Order parameters: Difference between revisions

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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
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#[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 10:16, 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)

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.


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)