Order parameters: Difference between revisions

From SklogWiki
Jump to navigation Jump to search
No edit summary
No edit summary
Line 19: Line 19:
with the largest eigenvalue (<math>\lambda_+</math>).
with the largest eigenvalue (<math>\lambda_+</math>).
From this director vector the nematic order
From this director vector the nematic order
parameter is calculated from (see Ref. 3)
parameter is calculated from (Ref. 5)
 
:<math>S_2 =\frac{d \langle \cos^2 \theta \rangle -1}{d-1}</math>
 
where ''d'' is the dimensionality of the system.
 
i.e. in three dimensions (see Ref. 3)


:<math>S_2 = \lambda _{+}= \langle P_2( n \cdot e)\rangle = \langle P_2(\cos\theta )\rangle =\langle \frac{3}{2} \cos^{2} \theta - \frac{1}{2} \rangle
:<math>S_2 = \lambda _{+}= \langle P_2( n \cdot e)\rangle = \langle P_2(\cos\theta )\rangle =\langle \frac{3}{2} \cos^{2} \theta - \frac{1}{2} \rangle
Line 37: Line 43:
#[http://dx.doi.org/10.1016/0167-7322(95)00918-3 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)]
#[http://dx.doi.org/10.1016/0167-7322(95)00918-3 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)]
#[http://dx.doi.org/10.1063/1.479982      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)]
#[http://dx.doi.org/10.1063/1.479982      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)]
#[http://dx.doi.org/10.1002/mats.1992.040010402 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)]
[[category: liquid crystals]]
[[category: liquid crystals]]

Revision as of 12:16, 22 June 2007

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)

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

where d is the dimensionality of the system.

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

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


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)