ABSTRACT:Volume relaxation in a-PMMA and a-PMMA/PEO amorphous blends was investigated by employing a mercury-in-glass dilatometer after a temperature down-jump from equilibrium above glass transition temperature, T g , to an aging temperature below T g . From volume contraction isotherms, volume relaxation rate, v ¼ À1=VðdV=d log t), was determined as a parameter quantifying the rate of volume changes, where V is the volume and t the aging time. The addition of PEO into blends has been found to considerably increase v .KEY WORDS Volume Relaxation / Amorphous Blend / PMMA / PEO / Polymer melt transforms to glassy state by cooling below glass transition temperature, T g . Due to the kinetic disability of the macromolecules to achieve appropriate conformations immediately, material is in a thermodynamically non-equilibrium state. This causes a process of structural relaxation to attain a closer packing and thus to achieve thermodynamically equilibrium conformations, when the polymer is cooled below T g . This aging process occurring on the level of microstructure is reflected in time dependent changes of macroscopic properties such as density, modulus, refractive index, dielectric constant and others.
1-3The macrostructural response of a material to the non-equilibrium state is usually studied by monitoring time-dependence of volume after temperature downjump or up-jump. In the former method a material is cooled from an equilibrium state above T g to an isothermal aging temperature, T a (below T g ), which is followed by monitoring isothermal volume relaxation, i.e. material contraction. 4 The latter method is based on heating of the sample in the glassy state, which causes its expansion.
5The volume relaxation process can be quantitatively analyzed by the volume relaxation rate, v , i.e. the slope of the contraction isotherms in the region where the volume, V, varies linearly with the logarithm of aging time, t:where is the relative departure of actual volume, V ðtÞ , from equilibrium volume, V 1 , defined as:The initial departure from equilibrium, i immediately after the temperature jump is related to the magnitude of temperature jump, ÁT:where Á is the difference between the volume expansion coefficient of equilibrium liquid and glassy states. Thus, increasing ÁT and Á leads to higher initial departure from equilibrium and subsequently faster volume relaxation rate. However, experimentally measured dependencies of v for many glassy polymers show a discrepancy between this expectation. v follows the relationship for lower magnitudes of ÁT, but for higher temperature jumps v becomes smaller than the predicted value. This is usually attributed to underestimation of v for bigger ÁT. 4,6 Another possible explanation is that for higher ÁT the process of volume relaxation becomes thermorheologically complex. 6,7 Among various blends a special kind of miscible blends, composed of one amorphous component and the other crystallizable, atactic poly(methyl methacrylate)/poly(ethylene oxide), (a-PMMA/PEO), has been lately ex...