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JBL used to do a device called CMCD, which stood for cone
mid-range compression driver. It might be worth searching for the term as JBL
were pretty good at releasing tech documents.
Which cone based systems are you comparing with which
compression driver based systems, that leads you to conclude that compression
drivers are harsh at 2KHz? With a well designed system they shouldn’t be.
Getting a 10” horn loaded drive unit to have a smooth
unprocessed response above 1KHz is tricky. If the point of the exercise is a
reduced output at 2KHz they should fit the bill.
All loudspeaker drive units have an upper roll off point,
sometimes referred to as the mass break point (because the upper limit is
mainly due to the coil/cone mass). Above that frequency the power available
efficiency starts to drop off.
The on-axis sensitivity can remain flat above that point,
because the directivity increases, so the power is radiated into a smaller
volume. A 10” drive unit will have a directivity index of about 12dB at 1.5KHz.
That is, the sound level will be 12dB higher on axis than if the acoustic power
was radiated omni-directionally. If the on-axis SPL is still flat at that
frequency it is actually putting out less than 0.1 of the power compared to
lower frequencies.
If you manage to make a horn with constant directivity, you
will lose the extended response, which comes from increasing directivity, and
it will require additional eq to regain the flat response. This is why high
frequency boost is needed on compression drivers fitted to constant directivity
horns, because they have a falling power response.
With 1” compression drivers the hf roll off happens at
around 4KHz, with 2” compression drivers it is about 2.5KHz. There is a lot
more variation in cone design, but a 10” driver could start to roll off well
below 1KHz. There maybe outliers that perform differently, but chances are such
a device will have been designed for a specific purpose.
With a horn, there is also a volume of air between the
diaphragm and horn throat. This air has a compliance which at low frequencies
behaves like an incompressible fluid, so all the air displaced by the diaphragm
passes into the throat of the horn. At high frequencies the mechanical
reactance of this air space becomes sufficiently low (i.e., the air becomes
compressible) so that all the air displaced by the diaphragm does not pass into
the throat of the horn. As the compliance tends to zero the roll off tends to
6dB/octave (determined by mass alone). By careful choice of compliance, the
space can be caused to resonate with mmd (moving mass) which extends the
response upwards, but the roll off then tends to 12dB/octave.
A final nail in the coffin, is that at higher frequencies
the cone doesn’t move as a single, solid diaphragm. Parts of the cone can be
moving forwards at the same time as other parts are moving backwards. This does
not help maintain a smooth response.
However, to quote Beranek:
It has been remarked that if one selects his own components,
builds his own enclosure, and is convinced he has made a wise choice of design,
then his own loudspeaker sounds better to him than does anyone else's
loudspeaker. In this case, the frequency response of the loudspeaker seems to
play only a minor part in forming a person's opinion.
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