impedance for 99

Ron Nossaman nossaman@SOUTHWIND.NET
Sat, 2 Jan 1999 13:27:37 -0600 (CST)


At 11:07 PM 1/1/99 -0800, you wrote:
>I promised I would be good and not post unless I had something really
important to say.  That time has come....

Welcome back, I hadn't noticed that you'd been 'bad'.

>
>I must say that I find this discussion soundboard impedance to be
fascinating.  As an electrical engineer I'm comfortable with the idea of
soundboard impedance.  I even think it wouldn't be that hard to measure
mechanical impedance.  If voltage is analogous to force and current is
analogous to velocity (not of the wave but of the displacement from the
force) if should be possible to mount a linear motor (like the motor from a
speaker) to the soundboard and measure the displacement with a laser
interferometer.  The first time derivative of displacement is velocity.  One
could then calculate both the real and imaginary parts of the impedance by
"doing the math".  It's ohms law for soundboards!  That would be something
like:  Force/Velocity = Impedance  The tricky part would be getting the
timing of the force and the measurement of the displacement to be
synchronous.  I'd be shocked if one of those HP Fourier Analysis thingy's
the gearheads (mechanical engineers) are always using!
> for vibration analysis couldn't be used to make this measurement.  Doesn't
sound tough to me, but wadda I know, I'm just a sparky (electrical
engineer).  We leave the greasy stuff to the gearheads :)  Thoughts?

*Yes, never go into a mechanical engineer's bar alone. Other than that, it
not only sounds plausible, I imagine it has been done. We need to go the
other way though, and anticipate results from design, rather than measure
after the fact.


>On another, but related note, I keep hearing piano technicians try to draw
analogies between soundboards and speakers.  Most recently Ron did this when
he wrote:  
>
>"In use, a soundboard assembly is a driven diaphragm, sort of like a
speaker cone, that has to accommodate and respond to frequencies ranging
from roughly 27Hz-4200Hz. That's woofer, tweeter, and crossover, all in one
unit. Let's see the audio engineers do that in a high performance speaker!"
>I'm not trying to pick on Ron, I'm sure he know exactly what he's talking
about or he wouldn't have used the phrase "...sort of like...".  

*Not a problem, I'm not touchy when people make sense at me.  

In actual fact an audio transducer (speaker to the rest of us) is nothing
like a soundboard.  A speaker uses a linear motor to drive a cone shaped of
stiff paper, appropriately enough called a cone, in a pistonic fashion.  The
resulting sound is highly direction and frequency dependent.  

*It's directional because of the cone isn't it? A flat diaphragm wouldn't be
nearly as much so, no?

Higher frequencies are more directional.  Lower frequencies are less
directional. Two people sitting in the same room, one on axis and the other
off axis, can have completely different impressions of the sound quality
because they are in fact hearing different things.  

*More on this further down.


Additionally, any normal sized speaker behaves as a point source of sound.
That is, the sound amplitude falls of as the inverse-square of the distance.
If you're twice as far away the sound is one-fourth as loud.

*Just like magnetism and gravity, but I think sound propagation is also
affected by air pressure, temperature, and humidity. I know the speed of
sound is, but I think the amplitude is too. May be wrong here.


>A soundboard, on the other hand, is driven with a bending wave initiated by
the bridge.  The bending wave travels to the rim and is reflected back.
Different modal patterns appear on the soundboard at different frequencies. 
*True, but a soundboard is also being driven in a pistonic fashion at the
driven point, like a speaker cone. Also, a speaker cone is not absolutely
rigid, and totally without inertia. There should be a bending wave traveling
up the speaker cone too, somewhat like the soundboard, with different modal
patterns appearing on that cone at different frequencies. Isn't that what
the concentric rings molded into a speaker cone are for? I propose that the
higher the driving frequency, the deeper into the cone the modal point
forms. This would be a function of the mass and stiffness of the speaker
cone (mechanical impedance, the stiffness goes up, and the mass goes down as
you get deeper into the cone, stiffness being calibrated by those concentric
rings), and account for the tighter directionality of the higher frequencies
because they originate closer to the 'focal point' of the cone. That would
be the narrow part of the diaphragm, and the frequency response, if not the
sound directionality, of a soundboard would correspond very closely with
what happens in a speaker cone. My 'sort of' referred more to morphology,
driving method, and any peripheral effects resulting from same than in the
resultant mechanical phenomena. I actually think they relate pretty well. 


 Doug Richards could probably make some pretty cool Finite Element Analysis
animations of the soundboard in motion, given enough time and "free"
computer time.  Anyway, the sound from a soundboard is not nearly as
directional as from a speaker.  Likewise, the sound does not fall off as the
inverse-square of the distance because the piano soundboard is not a point
source.
>These are just two of the differences between a speaker and a piano
soundboard.  There are others mostly having to do with what happens to the
speaker cone at higher frequencies.

*What does happen to a speaker cone at higher frequencies? 


>Anyway, I don't think a speaker and a piano have much in common.
>There is a new speaker technology being pushed by a company called NXT that
uses a carbon-fiber panel much like a soundboard.  A transducer initiates a
bending wave on the carbon-fiber panel.  The exact point of excitation is
very important.  

*So it is in a soundboard, for any given frequency.


FEA is used to find the right point of excitation.  I've only heard small (4
x 6") models, but the sound is much better.  I think you will be seeing flat
stereo speakers in the near future, based on the same acoustics as the piano
soundboard.  This is the woofer, tweeter, and crossover all in one that Ron
was asking for!  You can see a set of these new speakers by going to
http://www.cc-inc.com/home.asp and searching for item number 38830.  A
company called Benwin is making a set of PC speakers using NXT technology.
They're $129.95 (USD).
>Jory
>

*Ain't technology grand? So how does a single excitation point accommodate a
full frequency range in this kind of speaker? The soundboard response is
complicated a tad by having (nominally) 88 excitation points scattered all
over the place. Since it's unlikely that we can place each string
termination at the optimum point on the soundboard for the best response at
that particular frequency and string load, FEA or not, we have to
accommodate a relatively fixed range of termination placements by modifying
the response characteristics of the assembly in any given area. Maybe 'sort
of' like tinkering with the stiffness, weight, ribbing (beading, banding, or
whatever the concentric stiffeners/springs are called), and angle of a
speaker cone. Sorry, couldn't resist.

 Ron 



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