Estimation of Interlayer Thickness in Inorganic Particulate-Filled Polymer Composites

Abstract

The structure of the interlayer between matrix and inclusions affect directly the mechanical and physical properties of inorganic particulate-filled polymer composites. The interlayer thickness is an important parameter for characterization of the interfacial structure. The effects of the interlayer between the filler particles and matrix on the mechanical properties of polymer composites were analyzed in this article. On the basis of a simplified model of interlayer, an expression for estimating the interlayer thickness ( $δ_{i}$ ) was proposed. In addition, the relationship between the $δ_{i}$ and the particle size and its concentration was discussed. The results showed that the calculations of the $δ_{i}$ and thickness/particle diameter ratio ( $δ_{i} / d_{f}$ ) increased nonlinearly with an increase of the volume fraction of the inclusions. Moreover, the predictions of $δ_{i}$ and the relevant data reported in literature were compared, and good agreement was found between them.

Keywords

polymer composite inorganic particle interfacial model interlayer thickness prediction.

INTRODUCTION

It is generally believed that interfacial interactions between the dispersive phase and continuous phase play an important role in the determination of the properties of all heterogeneous polymer systems, including inorganic particulate-filled polymer composites. Due to the interaction between the inorganic inclusions and resin matrix there is a kind of matter between the two phases in polymer composites. This matter is usually called as interlayer or interphase, and its structure and property are different from either the inclusions or the matrix, such as density, crystallinity, and so on. Early in 1960s, Kwei and Kumins [1] investigated polymer–filler interaction in polymeric composites. Although this interlayer is only a tiny partial region, its structure and property affect, to a considerable degree, the properties of composites. Esmaeili et al. [2] studied a ternary composite system by presenting an interface layer around the particle, and demonstrated that a soft interlayer changes the shear band pattern around a hard particle and therefore, leading to changes in macroscopic resistance, mean stress, and normal stress. The results obtained suggested that a suitable combination of the stiffness of the particles and interfaces leaded to an improvement in the mechanical characteristics of the blended polymer. Therefore, the mechanisms of interlayer generation as well as the structure and property of the interlayer in polymer composites have been paid extensively attention during the past 20 years [3–5]. Wu et al. [3] studied the interlayer in particulate-reinforced composite materials. Liu et al. [5] researched on the influence zone and the prediction of tensile strength of particulate polymer composites. Recently, Yung et al. [6] proposed a Young’s modulus model of polymer-layered silicate nanocomposites using a modified Halpin–Tsai micromechanical model, and the results showed that the modified composite theory satisfactorily captured the stiffness behavior of the polymer/clay composites. Amdouni et al. [7] investigated the influence of the interlayer thickness on pre-yielding and fracture properties of epoxy composites filled with glass beads coated with liquid rubber, they found that an elastomeric layer improved fracture toughness, and an optimum thickness of elastomeric interlayer was between 2% and 2.8% of the ratio interlayer thickness to filler radius. Lü and Lu [8] researched the elastic interlayer toughening of potassium titanate whiskers–nylon66 composites and their fractal, and obtained the similar conclusions: the optimal fraction of epoxy resin was 1.5 wt% of whiskers, which corresponded to an interlayer thickness of 3% of the radius of whiskers.

Interlayer thickness is one of major parameters for characterizing the interlayer structure and plays an important role for the mechanical properties of composites. In 1999, several researchers applied some advanced instruments and techniques to measure or observe the interlayer of polymer composites, such as attenuated total reflectance Fourier transform infrared (FTIR) technique [9], atomic force microscope (AFM) [10] and pressing trace instrument, and so on. However, the measurement precision for the interlayer by these apparatus should be further studied. Because the factors affecting the interlayer are quite complicated, most of the studies on the quantitative analysis or prediction of the layer thickness are limited to numerical analysis or under critical conditions [3,5,6,9–11].

The objectives of this study are to investigate the relationships among the interlayer thickness and the volume fraction as well as size of filler particles of particulate-filled polymer composites.

THEORY

Basic Assumptions

The basic assumptions for the theoretical analysis in this article are as follows: (1) the dispersion and distribution of filler particles in resin matrix are uniform; (2) the fillers may be considered as spherical particles because their size is very small; (3) the interaction between the filler and matrix, such as stress concentration and crystallization, are obvious. In general, the formation and structure of the interlayer of polymeric materials may be divided roughly in to the following types: (1) the adsorption layer is produced due to the roughness and activity of filler surface; (2) the matter is generated by the chemical reaction between the chemical matter of the filler surface and the resin matrix; (3) the crystallization layer induced by the filler surface; (4) the remaining stress layer is caused by contraction difference when polymer and filler is cooling. Obviously, the reinforcing and toughening effects of filler on polymer will be increased distinctly as soon as the interlayer can transfer stress and absorb strain energy or fracture energy under action of loadings.

Modeling

Figure 1 shows the relationship among the three phases, filler and the interlayer as well as the resin matrix. Where $r_{f}$ represents the radius of filler particle, $r_{m} - r_{i}$ the matrix region, and $r_{i} - r_{f}$ the interlayer region. In this article, we define B as the parameter of volume fraction:

(1)

Figure 1

Diagram of interlayer model.

where $φ_{f}$ and $φ_{i}$ are the volume fraction of the filler and the interlayer, respectively.

If let $α$ representing the weigh constant of the interlayer volume fraction, then B can be also expressed as

(2)

From Figure 1 one may determine the relationship among the volume fractions of interphase and the radius of the three-phase regions. Thus, combining Equations (1) and (2), one may derive an expression of the interlayer thickness ( $δ_{i}$ ). That is

(3)

where d_f = 2r_f is the diameter of the filler particles. Equation (3) describes quantitatively the relationship among the interlayer thickness, filler particle diameter, and the fraction of the interlayer.

RESULTS AND DISCUSSION

Factors Affecting α

It may be seen from Equation (3) that the key for predicting the interlayer thickness is how to determine the value of $α$ . Lipatov [4] investigated the interlayer of particulate-filled polymer composites, and found that when the ratio of the interlayer thickness to the particle diameter ( $δ_{i} / d_{f}$ ) is 1.2 and the density ratio between adsorption layer and surface layer is 0.5, one can calculate the $α$ being about 0.2 (the weight fraction of the particle is 10%). In order to investigate the dependence of the interlayer thickness on the volume fraction of filler particles under different $α$ values, we calculate the values of $δ_{i} / d_{f}$ by means of Equation (3), and the results are as shown in Figure 2. It can be seen from Figure 2 that $δ_{i} / d_{f}$ increases nonlinearly with an addition of $φ_{f}$ when $α$ is constant, and the higher the particle concentration is, the more obvious for the effect of $α$ . This because that the interaction between the filler and the resin matrix will be enhanced with an addition of the volume fraction (or weight fraction) of the filler particles, and the fraction of the middle phase will increase correspondingly, leading to increase of the interlayer thickness. When the volume fraction of the fillers reaches up to the critical value (i.e., the maximum filling concentration which the ligament between the neighboring particles will tend to zero), resin matrix might transfer the interface [3]. In this case, the expression of the interlayer thickness under these critical conditions can be written from Equation (3):

(4)

Figure 2

Relationship between $δ_{i} / d_{f}$ and filler volume fraction at different α.

where $φ_{fc}$ is the critical volume fraction of the filler particles, and $δ_{ic}$ the critical interlayer thickness.

Effects of $\bphi_{\bi f}$ and $\bi d_{f}$ on $\bdelta_{\bi i}$

It is known from Equation (3) that the interlayer thickness of particulate-filled polymer composites is related closely to the filler content and size. It is, therefore, necessary to understand the effects of the filler content and size on the interlayer thickness. Maiti and Mahapatro [12] measured the mechanical properties of calcium carbonate-filled polypropylene (PP) composites, and found that the effects of reinforcing and toughening of the composites were the best when the volume fraction of the filler particles reached up to the critical value. The mechanisms that generated this phenomenon may be interpreted by using the brittle–ductile transition theory proposed by Margolina and Wu [13]. According to this theory, the critical volume fraction of the filler particles in polymer matrix is expressed as follows:

(5)

where $φ_{sc}$ is the critical volume fraction of stress sphere, $d_{sc}$ the critical diameter of the stress sphere.

Figure 3 illustrates the dependence of the interlayer thickness on the volume fraction of the filler particles at various particle diameters and α = 1. Similarly, $δ_{i}$ increases nonlinearly with an increase of $φ_{f}$ when $d_{f}$ is fixed, and the dependence of $δ_{i}$ on $φ_{f}$ increases obviously in the case of bigger particles. This indicates that the bigger the particle diameter is, the stronger is the interaction between the filler and the matrix. Liu et al. [5] made a numerical analysis on the effect region (i.e. interlayer) of the fillers in particulate-filled polymer composites by applying finite element difference (FED) method, and the results showed that the thickness of the effect region was 2–10 µm, and the $δ_{i} / d_{f}$ was 0.2–0.4. These are close to the results as shown in Figures 2 and 3. Kwei and Kumins [1] studied the interaction between the fillers and polymer matrix by means of observation of vapor absorption effect, and pointed out that polymer interlayer produced by the fillers might reach up to the same order of magnitude as the diameter of filler particles.

Figure 3

Dependence of $δ_{i}$ on filler volume fraction at various $d_{f}$ .

Discussion

From a point of view of the thermal movement of polymeric molecules or molecular chains, the particles filled into the matrix will block, to a certain extent, the macromolecular motion of resin, and will affect the mechanical consumption and thermal property of the composite materials. On the basis of these, Lipatov [4] proposed an expression between $α$ and heat capacity:

(6)

where $Δ C_{c}$ and $Δ C_{m}$ are the heat capacity increment of polymer composites and unfilled polymer under glassy-transition temperature $T_{g}$ , respectively.

Substituting Equation (6) into Equation (3), one has

(7)

Thus, after measuring the $Δ C_{c}$ and $Δ C_{m}$ under glassy-transition temperature, one may estimate the interlayer thickness of polymer composites with various concentrations and size of filler particles by using Equation (7). The research results published by Lipatov showed that $Δ C_{c}$ reduced with an increase of $φ_{f}$ . It is known from Equation (7) that the reduction of $Δ C_{c}$ will let $δ_{i}$ increase, that is consistent with the conclusions discussed above.

Gao et al. [14] proposed a new method for determining approximately $α$ by calculating parameter $α_{A}$ using dynamic mechanical analyzer (DMA) data, and then replacing $α$ in Equation (3) by $α_{A}$ . The parameter $α_{A}$ is expressed as:

(8)

where $α_{A}$ is defined as the area constant of the interlayer volume fraction, $Δ U_{g}^{f}$ and $Δ U_{g}^{0}$ are the variation of basic line for composite and neat resin, respectively. The unit of $Δ U_{g}^{f}$ and $Δ U_{g}^{0}$ is in mV, and they are related to the specimen section area (A), that is

(9)

The values of U₁ and U₂ may be determined as shown in Figure 4 [14]. Substituting Equations (8) and (9) into Equation (3), one may determine roughly the $δ_{i}$ values. That is

(10)

Figure 4

Sketch of determination of $Δ U$ from DMA curve.

Thus, there are different methods or ways to estimate the interlayer thickness of inorganic particulate-filled polymer composites.

Pukanszky [15] considered the effect of interfacial interaction on the tensile strength of particulate-filled polymer composites and proposed a following equation:

(11)

where $σ_{c}$ and $σ_{m}$ are the tensile strength of the composite and the matrix, $λ$ is the relative elongation, and m expresses the strain-hardening character of polymer, the B_i is the interfacial interaction parameter.

Moczo et al. [16] proposed an expression between B and interlayer thickness on their previous work, which is as follows:

(12)

where $A_{f}$ and $ρ_{f}$ are the specific surface area and density of the filler, $σ_{i}$ is the tensile strength of the interface.

It might be known from Equations (11) and (12) that the B value could be determined by measuring the tensile properties in experimental, and then the interlayer thickness might be estimated.

Comparison

Gao et al. [14] studied the interfacial layer thickness of ethylene–propylene–diene mischpolymere (EPDM) filled with Al(OH)₃ composites using the DMA method stated above when the diameter and volume fraction of Al(OH)₃ were 24.2 µm and 10%, and found that the

δ_{i}

of the composite pretreated with silane coupling agent was greater than that of the composite unpretreated with silane coupling agent, as presented in Table 1. This indicates that the interlayer thickness will increase as the action between the matrix and inclusions is enhanced, and the surface of Al(OH)₃ particles treated with silane coupling agent enhances the action between the matrix and inclusions. Table 1 lists the values of the determined

α_{A}

and calculated

δ_{i}

from the DMA data of EPDM/Al(OH)₃ composites. If substituting the parameters known into Equation (7), one may obtain the relevant calculation values of the

δ_{ic}

for the two composite systems, the results are listed in Table 2. The values of

δ_{ic}

for the two composite systems are about 0.149 and 0.181 µm, respectively. It is known by comparing Tables 1 and 2 that the calculations by means of Equation (7) are close to the data reported in reference.

Table 1

The interfacial layer thickness of EPDM/Al(OH)₃ composites [14].

Composites	$\bDelta U_{g}^{f}$ (V m⁻²)	$\balpha_{A}$	$\bdelta_{i}$ (nm)
Unpretreated	748	0.345	126.7
Pretreated	676	0.408	149.5

Table 2

Comparison between the $\bdelta_{\bi ic}$ and $\bdelta_{\bi i}$ of EPDM/Al(OH)₃ composites reported in Gao et al. [14].

Composites	$\bDelta U_{g}^{f}$ (V m⁻²)	$\balpha_{A}$	$\bdelta_{i}$ (nm)	$\bdelta_{ic}$ (nm)	$\bDelta\bdelta$ (%)
Unpretreated	748	0.345	126.7	149	14.97
Pretreated	676	0.408	149.5	181	17.40

Moczo et al. [16] researched into the acid–base interactions and interphase formation in particulate-filled polymers, and estimated the interlayer thickness of several calcium carbonates (CaCO₃)-filled polymer composites including PP, polyethylene (PE), polymethyl methacrylate (PMMA), and polyvinyl chloride (PVC). Table 3 listed the comparison of interface thickness calculated for composites containing uncoated and coated fillers, the volume fraction varying from 0% to 5%. It can be seen that scale of the interface thickness is from 0.1 to 0.4 µm, and good agreement is found between these data not only for the composite systems with uncoated fillers but also for the composite systems with coated fillers, and the predictions shown in Figure 3.

Table 3

Comparison of interface thickness calculated for composites containing uncoated and coated fillers [16].

Polymer	$\bdelta_{i}$ (uncoated, nm)	$\bdelta_{i}$ (coated, nm)
PP	0.117	0.150
PE	0.114	0.183
PMMA	0.175	0.386
PVC	0.226	0.400

Zheng et al. [17] researched the selective laser sintering of polystyrene (PS) modified by Al₂O₃/PS composite particles with core-shell structure when the diameter and weight fraction of Al₂O₃ were 60 nm and 5%, respectively, and observed the shell thickness using transmission electron microscope (TEM) and FTIR spectrometer. They found the shell thickness is about 10–20 nm. This is also close to the predictions (Figure 3).

Amdouni et al. [7] investigated the influence of the interlayer thickness on pre-yielding and fracture properties of coated glass beads epoxy composites. The diameter range of the glass beads was from 4 to 200 µm, and the volume fraction was from 2% to 30%. In their study, the average ratio of elastomeric interlayer thickness to particle diameter ( $δ_{i} / d_{f}$ ) varied from 0% to 6.5%. These are also close to the predictions (Figure 2).

In fact, the model shown in Figure 1 is a physical model, because the parameters in Equations (3), (7), and (10) are related closely with the interlayer properties including crystalline and dynamic mechanical properties. In other words, these equations describe the correlation among the interlayer thickness and the interlayer property parameters, and provide a simplified method to estimate the interlayer thickness of the inorganic particulate-filled polymer composites.

CONCLUSIONS

There are many factors affecting the interlayer in polymer composites. Based on the simplified conditions, a model on the interlayer of inorganic particulate-filled polymer composites was established in this article, and an expression for prediction of the interlayer thickness was derived correspondingly.

The interlayer thickness of inorganic particulate-filled polymer composites with various content and size of filler particles were estimated. The results showed that the increase of the predicted interlayer thickness was relatively obvious in the case of greater concentration or size of the filler particles, and these calculations were more close to the research results reported in references. The surface treatment of filler particles is beneficial to enhance the action between the matrix and inclusions, resulting in an increase of the interlayer thickness.

The estimations of the elastomeric interlayer thickness or the ratio of the thickness to particle diameter for inorganic particulate-filled polymer composites by means of Equation (7) were compared with the experimental data reported in literature, good agreement was shown between the calculations and the measured data.

References

Kwei

T.K.

Kumins

C.A.

(1964). Polymer-Filler Interaction: Vapor Absorption Studies, J. Appl. Polym. Sci., 8: 1483–1490.

Esmaeili

Tomita

(2004). Characterization of Micro- to Macroscopic Responses of Ternary Polymer-Based Composite System, Adv. Eng. Plast. Appl. Pts. 1-2, Key Eng. Mater. , 274–276: 313–318.

Q.S.

Chen

X.B.

Son

H.C.

(1985). Interlayer in Particulate-Reinforced Composite Materials, J. Compos. Mater., 2(3): 41–45.

Lipatov

Y.S.

(1995). Polymer Reinforcement , Chem. Tec. PublishingToronto.

Liu

Z.H.

Liang

N.G.

Liu

H.Q.

(1997). On the Influence Zone and the Prediction of Tensile Strength of Particulate Polymer Composites, J. Reinf. Plast. Compos., 16(16): 1523–1533.

Yung

K.C.

Wang

Yue

T.M.

(2006). Modeling Young's Modulus of Polymer-Layered Silicate Nanocomposites Using a Modified Halpin-Tsai Micromechanical Model, J. Reinf. Plast. Compos., 25(8): 847–861.

Amdouni

Sautereau

Gerard

J.F.

Fernagut

Coulon

Lefebvre

J.M.

(1990). Coated Glass Beads Epoxy Composites: Influence of the Interlayer Thickness on Pre-Yielding and Fracture Properties, J. Mater. Sci., 25: 1435–1443.

Lü

J.Z.

X.H.

(2001). Elastic Interlayer Toughening of Potassium Titanate Whiskers–Nylon66 Composites and their Fractal Research, J. Appl. Polym. Sci. , 82: 368–374.

Pangelinan

A.B.

Mccullough

R.L.

Keylley

M.J.

(1999). Attenuated Total Reflectance FTIR Analysis of Surface Induced Molecular Weight Segregation, Composites, Part A , 30(1): 67–74.

10.

VanLandingham

M.R.

Dagastine

R.R.

Eduljee

R.F.

McCullough

R.L.

Gillespie

J.W.

(1999). Characterization of Nanoscale Property Variation in Polymer Composite Systems: 1. Experimental Results. Composites, Part A , 30(1): 75–83.

11.

Bogetti

T.A.

Wang

Vanladingham

M.R.

Gillespie

J.W.

(1999). Characterization of Nanoscale Property Variation in Polymer Composite Systems: 2. Numerical Modeling, Composites, Part A , 30(1): 85–94.

12.

Maiti

S.N.

Mahapatro

P.K.

(1991). Mechanical Properties of iPP/CaCO₃ Composites, J. Appl. Polym. Sci. , 42: 3101–3110.

13.

Margolina

(1988). Percolation Model for Brittle-Tough Transition in Nylon/Rubber Blends, Polymer , 29: 2170–2173.

14.

Gao

N.K.

Peng

Z.R.

Xie

H.K.

(2000). Study on the Characterization of Interfacial Structure Parameters in EPDM/Al(OH)₃ Composites, Acta Mater. Compos. Sinica , 17: 124–126.

15.

Pukanszky

(1990). Composites, Influence of Interface Interaction on the Ultimate Tensile Properties of Polymer Composites, Composites , 21: 255–262.

16.

Moczo

Fekete

Pukanszky

(2002). Acid-Base Interactions and Interphase Formation in Particulate-Filled Polymers, J. Adhesion , 78: 861–875.

17.

Zheng

H.Z.

Zhang

S.Q.

Z.F.

(2006). Selective Laser Sintering of Polystyrene Modified by Al₂O₃/PS Composite Particles with Core-Shell Structure, Acta Mater. Compos. Sinica , 23: 63–68.