Here is the problem with applying a thin corrugated foam surface layer in order to ‘prevent’ reflection. (Note: This is not a thread simply comparing foam and fibrous material! Nor does it address acoustical impedance or permeability.)
First, we are concerned with controlling reflected energy – ALL reflected specular energy.
Energy content is not distributed evenly across the frequency spectrum. Long wavelength low frequencies have the largest energy ‘content’, while the energy content steadily declines with advancing frequency and the shorter wavelengths.
So when we refer to broadband absorbers, one might say we are really primarily concerned with low-midrange absorbers, as those are the more difficult frequencies to address. But, as addressing the low mids also effectively addresses the highs, all is well if our absorbers are indeed ‘broadband’.
And as such, we are not interested in effectively EQing the room’s energy content. We are content in large measure to simply control the dispersion of the direct energy in its original spectral content to the largest degree possible, as there are more appropriate places to EQ the direct signal.
Thus, with regards to broadband absorbers addressing specular energy, we do not want the treatment to selectively remove more of one part of the spectral content relative to another.
To those ends, it is important to recognize that the porous absorbers require ‘size’ in order to be seen by various frequencies. The lower the frequency of the energy, the longer the wavelength, and as such in order for a porous absorber to be seen and to prevent the wave from simply diffracting around it, the absorber must possess sufficient size.
A common depth for a broadband absorber tends to be 4” with a gap of 4” – making the panel effectively about 8” thick. (Using a simple model)That thickness alone will be effective to about 1687 Hz – and utilizing quarter wave mechanics, the effective thickness is thus (4 x 8)=32 inches and thus the lowest effective frequency becomes about 421 Hz. (Note, this is assuming normal incident angles for simplicity.)
Above, we already discussed how the amount of absorption decreases and the amount of reflection increases with increasing incident angles until the degree of reflection is maximized in the ‘grazing’ incident range of between about 60-85 degrees from normal (perpendicular).
Thus, the single most effective technique we can use to increase the degree of absorption in a panel is to orient it so that it is as near to perpendicular to the source as possible. But we often accept reasonable compromises here.
But as has been observed, reflections can indeed occur. If these are of sufficiently low energy content and gain, we tend to ignore them. But many times they are above the minimum levels we would like to see.
Which brings us to the topic of which fabric is most acoustically transparent in order to minimize this. This actually involves many factors, including acoustical impedance, porosity/permeability of the surface, the k factor, and other variables… subjects that are beyond the scope of this post (and which we simply do not know in the case above!). But let’s simplify things and assume that the permeability of the fabric is acceptable and that the largest determinant variable is the orientation of the panel with respect to the incident angle.
Thus, to use a metaphor, we are talking about whether we are dropping a rock directly from above (normal) to the surface of a body of water, or if we are throwing a rock so that it glances and skips off the surface at a high grazing angle like one skips rocks on the water. In order to reduce the refection, we ideally will reduce the angle of incidence of the incident signal.
So, if we do use a corrugated foam layer on the surface, what happens? (Oh, and for this we will posit that the corrugation is aligned perfectly perpendicularly with respect to incident energy for maximum effectiveness!)
The corrugations will present a less oblique angled surface – but ONLY for the small wavelengths that are smaller than the corrugations. The remaining energy simply diffracts around them as if they are not there.
And what wavelengths would those be?
Let’s see…So, what size corrugation do you want to use? Β½”; 1”; 1.5”?
So, if any of these dimensions are chosen, the effective low frequency cutoff will be ~27,000Hz; 13,500 Hz; or 9000 Hz respectively. In each case the effective frequencies are excessively high, and they effectively remove only a small part of the spectrum of energy and effectively EQ the reflected signal, leaving the remaining energy to be reflected.
And quite frankly, we don’t even care about those high frequencies as they are so short as to be stopped by ANY impediment and because they contain Very little energy. So you see, while such an application can have an effect, it is not a comprehensive solution, and creates undesirable spectral imbalance. (In the process of partially solving a problem, it introduces still others...)
Another common possibility that is often seen is that people will not simply keep the basic panel in place and add a foam surface, but often they will instead use, say, a foam panel that has a total thickness of 4 inches and from the 4 inch thickness, mass is scooped out (removed) to make the corrugated surface – with the net result that we are now missing part of the ‘original’ material – the stuff that dissipates the energy as heat as the waves moves through it. So now we have even less ‘stuff’ to effectively resist the wave energy and we lower the overall effectiveness of the panel to absorb the lower frequency energy. And this too tends to ‘EQ’ the reflected signal still further from the source signal. In order for corrugation to work, it needs to be large enough to be seen by all of the incident wavelengths with enough material present to effectively dissipate the energy – which requires that such material would be thicker than the original panel to maintain sufficient mass and to also provide the angled surface. But that is not what has been proposed, and as such, it fails to satisfy the broadband requirements of our broadband panel.
And in either case, we tend to affect the overall tonal quality of the total sound by modifying the spectral content of the component energy – which was not our original intent, which was to control all of the reflected energy without modification except in terms of gain.
So this is why we certainly “can” use foam as a covering, but we “may” not without unequally affecting the spectral balance of the reflection. And why, rather than adding a material that will affect one part of the spectral content, we prefer to address the issue in a manner that will address all of the specular energy in total.