Thank you very much Cosmik for taking the time to write an in-depth reply.
Basically to be a single acoustic source with uniform directivity at all frequencies, reproducing the signal as it is recorded in the time domain not just 'spectrally correct' - as much as is possible. (See my user profile for the full version!).
I looked at your profile . I share some of your skepticisms, notably about in-room measurements and "room correction". Excellent analysis of the flaws of "room correction".
Apparently you have a very comprehensive set of ideas about of what is right and what is wrong when it comes to loudspeaker design.
Could you clarify your concluding statement? "In audio, it is better to design things based on
feedforward logic and justified assumptions, rather than experimental
feedback which is, ultimately, based on unjustified assumptions." What do you mean by "feedforward" logic? The implication seems to be that you reject error-correction mechanisms, so what happens if your initial assumptions include mistakes? How does an assumption become "justified?" Why is experimental feedback ultimately based on "unjustified assumptions?" (Yes I read your paragraph about someone knowing they are taking part in a listening test, and that didn't convince me.)
On a more nuts-n-bolts level, how do you "compensate for directivity characteristics" using "calculated in-room EQ"? That is not something I would have thought of, so it sounds very interesting to me, whatever it is.
"1. [Dipoles] create reflections that do not resemble the direct sound and are therefore breaking mechanisms within human hearing that rely on similarities of envelope shapes and polarities of wavefronts to be perceived as reflections and not new sound sources - essential for correct imaging and soundstage.
So, if the ear/brain system uses the envelope shape (spectral balance) to identify reflections, then a dipole's reflections will be correctly classified as such. And if the ear/brain system uses the polarity of the reflection's wavefront, then a dipole's reflections will be mis-identified as new sounds and the imaging and soundstaging will be a disaster.
Am I understanding you correctly?
2. [Dipoles] create direct comb filtering that reflects from surfaces around the speaker."
It depends. Most dipoles have narrow vertical dispersion, so they generate fewer floor-and-ceiling reflections. Many dipoles have fairly narrow horizontal dispersion, and correspondingly generate less sidewall reflections (not to mention their nulls to the side). The backwave will generate comb filter effects that look like a total disaster in a frequency response measurement but will be benign to the ear, just as any live instrument in any room will have comb filter effects from room reflections that look horrible on paper but are benign to the ear.
3. [Dipoles] create egregious comb filtering that changes dynamically as the listener moves, heard as 'phasiness' and in-head effects.
If you are talking about dipoles with side-by-side line source drivers, then I agree, that's a source of comb filtering which changes the sound as the listener moves. Not the best choice for playing air guitar!!
4. [Dipoles] create indirect comb filtering from interactions of the positive and negative reflections.
The reverberant field will be decorrelated at medium and high frequencies whether the source is a dipole or a monopole. At low frequencies, the reverberant field transitions to being fairly well correlated, as the wavelengths become long relative to the room's dimensions. I think dipoles generally produce a more decorrelated low frequency soundfield than monopoles do, which would contribute to their in-room bass smoothness, and imo that's a good thing.
I don't see any obvious downsides to dipoles from "interactions of their positive and negative reflections."
5. In order to reduce (but not eliminate) some of these negative effects, [dipoles] become more difficult to position in the room.
Dipoles need sufficient space behind them to give a fairly long path-length-induced time delay to the backwave energy. I have explained why that matters, but can do so again if you would like. Horizontal spacing and toe-in angles are chosen using the same criteria as any other speaker, except that dipoles are not going to get boomy if placed right up against the side walls because they have nulls to the side.
I can't think of any other placement difficulties imposed by the "negative effects" you listed. Can you?
As I was careful to say earlier, I was replying to the whole open baffle 'school', not anyone in particular.
Really??
Here is the entire sentence, cut and pasted. These are your exact words:
"If you wanted to define
why a speaker should be a dipole, then I would be interested - rather than just saying that existing dipoles are often adequate and sometimes generate a really nice effect.”
The first half of the sentence is clearly addressed to one person, me. Did you REALLY transition to “replying to the whole open baffle 'school', not anyone in particular” halfway through the sentence?
I think you're much too good a writer to carelessly switch from second person to third person in the middle of a sentence.
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I guess I was hoping to find more common ground. Well, I do agree with you about this part: "Uniform directivity at all frequencies, reproducing the signal as it is recorded in the time domain not just 'spectrally correct' - as much as is possible" would be very nice to have.
(Ironically, some dipoles come pretty darn close to this ideal. For example, the classic SoundLab electrostat is a single fullrange driver whose radiation pattern is ninety degrees front-and-back at frequencies where the panel's directivity dominates, transitioning to the classic dipole figure-8 as the wavelengths become long relative to the panel width.)
Do you have a particular radiation pattern width or shape in mind for your uniform directivity?