Hi Stephen
Thanks for the first direct reply to this point. Tho there a couple of
points I am unclear on and I wonder if you could clarify. It almost
seems like you are saying that Youngs Modulus for pianostrings is
essentially indeterminable (for all practical matters) and that Youngs
Inharmonicity coefficient is in error to begin with.
To the later, If you look at the paragraphs surrounding equations 8 and
9, Young clearly states that there is a direct relationship between Q
and D. And in your example of Brass, Q (Youngs Modulus) should indeed
be lower (then steel) as a result of its higher density.
Young goes on in the later part of the paper to take an example from one
manufacturer who gives a spec for Youngs modulus that fits nicely that
same manufacturers spec for density if one employs the relationship
Young describes in/around equation 9 in his paper.
So... what is wrong with Youngs paper then...? Why is the relationship
Q/p = 25..5*10^10th that he gives not valid ?
Thank you kindly
RicB
>According to Youngs paper of 1952 the Modulus divided by the
>density of the string results in a consant (25.5*10^10th). It
>appears to me that this constant is supposed to be the same
>regardless of material, which would mean that E is the product of D
>* this constant.
Ric,
Young's modulus is not an easy parameter to determine experimentally.
Using bulk tensile testing, even with fancy equipment, you can't get
a very accurate value, partly because real materials never behave
completely linearly (even steel wire). There are additional
complications that make tensile testing of wire a very difficult
experimental procedure, adding to the inaccuracies in determining the
modulus for a wire specimen.
It is primarily a material dependent property, but can be affected to
some extent by mechanical working (and heat treatments).
Consequently, a small range of moduli will be relevant for a given
material according to how it has been physcially processed. Accurate
measurement of Young's modulus can be done by sonic and similar
techniques which measure the vibrations of the metallurgical
structure at the atomic level. All are involved and generally
expensive. There is no general correlation between density and
modulus. Compare brass, denser but the modulus is considerably lower
than that of steel.
>In any case it seems to me that there is some significant amount
>of confusion surrounding Young Modulus and it perhaps is more
>important in a practical scaleing sense then we assume.
It has little practical use for scaling since it is not a
controllable factor in wire manufacture. It is essentially determined
by the choice of material.
>This fits well with your call to empirical testing for breaking
strength / %'s
The only way to determine the capabilities of your wire is with
tensile testing.
Stephen
--
Stephen Birkett
http://real.uwaterloo.ca/~sbirkett
This PTG archive page provided courtesy of Moy Piano Service, LLC