Ido wrote:Brian, something relevant to the above and to GG, an actual case at hand:
regarding a resiliently mounted 2 layer drywall ceiling to be mounted below the original massive house ceiling.
there are limitations, such as the airspace can be max 1.4 " / 3.5 cm which only allows Kinetics iso-max AFAIK, and only 2 drywalls.
there will be LF music content.
the purpose is to do the best within the limits.
of course nothing should get worse.
I don't know if you talked of this before, a link would be great too:
1. will GG in such a setup constrain the negative resonances at MSM and such, to an extent that I don't need to worry about making things worse?
well, that question depends on the edge conditions of the ceiling and mechanical stiffness that is present.
sorry to be so slow to reply, BTW, somehow i missed this thread.
if the edges of a wall such as this are perfectly floating, then the impact of Green Glue is at a minimum. In, as a different example, a double stud wall with its fairly stiff studs to resist motion at MSM and shift system properties towards the mechanical, the GG has been shown to be very effective (typically the dip at MSM is 1-3 dB based on lab tests for a GG double stud wall, with large benefits at higher low-freq's also. i posted about this at SOS earlier)2. how do these neoprene resiliient mountings behave regarding damping?
3. another option (or combo with GG?) would be an interlayer (between the drywalls) of either lead, or, of a real cool damping layer we have here(it's like soft soundblock, with an adhesive layer) .
btw, in your graph above, might it be that for the standard single layer wall, the wide & erratic MSM region also shows the non-damped behaviour of single layer drywall, as opposed 2 layers ?
we never ever do single layers, not for anything.
thanks Brian,
Ido
:D ?
Brian Dayton wrote:...2 layers of drywall isn't better at MSM than just one. i have some data if you like on the progressive improvement when going from 1+1 to 1+2 to 2+2 layers of drywall on a single stud wall, other such data is available in IR761.
Brian Dayton wrote:[
... Because the air cavity is the primary source of stiffness in the "spring" system, it is the damping of the air cavity that is most important.
That is a challenging situation, 1.5" of cavity depth isn't alot, and generally the deeper an air cavity the better the damping...
Brian Dayton wrote:i guess i don't know much about the soft damping layer you describe.![]()
Ido wrote:Brian, thanks for answering.
I don't get it yet, and I think what's stopping me is the "stiffness" issue.
in theory, we want infinite stiffness, but in lightweight/drywalls, we don't, right?
and this is because.. we want to somehow limit the transfer of energy between the 2 sides? enable a degree of freedom between the 2 leaves? so this relates to the "construction" of the lightweight wall, and not to the leaves/drywall?
are these considerations frequency dependant? for the LF resonances you do want stiffness?
how about stifness in the leaf itself? in a theoretically fully decoupled 2 leaf wall, would you want max stifness on each independant leaf? would you want narrower spacings between studs?
regarding GG, are you saying it's max benefit is in setups that are stiff/rigid to begin with?
so there is a major difference in sonic energy transfer within a 2 leaf wall if it is structure borne or airborne? (as regarding GG?)
you see my confusion:D ?
Brian Dayton wrote:...2 layers of drywall isn't better at MSM than just one. i have some data if you like on the progressive improvement when going from 1+1 to 1+2 to 2+2 layers of drywall on a single stud wall, other such data is available in IR761.
interesting, I'd love to see that.
Brian Dayton wrote:[
... Because the air cavity is the primary source of stiffness in the "spring" system, it is the damping of the air cavity that is most important.
That is a challenging situation, 1.5" of cavity depth isn't alot, and generally the deeper an air cavity the better the damping...
but say the cavity is a given, how about the damping of the drywall itself? if it is indeed an allround good floating construction, is there no benefot to damping at LF resonance, be it GG or something else?Brian Dayton wrote:i guess i don't know much about the soft damping layer you describe.![]()
the material is called TECSOUND, the specific type I have is S 35 (3.5 kg per m2, about 2.5 mm thick) . I believe it's Spanish made.
it's like a very pliable MLV, with an adhesive side, I'm pretty sure it is good for damping.
and here it costs about half than the "proper" sound barriers.
http://www2.uah.es/innovaciones/0405/tr ... csound.pdf
I found this link, scroll down and it looks like there is some intereting data in there,
translation anyone? Adore?
Brian, I'd gladly send you a piece.
Ido
Brian Dayton wrote:..... but i'm american, and as a result of this i'm only interested in wood studs and english and i think budweiser is a really good beer and i think we are the source of democracy in the world and i don't care if world history class taught me differently.![]()
Ido wrote:Brian Dayton wrote:..... but i'm american, and as a result of this i'm only interested in wood studs and english and i think budweiser is a really good beer and i think we are the source of democracy in the world and i don't care if world history class taught me differently.![]()
![]()
thanks so much Brian. I got me some serious reading to do :D (a bit suprised on the Budweiser, but i'll let it go..).
you see, I was contemplating bringing over some of the green stuff.
,,,,,,Then take a constrained layer damping material, like Green Glue (or any other), ... it damps the mechanical element of a resonance, and if the mechanical element is dominant, all is well, but if the acoustic (Air) element is dominant, then its overall effectiveness won't be as high.
Ido wrote:Brian, thank you so much.
You explain beautifully with a combo of science and mechanical intuition which is the only way I personally ever understand anything.
I want to ask further clarification, and perhaps this might benefit others too:
To this day I still don’t understand stiffness/TL:
How does the theoretically perfect “infinite stiffness” relate to a practically excellent limp material such as lead?
is this solely relevant to low frequency isolation which is "stiffness" controled?
Is it because the real life stiffness is always compromised/non-infinite?
how does lead behave regarding LF isolation? only mass? it benefits from it's "internal damping"?
BTW, when you say “..edge conditions of the drywall, and whatever mechanical stiffness they introduce to the system”,
is this the basic definition for “stiffness of a panel” (as in the inherent stiffness of the material itself)?
or do you indeed emphasize the significance of the edge conditions (as in, the material at hand is secured firmly, or has freedom of movement)
,,,,,,Then take a constrained layer damping material, like Green Glue (or any other), ... it damps the mechanical element of a resonance, and if the mechanical element is dominant, all is well, but if the acoustic (Air) element is dominant, then its overall effectiveness won't be as high.
Can you please explain the difference in the mechanical behaviour between the energy transfer of vibration/resonance of the mechanical element (stud) and between the energy transfer of vibration/resonance via air stifness?
In the end, isn’t it the drywall itself that is set into vibration and “decides” the outcoming TL?
Does the drywall vibrate differently in the case of mechanical vibration versus the case of the airborne-induced vibration?
like above. if the panel is acting like a pure piston at resonance (like in the rarified case above), then the MSM has no mechanical element.
if the panel must bend, then it has a mechanical element, and damping materials are maximally effective. draw a picture of how any given construction has to move at resonance to gain an idea.Is there a frequency difference between the air-borne vibration transfer and the structure-born (stud) vibration transfer?
Regarding the above mentioned case in hand, of thin arrow air cavity and decoupled studs:
Do you think that in such cases the dedicated decoupling is perhaps an insignificant contributor?
I’m asking a lot here, I know. please don’t feel obliged to answer, but you see, I have to ask….
Thanks Brian,
Ido
Ido wrote:Brian, thanks again :D .
Andre, I think the following graphs seems interesting, what do they say? what is the scenario?
Brian Dayton wrote:Ido wrote:Brian, thanks again :D .
Andre, I think the following graphs seems interesting, what do they say? what is the scenario?
hey Andre, thanks for offering.
my biggest questions would be these
A) is the thickness of the material given
B) is the density or weight per area given
C) is the composition given? acrylic, vinyl, foam,
D) waht do those graphs ldo showed say. what are the walls in question?
from: http://www.texsa.com/desc/sistemasacustica_eng.pdf page 13
Another effective method, particularly for very rigid walls, is to use the
diaphragm effect. This consists of filling the cavity with a material comprising a thin
membrane with very low f0, positioned between two spring elements, such as felt or
mineral wool. The spring elements prevent movement of the membrane when it is hit
by the sound waves, and this causes greater dissipation of mechanical sound energy
with the consequent increased insulation. It is important not to use sheets of polystyrene
or other rigid foams which worsen the result from the acoustic viewpoint for the air
chamber filling.
Users browsing this forum: Google [Bot] and 1 guest