solid wave? Would a lighter cone not do as well? Is the higher energy in the heaver cone thus imparted to the air?

There air force on large cones are large enough that the cone has more air resistance such that you either need a strong motor to drive the cone completely, or you need cone interia to fight the air resistance to get more travel. I recall the resistance increases proportional to the squared velocity, this actually makes light cones act like they are soft clipped.

I think most heavy cones are also stiffer, so it cam maintain the same amount of air being pushed as in the beginning of the travel.
 
There is a guy at a german forum who removed the whizzer of a Beyma 12" fullrange driver and was very pleased with the result. He said all the sharpness was gone. The price was the need of a supertweeter, off course. For people like Lynn, who don`t like midrange compression drivers, this is probably a better solution than a coaxial with 1.5 kHz x-over, and it is closer to the Bastanis solution. And a crossover that is close to the 2kHz region where the human ear is most sensitive is problematic anyway.
By the way, I also thought that compression drivers are better kept away from the midrange, until I listened to the Martion Orgon at the Highend in Munich this year.
A question to Lynn: what compression midrangers did you hear?
 
Hi

and there is no real compelling reason for a dipole at lower freq.s.



I agree on the very first and obvious level of listening effects.

On a more closely examination there is a subtle interaction between the room and the loudspeaker in it.
Any box with a hole ( = the speaker ) basically also acts as Helmholtz resonator.
"The Scottish company" brought that into the mind of all audio people by their strictly policy of single speaker demonstration several years ago.

But sadly I can not compare from own experience now.


What makes the difference that you rate aperiodic over closed with the Rhytmic Audio subs?


Greetings
Michael
 
soongsc said:


There air force on large cones are large enough that the cone has more air resistance such that you either need a strong motor to drive the cone completely, or you need cone interia to fight the air resistance to get more travel. I recall the resistance increases proportional to the squared velocity, this actually makes light cones act like they are soft clipped.

I think most heavy cones are also stiffer, so it cam maintain the same amount of air being pushed as in the beginning of the travel.


Hi Soongsc,

probably there's a lower limit in the supension (spider, surround) compliance, to soft/flexible compliance and the driver might sags, and to reach lower frequency one has to depend on the mass of the cone.

I've heard multiple ceramic (stiff) cone driver showing huge amount of bass and large PA driver as well, what I notice is, with lower power amp (100 watt), we couldn't get the "punch" but the bass sounds very good and have good resolution.

one the other hand, normal speaker, even small ones when driven by large power amp (300 watt++) shows more punch, probably the "punch" came from : the amp lower bandwith limit(governed by input coupling caps) , or an intermodulation distortion inside the amp itself. when asked to deliver huge amount of power, the ground bounce in the circuit and the charging pulse of the capacitor might cause this "punch".

Edit: Everything else equal heavier cones have lower efficiency compared to light cones, and probably also has less real amp-speaker interface damping and need more power to drive. this might contribute to the sound as well.


Hartono
 
mige0 said:



What makes the difference that you rate aperiodic over closed with the Rhytmic Audio subs?


Greetings
Michael

In effect its all about controlling the driver at resonance.

In an aperiodic design you are basically targeting the driver's in-box resonance. This gives greater control at and near that region. The "price" to be paid is higher compliance distortion below resonance, but hopefully the servo system and driver (in tandem) are better than other offerings at these lower freq.s.

In a vented system with a *very* low tunning freq., (at *least* an octave below the in-box resonance and preferably an octave and a half), the vent effectively loads the driver and dampens it (..and not at just the driver's in-box resonance - and in this respect its rather like a poor servo). The lower vent freq. virtually ensures that the vent "operates" for a much greater passband than a normal venting "alignment". The price to be paid here is some additional compliance distortion (though less than an aperiodic and sealed), and greater vc heating. Additionally the actual vent resonance is cr@p, but presumably its down so low (both in freq. and output) that there is little detriment for most recorded material. The "upside" to this is some additional freq. extension (above the vent tunning freq.) & believe it or not, better time decay for both the driver and the vent (..except near resonance).

Unfortunately BOTH systems (when utilized properly), require larger enclosure volumes than either traditional vented or sealed designs.
 
I have been puzzled by a couple of the recent postings about LF drivers.

Cone weight surely relates to strength and rigidity for generating SPL whilst maintaining low system resonance when acting against any cabinet managed air-spring, not a deliberate intention for creating cone inertia ?
Inertia is stored energy, and this needs to be minimised in order to improve reproduction accuracy.

"Punch". Is this not an entirely false and undesirable characteristic caused by the heavier cone LF drivers being capable of generating considerable initial air-spring pressure in small sealed systems when powerfully driven by NFB controlled voltage drive at a sub-resonant frequency (initial drum kick or bass string pick), the stored energy of which then modifies/transforms the waveform due to loudspeaker system resonance after the initial empowering peak has passed ?
"Punch" does not arise with aperiodic or baffle LS systems, so these are of no use to ICE boomers.
 
"Punch" - hmm, that's an interesting one.

Small diaphragm speakers try, but don't quite succeed. I really think surface area has a lot to do with it - and oddly enough, line-radiators just sound wrong to me, weird somehow. There's a certain phasey quality that I'm very sensitive to - all those years working with quadraphonics and twiddling with high-order crossovers that were misaligned.

But big horns and arrays of LF drivers do sound big, in a realistic way. It's not so much "punch", which I suspect for hifi reviewers is a certain artificial quality of overdesigned minimonitors, but a big, solid, tactile quality. Back when I lived in Silverdale, I had a hifi friend named Gary Dahl, who played a full set of concert-quality tympani drums in the local symphony. Man, you stand 2 feet when those when he ran through his practice drumming, and you feel it, even though it didn't sound that loud. Everything else in the room was jingling and rattling along, but it still didn't sound all that loud, nothing like a PA or hifi system.

That's what I'm aiming for with this system (along with a classical-music tonal balance and a you-are-there spatial quality). Those of you who know drummers know how rare it is for hifi systems to get that part right - it sounds loud, all right, but the tactile quality isn't there. That's why I suspect magazine hifi reviewers don't really know what live, acoustic music sounds like - the sheer dynamism and bright, shimmering tone colors almost never happen with audiophile equipment.

P.S. Thanks, ScottG, for the reminder about the Jensen Neo 15-150. Not much Xmax (+/- 2mm), but the Q and Fs are just about right. A Midbass/Bass array of three of these things, in the delta pattern shown on Post #940 would certainly have the kind of tactility I've been talking about.

As you can see, I keep trying to drag things away from audiophilia, more towards horn dynamics, but not an all-horn multiway system. There's a fairly empty region in the audio ecosystem halfway between audiophile line arrays and prosound horns, and that's where I want to go.
 
"Punch" is a descriptor relating to the physical sensation occurring around the body's abdominal cavity resonance (i.e. the upper bass low midrange area 65-90 Hz). Its a concussive feeling in your gut - hence the "punch" appellation (..as in "punched in the gut").

High force, moderate to high mass drivers, in a moderately small sealed cabinet - seem to provide this sensation the best. However, its still a matter of force vs. mass vs. radiation ("forward directed" toward the listener offering the greatest sensation). This means that even small sd drivers can provide this sensation. Similarly, aperiodic and OB designs can also provide this sensation. It is however, a matter of "degree".

(example.. ask Paul W about the subjective difference in sound between his single BMS 18 inch driver vs. 2 10" Al/Mag Excel drivers.)

One notable attribute to this sensation is that exciting a room mode at this freq. (in anything but a very small room) does NOT enhance the sensation (rather it lends a "boomy" character to the sound if substantially elevated). Boundary gain does enhance this though.

All of the above is different than the subjective descriptor: Slam (..which is a lower freq. sensation and IS related to room modes and gain).
 
salas said:
Think about the 130Hz region. There lies average size chest resonance and there is where 'punch in the chest' is being experienced.

Yeah, thats a "hit and miss" thing.. one source says one thing, another says something else. I think the difference between the two is where the "listener" experiences it the most.. I.E. while the cavity resonance may well be 130 Hz for an average adult, this may not be the freq. for the greatest physical sensation.
 
Lambda Woofers...Acoustic Elegance

I used 50 Lambda woofers some years back because they just sound right. John Janowitz, the owner of Acoustic Elegance in GreenBay is said to be re-starting production of the Lambda line this summer. Following the philosophy of this thread with Lambdas, I would probably construct a 15"h * 0.5"w DIY dipole ribbon for 1K-20K, use the TD15M for the midrange down to 100Hz, and put a pair of the Qts=1 TD15D dipole woofers in a separate vibration isolated base baffle. I have found it necessary to go dipole from 20K Hz down to the room mode bass wavelength frequency (~ 30 Hz) to get the correct image. I have also found it necessary to put a diffuser on the wall behind the dipoles.


Here are the original TD15M specs:

T/S parameters:

Fs 30.5 Hz
Qms 4.47
Qes 0.29
Qts 0.27
Vas 405 Liters
Cms 0.4 mm/N
Mms 70 grams
Sd 855 cm2
Rms 3.0 Kg/S
Bl 27.6 T/m
Re 6.6 ohms
Z 8 ohms
Le 0.2 mH (low inductance due to underhung plus Faraday)
1WSpl 98.1 dB
Xmax (linear) 3mm
Xmax (mech) 10mm
 

Attachments

  • ribbon_lambda_dipole.jpg
    ribbon_lambda_dipole.jpg
    64 KB · Views: 1,138
Not exactly a line source, but a pair of 18Sound 8NMB420's in a vertical (MMT, not MTM) array look appealing as the wideband partner for either compression-driver or ribbon tweeters. (If ribbons are chosen, the best location would be directly to the left or right of the vertical driver array, with the ribbons on the "outer" edge of the L/R loudspeaker pair.)

Note the response curve, the smoothest I've seen for a prosound driver, and the resulting simplicity of the lowpass crossover. (I'd start with low-Q 2nd-order filters as a starting point.) As with the lower-frequency drivers, there is the option of separate lowpass crossovers for the 8NMB420, so the driver furthest away from the tweeter starts to roll off earlier, say at 1 kHz, while the upper driver rolls off at 2 kHz.

The cones are quite lightweight at 14.9 grams each, cone area (for two) is about equal to an 11" driver, and the combined power handling is rated 400W continuous pink-noise. The Theile/Small power efficiency for a pair is 98.6 dB/metre/watt, and the voltage sensitivity is a bit higher due to the 4-ohm load.

0.8dB compression happens at 40W input, or 114 dB/metre - plenty of headroom, I'd say. The Xmax is generous, so they should mesh well with the MB/B driver array.
 
Lynn Olson said:
Not exactly a line source, but a pair of 18Sound 8NMB420's in a vertical (MMT, not MTM) array look appealing as the wideband partner for either compression-driver or ribbon tweeters. (If ribbons are chosen, the best location would be directly to the left or right of the vertical driver array, with the ribbons on the "outer" edge of the L/R loudspeaker pair.)

Note the response curve, the smoothest I've seen for a prosound driver, and the resulting simplicity of the lowpass crossover. (I'd start with low-Q 2nd-order filters as a starting point.) As with the lower-frequency drivers, there is the option of separate lowpass crossovers for the 8NMB420, so the driver furthest away from the tweeter starts to roll off earlier, say at 1 kHz, while the upper driver rolls off at 2 kHz.

The cones are quite lightweight at 14.9 grams each, cone area (for two) is about equal to an 11" driver, and the combined power handling is rated 400W continuous pink-noise. The Theile/Small power efficiency for a pair is 98.6 dB/metre/watt, and the voltage sensitivity is a bit higher due to the 4-ohm load.

0.8dB compression happens at 40W input, or 114 dB/metre - plenty of headroom, I'd say. The Xmax is generous, so they should mesh well with the MB/B driver array.


Ah.. you've been thinking about what I suggested!:D

Note that Audax PR17M0, (in a vertical line of 4 drivers placed next to each other), will not behave as a line source at any reasonable* listening distance around 2 kHz.

(* at a distance of 6 feet the 4 driver PR17M0 will not display a line source character under about 5 kHz.)

A 4 driver array will also "naturally" increase the driver's output from about 450 Hz to 1.2 kHz. This compensates for the open baffle's loss (from the extremely narrow baffle).

Of course "combing" will exist, but its effect should *not* be substantial around 2 kHz.

Another factor to consider is that the PR17M0 has a vastly superior off-axis behavior at higher freq.s - which would work well with a non-directive tweeter like a ribbon or a planar (..horizontally speaking).

Now the 8NMB420 has a more directive off-axis output for use with tweeter'ed waveguides. So if you are still thinking compression tweeter then this would be a better driver.

Yes, the x-max of the Audax driver is pitiful.. but from about 500 Hz to 2 kHz in a 4 driver config. it shouldn't be a problem at even fairly high spl's. (..in fact I don't even think that a high-pass filter would be necessary for most users.)

On final note: The overall *efficiency* of the 4 driver (Audax) would be superior to the 2 driver 8NMB420. (..in fact with the 2 driver Jensens, I believe you could obtain a nearly stable 8 ohm impedance in a 2.5 way loudspeaker (parallel crossover) - with a sensitivity of over 99 db from 90 Hz to 20 kHz.)

Final note:

While I've recommended both driver's (for differing designs) in the past, of the two - I've only heard the Audax ..and I (and others) can tell you that it is *VERY* special.