@article{attwood_hall_2008, title={Solid-liquid phase behavior of ternary mixtures}, volume={54}, ISSN={["0001-1541"]}, DOI={10.1002/aic.11513}, abstractNote={Abstract}, number={7}, journal={AICHE JOURNAL}, author={Attwood, Brian C. and Hall, Carol K.}, year={2008}, month={Jul}, pages={1886–1894} }
 @article{attwood_hall_2004, title={Effect of the solid phase on the global phase behavior of Lennard-Jones mixtures}, volume={50}, ISSN={["1547-5905"]}, DOI={10.1002/aic.10157}, abstractNote={Abstract}, number={8}, journal={AICHE JOURNAL}, author={Attwood, BC and Hall, CK}, year={2004}, month={Aug}, pages={1948–1960} }
 @article{attwood_hall_2003, title={Global phase diagram for monomer/dimer mixtures}, volume={204}, ISSN={["0378-3812"]}, DOI={10.1016/S0378-3812(02)00251-0}, abstractNote={The basic features of the global phase diagram associated with the generalized Flory dimer (GFD) equation of state for mixtures of square-well monomers and dimers are calculated. We first extend the GFD theory to square-well monomer/chain mixtures. Theoretical predictions for the compressibility factor as a function of volume fraction are in good agreement with discontinuous molecular dynamics simulation results for monomer/dimer and monomers/8-mer mixtures. The GFD-predicted global phase diagram for square-well monomer/dimer mixtures is estimated using a brute force method. The locus of critical points in the P–T plane is calculated over a grid of points in the Λ–ζ plane, where ζ is a measure of the difference between the monomer and dimer well depths and Λ is a measure of the strength of the attraction between monomers and dimers. The major topographical features of our global phase diagram are similar to those predicted for other equations of state.}, number={1}, journal={FLUID PHASE EQUILIBRIA}, author={Attwood, BC and Hall, CK}, year={2003}, month={Jan}, pages={85–106} }