Article View: sci.physics.fusion
Article #1008silver (and other) wires
From: mitchell swartz
Date: Sat, 12 Dec 1992 20:55
Date: Sat, 12 Dec 1992 20:55
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5732 bytes
There has been, and continues to be, much talk on this forum
regarding nichrome and silver conductivity.
Some of the calculations (actually or rhetorically) requested
have been trivial, but the 'debate' continues, and so this table
and elementary exercise are provided.
For example [sci.physics.fusion:4480; Jed Rothwell; Subject:
Silver the same everywhere in the world; Date: Wed, 9 Dec 1992] states:
= "the heater is: Ni-Cr two-ply wire (0.1 mm diameter, 40 mm length).
= Just find out whether it is possible for any silver wire to generate
= as much heat as it does."
or [sci.physics.fusion:4515; Subject: What Jones said; 11 Dec 1992]:
= "Technical type people know damn well that the only way 6 cm of one wire
= can dissipate as much heat as 4 cm of another wire is if both
= have approximately the same resistance. They also know that it would take
= an impossibly thin silver wire to be as resistant as a 0.5 nichrome wire".
Now that Prof. Droege has vaulted this forum into discussions of
electrodynamics, an elementary reminder of practical electrostatics
is in order. Impossibly thin? How thin --->
The electrical resistance (lumped parameter) characterizing a
rod-like material is a function of the electrical resistivity,
the physical length, and cross-sectional area (presumed circular,
with total homogeneity of material properties therein) as in
rho * L = Resistance [ohms]
--------
A
So the resistivity [rho: ohms-cm] {micro-ohms-cm in the table below
which has the various materials listed by nichrome type
(including the constitutional elements composing the various types),
a common variety, and of course silver. Temperature coefficients
of the electrical resistance, and the effective temperature of that
Taylor series simplification are also listed.
The nickel-chromiums were discovered in 1905 by Marsh, from which
the electrical heating industry became generated. A high resistance
to oxidation, diverse patents based upon slight additions to the mix,
and a need for such materials have generated diverse alloys.
Notwithstanding the above, the electrical conductivity of a few
can be compared to silver.
ELECTRICAL CONDUCTIVITY OF A FEW MATERIALS
[based in part upon Chemical Rubber Tables, and Engineering Materials
Handbook (Mantell) and Rare Metals Handbook (Hampel) ]
---------------------------------------------------------------------
|MATERIAL| | microhm-cm | Temp coef | Temp Range |
---------------------------------------------------------------------
Ni | Cr | Fe | | |
---------------------------------------------------------------------
100 | 0 | 0 | 7.8 | | 20C |
---------------------------------------------------------------------
0 | 100 | 0 | 13 | | 20C |
---------------------------------------------------------------------
0 | 0 | 100 | 10 | | 20C |
---------------------------------------------------------------------
80 | 20 | 0 | 108 | 0.00011 | 20-500C |
---------------------------------------------------------------------
60 | 16 | 24 | 112 | 0.00015 | 20-500C |
---------------------------------------------------------------------
35 | 20 | 45 | 100 | 0.00036 | 20-500C |
---------------------------------------------------------------------
Inconel X (annealed) | 122 | [m.p.1399C] | |
---------------------------------------------------------------------
Silver| | | 1.59 | [m.p. 960C] | 20C |
--------------------------------------------------------------------
In short, in can be seen that the relative electrical resistivity
for nichrome to silver (in this simple matter) is:
rho (Nichrome)
------------- = 69.5 (average)
rho (silver)
with a range of 62.89 to 76.73
for this exercise. Therefore, one can use 70 as an general ratio.
How thin must a silver wire be, to equal the nichrome wire?
Hence a silver wire must be a little less than 1/8th the diameter
of a nichrome wire to yield a relative area of 1/70th, so as to insure
an equivalent lumped parameter resistance, for an equal length of wire.
Other length-area-resistivity problems are similarly calculated.
Disclaimer: Of course, this ignores contact potentials, inhomogeneities,
method of contacting said wire, surface vs. volume conductions, and
the impact of electric and magnetic fields, &tc.
As for melting, the melting temperatures of the respective materials
are listed in the Table above. The next interested respondent
is welcome to estimate the thermal barriers surrounding this gendanken
wire, given any putative applied (thermally dissipative) electrical load.
===================================================================
Mitchell R. Swartz JET Technology
mica@world.std.com (617) 239-8383
Technical Details
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Newsgroups: sci.physics.fusion Path: arc1-ca.pugleaf.net!sparky!uunet!wupost!gumby!yale!yale.edu!ira.uka.de!sol.ctr.columbia.edu!eff!world!mica From: mica@world.std.com (mitchell swartz) Subject: silver (and other) wires Message-ID: <Bz5zG6.3pI@world.std.com> Organization: The World Public Access UNIX, Brookline, MA Date: Sat, 12 Dec 1992 20:55:17 GMT Lines: 112