Pure glyceryl tristearate was prepared as solid fat particles by complete hydrogenation of olive oil, and pure glyceryl trioleate was prepared as liquid oil by solvent fractionation of olive oil.
The rheological properties of mixtures of these two components were investigated in comparsion with their microstructure revealed by X-ray diffraction. The flow curves of various mixtures were measured by a Weissenberg rheogoniometer and the temperature dependence of viscoelasticity was studied by an forced oscillation apparatus. Two kinds of specimen were prepared. One is a suspension body, that is, simple mixture of triolein and tristearin which is uniformly mixed by stirring it with a glass rod at room temperature, and the other is a molten body, that is, the mixture of tristearin and triolein which is molten at 90°C and recrystallized at 0°C. In each mixture the fraction of tristearin is from 5 to 45% by weight.
All the flow curves for mixtures of 5 to 25% tristearin were typically non-Newtonian. From the relation between the apparent viscosity η and the rate of shear γ, the shear rate dependence of viscocity -(d logη/d log γ) was calculated at a high rate of shear 20sec.
-1 and at a low rate of shear 1 sec.
-1. From the relation between the fraction of tristearin and -(d log η/d log γ), it was observed that the shear rate dependence of viscosity was much larger for the suspension body and at a lower rate of shear. These results suggest that a firm texture is developed in the specimen after the melting of suspension due to the formation of network structure of crystallites of tristearin.
The temperature dependence of dynamic elastic modulus
E* and loss factor tan δ has been measured for mixtures of 25 to 45% tristearin. It has been found that the mixtures of 25 to 40% tristearin show entropy elasticity, that is, the elastic modulus increases with the rise of temperature and that on the other hand, a 45% tristearin mixture shows energy elasticity, that is the elastic modulus decreases with the rise of temperature. It is reasonably assumed that a network structure having crosslinked molecular chains such as exists in rubber in the present mixtures. A number of small crystallites of tristearin would produce the crosslinking points. The molecular weight between crosslinks was tentatively calculated from the elastic modulus at room temperature using Kuhn's theoretical equation for rubber elasticity and found to be in the same order with the molecular weight of tristearin and triolein.
The variation of
E* and tan δ was followed during the heating and cooling at a fixed rate for the same samples. Heat treatment profoundly alters the physical properties of mixtures. After a cycle of heating and cooling,
E* at room temperature increases and tan δ decreases. Observation by X-ray diffraction shows that the degree of crystallinity increases slightly after the heat treatment and also that the habit of crystals changes from β type to β' type. It is seen, however, that log
E* increases almost linearly with the degree of crystallinity for both β and β' types, and that these two lines are almost parallel in the range of crystallinity investigated less than 40%. The value of tan δ is largest at the fraction of tristearin 30 to 35 percent where the rubber-like property is observed most obviously.
The results for the present mixtures where the melting temperatures of two components are far apart would give some useful knowledge to consider the physical properties of more complicate mixures of oils and fats. The network structure formed by the small crystallites and the mobile molecules between them crosslinked by these crystallites would give an interesting model for ellucidating the mechanical properties of ordinary fats.
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