The Acoustic Treatment survey (take survey) hasn’t even closed yet and it’s already very clear in what direction XIX Acoustics needs to head. The survey asks professional audio engineers what kinds of acoustic problems they have in their main listening rooms and what kinds of solutions they are currently using.
Most of the respondents listen primarily in a dedicated home-based critical listening environment. Most have never scientifically tested the acoustics in their space. Most feel that they have acoustic problems. The three most common perceived problems are:
Room shape and size
Bass accumulation or lack of bass trapping
Interfering outside or ambient noise
Half of the engineers that responded use no acoustic treatment whatsoever. About 30% are using DIY absorbers or bass traps. When asked why they haven’t addressed the acoustic problems with acoustic treatments the biggest reason is that
ACOUSTIC TREATMENT IS TOO EXPENSIVE.
So what XIX Acoustics needs to do is create an extremely inexpensive way to:
Fix weird room shapes
Reduce accumulation of bass frequencies to smooth out bass response
Reduce ambient noise
This shouldn’t be too hard to do with the right research. We need early adopters that are willing to be guinea pigs for the cause. Please get in touch if you are interested in helping out.
We have recently received a number of questions from people planning to install an array of Acoustic Ramps in their listening rooms. Most people are interested in the differences between the two installation styles: permanent and temporary.
Use the temporary installation if any of the following are true:
You don’t own the space in which you are installing the Ramps
You want to be able to use the Ramps in multiple locations like for diffuser gobos (see the Studio 44 photos)
You don’t want to drill holes in the Ramps
You want the most flexible installation possible
You don’t want/need a horizontal installation
Use the permanent installation if:
You own the space and you want the most rigid and secure installation possible
The Ramps come with the hardware for temporary installation: a hanging “J” hook and a cross piece that is installed on the rear of the Ramp. This is the easiest type of installation. Essentially you screw the “J” hook to the wall. Then you attach the cross piece to the back of the Ramp and hang the Ramp on the hook. Very simple.
You install the hook on the wall at least 2¼ ” from the ceiling using a level and appropriately strong fasteners (like 3″ drywall screws into studs.) Use a level to make sure the hook is level. Next you install the hanger bracket cross bar to the back of the Ramp. Then simply hang the Ramp on the hook. The Ramp will drop into place and be pressed against the wall.
Photos of Prototype A (left) and Prototype B (right) installed in a home studio. The left Ramp is installed permanently with molly toggle bolts and the right one is hung with the included mounting bracket.
We now have a way of comparing apples to apples! Using the methods described in AES-4id-2001 (r2007) “Characterisation and measurement of surface scattering uniformity,” we now have a direct comparison of the Acoustic Ramp and RPG’s QRD 734.
The black line is the QRD 734 and the green lines are the Acoustic Ramp™. Please note that BOTH of the green lines are happening at the same time, so you’re comparing both the green lines to the black line. As you can see the Ramp™ extends the frequency range way above and below the 734.
So we’re actually comparing a super-yummy Ginger Crisp apple to a mealy Red Delicious. Which is which?
Acoustic Diffusion is not an easy thing to test or describe. In fact in the academic acoustics world there is a big controversy about the best way to describe and measure diffusion: the Scattering Coefficient or the Diffusion Coefficient.
“You will know it works when you hear it,” is true but probably not a good explanation. I am going to avoid this whole dispute by publishing the actual data of all frequencies and amplitudes in my tests.
I did several rounds of acoustic testing on the Ramps and here is what I found:
The Acoustic Ramp scatters frequencies horizontally from about 300 Hz to about 4000 Hz (4kHz), but doesn’t do a lot below or above this bandwidth
The Acoustic Ramp scatters and reflect frequencies vertically from about 300 Hz all the way up to 20000 Hz (20kHz)
The Ramp does both of these things at the same time. So if you install the diffusers on their sides, it only changes which orientation scatters and which one reflects and scatters.
Why Do We Want To Scatter the Sound Anyway?
When sound strikes a hard flat surface most of the sound bounces off the wall as an echo. That echo can interfere with the sound that is headed towards the wall by cancelling out certain frequencies and emphasizing other frequencies. This effect is called comb-filtering. You just cannot hear sound accurately in a room that has comb-filtering problems. Scattering the sound breaks up echoes into many little tiny echoes diminishing their effect. The Ramp also reflects sound away from the sound source, further minimizing the effect of comb-filtering.
Reflections can also be controlled with absorption of course, but absorption-only treatments tend to yield rooms that sound dead and lifeless.
How Do you Read Those Diagrams?
Those diagrams are called “sonograms” and they were generated from data gathered using the software package ARTA. There will be a later post about the testing procedure, but for right now let’s focus on the diagrams.
The Sonogram shows Amplitude (color), Frequency (x-axis), and Directivity (y-axis). The above diagram shows what happens when you place a loudspeaker directly in front of a flat panel. The bright yellows and reds show loud levels and the blues and dark blues show quiet levels. The stripe of brightness that goes horizontally across the center of the diagram shows that sound is bouncing right back towards the speaker. At about 500 Hz the sound is bouncing at about 30 degrees and 50 degrees off-center. And from about 300 Hz and below the reflection pattern is pretty wide.
If there is pretty good diffusion at a specific frequency the diagram will show a vertical band of similar colors. Horizontal bands of similar color means that there is an intense specular reflection at a specific angle. For instance, in the above flat reflector model, there is a very strong reflection at 0 degrees, meaning that sound hitting the reflector is bouncing straight back to the loudspeaker. If the reflector had been angled at 45°, we would expect there to be an intense band at around 45° as well.
In the horizontal test of the Acoustic Ramp™ you can see that nearly all of the energy is directed away from bounding back towards the sound source because the center of the diagram shows darker blue colors.
In the vertical test of the Ramp you can see the scattering of frequencies from about 300 Hz to around 4 kHz.
There are several reasons why the Acoustic Ramp™ works better than traditional diffusion treatments, but we’d like to focus on two major improvements in this post.
The Ramp scatters acoustic energy horizontally while at the same time it reflects the energy over 4 different angles vertically.
The depth of the wells of the Ramp are continuously variable leading to increased functional bandwidth.
In order to understand why these factors are important we need to discuss a few things about diffusion in general. There are two different types of diffusers that have been thoroughly tested and evaluated in the academic and in the ‘real-life’ community: the 1-Dimensional (1D) Diffuser and the 2-Dimensional (2D) Diffuser.
1-Dimensional Diffusers
1D Diffusers are probably the most commonly used diffusers in studios and critical listening rooms and offer very predictable results. These diffusers scatter energy in a semi-circular pattern horizontally. Some examples of this type of diffuser are the following:
RealTraps Diffusor (http://www.realtraps.com/diffusor.htm) This diffuser combines the QRD (Quadratic Residue Diffusion) math from Schroeder’s work with low frequency absorption.
Primacoustic Razorblade Quadratic Diffuser (http://www.primacoustic.com/razorblade.htm) The diffuser uses a sequence of depths that doesn’t appear to be strictly a quadratic residue sequence, in that it is aperiodic and the width of the zero-depth reflectors isn’t consistent. The diffuser does offer a tremendous amount of phase-complexity and probably works very well indeed.
2-Dimensional Diffusers
2D Diffusers are most commonly referred to as Skyline diffusers after RPG Inc’s model with that name. They scatter acoustic energy in a hemispherical pattern, both horizontally and vertically. Here are some examples of 2D diffusers:
RPG Inc’s Skyline Diffuser (http://www.rpginc.com/products/skyline/index.htm) This diffuser is based on a primitive root number sequence instead of the more commonly used quadratic residue number sequence.
Auralex Acoustics’ Wave Prism (http://www.auralex.com/sustain/waveprism.asp) The Wave Prism uses a grid of dividers to separate the blocks of different heights which, according to Schroeder, offers better diffusion properties.
According to Schroeder’s research, both types of diffusers work on the same basic principles. The width of the wells (or the blocks) determines the upper frequency limit. The depth of the wells (or the blocks) determines the low frequency limit. The math behind this is as follows:
The wavelength (λ) of a frequency is equal to the speed of sound (c) divided by the frequency (f).
The low frequency limit of effectiveness is defined by frequency whose wavelength is four times the depth of the deepest well (or tallest block).
The high frequency limit of effectiveness is defined by the frequency whose wavelength is 2 times with width of the wells (or blocks).
Let’s use RPG Inc’s QRD 734 as an example. The wells of the 734 are roughly 9 inches deep and roughly 4 inches wide providing the following bandwidth:
Or roughly from 375 Hz to 1700 Hz.
In independent tests performed on RPG’s QRD, the actual bandwidth of diffusion extended to approximately double what Schroeder’s theory predicted. We also found in our testing that the upper limit was significantly higher than the formulas predicted.
The depth of the wells is another area where the Acoustic Ramp™ has a major improvement over previous diffusive treatments. The wedge-shape of the diffuser means that the depth of the wells are continuously variable, which means that the frequency response is much wider than a typical 1-D diffuser.
Additionally, the Acoustic Ramp™ varies between a depth of 12 inches to a deep of less than a half inch. The deepest part of the diffuser is usually installed in the corner where the ceiling meets the wall, taking advantage of typically unused space in the room. The diffuser tapers as it descends the wall allowing racks, furniture and other equipment to be placed against the wall without trapping space.
The angles formed by the wedge shape of the wells allow the installer to direct reflections away from the sound source. In the most common installation, the wedge shape would direct reflections down toward the floor. In alternative installations, and array of Ramps could be used to direct reflections towards the side walls. In both of these cases, directing sound energy away from the sound sources helps to significantly reduce the effects of comb filtering.
This video slide-show depicts David Shotzberger assembling the first commercially manufactured Acoustic Ramp™ at Redco in CT. Please imagine dramatic music composed by John Williams in the background.
It takes about 20 minutes to assemble one of the Acoustic Ramps™ with only a screwdriver, and it could even be done by an intern if necessary!
The first two commercial prototypes of the Acoustic Ramp have been produced and assembled for the initial round of Quality Assurance. Creation of the prototypes was masterminded by David Shotzberger who generated the CAD drawings and supervised the production.
The new commercial version of the Acoustic Ramp is manufactured from 1/8″ Aluminum Stock, as produced by Keith at Redco, and 1/2″ pre-finished maple plywood as produced by The Old Lumberyard, Inc. The manufacturing is expensive, especially when compared to least-common-denominator companies, but worth every penny.
The Acoustic Ramp™ (Patent US20120018247) is a unique diffusion-type of acoustic treatment that both scatters and reflects acoustic energy. The wedge shape of the Ramp allows the installer to direct reflections away from both the sound source and the listener drastically reducing comb filtering while creating a sense of acoustic open space.
Diffusion is one of the most misunderstood tools for controlling acoustics in rooms. Diffusion diminishes flutter echo and hard reflections that create confusion in both the time and frequency domains. Many acousticians consider diffusion to be the icing on a cake made from wide bandwidth absorption. Many listeners strongly prefer experiencing music in a environment where at least the back wall is diffusive.
The Acoustic Ramp is based on the work of physicist, Manfred R. Schroeder, who invented Q.R.D’s or Quadratic Residue Diffusers. Our improvement over Schroeder’s design is that the diffuser is wedge-shaped and the well depths increase along the length of the ramp. This greatly widens the bandwidth of the affected frequencies. Also the backs of the wells are angled which reflects and redirects energy away from the direction from which it came.
Currently, the Acoustic Ramp is available in the following size:
2×4: 24″W x 48″H x 12″D (>282.5 Hz)
Currently all orders are custom-made to your order. We recommend that 2 or more diffusers are used together as an array on the rear wall of critical listening spaces or control rooms.
Please call (781) 710-4521 to discuss your acoustic treatment needs and to place an order.