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Author(s): |
Edgard Goncalves Fernandes Junior
Total Authors: 1
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Document type: | Master's Dissertation |
Press: | São Paulo. |
Institution: | Universidade de São Paulo (USP). Conjunto das Químicas (IQ e FCF) (CQ/DBDCQ) |
Defense date: | 2001-11-29 |
Examining board members: |
Maria Regina Alcantara;
Rosangela Itri;
Frank Herbert Quina
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Advisor: | Maria Regina Alcantara |
Abstract | |
This dissertation shows the results obtained on the rheological characterization, using rotation and oscillatory essays, for nematics and cholesterics lyotropic liquid crystals based on decylammonium chloride (CDA). The cholesteric systems were obtained adding chiral inductors, hydrophobic (Cholesterol) or hydrophilic (D-(+)-Mannose) to nematic matrixes, inducing a helical arrangement on the liquid crystalline stn1cture. The effect of the inductor concentration besides of its nature and the amount of solvent in these mesomorphic systems were correlated to the rheological properties obtained. The rotation essays were done using constant and varied shear rates. The obtained results showed a change in the rheological behavior dependent of the chiral inductor nature. Phases with hydrophobic inductor presented viscosity decreased with the increase of cholesterol concentration, while the increase of D-(+)-Mannose concentration leads to the viscosity increase. Changes in the rheological behavior were also observed according to the amount of solvent present on the phase. For systems with cholesterol and larger amount of water, the viscosity increases along the time until reaching a maximum value, followed by a decrease. This behavior should indicate that in these systems, the phases should suffer some kind of deformation until reaching a maximum of tension. After that, an accommodation process of the structure causes the viscosity decrease. For the systems with hydrophobic inductor and with smaller amount of solvent, the viscosity decreases until reach a minimum value, that is reached later as larger it is the inductor concentration. After that, there is an increase of the viscosity until a constant value be obtained. It suggests the occurrence of a breakdown of the stn1cture, proceeded by its reorientation by flow. For the systems with D-(+)-Mannose, the rheological behavior observed is quite similar for phases with larger or smaller amount of solvent, i.e., increase of the viscosity to a maximum value, followed proceeded by its decrease. The difference is that in systems with larger amount of solvent, the maximum is reached earlier. The increase of the viscosity should characterize a deformation of the stn1cture that after reaching a maximum tension, it will be orientated in a preferential direction, causing the decrease of the viscosity without break of the cholesteric building. The flow activation free enthalpy (ΔH≠) determination shows a decrease of energy value for increase of inductor concentration in lyotropic cholesteric liquid crystal that used cholesterol as inductor. When D-(+)-Mannose was used, the flow activation free enthalpy value increases. In the systems that hydrophobic inductor is used, the chiral forces should help in micelles flow orientation process, seemingly, after the movement of a micelle, the others would be dragged by the elastic forces, decreasing the flow activation enthalpy. When it is used a hydrophilic inductor, flow activation enthalpy increases with increases of inductor concentration, probably because the inductor nature that has a greater interaction with the solvent, acting as a barrier against the micelles flow orientation. The oscillatory essays show that the storage energy capacity, determined by the value of the storage modulus (G\') is larger than heat or diffusion dissipation capacity of the particles, obtained by the loss modulus (G\"). Both modulus (G\' and G\") decrease for the phases with smaller amount of available water and stay constant for the systems with larger amount of water. The lyotropic mesophase studied can be described by a Burger model modified by taken into account a temporary dependence to the elastic Maxwell component. This effect should be probably due to the inertia of the system. (AU) |