Franz J. Vesely > Lectures > LJ Sticks 

 
 
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  EXISTING MODELS


  • The need for "generic" models



     
    • 5CB, a popular liquid crystal molecule

    • It may be modeled by 19+ LC centers, different in size and depth, and positioned as shown

    • Used for realistic simulations, to be compared to experiment

    • Less suited for theory

    • PMMA (= vinyl glass): more linear, but even more centers





  • Multisite model
     
     
    • Several (4...8) identical LJ sites in regular distances

    • Pro:
      • captures some of the physics - see balls-and-sticks models

    • Con:
      • many interactions per pair
      • not convex everywhere
      • hard body limit (= fused hard spheres) afflicted by metastability

    • But useful for gauging the Gay-Berne potential (see below)




  • Kihara model
     
     
    • Find the points of least mutual distance along the two axes, then place an LJ center in each of these "proxy points"

    • Pro:
      • very quick (only one LJ interaction)
      • hard body limit is the well-studied spherocylinder (HSC)
      • exhibits pronounced LC behaviour (nematic+smectic)

    • Con:
      • physics is wrong: side-by-side interaction is no stronger than end-to-end (compare 4LJ: factor $\approx 5$)




  • Gay-Berne model
     
     
    • Great math, due to Berne-Pechukas; see here

    • But: fuzzy physics; see here

    • Gay-Berne: adapted Berne-Pechukas and defined standard parameters by comparing to 4-Lennard-Jones model (see above); later modified by Luckhurst. See full GB formula

    • The Gay-Berne potential has four adjustable parameters

    • Pro:
      • may be adjusted to represent anything from saucers to cigars
    • Con:
      • parameters must be gauged anew for any shape; not suited as reference potential
      • Hard body limit: "Hard Gaussian Overlap" (HGO) model; has no definite shape; no pronounced LC phases




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vesely nov-2006