Analysis of interactions in multicomponent polymeric systems: The key-role of inverse gas chromatography

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Abstract

The properties of a polymeric system are a consequence of the interactions that occur between the various components of these complex systems. These components may vary significantly in terms of chemical nature (e.g. organic/inorganic), physical properties (e.g. particle size, surface area, molecular weight), structural characteristics and proportion in the formulations composition. This review paper addresses the major approaches in use regarding the analysis of the interactions that occur between the polymeric system components and the use of such approaches in the interpretation of the chemical, physical and thermodynamic properties of these systems. Special attention is given to the technique of inverse gas chromatography.

A case study is presented, where use was made of inverse gas chromatography to characterize thermodynamically the surface of the major components of pigmented PC/PBT blends. The concept of Lewis acidity/basicity was used in the interpretation of the intermolecular interactions nature and potential in these blends, as encountered in phase separation and phase preferences phenomena and as expressed in the morphology, the physical and the mechanical properties of these commercially important composites.

Introduction

The strong correlations that exist between the morphology, the processing and the physical and the mechanical properties in multicomponent polymeric systems are well-recognised [1], [2]. These aspects and correlations are a consequence of the interactions that occur between the various components of polymer-based systems. As the number of constituents in these systems increases, the ways in which the various components interact and become dispersed/segregated during processing and in service, become increasingly important. Among these added materials are the stabilisers, plasticizers, reinforcing fibres, pigments and other polymers.

In the particular case of polymer mixtures, the morphologies of two-component polymer blends have been widely discussed in the literature as these represent the more common commercial form of polymer blends. In response to commercial pressures and to the need for precisely tailored physical properties, more complex blends that consist of multiple components are under active development. In such blends, morphological concerns go beyond questions concerned with the dispersed phase size, anisotropy, etc., to include other issues, such as why one of the dispersed polymer phases may spontaneously encapsulate another [3] or encapsulate the filler particles [4]. Obviously, in multiphase polymer systems, interfaces and interphases must exit. Therefore, it is reasonable to assume that under equilibrium conditions, such effects must arise from interfacial energy differences among the blend components. Surface and interfacial phenomena have been proven to influence:

  • (i)

    the dispersion of minor phases in polymer matrices [5], [6];

  • (ii)

    the processability of polymer blends and composites [7], [8];

  • (iii)

    the mechanical properties of polymer blends [9], [10].

Moreover, it is well-known that, for polymer blends, the apparent properties and morphology often do not indicate an equilibrium situation [11]. For instance, in blends of an amorphous polymer and a semi-crystalline polymer, the phase behaviour is strongly dependent on blending and the cooling conditions. In the case of partial miscibility or of complete miscibility of the components in the molten state, the cooling rate and the kinetics of non-isothermal crystallisation influence the final extent of phase separation at room temperature. The attainment of the thermodynamic equilibrium is determined by the nature and magnitude of the interactions between the components of these systems, as reflected in the existence of intermolecular forces.

The use properties of polymer blends depend strongly on the miscibility (compatibility) of the polymers. Miscibility occurs when specific interaction forces develop between the two (at least) polymers [12], [13]. Specific interactions may be in the form of hydrogen bonding, charge transfer complexes, acid–base type interactions, dipole moments and electron donor–acceptor complexes [14], [15], [16], [17], [18]. These specific interactions are of a highly directional nature and are present in addition to the dispersive forces. A current view, pioneered by Fowkes [14], [19], [20], [21], [22], [23], [24], [25], which is increasingly accepted, suggests that the totality of specific interactions may be viewed as Lewis acid–base forces. This approach has been supported by experimental results [24].

Intermolecular forces that are operating between molecular segments of polymers and at particulate interfaces are frequently cited in the literature [3], [26], [27], [28], [29], [30], [31], [32], [33], [34], [35] as being responsible for the properties of the system as a whole. In the particular case of polymer nanocomposites, e.g. polymeric matrices filled with well-dispersed, high shape-factor nanofillers, the self-organisation of the polymer chains has been reported to be significantly influenced by the nature and magnitude of the intermolecular interactions between the inorganic and the polymeric components. For instance, in polyamide (e.g. Nylon-6) matrices filled with organoclays, important changes in the crystallisation behaviour of this polymer have been reported [36], [37], [38], [39].

Control of Lewis acid–base (specific) interactions has gained increasing significance in industrial practice for optimising the performance of polymer composites [14], [40], [41]. This is because such intermolecular forces are known to dominate over dispersion intermolecular forces and dipole–dipole intermolecular forces [2], [5], [12], [13], [14], [16], [31], [34], [35], [40], [41], [42], [43], [44]. This is clear in the definition of specific interactions, given by Huyskens et al. [16], “specific interactions are short-range, site-bounded cohesion forces that considerably weaken a given chemical bond of one of the partners”. Furthermore, from a thermodynamic point of view, specific interactions between chemical moieties are required in order to obtain a negative excess free energy by mixing [45].

From the above description, it is clear that there is a link between component interactions on the one hand and the rheological, physico-chemical and mechanical properties of the system, on the other.

Section snippets

Thermodynamic requirements for miscibility in multicomponent polymeric systems

The basic question when considering a multicomponent polymeric system concerns the extent of thermodynamic miscibility. Several polymer pairs are known to be miscible or partially miscible and many of these have become commercially important [2]. Considerable attention has been given to the origins of miscibility and to binary polymer–polymer phase diagrams. It is usually observed that high molar mass polymer pairs, showing partial miscibility, exhibit phase diagrams that indicate a lower

The solubility parameter

One widely used approach to the quantification of interactions that occur in multicomponent polymeric systems is through the determination of “solubility” or “cohesion” parameters, δT. This parameter is, in effect, the square root of a cohesive energy density, as defined by Hildebrand in Eq. (3) [51], [52], [53]:δT=ΔHvV1/2

Here, ΔHv is the molar vaporisation energy of the substance and V is its molar volume.

The solubility parameter was originally intended to be applied to substances whose

Interaction parameters from polymer solution theories

Polymer solution thermodynamics, as developed firstly by Flory and Huggins (cited in refs. [56], [57], [58], [59], [60]), expresses the interaction between a polymer and a liquid in terms of a dimensionless parameter, χ1,2. This can be written as Eq. (4):χ1,2=μ1μ2RTφ12lnφ1+1V1V2φ2φ2

The subscripts 1 and 2 denote the liquid (solvent) and the polymer (solute), respectively, μ the chemical potential, φ the volume fractions and V denotes molar volumes. Miscibility occurs when χ1,2 is lower than

Work of adhesion and interfacial tension

Researchers, such as Raetzsch et al. [9] and Liang et al. [24] studied miscibility phenomena of polymer blends based on the presence of interfaces in multiphase polymer mixtures, employing the thermodynamic work of adhesion between two different solids and interfacial tension determinations. This specific thermodynamic adhesion energy (Wa) or, in the case of a known adhesion distance, the specific adhesion strength between two solids, can be determined from the respective surface tensions, γ1

Introduction to inverse gas chromatography (IGC)

The growing awareness of the importance of solid surfaces, interfaces and interphases in determining the useful properties of polymeric systems, has led to the development of inverse gas chromatography as a useful technique in evaluating the potential for interaction of different components of polymer blends, composites and multicomponent polymeric systems. Data obtained from IGC experiments may, in favourable cases, correlate directly with observed performance criteria, such as colour

Conclusions

The intermolecular forces operating in multicomponent polymeric systems contribute decisively to the useful properties of these systems. Several approaches exist that allow for an interpretation, forecast and optimisation of the interactions occurring in such complex systems. These include the use of solubility parameters, of interaction parameters from polymer solution theories, of the concept of work of adhesion and interfacial tension and of diverse thermodynamic parameters and

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