April 2012

Foaming At The Mouth
Article By Jeff Poth
Difficulty Level
Boy,
do I wish all titles were as easy and appropriate. We're talking about a
wonderful tweak I've been working with for a little while, that is acoustic
absorption at the mouth of a horn. You may have seen this in some commercial
horns -- the Urei studio monitors had a coaxial horn tweeter (very similar to
the coaxial Altecs) and used a foam treatment around the edge of the mouth.
Peavey also utilized a foam inset edge on their "Quadratic Throat Waveguide", linked is
their
PDF of this, yet it doesn't cover the foam but is very
worth reading as a historical interest piece on horns.

As you can see, the mouth of a plain conical horn (and the
vast majority of horns, overall) has a very sharp edge, where some modern horns
incorporate a roundover. When a horn ends and the wavelength exceeds the
pathlength on the horn, it ceases to load the compression driver and transitions
from the radiation pattern defined by the horn to one of free-air radiation. At
this point, the edge acts like a secondary sound source. Just as with the
edges of a box loudspeaker, the more gradual you can make the transition the
more benign the effect of the diffraction in the loudspeaker. With horns this
transition is even more dramatic than in a box speaker, as you're not going
from 180 degrees to 360 but from 90 or less degrees to a full free-air (360
degree) radiation. By making the transition gradual, a minimum of diffraction
peaking takes place and you maintain the cleanest transition from the horn
loaded bandwidth to the unloaded "free air" portion. The price paid for a
very thorough smooth transition from loaded to unloaded is an increase of the
mouth size. The pic below shows a moderate horn termination, this termination in
some horns is two or three times as large.
As you probably know,
it's desired to get the centers of each loudspeaker
driver as close to each other as possible. This prevents pathlength
differential, and ensures that the output from each driver adds to the output
from the other driver(s). If you're half-wave (180 degrees) closer to one
driver than the other, then the output from the two drivers will cancel each
other. This is incidentally why the dispersion in a loudspeaker driver decreases
with increasing frequency. At some higher frequency (shorter wavelengths) the
width of a cone becomes significant relative to the wavelength and different
distances from your ear to one side of the cone/dome or the other are half-wavelength (180 degrees) and thus
there's a minimum of output because the wave
is cancelling. The peaks and valleys caused by this are called "comb filtering" because the regular pattern of peaks and valleys looks like the
fingers of a comb.
So, we have conflicting requirements. On the one hand, a big horn with a large
mouth termination is desirable to allow the horn to control to the lowest
frequency and transition smoothly from its defined radiation pattern into
free-air radiation. The drawback is large center-center spacing, and accordingly
you get smooth off-axis response from a clean mouth termination, but get
cancellations and "comb filtering" of the off axis response due to the large
spacing. Alternatively, you can try to use a less thorough termination of the
horn, and live with the diffraction-based ripple and inconsistent off-axis
low-end response, but achieve better summation behavior between the two drivers.
Problem
Solved
Well, maybe not, but there is always more than one way to skin a cat. Instead of
a lossless method like a large mouth termination (all acoustic energy is
preserved) we can move to a lossy termination. This is where foaming at the
mouth comes in. Acoustic foam (and other materials, one could use felt or
another material, but foam is probably best here) can absorb the unwanted energy
that's passing around the horn termination. Think of it as an egg. If you
gently roll it down a ramp to the floor, it goes in the direction of the ramp
without breaking. If you simply drop it, it breaks and goes in all directions.
The third option is to drop it onto something soft and absorbent- the foam. This
way it doesn't break. The kinetic energy of the fall is not preserved as in
the way the egg rolls after coming off the ramp, but you don't need a big ramp
to accomplish the desired effect of the egg not breaking. So the foam on a horn
edge acts to absorb the wavefront outside the desired coverage pattern, rather
than preserving it and allowing the coverage pattern to gently expand to the "final" unloaded 360 degree pattern. The critical part is that the egg
doesn't break. That diffraction energy scattering everywhere creates its own
comb filtering, and contributes to a harsh and/or vague character at the bottom
of the horn's passband.
What To Use
The great thing about foam is that it's common. You can get acoustically
useful foam from a variety of sources. Foams are made up of a variety of air/gas
filled cells; the critical component is that it's relatively open in its cell
structure. It's important to note, from a
safety standpoint, that large amounts of foam can be a fire hazard unless it's
treated, flame retardant foam. The problem is twofold- some foam lights quickly
and burning plastics create VERY nasty fumes. Do exercise some caution with heat
sources and any foam you choose and only use foam sold as flame retardant
treated acoustic foam if you have any residual concern. The correct
material is soft, usually charcoal grey in color, and does not stop air from
flowing through it. Yep, pucker up, you're blowing through it to make sure.
The right stuff is open cell foam, meaning that the cellular structure of the
foam has at least one, usually a couple, walls removed from each cell. The
extreme version of this is the reticulated foam as used in the throats of horns,
as seen in my waveguide article.
Reticulated foam is a fully "open cell" foam, there are no
cell walls remaining, just a ‘web'. There is also closed cell foam, which
will not allow air to pass through, which retains all of the cell walls. If you
do the pucker test and find a modest resistance to airflow, but not a stoppage
or a lot of force required, it's suitable. Appropriate foams are often found
in material packaging, I used packaging from laptop shipping boxes for mine.
Thicker is generally better for this purpose, but naturally you're limited by
how the foam would interact with the other speaker drivers, you don't want to
absorb the wavefront from the other drivers, if you're adding it to an already
well-tuned system. In some cases this may not be an issue.
So, what does it do
in the real world?
In this first example, there's a thin sleeve around the
outside of an already rounded mouth. This is just a simple way of making the
mouth roundback act like it is larger than it already is. In this case I noted a
reduction of midrange energy outside of the coverage pattern and a slight
increase in intelligibility. Foam is applied to the whole back of the horn,
creating a "deadzone" for unwanted energy. The rear view better shows the
circular foam applied around the mouth. This is the Oblate Spheroid Waveguide (OSWG)
as in my article above.

The second example is with a "Progressive Transition" waveguide, a JBL
design. In this instance, thicker foam was used as the termination of the
waveguide does not have the attention paid in the OSWG. As you can see, the foam
projects forward from the waveguide, acting as a lossy extension of the horn,
this is a more dramatic take on the foam treatment shown above. The desired
frequencies (where the horn loads effectively) are largely unaffected as their
coverage is defined by the horn prior to the effort on the termination, but the
frequencies around and about the cutoff of the horn (where it ceases to load)
are dramatically improved. This waveguide shows a peak in the 1 to 1.2 kHz
range, and the foam reduced this about 2dB on-axis, and dramatically improved
the behavior off axis between 800 Hz to 1.2 kHz.


Done!
All in all, this has been one of those few tweaks that is not
a double-sided sword. Not only was I able to scrounge the foam for free, but I
got all improvement and no drawback. Different horns, as shown, will require
different levels of treatment, and different solutions to fabricate the foam.
That part I leave to you- it's not difficult though. The most clever amongst
you may have come up with the idea to try foam-loading the front baffles of your
box loudspeakers in addition to horns- GO FOR IT! Results will vary widely but
in many cases, there's improvement to be had. People have used felt on
loudspeaker baffles for decades; this is very similar in concept. Foam it up,
have fun, and remember- you may run into Wife Approval Factor issues -- foam may
look cool to you but doesn't pass muster in very many decorating schemes.