格子上的硬杆

A. Baumgärtner
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引用次数: 9

摘要

精确计算和枚举了在L×L方格上以封闭堆积密度分布的硬刚性棒系统,其中每根棒在L/N bbbb2中占据N≤11/36,并且随着系统L/N的增大而不断减小。我们的系统的每根棒的熵表现为S N α N−1 ×ln N为N→∞。还简要地考虑了立方晶格上的硬杆。本文讨论了本研究结果对液晶、聚合物液晶和当前聚合物熔融理论的一些影响,并给出了计算结果和计算结果,计算结果与计算结果一致,计算结果与计算结果一致,计算结果与计算结果一致。压杆占用N≤11/36,压杆占用N≤11/36,压杆占用N≤11/36,压杆占用2,压杆占用N≤11/36,压杆占用N≤11/36,压杆占用N≤11/36,压杆占用N≤11/36,压杆占用N≤11/36。L'entropie par barre de nos系统是comte comcoms N -N−1 Log N (N→∞)。Les barres rigides sur des reseaux cubiques是一种典型的立方体。在考虑聚合效应的基础上,我们得到了聚合体的聚合体,聚合体的聚合体,聚合体的聚合体的聚合体
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Hard rods on lattices
Exact calculations and enumerations of systems of hard rigid rods distributed at closed packed density on L×L square lattices, where each rod occupies N ≤11/36 for L/N>2 and decreases continuously with increasing size of the system L/N for all N. The entropy per rod of our systems behaves as S N α N −1 ×ln N as N→∞. Hard rods on cubic lattices are also briefly considered. Some implications of our results are discussed with respect to liquid crystals, polymeric liquid crystals and current theories of polymer melting On presente des calculs exacts et des resultats d'enumeration pour des barres rigides distribuees a densite maximale sur des reseaux carres L×L. Chaque barre occupe N ≤11/36 pour L/N>2 et decroit continuement pour tout N lorsque le rapport L/N augmente. L'entropie par barre de nos systemes se comporte comme S N -N −1 Log N lorsque N→∞. Les barres rigides sur des reseaux cubiques sont aussi discutees. On considere quelques consequences de ces resultats sur la physique des cristaux liquides, des cristaux liquides polymeriques et sur les theories actuelles de la fusion des polymeres
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