Zilch is measuring mids and tweets only in a pair of speakers whose woofers have been removed for refoaming (and from the photo he has posted, the stuffing has apparently come out as well). So as measured so far, these speakers have no stuffing.
3a's are loose-stuffed. The stuffing is determined by weight and fluffed to distribute evenly throughout the cabinet, so should not be concentrated in any particular region of the cabinet volume. The mid and high drivers both have closed backs, not open as in the woofer.
I think cabinet-related issues being discussed so far are not resonance, but possible interference caused by portions of the structure that may protrude into the drivers' sound fields.
Now THERE's a thought.... :scratch2:Zilch,
Please tell me you aren't going to econowave these :nono:
See the polars I just posted @ #1.... :yes:Oh, and it sure looks like resonance to me.
Hi, Pete!I referenced it here, and there is some discussion of the #7 vs. #9 woofer inductor, do you know which is used in the systems you're testing?
See the polars I just posted @ #1.... :yes:
None of note.It may be because I just got in from a dinner out where I may have had a bit too much, but I need to be whacked over the head with obviousness right now. What kind of cabinet resonance do a mid and tweeter with sealed backs produce?
Ok, it just hit me. Cross out "interference" in my previous post and substitute "diffraction."
They didn't publish those curves in the literature, of course.Now we reinstall the grille cloth molding and make the front of the molding flush with the inside of the smooth chamber wall. Fig. 5 shows the on-axis response obtained with the level controls still set at maximum. The mere presence of the molding produces increased level (on axis) in the range of 300 to 1000 Hz, a 5 or 6-dB notch at 1400 Hz, and miscellaneous perturbations on up in frequency.
Figs. 6 and 7 are 15° families of the complete system, taken in a horizontal arc, first in one direction away from the system axis and the in the other. The grille molding is in place and the level controls are at maximum. It is difficult to assess performance because the output level changes rapidly, not only with frequency but with small angular increments as well. And one must keep in mind that the output variation has been observed only in one plane around the system.
When using loudspeaker systems that have low directivity factors at all frequencies, listeners at typical listening positions in virtually all living rooms are well within the area in which the reverberant field dominates.
The reverberant field spectral balance is determined primarily by the acoustic power frequency response of the loudspeaker system. Thus, the single most important factor in assessing the "frequency response" of a loudspeaker system is the integrated output at all angles.
None of note.
I haven't identified any resonances per se, as yet. They characteristically remain constant no matter the measurement angle. Interferences, on the other hand, will vary as that changes, which is why I pointed Paratima to the polar measurements; off axis in the one direction, the 1.8 kHz null becomes a peak.Must be me, but I'm still confused. If there is none of note, what effects are you measuring that appear to be the result of "resonance?"
Even when the individual speakers [drivers] in a high-fidelity speaker system radiate energy in a smooth and uniform manner at all forward angles, if each is measured by itself on a flat baffle, the system in which they are used does not do so. Interference between speakers in crossover frequency regions causes reinforcement at some frequencies and cancellations at others. The frequencies at which these effects occur change with the angle from the system axis at which the direct radiation is measured, because the speakers cannot occupy the same space on the mounting plate; therefore, as the microphone is moved around the cabinet, the differences in path lengths change.
Another source of similar perturbations in the system's radiation pattern is diffraction, which is really a form of self-interference. Mounting surface discontinuities, the grille cloth molding, and the dimensions of the cabinet itself all produce diffraction that affects the direct-wave radiation in a complex manner dependent on the angle of the cabinet with respect to the microphone.
I haven't identified any resonances per se, as yet. They characteristically remain constant no matter the measurement angle. Interferences, on the other hand, will vary as that changes, which is why I pointed Paratima to the polar measurements; off axis in the one direction, the 1.8 kHz null becomes a peak.
That's what Allison said it was, nearly 40 years ago.I'd say interference with the raised edge to the left of the mid, which might be about 4 inches away. That's my guess.:thmbsp:

I'd say interference with the raised edge to the left of the mid, which might be about 4 inches away. That's my guess.:thmbsp:
That's what Allison said it was, nearly 40 years ago.
He also said it is inaudible, postulating that it is "filled in" by the reverberant sound field, which dominates the direct in normal home listening environments using AR3a....![]()
To hear it?So now you have to go find an anechoic chamber somewhere... :scratch2:
That's what Allison said it was, nearly 40 years ago.
He also said it is inaudible, postulating that it is "filled in" by the reverberant sound field, which dominates the direct in normal home listening environments using AR3a....![]()
Ultimately the "Max dispersion, max artificial soundstage" approach fell out of favor, and loudspeaker designers focused instead upon cleaning up the direct field to achieve improved imaging and accuracy, while minimizing reliance upon room reflections and the reverberant field.
[Except one well-known purveyor of "Direct Reflecting" technology....]
In the light of thise findings we believe that typical operating settings for loudspeaker high-frequency balance controls should be well below the settings which produce flat acoustic energy if the objective is a spectrum similar to that produced at a concert hall seat. In view of the variations found in both living room and concert hall frequency balance, and the manner in which these variations occur, we think that home listeners should be encouraged to make more liberal use of amplifier tone controls.
Certainly, in view of current recording practice, flat electrical response in the playback system is more likely to be wrong than right, particularly if the loudspeaker systems used for playback are able to deliver nearly flat acoustical power output and are adjusted to do so.
Does this include the good Doctor Geddes?Ultimately the "Max dispersion, max artificial soundstage" approach fell out of favor, and loudspeaker designers focused instead upon cleaning up the direct field to achieve improved imaging and accuracy, while minimizing reliance upon room reflections and the reverberant field.
[Except one well-known purveyor of "Direct-Reflecting" technology....]