For a slightly higher DI -
It's actually better on diagonal (SPL_D chart). This is 14" wide, 1.4" throat. The cyan line is for 45° off axis (7.5° step).
Dmitrij_S - good points, I suppose.
It's actually better on diagonal (SPL_D chart). This is 14" wide, 1.4" throat. The cyan line is for 45° off axis (7.5° step).
Dmitrij_S - good points, I suppose.
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It is actually about 90° coverage nominally (the first one).A flatter waveguide is always going to be smoother, but with less DI control. As the DI gets raised there will be more problems. ...
Will try to test a bigger one with 1" throat.
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This is also funny: Today, solely by mistake, I tried something I didn't want (what could be considered as an error), but hey, the result is one of the best I have seen -
Now I know how to improve things! 😀
There you go 😉
I suppose, revolutionary improvement would mean
* Flat acoustic loading from 200-300Hz and up to the last audio octave (e.g. like Heavise or step Sigmoid function).
* Constant directivity in the same frequency range. (I suppose beamwidth of -+(20-30)° in all directions would be ok, at least for home audio).
*Horn-related acoustic nonlinearities would be comparable to that of the direct radiator.
*Perhaps, some kind of numerical criterion should specify a minimum value of HOMs amount.
"Revolutionary design" should improve all the point above at the same time. But as we know, "the horn reality" is completely different. Numerical optimisation helps to find a certain balance of contradictory horn parameters 🙂.
You mention 4, of which I came up with 3 myself.
Now some of Einstein's quotes would be appropriate, but redundant.
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So, this is 16.1" x 15.5" horn, 1" throat. There are obviously some wiggles from the analysis as this was still only a coarse setting. Otherwise pretty good, isn't it.
Again, cyan line is for 45° off-axis.
Again, cyan line is for 45° off-axis.
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OK, this is the magic (or half of it). I guess it would be even patentable 

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The same for a circular one (16.2") - there is a very slight narrowing just below and around 2 kHz compared to the rectangular one.
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The narrowing doesn't seem serious.
Are the parameters of the circular identical to the rectangular, apart from those defining the mouth shape?
Is the pure OS wg the "old one" (52cm Ø)?
Are the parameters of the circular identical to the rectangular, apart from those defining the mouth shape?
Is the pure OS wg the "old one" (52cm Ø)?
It probably isn't serious but it isn't nice either. This is what striked me the most - how perfect is the rectangular one in this regard. Not seen so often.
The parameters are the same. I'm not sure about the effects on different shapes.
The parameters are the same. I'm not sure about the effects on different shapes.
No, this is a different one, about 16" across. Matching in size the one before.Is the pure OS wg the "old one" (52cm Ø)?
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Basically what is done here are protrusions and grooves made in the surface but not in a symmetric manner. When you directly compare the pure OS (on the left) and the one with grooves, the latter is a bit better. Not a huge effect but definitely in the right direction.
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I wonder what would happen if you made the 'ridges' more pronounced.
The difference between pure OS and 'ridged' ('ribbed' ?) is small, but clearly visible indeed.
The difference between pure OS and 'ridged' ('ribbed' ?) is small, but clearly visible indeed.
* Flat acoustic loading from 200-300Hz and up to the last audio octave (e.g. like Heavise or step Sigmoid function).
* Constant directivity in the same frequency range. (I suppose beamwidth of -+(20-30)° in all directions would be ok, at least for home audio).
*Horn-related acoustic nonlinearities would be comparable to that of the direct radiator.
*Perhaps, some kind of numerical criterion should specify a minimum value of HOMs amount.
My comments would be (in order)
* since loading is almost irrelevant to performance, I don't see this as very important.
* this is achievable now with a no-compromise design. Its the size and other details which when compromised create the performance degradation.
* since the acoustic nonlinearities in the waveguide are insignificant, this isn't very important.
* as the design becomes less diffraction oriented, the driver dominates the generation of HOMs. Hence, this is not really an aspect of the waveguide that is of concern. It is, of course, a big concern in waveguides where HOM generation is not taken into consideration, but for the "perfect" device we are talking about, the HOM generation in the waveguide is dwarfed by that generated by the driver.
Basically what is done here are protrusions and grooves made in the surface but not in a symmetric manner. When you directly compare the pure OS (on the left) and the one with grooves, the latter is a bit better. Not a huge effect but definitely in the right direction.
Honestly, I don't see much difference since you say that the small glitch at 4.5 kHz is numerical (which seems right to me as it looks like a single point.)
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The difference, although small, is immediately obvious if you switch between the two pictures back and forth (easily by opening them in two different panes of the web browser).
As the design becomes less diffraction oriented, the driver dominates the generation of HOMs. Hence, this is not really an aspect of the waveguide that is of concern. It is, of course, a big concern in waveguides where HOM generation is not taken into consideration, but for the "perfect" device we are talking about, the HOM generation in the waveguide is dwarfed by that generated by the driver.
So far I have only seen one (exotic) manufacturer, or rather his son, who seems to have taken this into account when developing custom driver / horn combinations. These are clearly modern revisions to Salmon horns and companion drivers, but an interview with the guy revealed that he extensively modeled, simulated and optimized the drivers (phase plugs) and horn interface(s) in COMSOL in order to suppress the modes.
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