Absorption, Reflection, Diffusion
Three things and only three things happen to sound energy. Sound energy is absorbed, reflected, or diffused. Absorption converts sound energy to heat and then sound energy is lost forever. We have to be careful losing energy in order to manage it in our small room acoustic situations. Reflections are always with us from our room boundary surfaces. Diffused sound takes a conscious design goal to achieve proper results.
One method of diffusion that is widely known but not well understood is quadratic diffusion. Quadratic diffusors have been around for years and Peter D’ Antonio’s company, RPG, was the first company to make them commercially available. Quadratic diffusors have a series of wells or troughs of different depths, that when sound energy enters these wells or troughs it is bounced around inside the well and returns from its journey in a smaller version of itself spread out in a 180 degree, fan like array of energy. A QRD diffuser comprises wells of different depths, causing a mixture of phase shifts that diffuse reflected sound. They are used to control reflections in the listening environment, particularly from rear walls and first-reflection points.
More Than One Needed
Quadratic diffusors can be used alone but the best way to achieve good results is to use multiple panels, side by side. A quadratic diffusor that is placed vertically, will diffuse sound energy back into our rooms in a horizontal, fan like array and a diffusor place horizontally in our room, will spread sound energy out that enters it in a vertical, fan like array. With both vertical and horizontal diffusors, one can have a two dimensional diffused sound field.
Formula For Well Depth
There is a formula for calculating the amount of wells or troughs we need to use and what those wells or troughs depth dimensions need to be. The well depth = (well position) squared mod N where N equals the number of wells and is a prime number.The squared portion of the equation determines the phase shift introduced by each of the wells and the mod operator keeps the shift within the range from 0 to 360 degrees. Raising a number to a power is known as a quadratic operation. Applying the modulus operator divides a number by the modulus and only keeps what’s left over, known as the residue. This explains why the design is called a Quadratic Residue Diffuser, or QRD diffuser for short.
Formula For Well Width
The width of the wells determines the high Frequency (HF) cutoff frequency, where the width represents one half-wavelength. This is only for the incoming signal straight-on. For other angles of incidence, the HF cutoff is decreased, falling to zero for a signal striking from side-on. The period width has to at least equal the wavelength of the lowest frequency diffused. Software is available to assist one in the calculations.
Below the design frequency, diffusion no longer occurs, but it is generally accepted that scattering is available down to one octave below the diffusion limit. For diffusion to occur, the wavelength of the lowest frequency diffused must be no larger than the period width of the panel. If this rule is not met, then the lowest frequency diffused is the frequency that does fit into the period width. This frequency is referred to as f period, and the new scattering limit becomes one octave below this.
For the interference patterns to fully develop into a diffuse field, it is recommended that the minimum seating distance be three times the longest wavelength diffused. Diffused wavelengths need time to form completely before they reach the listening position. If one is seated too close or has the diffusor too close to the speaker or sound source, the diffused wave does not have time to properly form and you can have image shifting.
Diffusion lobes are created when a number of repeats of a periodic surface are placed together in a sequence. For multiple QRD panels, the number and angle of the diffusion lobes varies with the panel order and panel width, and the frequency and angle of incidence of the incoming wave. For a signal straight-on, there are usually three lobes at the design frequency, and at the HF cutoff frequency there are often the same number of lobes as there are wells.
As the angle of incidence is increased, starting frequencies for each of the lobes decreases slightly for lobes on the same side of the diffuser as the incoming signal. Lobes on the other side shift to a higher starting frequency by a larger amount. The angle of the lobes also changes, as does their relative angular spacing. In addition, the apparent wavelength of the signal changes as far as the wells are concerned, leading to a lowering of the HF cutoff frequency. When the angle of incidence reaches +/-90 degrees, the HF cutoff falls to zero, meaning no diffusion.
How Many Wells?
One can calculate what design frequency to use for any situation. As a general rule, one must use a prime number that can produce as many wells or troughs in the diffusion array as space permits. The more wells, the more frequencies diffused. A quadratic diffusor based on the prime number 23, will have 22 wells and 23 well dividers. If each well is 1″ wide and each divider is 1/4″ wide, we will have a diffusor that is approximately 28″ wide for each array. If we have a wall space that is 12′ wide, we will need 5 separate units placed side by side across the wall surface.
Quadratic diffusion is a powerful tool to manage room boundary reflections. It is a tool that can take the reflection and “break” it down into smaller “reflections” that can then be spread out into the room into vertical and horizontal directions without any change in the signals time signature. Build a diffusor that can diffuse as much energy as your space permits by using the free software available today.