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Diffraction from baffle edgesLoudspeaker cabinet edge diffraction is a subject of never ending debate. I am not aware of any scientific study as to the audible effects of diffraction, but since it adds ripples to the steadystate frequency response of a loudspeaker, especially for symmetrical driver layouts, there are many claims to its detrimental effects. Especially popular are time domain explanation using a sound impulse or pressure step of infinitely short rise time. In reality the fastest rise time is given by the tweeter's high frequency cutoff. At those frequencies almost all tweeters are highly directional and little sound reaches the cabinet edge to be diffracted. Thus, the portion of a sound pressure step that travels along the baffle surface has a much slower rise time than the portion that propagates onaxis. Consequently the magnitude of any diffraction effect is greater at the low frequency end of a driver's range. All this must be taken into account when modeling radiation from a loudspeaker on the computer, otherwise the effects of diffraction are overestimated. I have tried to explain the physics of diffraction in FAQ 8. Here I give some measured examples. For a source I used a small Neodymium magnet tweeter of 38 mm outer diameter, with a soft dome and 25 mm voice coil. Baffles of circular and rectangular shape are mounted to the tweeter. The baffles are 1/8th inch thick and cause a maximum of diffraction. Real cabinet edges are usually at 90 degrees or rounded, which reduces the magnitude of the diffracted wave, since the wave does not immediately expand into 4p space upon reaching the edge. The benefits of edge rounding come into play only when the radius is greater than 1/8th wavelength. Thus a typical 1/2 inch radius begins to diffuse the diffracted wave at frequencies above 3.4 kHz, but will decrease in relevance at higher frequencies, when the driver illuminates less of the edge due to its increasing directivity. With most speaker cabinets the radius or chamfer is acoustically too small and is primarily cosmetic.
The impedance (1) of the tweeter shows a 3.2 kHz peak due to its mechanical resonance and a slight irregularity at 13 kHz. It can be expected that the frequency response rolls off at 12 dB/oct below the mechanical resonance as for any closed box dynamic driver. This rolloff behavior can be seen in the onaxis frequency response of the unbaffled driver (2). There is also a peak corresponding to the impedance irregularity at 13 kHz. The low frequency rolloff has no influence on the results of the following diffraction investigation since only the change in onaxis response due to the different baffles is of interest. For a 3 inch circular baffle with a point source at its center there should be a 4.5 kHz peak, a 9 kHz dip, a 13,5 kHz peak, a 18 kHz dip and so on, whenever the edge is at multiples of a half wavelength from the source. Note that above about 14 kHz the baffle has no effect, because the dome has become too directional to illuminate the edge. The dome diameter becomes acoustically too large at higher frequencies to be considered a point source and the shape of the response ripples is smeared. Below 1000 Hz the baffle has decreasingly less effect. The source becomes omnidirectional. With increasing frequency, though, the onaxis SPL of the 3" arrangement increases faster than for the bare tweeter. This is the so called "baffle step", where radiation contracts from 4p space to 2p space. An increase in baffle diameter to 6" causes the baffle step to begin at half the frequency of the 3" baffle (3). The onaxis pressure increase due to diffraction can be up to 10 dB for a circular disc. This is approached at 2 kHz in (3) and at 1 kHz in (4) for the 12" disc. Note the increased number of peaks and dips as the baffle diameter is increased, and the peak to trough amplitude variation is not much different. The diffraction ripple amplitude generally decreases with increasing frequency, because of increasing directivity of the driver and a sound pressure that is inversely proportional to the distance from the source to the edge (4). The onaxis response for a thin circular baffle represents the worst case of diffraction. The typical rectangular baffle is more benign, because the distance from the tweeter to the edge varies and there are no frequencies for which all the distances are multiples of a half wavelength. A point source in the center of a square baffle is the worst case amongst rectangular baffles, because of symmetry. A small 3" square baffle gives only a slight reduction in diffraction ripple compared to a 3" disc (5, 2), because of the large dome size relative to the baffle. More effective is the 6" square baffle (6, 3). Note that above 6 kHz there is little difference in the response to a 3", 6" or 12" square baffle (5, 6, 7). The main differences are below this frequency. Reducing the width of the 12" square baffle to 6" has only effects below 5 kHz (7, 8). This even holds when the width is further reduced to 3" (7, 8, 9). The baffle step shifts up in frequency as the baffle becomes narrower, as would be expected. I hope that the illustrations and FAQ 8 will give a little more insight into the complexities of diffraction and that it is difficult to speak in generalities about the effects of cabinet width, cabinet shape and driver diameter since they are wavelength dependent and change with frequency. It has been my experience that the onaxis and offaxis frequency response of a given driver and baffle combination must be measured to assess overall uniformity of response, and that computer models give pessimistic predictions, because the underlying assumptions do not sufficiently describe the real acoustic behavior of drivers and of cabinet shapes. While I try to minimize visible diffraction ripples in the frequency response for good measure, I have no evidence that even strong diffraction effects have significant audible consequences, except for the transition region, the "baffle step", where radiation goes from omnidirectional to forward firing. Note that there is no baffle step at 90 degrees offaxis, and boosting low frequencies for a flat onaxis response will add to the downward sloping trend of the frequency response offaxis. This causes a spectral imbalance of the reverberant sound field in the room and is a major reason why I prefer dipole radiators. Diffraction effects are always spatially localized and a slight shift in listening position will change their magnitude. While the "baffle step" cannot be avoided, the additional higher frequency ripples can be easily reduced to a magnitude that is much smaller than the first arriving direct sound, by simply optimizing the proportions of a rectangular baffle. The absolute width of a cabinet is not the critical parameter that many people think it is. Much is hypothesized, little is proven and much is overrated when it comes to diffraction.
 Diffraction  FAQ 38 
