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<DIV> <FONT size=3> Ok, now this is an interesting discussion.
Admittedly not being a math guy I'm still interested in putting some numbers=
on
some scales of things I've seen as a bench marks for comparison.</FONT></DIV=
>
<DIV><FONT size=3> Let's just take one case I have first=
hand
knowledge of. I rebuilt & 1960 Stwy L 3 years ago that lived in a
Fresno area church from the beginning of it's creation to the present so it =
has
survived wonderfully well.</FONT></DIV>
<DIV><FONT size=3> I was keenly impressed by the balance =
of
sound, both in power & sustain. I measured the bearing with =
a
lowell gauge & though I don't have numbers any more to give you my recal=
l is
that the top capo had over 2 degrees of deflection & the 2nd capo
about 2 or more & the middle was 1 1/2 degrees
tapering down to 1/2 in the bottom & the bass had positive bu=
t
minimum bearing as it should be with a cantalever. The crown string
stretched across the boards underside revealed lots of residual crown in the=
strung condition & more than any other C.C. board I've ever seen up
to that time. All that to say it was in my opinion a text book
Steinway/belly set up both in terms of crown & bearing.  =
;
These are IMO the kinds of observations that are important to make
when we find something that is working really well. </FONT></DIV>
<DIV><FONT size=3> The Stwy L scale as I recall has an average trebl=
e
tension at 160 lbs per string. It is obvious to see that the majority of the=
bearing pressure on the long bridge is increasing gradually the higher=
up
the scale we go. </FONT></DIV>
<DIV><FONT size=3> So knowing all of the above, what is the equation=
that
will calculate an approximate string bearing load under the conditions I
describe?</FONT></DIV>
<DIV><FONT size=3> If it's the one- 40th rule for simplicity then&nb=
sp;
40 divided into 160 strings equals 4 pounds per string. Let=
's
remove most of the bass strings from this equation for now, since theoretica=
lly
there isn't much bearing there & we have approx. 160 strings times 4 pou=
nds
equals 720 lbs. add in say 80 lbs for the bass & it's about 800 tot=
al
pounds give or take</FONT></DIV>
<DIV><FONT size=3> There is a much more accurate &=
amp;
glamorous formula for this but I dont' have it at my finger tips. If t=
he
scale tension averages 180 lbs per string then we're talking 4 1/2 pounds pe=
r
string which bumps total bearing load up another 100 ish
pounds.</FONT></DIV>
<DIV><FONT size=3> My point in all this is that if we are using stro=
nger
engineering materials & principles which building better stronger rib
structure, which we are<STRONG>, <U><EM>then</EM></U></STRONG><U><EM> surely=
our
rib crowned & supported boards will survive as well & IMO longer tha=
n
this example of a C.C Steinway L I cited above </EM></U></FONT></DIV>
<DIV><FONT size=3> Don't you think?</FONT></DIV>
<DIV><FONT size=3> Dale Erwin</FONT></DIV>
<DIV><FONT size=3></FONT> </DIV>
<BLOCKQUOTE
style="PADDING-LEFT: 5px; MARGIN-LEFT: 5px; BORDER-LEFT: blue 2px solid"><=
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<DIV dir=ltr><SPAN class=953463523-18022006><FONT face="Comic Sans M=
S"
color=#000080 size=3>Consider a basic scale of moderately high tension=
. Say
40,000 lbs. overall. With this string tension 1,000 lbs of string down for=
ce
equals 2.5% of scale tension. That is quite a lot considering that most
companies are claiming string down force more on the order of 0.5% to 1.5%=
of
string tension (which would be 200 to 600 lbs). I thought I was setting my=
initial string down force pretty high at around 1.0 to 1.5%. I don't like
thinking about what I'd be doing to a board loading it up to 2.5%. I can't=
imagine it being happy enough at that level to want to stay
there.</FONT></SPAN></DIV>
<DIV dir=ltr><SPAN class=953463523-18022006><FONT face="Comic Sans M=
S"
color=#000080 size=3></FONT></SPAN> </DIV>
<DIV dir=ltr><SPAN class=953463523-18022006><FONT face="Comic Sans M=
S"
color=#000080 size=3>Del</FONT></SPAN></DIV></FONT></BLOCKQUOTE></DIV>
<DIV></DIV>
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