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--></style><title>Re: stretching wire -- an anecdotal
analysis</title></head><body>
<div>At 21:20 -0500 19/4/08, kurt baxter wrote:</div>
<div><br></div>
<blockquote type="cite" cite>
<blockquote>If you take patented steel wire beyond its elastic<br>
limit, it will neck and break, perhaps right now, perhaps
tomorrow</blockquote>
<blockquote> but very soon.<br>
</blockquote>
</blockquote>
<blockquote type="cite" cite>The point when when you go from
"elastic" to "plastic" is when the wire<br>
permanently changes shape, never to return, right?</blockquote>
<div><br></div>
<div>Yes, and with patented wire this point is very close to the
breaking point</div>
<div><br></div>
<blockquote type="cite" cite>So I would say that when a string bends
around the tuning pin, and<br>
for sure when it dives into the becket, it changes it's shape for
good.<br>
<br>
If you slightly "kink" a wire, you have taken it to it's
plastic point... right?</blockquote>
<div><br></div>
<div>Yes and no. When you make the becket on the wire the part
near the outside corner is weakened but the core and inside corner
are, if anything strengthened by compression.</div>
<div><br></div>
<blockquote type="cite" cite>So if a "kink" type load can
take the string beyond it's elastic point<u> without breaking</u>, why
not "stretching" type load?</blockquote>
<div><br></div>
<div>Also when the wire is initially coiled or when I straighten it
for stringing or making bass strings it takes a permanent set.
Exactly what stresses are involved I can't say, but experience
suggests they are not detrimental.</div>
<div><br></div>
<div>When I (or others) make bass strings I flatten the wire with a
hammer and die to hold the copper at the ends. If a string is
stretched to breaking point it will never break at the flattening but
either at the eye or at the becket or some point of friction UNLESS
there is a sharp angle at the ends of the flattened portion.
When I had my first flatteners made 25 years ago, which I still use
today, we got a chamfered end on the flattening that created too
sudden a change from the flattening to the cylindrical wire and this
caused a severe weakening. Once we had ground off and radiused
the top corner to the die, there was no problem.</div>
<div><br></div>
<div>These things do cause work-hardening and it's quite likely that
the flattening process actually increases the tensile strength of the
wire, but when we simply stretch the wire I think there is no
work-hardening</div>
<div><br></div>
<blockquote type="cite" cite>Isn't there a big difference between
"elastic limit" and ultimate limit?</blockquote>
<div><br></div>
<div>As I've mentioned before, some people use the manufacturer's UTS
as the datum and take care not to strain the wire beyond 55% of this
and others, like me and Paulello use another figure and and take care
not to strain the wire beyond 70% of this. This allows a safety
margin needed to take into account friction points, weakening through
work (say at the eye) etc. From what I have read, the elastic
limit of patented wire is almost coterminous with the breaking strain
and there is no separate "yield point" below the breaking
strain as there is with some other materials. In other words
once plastic deformation begins the string is going to break, whereas
with some other materials the wire would stretch (irreversibly)
without breaking over a range of tensions between the yield point and
the breaking strain. We are not concerned with such
materials.</div>
<div><br></div>
<div>The figures I use are as below, with the tension in pounds.
70% of this figure is what I do not exceed in designing bass strings
-- so 283 lbs would be the maximum tension I'd have for a covered
string with a No. 21 core.</div>
<div><br></div>
<div>12 0.725
174<br>
12.5 0.750 185<br>
13 0.775
196<br>
13.5 0.800 207<br>
14 0.825
218<br>
14.5 0.850 229<br>
15 0.875
240<br>
15.5 0.900 251<br>
16 0.925
264<br>
16.5 0.950 276<br>
17 0.975
288<br>
17.5 1.000 300<br>
18 1.025
314<br>
18.5 1.050 326<br>
19 1.075
339<br>
19.5 1.100 339<br>
20 1.125
371<br>
20.5 1.150 387<br>
21 1.175
405<br>
21.5 1.200 421<br>
22 1.225
439<br>
22.5 1.250 455<br>
23 1.300
479<br>
23.5 1.350 504<br>
24 1.400
532<br>
24.5 1.450 570<br>
25 1.500
609<br>
25.5 1.550 660<br>
26 1.600
726</div>
<div><br></div>
<div>JD</div>
<x-sigsep><pre>--
</pre></x-sigsep>
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