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Impact of bassreflex port surface area on small signal sensitivity

stoneeh

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Hello folks.

Large signal differences in compression, distortion, and port noise in bass reflex speakers have been exhaustingly documented in the longstanding literature (such as). The following research of mine, which originally was published in 2020 in German, and only recently translated to English, addresses large signal behavior of bassreflexes as well, but the main point / focus lies on small signal sensitivity differences of different vent sizes, which I am not aware have ever been discovered & empirically documented before.

Multiple port sizes and shapes on multiple enclosures each were compared, and diagnosed thoroughly. I'd say it goes quite in-depth. Enjoy.

Regarding the method of publication, I realize a PDF or forum post would have been preferred, but I am not a commercial entity, and you're getting the benefit of my countless hours of work for free, so I get to choose how & where ;)

I recommend viewing the video on a desktop or laptop, pausing it, and using the left and right arrow keys on your keyboard to move through the text at your own pace.




For completeness' sake, some minor attempts at theoretical explanation. An empirical observation like the one made within this research stands on its own and doesn't require a theory behind it. However, it can be satisfying, and also often useful/helpful, to be able to explain what you're observing - so it is valid to also put some effort into the theoretical background.

In a German webforum discussion about the paper, a former Elac engineer offered Small's loss model (Qb, Ql, Qa, Qp) as a possible explanation. He offered no proof, and even Small's model itself is a purely theoretical one that has never seen an empirical verification. Still, I'll throw this possible explanation in the ring.
If the cause was related to Small's model however, it would have to purely be differences in Qp (friction within the port), since Qa (absorption losses) and Ql (leakage losses) do not apply to a sturdy, sealed enclosure; and Qp alone causing such a huge difference at very small signals (-> very low vent air movement) does not seem plausible.

Another, or perhaps rather an additional possible explanation might be the differences in air mass within the vent. In the first test subject, the 1/8 sd port has 0,65g (500cm³), the 1/4 sd port 2,9g (2250cm³), and the 1/2 sd port 11,9g (9150cm³) air mass. Relative to the woofer's 104g moving mass (mms), these values might already be entering significant territory. I doubt this scale of air mass changes is responsible for dBs of measured difference, but, perhaps combined with some minor friction loss differences in accordance with Small's theory (Qp), the combined effect could be large enough to account for the measured SPL differences.

These are two theoretical explanation attempts. Make of them what you will, feel free to entertain your own, or, again, also feel perfectly comfortable entertaining none and just concentrating on the observation.

- Stoneeh
 
Awesome work as usual. A combination of port radiating area and friction losses (Qp, mostly for the smallest port as they are ~1/r^4) and a bit of Mms (mostly for the biggest one) seems reasonable enough as an explanation.

Evidently, the PA sub designer's motto should be "I like big ports and cannot lie". ;) Gaining 3+ dB at 50 Hz just like that is significant. (Rodent-proofing required!)
Those port resonances are getting awfully close for comfort though, I wonder whether they could be tamed somehow. Or will it always remain a tradeoff? There's no way around making a larger port longer if you want the same tuning, and that's ultimately the problematic dimension if I'm not mistaken.
(I guess one could make use of this problem by turning the whole affair into a backloaded horn or TQWT instead. Better not ask about the size then, mind you.)
 
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Thank you Steph.

Almost all commercial PA subwoofers nowadays do feature large ports, if only for prevention of compression. It's really a no-brainer - it adds relatively little to the sub's size and weight, the port's own resonance rarely becomes an issue as it's usually around an octave above XO, but you do gain a lot of max. SPL potential.

I doubt any of the developers are really aware they're also increasing general sensitivity via larger ports; otherwise, I'm sure someone would have taken the time to document it in a paper by now, or slap a fancy term on it and use it for marketing.

On fullrange speakers, the port's own resonance indeed does tend to become a problem on larger ports, but a variety of types of absorption methods are available to minimize it. KEF and AudioSmile use flexible inner portions of the port. Holes at the pressure maximums, wrapped with foam, can work. Helmholtz type absorbers can be used. Etc etc.
 
You did great work with interesting, but not really surprising results.
A speaker driver is all about transmitting energy into a room. The larger the cone area, the better. A small source of a wave transitions into a large room.
If we use a ported cabinet, the vent /opening is at the border to the room, the larger it is, the better the transmission of energy will be.
Think of extremes, first a small hole in the cabinet as a vent, or more a ventury. The wave will be very fast at the exit and will not stimulate the room well. Its area compared to the room is too small. The closed box is the smallest vent we can think of, it has the worst efficiency.

Second, make the port a large opening. The wave comming out of the port is much larger and its size will couple well with the room.
The ultimate port, in the end, will be a horn, the larger the better. Like using the corners of a room as extention of the horn. The result is a perfect coupling of the cone area to the room volume, resulting in very high efficiency.

A good example is the so called horn reflex principle, in the middle between a backloaded horn and a vented cabinet.

There is a volume where we find a speaker is more working like a helmholz resonator. At some point the volume of the HR gets so small, we will find it working as a pressure chamber. When the opening of a vent becomes conical, exponentiell or hyperbolic, we call the vent a horn.
Once we understand this mechanism and how the principles morph into another, the better we can predict what happens.

There are other factors involved, like loss due to turbulence, but in the end we will be able to find an optimal construction for any given driver. High Qts for closed, medium for vented and low for horn constructions, this is nothing new...
 
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