Ro wrote:
1) IF I go for the agglofoam with woodfloor (1x15mm is lightweight indeed, might consider that again) isn't a more dense material beter when mass increases? That's what I've been wondering all along, what if I calculate the dead and expected live load. HOW to choose the right density?
Yes, again... it's something I've been thinking about for a long time. Asked about options in this very thread with little results however. Why on top of the floor? It's to keep my walls from the existing floor. Thought about the weight and all, hence the questions above. Still looking for a good solution.
.... so much questions.. so much to consider. thanx for your expertise so far Eric. I will look into the link you gave me. I've been on the akoestikon site before, gonna check'm again. :idea:
Ro,
Ask the supplier, if you speak about densities and deflection. I told this is measured, hence they should find that, being able to help you.
Ro these are relative cheap and relative good materials.
I know this material very well from very long ago (before akoesticon was even established).
But I'm on the net to share principles, not doing individual project calculations.
If you just use it for a lightweight floating floor the 60 kg/m3 is OK.
Depending on the thickness your floor will really feel a bit springy then. Hence you can't go lower, while at the other hand the MSM will still be too high for pro results. Hence it's ALWAYS good to make that top floor as heavy as possible, and make the live load relative insignificant versus the dead static load.
Those materials are not tested for critical applications in the long run as e.g. Sylomer, but which costs a multiple as well.
Edited:
Just copied part of another post of me here since the basic principles are equal.
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The basic principle: The higher deflection under load the lower the resonance frequency = the better decoupling.
But if by bringing the deflection to a frequency point where vibration levels are dominant than you introduce a problem yourself.
For linear springs the relation deflection/resonance frequency =
Metric
fo = 15.8/sqrt(d)
d=(15.8/fo)^2
fo = resonance frequency
d= deflection in mm
Imperial
the same in imperial:
fo = 3.13502/sqrt(d)
d=(3.13502/fo)^2
fo = resonance frequency
d = deflection in inches
Note that depending on material this can deviate somewhat. The above assumes linear springs, but is a good rule of thumb.
Some materials are made just to improve high frequencies (impact noise).
They have there resonance in an unhealthy spot, but since rather damped don't cause practical trouble and below that frequency that material doesn't work as a decoupling anymore.
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