Order parameters: Difference between revisions

From SklogWiki
Jump to navigation Jump to search
mNo edit summary
m (Added short intro.)
Line 1: Line 1:
==Liquid crystals==
An '''order parameter''' is some observable physical quantity that is able to distinguish between
two distinct phases. The choice of order parameter is not  necessarily unique.
==Solid-liquid transition==
Possible choices:
*Fourier transform of the density
*Shear modulus
==Isotropic-nematic transition==
The '''uniaxial order parameter''' is zero for an isotropic fluid and one for
The '''uniaxial order parameter''' is zero for an isotropic fluid and one for
a perfectly aligned system.
a perfectly aligned system.

Revision as of 10:50, 27 February 2008

An order parameter is some observable physical quantity that is able to distinguish between two distinct phases. The choice of order parameter is not necessarily unique.

Solid-liquid transition

Possible choices:

  • Fourier transform of the density
  • Shear modulus

Isotropic-nematic transition

The uniaxial order parameter is zero for an isotropic fluid and one for a perfectly aligned system. First one calculates a director vector (see Ref. 2)

Qαβ=1N∑j=1N(32e^jαe^jβ−12δαβ),α,β=x,y,z,

where Q is a second rank tensor, e^j is a unit vector along the molecular long axis, and δαβ is the Kronecker delta. Diagonalisation of this tensor gives three eigenvalues λ+, λ0 and λ−, and n is the eigenvector associated with the largest eigenvalue (λ+). From this director vector the nematic order parameter is calculated from (Ref. 5)

S2=d⟨cos2θ⟩−1d−1

where d is the dimensionality of the system.

i.e. in three dimensions (see Ref. 3)

S2=λ+=⟨P2(n⋅e)⟩=⟨P2(cosθ)⟩=⟨32cos2θ−12⟩

where S2 is known as the uniaxial order parameter. Here P2 is the second order Legendre polynomial, θ is the angle between a molecular axes and the director n, and the angle brackets indicate an ensemble average.

See also

References

  1. Joseph P. Straley "Ordered phases of a liquid of biaxial particles", Physical Review A 10 pp. 1881 - 1887 (1974)
  2. R. Eppenga and D. Frenkel "Monte Carlo study of the isotropic and nematic phases of infinitely thin hard platelets", Molecular Physics 52 pp. 1303-1334 (1984)
  3. Mark R. Wilson "Determination of order parameters in realistic atom-based models of liquid crystal systems", Journal of Molecular Liquids 68 pp. 23-31 (1996)
  4. Denis Merlet, James W. Emsley, Philippe Lesot and Jacques Courtieu "The relationship between molecular symmetry and second-rank orientational order parameters for molecules in chiral liquid crystalline solvents", Journal of Chemical Physics 111 pp. 6890-6896 (1999)
  5. Anna A. Mercurieva, Tatyana M. Birshtein "Liquid-crystalline ordering in two-dimensional systems with discrete symmetry", Die Makromolekulare Chemie, Theory and Simulations 1 pp. 205 - 214 (1992)