The second virial coefficient, B2, has been calculated for square-well
chain molecules of lengths n = 2-50 and well widths of lambda = 0.25-
1.0 by Monte Carlo integration. The theta temperature, at which B2 = 0
, is independent of chain length around lambda = 0.5, increases with c
hain length for lambda > 0.5, and decreases with chain length for lamb
da < 0.5. A scaling relation, T(theta)(n)-T(theta)*(infinity) is-prop
ortional-to n(-phi), accurately describes the departure of the theta t
emperature from the infinite chain length value for lambda greater-tha
n-or-equal-to 0.6. A closed-form expression for the second virial coef
ficient of square-well chains is presented which accurately fits the M
onte Carlo data for n = 2-50 and lambda = 0.25-0.75. When compared to
the Monte Carlo results, the second virial coefficient predicted by th
e generalized Flory-dimer theory for square-well chains is found to be
increasingly inaccurate as chain length increases. If we correct the
generalized Flory-dimer equation of state by forcing it to have the co
rrect second virial coefficient, the compressibility factor is accurat
ely predicted at densities below eta = 0.04.