an analysis of downbearing, etc.

gordon stelter lclgcnp@yahoo.com
Mon, 2 Feb 2004 06:12:46 -0800 (PST)


Thank you very much Mark for this level-headed,
dispassionate discourse. This is how I have always
undersood things to be.
     Thump

--- Mark Kinsler <kinsler33@hotmail.com> wrote:
> I don't know if postings from a non- (or not-yet)
> technician are permitted 
> here, but I believe I can contribute a bit of
> engineering insight here that 
> could clear things up.
> 
> Mechanical impedance is the result of the
> springiness and inertia of a 
> mechanical part.  Your sounding board has some
> inertia due to its mass.  It 
> also has some springiness.  Wood (and most other
> materials in a piano) will 
> push back in direct proportion to the amount of
> deflection applied to them. 
> (Exceptions: felt and buckskin, by design.)
> 
> The sounding board's springiness derives from the
> behavior of wood in 
> compression and bending.  From an engineering
> standpoint, a crowned sounding 
> board that's glued at its rim to a rigid piano frame
> is an arch.  When you 
> push down on the crown of an arch, the ends of the
> arch try to spread.  
> (This force is due to the downbearing of the strings
> on the bridge.)  Since 
> the arch 'ends' (in this case, the glued rim of the
> sounding board) cannot 
> move, the material of the arch is compressed.  Wood
> in compression behaves 
> like a spring.
> 
> The situation is really a bit more complex than this
> because of the 
> stiffening ribs.  These experience bending stress,
> but also behave like a 
> spring.  It doesn't matter very much from a purely
> physical point of view, 
> but since the wood in a crowned sounding board is
> under compression, we get 
> a somewhat stronger structure since wood is a bit
> stronger in compression 
> than in tension, especially across the grain.
> 
> I don't think I've told anyone here anything new
> thus far.  But there's a 
> bit more.
> 
> If the impedance of two coupled mechanical
> parts--say the string and the 
> sounding board--are different, any energy applied
> from part #1 will not be 
> completely transferred to part #2.  What happens to
> the energy that's not 
> transferred?  It isn't lost: it is _reflected_ back
> into part #1.
> 
> In a piano, the impedance of the string is different
> from that of the 
> sounding board.  Thus part of the energy imparted by
> the hammer to the 
> string is reflected back into the string.  We want
> this to happen: it's what 
> makes the string keep vibrating.  If all of the
> energy from the string went 
> into the sounding board, we'd hear only a dull thump
> instead of that 
> splendid ringing sound.
> 
> The piano is a highly efficient system.
> (System=chain of parts.) The energy 
> that's reflected back into the spring is not lost,
> but stored in the 
> vibrating string.  It is transferred to the sounding
> board gradually, on 
> each vibration.
> 
> Could the sounding board have a negative crown (like
> a dish), and the 
> downbearing be "upbearing?" From a physical
> standpoint, yes.  There would be 
> no difference in the behavior of the system, though
> the bridge would peel 
> off the sounding board pretty quickly and the design
> of the bridge pins 
> would be interesting.
> 
> Or, in another possible configuration, could the
> sounding board have a 
> negative crown and the downbearing still exert force
> downward?  Again yes.  
> (The bridge would have to be rather high.)  The
> sounding board's wood would 
> be in tension and the rim of the sounding board
> would tend to be pulled away 
> from the frame, but again from a purely physical
> standpoint the system would 
> work about like a normal piano.  Structurally, of
> course, this configuration 
> would be a disaster, but the sounding board and
> strings would behave pretty 
> much normally if the whole works didn't peel apart.
> 
> The relationship of the sounding board to the
> outside air is a bit more 
> complex than the relationship of string to sounding
> board.  Ideally, we want 
> the impedance of the sounding board to match that of
> the outside air.  This 
> makes the piano loud enough to hear.  And the
> sounding board does just that: 
> it's an 'impedance matching' device that tries to
> match the impedance of the 
> strings to that of the air.  (Side note: the bell of
> a brass instrument is 
> also an impedance matching device.)
> 
> >From an efficiency standpoint, we do not want
> energy from the air to be 
> reflected back into the sounding board.  From an
> artist/craftsman 
> standpoint, we _do_ want this to happen, because
> that's part of what gives 
> the piano its tone.
> 
> It's also worth examining the resonant frequency of
> the strings vs. that of 
> the sounding board.  The resonant frequency of each
> string is obvious to 
> anyone.  The resonant frequency of the mounted
> sounding board is known to 
> the technician, who can determine it when the piano
> is unstrung: only one 
> note sung into the unstrung piano will resonate
> loudly, and that's the 
> resonant frequency of the sounding board.  (This is
> the simplest case: a 
> real sounding board will resonate at several
> different frequencies.  The 
> resonant frequency of the sounding board will also
> change somewhat under the 
> force and mass of the strings.)
> 
> We really don't want the resonant frequency of the
> sounding board to be a 
> large factor in the behavior of a piano.  Ideally,
> the sounding board should 
> be forced to vibrate at the frequency of the struck
> strings.  In practice, 
> however, this is not the case.  I don't know if the
> terms are equivalent 
> from one sort of instrument to another, but in the
> bowed string instruments, 
> we get what's called a 'wolf' tone when the string's
> resonant frequency 
> approaches that of the sounding board.  On the
> 'cello, this occurs at the F 
> played on the C string.  I have read about 'wolf'
> scales on the piano, and 
> perhaps this is the same phenomenon.
> 
> So as it happens, the resonant frequency of the
> piano sounding board is a 
> factor in its behavior, but it's not necessarily a
> bad thing: it contributes 
> to the overall tone of the instrument, as do all the
> other 'imperfections.'
> 
> I have read the other posts in this thread, and it's
> clear that everyone has 
> a good understanding of these concepts.  However,
> descriptions, terms, and 
> experiences vary, thus making the various
> contributions appear inconsistent. 
>   What I've given here are the terms used in
> engineering and physics.  I 
> gladly defer to the experience of the craftsmen who
> read this list.  A far 
> better treatment of the matter is given in an old
> Scientific American 
> article called 'The Physics of the Piano.'  I
> believe that the complete 
> reference is given in Art Reblitz' textbook.
> 
> Mark Kinsler
> 512 E Mulberry St. Lancaster, Ohio USA 43130
> 740-687-6368
> http://home.earthlink.net/~mkinsler1
> 
>
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