Order Parameter Theoretical Model 1. Free Energy

where   θ H n cos H ˆ    ,   T k H h B 2 χ Δ  is the dimensionless parameter of the magnetic field, and     S cos 2 1 θ 3 1 2   . If this is applied to the swollen LCE, which has two kinds of mesogen with different volume fraction, then the total energy is the sum of each component as follows :             14 2 1 φ 2 1 φ 13 2 1 φ 2 1 φ 2 2 3 1 1 1 3 1 2 1 2 2 3 1 1 1 3 1 2 1 2 1 S S h f S S h T k N F F F F mag B t mag m m mag            

2.2. Order Parameter

Orientational order is the most important feature of liquid crystals. The average directions of the long axes of the rod-like molecules are parallel to each other. Because of the orientational order, liquid crystals possess anisotropic physical properties; that is, in different directions, they have different responses to external fields such as an electric field, a magnetic field, and shear [23, 24]. In mixtures of liquid crystals, the molecules of different components may possess different degrees of nematic ordering. In the mixture, the order parameter expressed by [25, 26]: where     1 3 2 1 2   x x P is the second Legendre polynomial, i θ is the angle between a reference axis and the director of a mesogen belonging to component i i=1 for solute and i=2 for solution, and θ θ π 2 d sin d i  Ω . The function   i f θ is the normalized orientation distribution function which may be expressed by:     17 θ 1 θ T k V exp Z f B i i i      where i Z is partition function defined as:     18 θ π d T k V exp Z i B i i       Ω and   i V θ is the potential field describes intermolecular interaction. In the Maier-Saupe model, the potential   i V θ expressed by:           21 α 20 1 θ θ 19 1 θ α θ 2 2 3 2 2 3 T k S m cos T k m V cos S V B i i i B i i i i i            where α is orientational interaction constant and i m is dimensionless mean field parameter. Substitution Eqs.17, 18, 19, and 21 into Eq.16, we obtain :                     2 2 2 2 2 2 cos cos exp sin d cos exp sin d cos exp cos sin d 3 exp cos sin d i i i i i i i i i i i i S P P kT S S P kT P m P S m P                                       22 2 The order parameter i S can be obtained by numerically solving of Eq.23. The average value of order parameter S in binary mixture is given by [27]: 4 2 φ φ 2 2 1 1 S S S   where 1 S is order parameter of mesogen in solute and 2 S is order parameter of mesogen in solvent.

2.3. Phase Transition under Magnetic Field