To follow up on helloworld922's response, here is some quantitative analysis of the NIST Table 2 data, both from 100-800 K and from 200-500K (=-73.15K to +226.85 K, a range that is closer to the working range of motor windings) using PyLab:
# copper conductivity fit from NIST:
# Journal of Physical and Chemical Reference Data
# Electrical Resistivity of Copper, Gold, Palladium, and Silver
# R. A. Matula
# JPCRD 8(4) pp. 1147-1298 (1979)
# http://www.nist.gov/data/PDFfiles/jpcrd155.pdf
# numerical data from table 2
import numpy as np
import matplotlib.pyplot as plt
T0 = np.array([ 100, 125, 150, 175, 200, 225, 250, 273.15, 293, 300, 350, 400, 500, 600, 700, 800])
r0 = np.array([ 0.348, 0.522, 0.699, 0.874, 1.046, 1.217, 1.387, 1.543, 1.678, 1.725, 2.063, 2.402, 3.090, 3.792, 4.514, 5.262])
T = (T0, T0[4:-3])
r = (r0, r0[4:-3])
f = [np.polynomial.chebyshev.Chebyshev.fit(T[0],r[0],4), np.polynomial.chebyshev.Chebyshev.fit(T[1],r[1],4)]
for i in range(0,2):
plt.figure(i+1)
plt.plot(T[i],r[i]-f[i](T[i]))
plt.plot(T[i],r[i]-f[i].truncate(2)(T[i]))
What this does is to approximate the resistivity vs. temperature data with 4th-degree polynomials, and plot graphs of errors in the polynomial approximation vs. temperature, for the 4th-degree polynomial and for a linear polynomial.
The Chebyshev coefficients* for a polynomial fit are:
100-800K: 2.77689151e+00, 2.44286730e+00, 3.00859915e-02, 1.44364826e-02, -2.64166679e-03
200-500K: 2.06557521e+00, 1.02015113e+00, 2.57505898e-03, 1.80482498e-03, -1.11397377e-04
Over 100K - 800K:
Here I would definitely say that a linear approximation is close but not sufficient for precision applications. The error in a linear approximation is close to 1% of the resistivity value (slightly higher for <200K). I would use a quadratic or cubic approximation. (the 4th degree coefficient is small enough that it's not worth the extra complexity)
Over 200K - 500K:
Here the linear approximation does much better due to the reduced range; maximum error of a linear approximation is about 0.15% of the resistivity value. I'd probably live with a linear approximation.
*Chebyshev coefficients: Chebyshev approximation is a technique for approximating functions with polynomials + quantitatively evaluating the accuracy of those approximations. The subject is too detailed to discuss it much here. If you have a copy of Numerical Recipes go read about Chebyshev approximation. I also just wrote a blog post about Chebyshev approximation which might help explain.
edit: The JPCRD Matula reference refers to ultrapure copper exceeding IACS levels. "Standard" commercial copper is slightly lower conductivity than ultrapure (about 2.5% lower) and has a lower tempco of 0.00393. See NBS Handbook 100