Acoustic Horn Design – The Easy Way (Ath4)

When you have heard a well designed MEH you know why you do it.
Here is a prototype I'm working on atm.
Where the drivers face each other in order to minimize the vibrations in the horn.
Maybe it's a good idea, maybe it's a bad idea.
One way to find out 🙂
mehproto.JPG
 
Mabat,
What filament type do you use? pla? abs?
Thanks,
Paul
Mostly PLA, but I don't have much experience with different materials. Tried PETG a few times, it's really light. But those were all basically prototypes. I would definitely use something more sturdy for the final adapters (maybe I would even try to cast them instead). For petals I guess it's already good enough, as I tend to make them rahter lightweight and basically hollow with only a very sparse infill. The thickness alone seems to do a lot.
 
A460G2 / BMS 4554 (16 ohm), long adapter, electrical impedance.

What to take from this?

1735822060748.png


The "noise" between 700 Hz - 2.5 kHz is remarkably stable (averaging does nothing). It changes a little bit only with a different orientation of the waveguide relative to the environment. So this must be the driver picking up the sound field (?) and I guess the curve would be cleaner in an anechoic room.

Which leads me again to wonder how much is the impedance "modulated" by the picked-up signal of the reproduced sound field during playback. The driver acts as a microphone at the same time, right? I guess that a high sensitivity doesn't really help in this regard.
 
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The second 4554 driver sitting on the table, without a horn, with the exit open (red) and covered with a blanket (black).

1735824171770.png


- I would think that if the wiggles were due to a microphone action, they should be smaller with a series resistor but maybe I'm wrong. I'm hopelessly dumb at electronics and I gave up a long time ago.

So, what causes the wiggles?
 
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How about connecting the driver as a microphone and analyze the recorded sound?

Also during the impedance measurement the driver is connected to the amplifier via a resistor with a higher impedance. This might have also some influence on the measurement.
 
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A460G2 / BMS 4554 (16 ohm), long adapter, electrical impedance.

What to take from this?

View attachment 1401718

The "noise" between 700 Hz - 2.5 kHz is remarkably stable (averaging does nothing). It changes a little bit only with a different orientation of the waveguide relative to the environment. So this must be the driver picking up the sound field (?) and I guess the curve would be cleaner in an anechoic room.

Which leads me again to wonder how much is the impedance "modulated" by the picked-up signal of the reproduced sound field during playback. The driver acts as a microphone at the same time, right? I guess that a high sensitivity doesn't really help in this regard.
The driver is fed by high impedace?
What about damping the "bell" of the 460? Something rubbery with high density...
 
When you add the resistor in series, while it should reduce current from microphonics it also reduces electrical damping. Try with capacitor in series for poor electical damping and "high" current from microphonics. Try also with series resistor plus an inductor between the driver and resistor, parallel to driver, to make a "sine-cap" highpass filter. This maintains low impedance at the main resonance for electical damping, while puts higher impedance higher up to reduce microphonics.

Anyway, I think the high impedance, or wiggle, is some extra velocity of the moving parts. Extra in sense that diaphragm moving induces current whose vector sum with current from amplifier (if moving parts were clamped down) makes total circuit current to reduce = impedance to increase. Thinking other way around, when there is impedance peak the diaphragm moves more than it should, with given excitation by the amplifier. ~Everything that makes impedance vary beyond Re + Le is from movement of the diaphragm, and varying forces affecting that movement, which affects circuit current (since amplifier voltage is constant).
 
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Do you have the simulated acoustical impedance curves of the A520G2 and A460G2 with the T520-4554-EXT Adapters? Maybe some differences are visible?

If I remember correctly, the first simulations of an extend throat did show some ripples in impedance?
 
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