Seems like there's is lot of to rethink.
True! There always is. When I'm designing a studio, I seem to spend quite a bit of time re-thinking things, then re-thinking again, to optimize... and also to compromise.
I know that I'm not going to get the room perfectly flat, regarding my budget and my experience.
It's a decently sized room, so it can get reasonably close to flat. I'd guess you should be able to get within +/-6 to 8 dB across most of the spectrum, and decay times within about +/- 80 to 100 ms of each other across the board, between most frequency bands. That's pretty good, for a home studio / project studio. Even some pro studios don't get better than that.
Of course, it would take a lot of work and careful design to get there, plus final tuning, but it's feasible. It all depends on ho far you want to take it, and how good you want your room to be.
I just want to be able to have a more correct judgement on the low-end,
Ahh! The low end. Yup. That's always the biggest problem, in any room. And that's one thing the soffits will do for you, if you do decide to go that way. Soffiting your speakers extends and tightens your low end. And good bass trapping smooths out the decay times. And good room design reduces SBIR from the rear wall. Then there's a couple of other secrets that I have for doing the final tweak, if you want to go that route...
I am glad to hear that it actually would make sense to soffit mount my Adams
Definitely! No doubt about it. Here's an interesting thread from a forum member who started out with his speakers on stands, and then rebuilt his room with soffit mounting:
http://www.johnlsayers.com/phpBB2/viewt ... =1&t=20895
And Thanks for the Post regarding floated floors.. This actually prevented me of spending money for something which probably would make everything worse!
There are alternatives, and what you mentioned could be adapted to do a "semi-decoupled damped riser floor", but it probably won't give you as much improvement as you are hoping for if you don't isolate the rest of the room. If you have read many threads where I have commented on isolation, you might have seen my "fish-tank" analogy before: Imagine a guy who wants to build an aquarium in his living room, and buys the metal frame to make it. Then he thinks:" "Well, I only need to see the fish from the front, so I'll only buy one piece of glass for that side"... How well do you think his aquarium will hold water?
That's roughly what happens if you try to isolate just one side of a studio. Just like the aquarium guy would have water splashing around all over and flooding the whole place, despite the glass on one side, so too a room will leak sound all over, despite the isolation on one side. In other words, isoalting only your floor is like building a fish tank with glass on only one side...
The thing is, sound is a lot like water in many aspects: once the water is out, it flows wherever it wants, in all direction, including right in front of the glass... Ditto with sound: once it is out, the it is out everywhere, and will get around all over... including on the other side or the "isolated" wall, floor or ceiling. So even though your intentions are good in wanting to prevent sound from annoying your neighbors, isolating your floor will not accomplish that... unless you also isolate the rest of the room. Just like the guy with the aquarium, who really needs glass on all sides if he wants to keep the water in, a studio needs isolation on all sides if you want to keep the sound in.
So do you think I shouldn't work at all with membrane absorbers?
I have used them very occasionally, for very specific issues, but I'm not a big fan. They do work, if you tune them correctly, but tuning them is nowhere near as easy as the textbooks make it sound. You need a method for accurately testing the tuning of your finished device, to find out what it's REAL resonant frequency is (not the predicted one...), and a method for adjusting that to get it where it is supposed to be, because it very probably won't be what you thought it would be.
Another thing the text books also don't tell you, is that membrane traps need to be very large if you want to get a big difference in your acoustic response. Think of it this way: assume you have a problematic axial mode forming between the side walls, and they measure 27 long by 10 feet high. So each side wall has a surface area of 270 square feet. Then you build a membrane trap with a full sheet of plywood (4' x 8'), but you are only affecting 11% of the wall area, so at best you are treating 11% of the problem. If you stacked 5 such devices along each wall, you'd still only be covering 59% of the total wall area, so there would be over 40% of the problem still untreated. But 5 such devices would essentially take up the entire wall, in practical terms (especially if you have doors, windows, and other treatment on that wall, plus a cloud, hanging lights, artwork, gear, etc.), so how would you treat the other two or three modes that are also associated with that wall? There's no space left for that. So even by filling most of the usable area of a wall with membrane traps, you only affect half of one problem, and can't do anything at all about other problems.... That's one of the reasons why I'm not a big fan of tuned devices in general: they take up a lot of space, for little result.
What other options do I have?
Porous absorption...
As I know porous absorption doesn't do much under 100Hz...
That's one of those myths that continues to float around the internet, and get repeatedly chanted religiously, as though it were written in stone by the finger of God himself! People often quote the "half-wave rule" or the "quarter-wave rule", spouting about absorber only being able to affect waves where the thickness of the absorber is at least one quarter wavelength, or more. They say that if you have a 50 Hz tone, the wavelength is 22 feet, so you need an absorber (22/4=) 5' 5" thick.
Garbage.
In reality, a porous absorber can have a very decent effect on a wavelength when the thickness of the absorber is just 3.5% of the wavelength. So that 50 Hz wave can be dealt with by a porous absorber just (22*.035=) 9 1/4" thick. That's reality, and easily shown from simple math and empirical results. Yet, people still bandy around the "It must be quarter wave thick or it wont work" myth.
Not only that, but we are talking about normally-incident sound so far: sound that strikes the absorber head-on, at an angle of 90°. Sound coming into your 9" absorber at that angle will go through 9" of absorber (duh!), but if sound strikes at any other angle, it must go through MORE absorber. Think about it. If the sound wave strikes at 30 instead of 90°, it "sees" the 9" absorber as though it were 18" thick. And since most of the sound waves in your room are NOT arriving normally incident, and ARE arriving at random angles less than 90°, it's safe to assume that your absorbers seem a lot thicker than they really are to most of the sound waves.
The "quarter wave" rule is not wrong: it's just not applicable here. It is NOT talking about thick porous absorbers close to the wall. It was actually meant originally to describe thin absorbers at a large distance from a surface, and it refers to the gap, not the thickness. More specifically, it is useful for describing the absorption of drop-ceiling tiles, which are acoustically very thin (just a few mm) compared to the wavelengths passing through them, but they are spaced a long distance from the ceiling behind them, and there is a measurable effect due to that spacing, not due to the thickness. Drop ceiling tiles do have a small effect on waves that are 4 times longer then the gap size, hence the "quarter wave rule". That's because the tile sits at the point where the particle velocity is highest: the quarter wave distance. But the "rule" has nothing at all to do with the thickness of the tile: it's about the spacing, not the thickness, and refers to acoustically thin absorbers, not thick ones.
Somehow, that got all muddled up into a new mangled, mungled munged "rule" that supposedly requires absorbers to be one quarter wave thick. Not true! You get very good absorption at 7% of the wavelength, and still usable absorption at 3.5% of the wavelength. (Now, if you also move it away from the wall, to get a gap behind it, then you get the best of both worlds...)
Oh, and there's one other thing that the myth-mongers don't take into account: when sound waves move through air, they are attenuated slightly by the air itself: they lose energy. This happens any place where the air pressure increases, such as when a sound wave passes by. Where does that energy go? Converted to low grade heat, which stays in the air, exactly where it was left behind by the passing of the wave. That's called "isothermal" heat dissipation. But that's NOT what happens when a wave loses energy as it moves through a porous absorber! The absorber itself changes the way the air behaves, to "adiabatic". The fibers of the absorber can carry away some of the heat from the places where the temperature has increased due to sound energy being converted to heat. So the heat doesn't stay behind in the air at the point where the pressure hanged as the wave passed: rather, the heat is removed. This is a whole different ball game. To cut a long story short (and a long equation too): Due to adiabatic heat transfer, a porous absorber appears to be about 20% thicker than it actually is. Sounds waves "see" more thickness than is really there, by a factor of roughly 1.2.
There's more to it than that, but even from this simple explanation, you can see that porous absorbers do, in fact, work down to very low frequencies. They still have to be thick to be effective, but not twenty feet thick like the myth-mongers would have you believe!
Here's the real situation, in graphic forum:
This is what you get for a 30cm thick (12") porous absorber right up against a wall, for randomly incident sound:
Porous-absorber-graph-30cm-random-incidence-CRP.jpg
Not too shabby at all! According to the "quarter wave or die!" folks, that device should have no absorption at all below about 280 Hz (aprox. quarter wave for 30cm), yet the graph says something very different: it shows that at two entire octaves
below that (70 Hz.), you STILL have a coefficient of 0.7, and even way down at 40 Hz (nearly three and a half octaves below where they say it doesn't work) it is still giving you better than 0.5.
So lets go a little thicker, and make the absorber 16" thick, and this is what you get:
Porous-absorber-graph-40cm-random-incidence-CRP.jpg
The entire darn spectrum is covered! Even down at 20 Hz, you are still getting better than 0.4, and everything above about 38 Hz (the bottom end of the bass guitar) is over 0.6 coefficient, which is considered to be very usable.
For both of those graphs, I assumed typical porous absorption with a gas flow resistivity of 9,000 MKS rayls. If you went hunting for lighter stuff that has lower GFR, you could probably improve on that even more.
(Now, that's for an absorber up against the wall: move it away a bit, and things get even better...)
So, consider that a typical superchunk is 36" along the faces, and therefore about 25" thick in the middle of the diagonal, and you can appreciate why they do such a good job as bass traps. This is what a 25" thick superchunk porous absorber would get you:
Porous-absorber-graph-63cm-25-inch-superchunk-style-random-incidence-CRP.jpg
Well gosh darn my goodness gracious golly me!! It sure looks to me like that would get you a "very usable" 0.6 absorption coefficient for everything above about 33 Hz!.
So much for the "it has to be a quarter wave thick" guys, and the "porous absorption doesn't work below 100 Hz" guys....
Hangers will give you similar performance. I sometimes do superchunks in the rear corners of the room, with hangers between them, across the rest of the rear wall.
However, the danger (as I mentioned yesterday, and as you can see in the graphs), is that even though these thick things are retty good for bass, they are also incredibly good at sucking up everything else too! Even stuff that you did NOT want sucked up. For everything over 1 kHz, these guys have an absorption coefficient of practically 1. Allowing for edge diffraction, it can actually be greater than 1. But most rooms do NOT need absorption in the high end, and even the rooms that do need it, do not ever need as much as you see here. So you need to design your bass traps such that they ONLY trap bass, and reflect back most of the mids and highs.
Are hangers absorbing down to like 40Hz?
Yup. And lower. Just like porous absorbers.
And no, I wasn't aware, that membrane absorber could extend the reverberation time due to inertia.
It's logical when you think about it: A membrane trap has a membrane on it (duh!), and the membrane has mass. It's the mass that determines the resonant frequency: the lower you want to go, the more mass you need. But mass implies inertia: If you have ever tried to push a car by hand, you know that you need to push really hard for quite a while to get the car moving fast enough... because the car has mass. And once it is rolling pretty fast, when you stop pushing it will actually keep on going for quite a long time before coasting to a stop... because it has inertial mass. The exact same thing happens with your membrane trap: The incoming sound wave causes the panel to resonate, yes, but it takes a little while to "get up to speed", because the panel has inertia. So it does not react immediately to the wave you are trying to damp. It takes a few cycles of the wave before the panel can get up to speed, so that it is in sync with the wave and converting some of the acoustic energy to heat energy, in the porous absorption inside it, thus removing energy from the wave. But when the wave stops, the panel doesn't! It has inertia, and just like the car, it continues to "coast" for a while, as that excess energy is absorbed by the porous absorber inside. So even after the wave is no longer exciting it, the panel still carries on for a few cycles, until it eventually stops. Because it has mass, and therefore inertia. The lower the wave it is targeting, the more mass it needs, so the longer it carries on, because it has more inertia.
Now, you might not think that this is such a big deal, but do the math. Let's say that you have a membrane trap tuned to 40 Hz, and that it's a really good one that only continues for 3 cycles after the exciting tone stops. At 40 Hz., three cycles of 40 Hz is 0.075 seconds (do the math). So the device will still be "coasting" for another 75 milliseconds after the triggering wave has gone away. And since a membrane trap is basically just a giant speaker in reverse that absorbs sounds, it also works the other way: If you make it vibrate, it will produce sound. If it is vibrating at 40 Hz for 75 milliseconds when there is no sound in the room, then it is acting like a speaker and creating a 40Hz tone that was not there!! In other words, the vibrating panel has extended the note by an additional 75 ms. So instead of bringing
down your decay time at 40 Hz, it can potentially
increase the decay time. Yes, it did absorb some energy when the original tone was present, but it only did so starting 75ms after the problematic wave started, and then it carried on "giving back" some extra sound for another 75 ms after the problematic wave went away.
In other words, it extended the decay time, instead of reducing it, which is not what you wanted.
Now, a membrane trap that can stop in just 3 cycles is pretty good. A large, massive membrane with lots of inertia might carry on running for 6 or 7 cycles... at 40 Hz, that would be nearly 200 ms.... which is a LOT! (and audible.......)
Here's a simple exercise to see what I mean. Go get yourself a ruler. I don't know if you ever did this in school to annoy the teacher, but... :
vibrating-ruler.jpg
The ruler can continue vibrating for several SECONDS like that, because it is not damped at all: it just resonates at it's natural frequency, just like the membrane panel would, if it was not damped. Now tape a piece of cotton wool to the end of the ruler, and try again: It no longer carries on for several seconds, but it DOES still carry on! It still goes for a few cycles before stopping. Just like a membrane trap does.
So, if you do want to build membrane traps, do design it so that it has as little mass as possible, so that it won't carry on playing tones that you didn't want, after they already stopped.... But in order to have a low mass panel tuned to a low frequency, you need a large cavity depth... Ooops!
Even if you use a limp mass, such as MLV, you still have this problem of the inertial issue, because it's not just the panel that vibrates: the entire thing is a tuned system, and the air inside is vibrating along with the panel...
This is another reason why I'm not a big fan of membrane traps. And the simplified text books don't tell yo about this, but it's very logical and obvious once you think about it...
On the other hand, porous absorbers do not suffer from this problem: they are very light mass, especially when you consider that it is the individual tiny fibers of the absorber that are doing the work, and each little fiber has practically no mass at all! They act individual (each fiber vibrates all by itself, in response to the wave hitting it), and since each fiber has such low mass, it can start and stop instantly....
Which materials would be bad / good for the membrane?
Low mass, and limp (self-damping). I normally use MLV. But that implies a deeeeeep cavity... probably just as deep as it would be for a superchunk... in which case a superchunk would be better, because it absorbs ALL low frequencies, not just the one you tuned your MLV for...
Tomorrow I will see if the way I build it actually workout well. I used a 5mm MDF board
MDF has a density of roughly 750 kg/m3. Fiberglass insulation has a density of roughly 25 kg/m3. Which one has more inertia?
a 5mm thick MDF panel has the same surface density as a piece of fiberglass insulation 150mm thick (6", roughly). But once again, the MDF panel acts all at once, as one single solid piece of mass. The insulation does not: it acts as a whole bunch of very tiny, very VERY low mass fibers, each doing it's own thing....
Most of the rooms I design just use porous absorption as the main ingredient. Some of it (or a lot of it) is covered with some type of foil, or wood slats, something like that, which serves several purposes, but mainly to keep the highs in the room and let the lows through to be absorbed. Regarding diffusion, I only use diffusion in very large rooms, and I seldom used membrane traps, unless there's a really stubborn problem that refuses to react the way I want to other treatment. In Studio Three Productions (the link I gave yesterday) there's a HUGE amount of porous absorption in there, as bass traps. Mostly in the ceiling, above the cloud and above the soffits, but also in horizontal superchunks that run across the tops of the walls, just under the false ceiling, and vertical superchunks hidden in the rear corners. There's no hangers at the back of the room (due to the window), but there are hangers under the speakers inside the soffits, and inside the center area between the speakers. That room actually does have a small MLV membrane trap (not visible in the photos), but it turned out to not be as effective as I wanted. There's also other treatment in there, that I'd prefer not to go into, but the vast majority of the treatment in there is plain old porous absorption. Mountains of it. The owner of the studio (Rod) could not get over the truck loads of insulation that went into that place. He thought I was a bit nuts when I kept on telling him to load up more rolls of fiberglass insulation... until we did the initial tests, and he heard (and saw on the graphs) just how well the lows are controlled. Then he was convinced that it was all worth it. That's a big part of the "secret" of how I got the low end of that room so tight, and flat, and smooth: Stacks and stacks of porous absorption. Your room is similar to his in overall volume, but not the same shape or dimensions. So you could theoretical get similar results, if you wanted to go into the same very detailed design and tuning. It's possible. But I would do three things, principally: 1) Soffit mount your speakers. 2) Load in mostly porous absorption, especially on the rear wall, and 3) tune the absorption with foils, slats, and other tricks, to balance the frequency response and time-domain response, such that it gets close to ITU BS.1116-3 specs. That would be my general plan. But of course, there's a lot more to it than that!
Thank you so much for your time, Stuart! It's a huge gift,
!
- Stuart -