1991
DOI: 10.1103/physreva.44.5306
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Effective-liquid approach to the generalized Onsager theories of the isotropic-nematic transition of hard convex bodies

Abstract: Recent attempts to generalize the classical Onsager theory of nematic ordering to finite-density systems of finite-length hard convex bodies are related and compared. It is pointed out that, although good results can be obtained in three-dimensions (3D), in two dimensions (2D) the underlying factorization approximation of the radial and angular variables always implies a second-order isotropic-nematic transition instead of the crossover from a weakly first-order transition to a continuous (Kosterlitz-Thouless)… Show more

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Cited by 15 publications
(11 citation statements)
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“…Ward and Lado [26] found based on the Percus-Yevick (PY) integral equation theory that the I-N transition does not take place in a fluid of hard ellipses although orientational ordering is allowed. While, the density-functional theory (DFT) [27] and the effective-liquid approach [28] indicate that the I-N transition is continuous for hard ellipses with arbitrary aspect ratios. The other forms of DFT [29,30], the Onsager theory-based approach [31], and the scaled particle theory (SPT) [32] predict the existence of the I-N transition in hard ellipses, but its location differs from these theoretical predictions.…”
Section: Introductionmentioning
confidence: 99%
“…Ward and Lado [26] found based on the Percus-Yevick (PY) integral equation theory that the I-N transition does not take place in a fluid of hard ellipses although orientational ordering is allowed. While, the density-functional theory (DFT) [27] and the effective-liquid approach [28] indicate that the I-N transition is continuous for hard ellipses with arbitrary aspect ratios. The other forms of DFT [29,30], the Onsager theory-based approach [31], and the scaled particle theory (SPT) [32] predict the existence of the I-N transition in hard ellipses, but its location differs from these theoretical predictions.…”
Section: Introductionmentioning
confidence: 99%
“…We mention here that for the isotropic (p(x) = p) and nematic (p(x) = ph(u)) phases, (7) reduces to the same expression as that obtained from the factorized dcf in [18] (cf. [26]). This can partly explain why the latter leads to succussful results for the I-N transition of hard ellipsoids.…”
Section: The Direct Correlation Functionmentioning
confidence: 93%
“…This is due here to the perfect alignment of the HSCs, causing their excluded volume to be exactly 8v, just as for HS systems. This degeneracy disappears when the HSCs are free to rotate [26]. It could be interesting to replace the r.h.s, of (9) by the more general HS expression:…”
Section: The Nematic Phase Of Phscmentioning
confidence: 97%
“…The phase behavior has been explored extensively by various theoretical approaches and simulations in both two-dimensional hard ellipses [14][15][16][17][18][19][20][21][22] and three-dimensional hard ellipsoids.…”
Section: -13mentioning
confidence: 99%