ISSN:
1435-1536
Keywords:
Mesophase
;
fibrous
;
particle
;
sized composites
;
adhesion
;
unfolding models
Source:
Springer Online Journal Archives 1860-2000
Topics:
Chemistry and Pharmacology
,
Mechanical Engineering, Materials Science, Production Engineering, Mining and Metallurgy, Traffic Engineering, Precision Mechanics
Notes:
Abstract The degree of adhesion developed between matrix and inclusions in composites is among the main factors characterizing their mechanical and physical behavior. The quality of adhesion depends mainly on the boundary layer created between inclusions and matrix because of chemisorption, physisorption and mechanical constraint phenomena developed between the main phases in the RVE of a composite. The extent of this boundary layer, which is called mesophase or interphase, may be a potential means for defining the quality of adhesion. While almost all previous models describing the mechanical and physical properties of composites are based on the concept of mathematical and smooth interfaces constituting the boundaries of the phases, a series of recent models developed by the author and his collaborators consider a more pragmatic situation at the interfaces between phases assuming the existence of boundary layers between phases ensuring a continuous transition of the properties of adjacent phases, which should be accepted as being in conformity with the physical and chemical procedures happening at these boundaries. The unfolding type of models introduced by the author aims to fill the gap by trying to accommodate the properties of neighbouring phases by transition boundary layers with varying properties between the bounds of the limiting phases. Thus, the unfolding models constitute a powerful means, where the notion of mesophase was introduced for defininig the RVE of a composite. The RVE was considered as consisting of the two main phases (the reinforcement and the matrix), coupled together by the intermediate phase, whose variable mechanical properties unfold from those of the reinforcement to those of the matrix. The extent of mesophase was evaluated by the three different and alternate methods, that is: i) by considering the variations in the heat capacity jumps,ΔC p , of the matrix material and the respective composite, appearing at the respective glass-transition temperatures of both substances. Based on thermodynamic measurements with differential scanning calorimetry, the extents of these jumps were accurately measured and these defined the thickness of the mesophase. It was further assumed that the steep variations of the mechanical properties in the mesophase follows negative-power laws, whose exponents were derived by measuring the moduli of the matrix, inclusions and the composite and assuming the validity of an improved law of mixtures. § ii) by evaluating the extent of mesophase along the whole range of temperature by using exclusively the mechanical properties of the storage and loss compliances and moduli of the composite and the matrix, without making recourse to thermal or other types of measurements and without limitations at the glass transition temperatures, and § iii) by defining the extent of the mesophase by the same method, but evaluating the properties of the mesophase or mesophases by methods based on diffusion laws of mutually soluble phases or impregnations. This method is convenient for studying polymer-polymer composites and composites with encapsulated or sized phases. By applying all three variations of the unfolding model it was shown that all three possibilities of defining the extent and the variable properties of mesophases are equivalent and, furthermore, they yield reasonable results. Moreover, experimental evidence with either particulates, or fiber composites indicated clearly that the introduction of the mesophase yields a better and more flexible model for interpreting in a realistic manner the complicated phenomena appearing in all composites used in engineering applications.
Type of Medium:
Electronic Resource
URL:
http://dx.doi.org/10.1007/BF01412500
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