- freely available
Int. J. Mol. Sci. 2009, 10(12), 5257-5284; doi:10.3390/ijms10125257
Abstract: This review covers recent advances and work on the microstructure features, mechanical properties and cracking processes of conducting polymer film/coating- substrate structures under different testing conditions. An attempt is made to characterize and quantify the relationships between mechanical properties and microstructure features. In addition, the film cracking mechanism on the micro scale and some influencing factors that play a significant role in the service of the film-substrate structure are presented. These investigations cover the conducting polymer film/coating nucleation process, microstructure-fracture characterization, translation of brittle-ductile fractures, and cracking processes near the largest inherent macromolecule defects under thermal-mechanical loadings, and were carried out using in situ scanning electron microscopy (SEM) observations, as a novel method for evaluation of interface strength and critical failure stress.
Conducting polymer films or coatings, such as the polypyrrole (PPy) and polythiophene (Pth), are widely used as functional, protective and decorative materials in diverse engineering applications, chemical sensors or biosensors [1–5], battery electrodes and as protection against oxidation or corrosion [6–9]. In addition, conducting polymer films or coatings are also widely exploited due to their special features such as low densities, high strength, ease of fabrication, design flexibility, stability and low cost. The promise of combining these desirable physical properties with electrical properties has prompted great interest in conducting polymers over the past few decades, and it is clear now that polymers and electrical conductivity are no longer mutually exclusive.
The search for conducting polymers began in earnest at the end of the 1970s, when an increase in conductivity by 12 orders of magnitude was observed in polyacetylene upon charge transfer doping . This was closely followed by the fabrication of free standing polypyrrole films or coatings by the oxidative electropolymerization of pyrrole .
However, for some time, the practical applications of conducting polymers were limited by their intractability and insolubility, especially in the doped state. These problems were overcome by using 3-substituted thiophenes [12,13] and aniline derivatives , which not only produced processable conducting polymers, but also allowed the polymers to attain the full range of physical and mechanical properties.
Polythiophenes have been usually featured in more general reviews on conducting polymers [15–17] or on more specific topics, such as electropolymerization [18–20], electrochemistry  environmental stability , optical properties  and microstructure-thickness-mechanical properties [24,25]. However, so far there have been at least three reviews which have focused entirely on the synthesis, functionalization and applications of polythiophenes [26–28]. The first one was published in 1986 , the second—an excellent work by Roncali —was published in 1992, the the third—on the synthesis, characterization and applications of thiophene-based functional polymers was published in 1998 . We feel that it is timely to give an up-to-date account of functional polymers based on the thiophene family, as much progresses have been made since 1992. At the same time, these reviews have reported on the synthetic trends for the preparation of low bandgap and regioregular materials that occupy a central place in recent advances in polythiophenes, since so many of their properties are profoundly dependent on the regioregularity of the polymer, as are other special properties like chromatism and luminescence. The effect of fullerenes on the mechanical or conductive properties of polythiophene Langmuir-Blodgett films has received much attention over the past two decades, accounting for a great deal of the activity in the material science areas. Conducting polymer films or coatings however face the challenge of how to conform the internal stresses, failure models and failure behavior/mechanisms in order to meet current design requirements for practical applications, especially when the thickness of film or coating is relatively thin and relatively wide. For example, Francis et al.  studied the origins of internal stresses in polymer coatings and the available methods to measure them by using the determination of curvature or deflection of a coated elastic substrate (e.g., wafer or disk, strip, cantilever). In fact, most polymeric films or coatings shrink during and after solidification due to chemical reactions, solvent evaporation, phase separation, or some combination thereof. The strength of coating adhesion on the substrate and internal stress in the coating layers can easily cause the shrinking of the coating, leading then to brittle cracks in the coating layers or blisters from the substrate. Edge effects and thickness nonuniformities can also cloud the interpretation of stress evolution phenomena. These issues have been visited in a large body of literature [30–33]. Wang et al. [24,25,34] were concerned with the effects of thickness and microstructure on the mechanical properties of conducting polythiophene films, with special emphasis on failure behavior. In addition, they also demonstrated that the failure behaviors of film/coating-substrates under bending loadings or under thermal-mechanical loadings were dependent on complex factors, such as plane stress state or strain state, thickness of the layer of film and interface adhesion strength, which were in turn dependent on the synthesis processing technology used [35–39]. Baumert et al.  showed the factors affecting the forming behavior of ultra-thin polymer coatings on ductile substrates, while an extensive literature exists for the reverse case, metal films on polymer substrates, or brittle films on deformable substrates. For these cases, advanced models exist, mostly based on the so-called shear lag approximation. The heterogenous, highly localized strain and stress distributions, typical of ductile substrates, as well as out of plane displacements at the interface were disregarded, but could not be neglected at the high strain levels of interest for elastic polymer films. The role of slip bands in cracking of ultra-thin polymer films was studied. These results indicated that if the film/coating layer is thin enough relative to the thickness of a substrate, the failure behavior or model of film/coating-substrate structure may be changed. Understanding the failure transforming mechanism is still a rather complex problem and it needs to be confirmed by more experiments, although some works have found that there is a size effect. For example, the physical undulate effect on the failure model or plane stress state must also be considered. However, the most common method to determine internal stress in coating layers is only by measuring the curvature or deflection of a coated elastic substrate. This method dates back to Stoney’s work in 1909 . The basic assumptions and methodologies of curvature and deflection-based measurements of stress in Stoney’s work are outlined below, and a brief discussion of other stress measurement methods and supporting characterization is presented. Relatively complete descriptions of the mechanism involved in curvature and deflection-based techniques [42–45] and reviews of internal stress measurement methods [46,47] can be found in the general literature. The internal stress in a coating may cause a deformation and result in a curvature of the system. It was argued that the failure in film/coating layers customarily might also occur in cases when the curvature or deflection of substrate might be very relatively small relative to the micro scale. Therefore, the above mentioned estimation method is very difficult or more errors exist. However, these aspects were seldom reviewed, especially with regard to the failure behavior, failure criteria stress and failure mechanisms of conducting polymer film/coating-substrate structures. Therefore, the quantificational understanding of how these issues dominate the mechanical properties of film/coating-substrate structures in reliable designs of electronic devices is an important and pivotal problem. In this review, combining both references and our own recent work, the different estimation methods, the failure behavior in thin film/coating, the cracking process and microstructural features on the meso- or micro- scale were carried out by using the SEM in situ technique. The effects of microstructure and the dependence on the synthesis and doping methods of the mechanical properties of conducting polymers are also characterized and discussed.
2. Typical Preparation and Processing of Conducting Polypyrrole/Polythiophene Coating-Substrate Structures
A polythiophene (Pth) thin film/coating was synthesized in a one-compartment cell with the use of an EG&G model 283 potentiostat under computer control. This system, which consists of working-, counter- and reference-electrodes is called a three-electrode system [48–50]. The working-electrode acts as the substrate for the electrodeposition of the Pth (or other polymers). Since the process of deposition of the conducting polymeric film/coating is an oxidative process, it is necessary that the electrode not be able to concurrently oxidize the aromatic monomer. For this reason only inert electrodes such as stainless steel substrates were used. The working- and counter-electrodes were AISI 304 stainless steel sheets (L × W × t: 45 mm × 2.5 mm × 1 mm) placed about 5 mm apart. The reference electrode was Ag/AgCl. The electrolyte solution was freshly distilled boron trifluoride-diethyl etherate [BF4]− containing 30 mM thiophene at a constant potential of 1.3 V. All residual solutions were deaerated by a dry argon stream and maintained at a light overpressure during fabrication. The total charges exchanged during the deposition process were used to control the thickness of the deposited films/coating. If one wishes to obtain a solid film, the film has to be washed with distilled ethyl ether and it should be dried under vacuum at 80 °C for about 24 hours.
Another typical electrolytic solution used for polypyrrole (PPy) consists of mixtures of isopropyl alcohol (IPA, Tianjin No.1 Chemical Regent Plant, China), boron trifluoride diethyl etherate (BFEE, Beijing Changyang Chemical Plant, China), diethylene glycol (DEG) or polyethylene glycol (PEG, mw = 1,000, Beijing Yili Fine Chemical Corporation Ltd.). All solutions were deaerated by a stream of dry nitrogen for 10 minutes before the experiment and a slight nitrogen over-pressure was maintained during the experiments. The polymerization of pyrrole was performed at the ice bath temperature of 0 °C, except when indicated otherwise. PPy film/coating was grown potentiostatically. After polymerization, the PPy film/coating surface was washed repeatedly with acetone .
Occasionally, to enhance the adhesion strength between the polypyrrole film/coating and a substrate, the substrate should not be easily oxidized. For strongly adherent polypyrrole coatings on substrates such as smooth iron or mild steels, a treatment by 10% aqueous nitric acid that inhibits iron dissolution without preventing the pyrrole oxidation was studied . Very adherent thickness-controlled PPy films were obtained at constant-current in various aqueous media containing Na2SO4, K2C2O4 or KNO3. A maximum coulombic efficiency of 95% was obtained in the presence of KNO3 for a current density lower than 10m A/cm2, but it dropped to 70% and 50%, in the presence of Na2SO4 and K2C2O4, respectively, and for a current density between 2 and 4 mA/cm2. Among the various surface pretreatments under study, the 10% nitric acid treatment was found to be the only one able to modify the surface, leading to an important passivation of the iron electrode and allowing the formation of the thickness-controlled, strongly adherent PPy films.
3. 3-Dimensional Nucleation Behavior of Coatings on Substrates Based on the Electrochemical Synthesis Method
Figure 1 shows an evolutionary process with a macromolecular nucleation mechanism (Figure 1a) and free surface morphology (Figure 1b). This processing can be described as small island structural formation. Results are similar to most of the studies that provide evidence of nucleation and three-dimensional growth [52–54]. It is only very recently that 2-D growth has been demonstrated for electronically conducting polymers (ECP). Li and Albery [55,56] have also established the progressive nucleation and 2-D growth (2DP) for poly(thiophene-3-acetic acid). For example, Kontturi et al.  reported how the substrate material depends on the initial stages of molecular adsorption by 2-D layer by layer growth and on the high resistance of the growth film/coating. The common denominators for all these phenomena are the OH functions. C-O-C bonds are introduced in the polymer, which lead to a film with lower conductivity than normally observed for electronically conducting polymers. The low conductivity of the growing film causes the polymer to grow mainly in the direction parallel to the electrode surface (2-D growth), the potential drop between the metal electrode and the electrolyte increasing with increasing film thickness. As the amount of high resistance polymer on the electrode increases, passivation of the electrode becomes evident. The adsorption properties of the OH group are likely to contribute to the formation of an adsorbed monolayer of poly(thiophene-3-methanol) (PTM).
The layer-by-layer growth forms a compact solid structure with a certain adhesion strength, and variable conductivity of the PTM film/coating makes this polymer a possible candidate in many applications. Aside from the substrate materials, the other nucleation conditions (homogeneous nucleation or heterogeneous nucleation) can strongly influence the mechanical properties, conducting performance and microstructure feature of films/coatings. The effects on conductivity may also be significant for the protective properties against corrosion of the metallic substrate. For example, Rohwerder et al. recently reported a conducting polymer for corrosion protection that makes all the difference between failure and success . For this purpose, Freitas et al.  and Akundy et al. [60,61] made great efforts to deposit or synthesize conducting polymers on different metal substrates, such as steel and aluminum. An optimization is required to balance the prevention of macroscopically extended percolation networks and ensuring enough particles in the coating to be effective. Very powerful novel corrosion protection coatings may thus be developed, based on a highly effective case sensitive inhibitor release. Therefore, the deposition process of conducting polymer on the metal substrate is similar to an island in the initial state, and it forms the thin coating layer through linking these islands reciprocally. Wang et al.  observed the certainly instantaneous morphology of deposition islands by a SEM method as shown in Figure 1.
When the surface layer of island maintains a stable state, the surface tension of island is equal to the interface tension increment as follows:
So the volume of this island formed with A′ can be expressed by Equation (4) as follows:
The effect of all substrate materials on the nucleation behavior of conducting polymer film/coatings should be attributed to the action of the wetting angle θ and the interface tension magnitude during the nucleation process. However, these influencing factors depend strongly not only on the free surface quality and consistent contact between the substrate and conducting polymer solutions, but also on the electrosynthesis conditions, such as the temperature, time, electric current, etc. [24,57,59–61]. For instance, Kontturi et al. , Fleischmann et al.  and Harrison et al.  have described in detail nucleation models involving progressive nucleation followed by 1-D growth, instantaneous nucleation followed by 2-D growth, and 2-D growth with slow diffusion, respectively. These models have been developed for the growth of separate metal nuclei without consideration of overlap effects, and the position of electronically conducting polymers (ECP), since the deposition processes of ECPs have some differences and are usually faster than those of metals. They thought that these models of metal electrodeposition provide a good basis for analysis of the electrosynthesis of ECP, given some important clues on the nucleation and growth mechanism, and in the case of 2-D growth, on the magnitude of the spreading rate. With increasing thickness of the thin film/coating layer, polymer molecular groups are added, filling the cavities between the islands that then forming a final free surface structure of film or coating as shown in Figures 1b and 3b. Johanson et al.  gave a similar space-filling nucleation model of the planar HF/6-31G(d) optimized nitrate complex of a pyrrole pentamer dication. However, when the thickness of film/coating layer is over than 2–3 times that of h, the effect of substrate material on the nucleation behavior of film/coating becomes weaker and weaker indicating that there is a weak adhesive strength between the island’s interfaces. For example, the average h of polythiophene film/coating on stainless steel is not more than 1–2 μm, as shown in Figures 1a and 3a. Therefore, the average h of a PPy film/coating on stainless steel is also not more than 2–3 μm, as shown in Figure 3b. The interface or surface tension between islands may be decreased, leading easily to the formation some defects (cracks and voids) in the free surface or in the cross-section surface . These defects near the free surface layer might cause the mechanical properties to gradually deteriorate, especially considering the effect of a residual stress  as shown in Figure 4 and the literature [24,25]. If the volume of molecular group remains a constant, with decreasing of the wetting angle θ, the ratio of h/r has to decrease. Then the molecular group/island on the substrate will become a more coplanar island layer. However, the work or energy of a nucleation molecular group/island can be calculated similarly to the nucleation model of metal as following as:
In addition, Beck et al.  have also given an estimation method for the effective thickness of polymer films on iron substrates as follows:
4. Microstructure-Mechanical-Conductive Properties of Polymer Film/Coating
Based on the above mentioned deposition models of electrochemically synthesized conducting polymer film/coatings [57,62–64], the microstructure of the free surface or fracture cross-section depends strongly on the synthesis conditions. The perfect microstructure of a conducting polymer should satisfy the requirements of mechanical and physical properties such as stiffness, mass and temperature. For example, Chainet et al.  suggested that the polypyrrole morphology under different doping states should be studied in situ with scanning tunneling microscopy (STM). Their results indicate that the electronic conducting polymer was submitted to strongly structural variations during the doping (or dedoping) process due essentially to the inclusion of anions in its structure. The insertion of ions induces a swelling phase and therefore modifies the surface morphology. They obtained an evolution of the cross-section profile of the polymer strands as a function of the potential applied to the thin film. Surface roughness of conducting polymer coating layer was found to be rather low in comparison to other polypyrrole salts, even at thicker layers . The change of morphology caused necessarily a change of the mechanical properties of the conducting polymer. This is because the morphology change may cause a structural defect or a geometrical notch. For the surface morphology and defects capacity per unit area of conducting polythiophene film, Zuo et al.  suggested that the fractal characteristic of surface morphologies and defects capacity in a unit area might be described by using fractal theory. Fractal results are indicated to be of value in the quantitative characterization of surface morphologies and defects capacity per unit area of electrochemically synthesized polythiophene films. The fractal characterizations of surface morphology and defects capacity in the unit area depended mainly on the grizzly threshold on these SEM images. The relationship between the threshold and the fractal dimensionality can be expressed as a function. The fractal dimensionality is as follows:
Figures 5 and 6 show the typical free surface morphology and cross-section fracture of conducting polymer films which were prepared in mixed electrolytes of IPA + 5% BFEE in an ice bath at 15 °C and 0 °C respectively. Figures 5a and 5b show the free surface and cross-section fracture of PPy film synthesized in an electrolyte of IPA + 5% BFEE + 5% PEG1000 at 15 °C, respectively. The results indicate that there are rather larger and flatter agglomerated groups and rather more grooves on the free surface, which forms a smooth cross-section surface of fracture as a result. The characterizations confirm the film has a poor toughness, whose elongation at break is about 4.47% and its tensile strength is about 36 MPa, as shown in Table 1. This is because the adhesion strength among the agglomerated groups is rather low. The surface cohesive force of this microstructure may be weaker than that of cap shape aggregation structure formed by capillarity or island microstructure formed by 3-D nucleation.
Figures 6a and 6b show the typical free surface and cross-section fracture of PPy film synthesized in an electrolyte of IPA + 5% BFEE + 5% DEG in an ice bath at 0 °C. Tensile strength and toughness were improved in an ice bath at 0 °C, especially the tensile strength of the conducting polymer. In view of surface morphology either free surfaces or fracture cross-sections as shown in Figures 5 and 6, there are some differences. For example, there are less grooves in Figure 5a than in Figure 6a. This means that there is a rather stronger aggregation structure in Figure 6a than in Figure 5a, and that there is more roughness in Figure 6b than in Figure 5b. Therefore, the mechanical properties and microstructure as shown in Figure 6 are better than those in Figure 5, where the tensile strength is about 60.30 MPa and the elongation about 6.38% as shown in Figure 6, and the tensile strength is about 30.10 MPa and the elongation is about 4.47% as shown in Figure 5. The relative increments of tensile strength and elongation under different synthesis conditions reach 67.04% and 42.73%, respectively.
In order to enhance the strength of film, the focus of most studies is the application of methods of doping ions, fibers and particles into the matrix. These studies have been greatly promoted in the recent several decades. For example, Tjong  investigated how to reinforce the mechanical properties of polymers with lower volume fractions of nanocomposites, carbon nanotubes. Tjong described that the mechanical properties with nanocomposites depended greatly on the chemistry of the polymer matrices, nature of nanofillers, and the way in which they are prepared. The uniform dispersion of nanofillers in the polymer matrices is a general prerequisite for achieving the desired mechanical and physical characteristics. He also described in detail current developments on the processing, structure, and mechanical properties of polymer nanocomposites reinforced with layered silicates, ceramic nanoparticles and carbon nanotubes, respectively. In addition, Somanathan et al.  and Andreatta et al.  suggested that both the conductivity and tensile strength of a polymer were strongly affected by both inter- and intra-chain interactions. However, after comparison of the conductivity results of P3c6T with P36T, Moulton  expressed that the effect produced by drawing is very pronounced in the case of P3c6T. The mechanical and morphological aspects of P3c6T at different temperatures clearly showed the brittle-ductile transition that taken place in the material and the film formed into a compact structure. In addition, Wang et al.  analyzed the effects of the addition of amounts of montmorillonte with different doping nanocomposite particles on the mechanical properties of polyimide nanocomposite films based on the cross-section fracture analysis of the film. The incorporation of montmorillonite nanolayers into the polymer matrix can results in an evident enhancement in the Young’s modulus, but the elongation decreases. The Young’s modulus increase is almost solely attributed to the reinforcing effect of the dispersed montmorillonite nanolayers. The analysis of fracture morphology also showed also that the incorporation of 1 wt% montmorillonite content produced the best tensile behavior. Therefore, the improvement of mechanical properties could be ascribed to the uniform exfoliation and dispersion of the nanolayers and enhancement of interfacial strength which depended on the size of the composite sheet between the montmorillonite content and matrix phases. At the same time, Pettarin et al.  reported the relation of morphology and mechanical properties of polyethlene/(organo-montmorilloite) composites modified with ethylene/methacrylic acid copolymer. All polyethlene/(organo-montmorilloite) composite morphologies were examined using X-ray diffraction (XRD), scanning electron microscopy (SEM) and transmission electron microscopy (TEM) technologies. The mechanical properties were evaluated under static conditions. A slight reinforcement was achieved only when the organoclay montmorillonite (OMMT) was added to polyethylene (PE). The addition of a small amount of ethylene methacrylic acid copolymer (EMAA) to the composite films could result in improvements of the level of exfoliation [81,82], but there is no positive effect on exfoliation when EMAA was added to the composite morphology. XRD patterns of PE/OMMT/EMAA exhibited a peak with lower d-spacing than OMMT. Uniaxial tensile tests and heat distortion temperature (HDT) followed the same tendency: as EMMA was added to the system, the properties of composites deteriorated approaching the level of the pristine matrix. Also, SEM micrographs provided some evidence of OMMT encapsulation by EMAA. Jordan et al.  have reviewed the recent work polymer matrix nanocomposites. In their review, they provided an overview of the processing technology and trends in the mechanical behavior and morphology of nanocomposites. In general, the mechanical properties of polymer nanocomposites are superior to those of the pure polymer matrix or composites with larger sized inclusions or other defects such as voids. The effects of the nanoparticles are dependent on many variables parameters, especially upon the relative crystalline or amorphous nature of the polymer matrix, and the interaction between the filler and matrix. As for the effects of micro-inclusions or micro-voids on the mechanical properties of materials, Wang et al. [84–90] have provided a significant amount of SEM in situ observation results. Although the results referred to metals with micro-inclusions or fatigue problems, the investigation method and effects of the mechanism of inclusion on the mechanical properties of materials are still applicable to the characterization of polymers filled with other materials. These results indicated mainly that the mechanical properties, including to the fatigue properties, are not only dependent on the added amount of particles, critical size, shape, types of particle and the ratio of hardness level between particle and matrix, but also on the obliquity between the longest axis of particle and applied loading direction, especially for a rectangular hard inclusion or doping of hard particles. This effect is most dangerous when the angle between the longest axis of the particles and applied loading direction is about 90°. This is because micro-cracks then occur easily at the interface between particle and matrix, and the crack easily propagates along from the interface to the matrix, even if the adherence strength between the particle and matrix is great enough.
Kaynak et al.  demonstrated the changes to the mechanical and electrical properties of polypyrrole films with concentrated dopants and oxidative aging. They described the process of mechanical and electrical properties loss for up to 12 months of aging in air at room temperature. The results indicated that the tensile strength of films highly doped with p-toluenesulphonate was lower than that of lightly doped ones. The difference was attributed to the presence of stress concentrations on the nodular surfaces of the films with high concentrated dopant. Highly doped films were electrically more stable, with a lower rate of loss of conductivity with time, compared to lightly doped ones. The conductivity of the latter initially decreased at a different rate from that observed after a prolonged time, exhibiting two distinct aging behavior regions. In contrast, highly doped PPy films followed first-order kinetics with a very small loss of conductivity over the aging period. The conductivity decline rate was dependent on aging time, dopant type, and concentration, resulting in a complex conductivity decay mechanism.
As another mechanical property parameter of conducting polymer film/coatings, the elastic modulus of the conduction polymer is very important in its applications, such as microelectronics, energy storage, electrocatalytic systems, photovoltaic devices, electrochromic devices, etc. In the case of conductive polymers potentially useful in electrical applications, the elastic modulus is a key mechanical parameter in the above mentioned applications. However the process of accurately measuring the mechanical parameters of a polymer is rather difficult. This is because how its constitutive stress-strain equation is obtained depends directly on its reliability, but the deformation of high flexibility films cannot be measured by the general methods. Wang et al. [25,35,39,78,92,93] used an electronic speckle pattern interferometry (ESPI) technology [94,95] and the digital image correlation (DIC) method [96,97], respectively, for measuring the deformation of highly flexible specimens of conducting polymer. Figure 7 shows a typical electronic speckle pattern interferometry system for measuring the in-plane displacement of a free surface by electronic speckle pattern interferometry (ESPI) technology. The laser beam is reflected from a mirror, and then split into two beams with a splitter. One is expanded by a spatial filtering setup and is used as the object beam illuminating a diffuse object; and the other is reflected from a mirror and is expanded by another spatial filtering setup, forming the reference beam. A zoom system is used to focus the object onto the sensor of a CCD camera. Thus, each sensor receives the coherent superposition of the object beam and the reference beam. The interference intensity distribution of a subtractive speckle correlation fringe pattern can be expressed by Equation (11):
A rectanglular sample of Pth film usually undergoes considerable shape changes as it is subjected to L even a small external force. The change takes place mainly lengthwise because of the ratio , where L is the length of the sample, and W is the width. The micro-change in the y direction, which is subjected by the applied loading direction, can be detected by the ESPI system. About 12 fringe patterns of the Pth beam under different the applied loading levels were recorded. Two typical fringe patterns are illustrated in Figure 8. It is clear that the significant fringe patterns are displayed. According to the number of the fringe patterns, the amount of deformations of Pth film in the applied loading direction can be calculated easily by the above equations. The engineering stress-strain curves of Pth films of different thicknesses are shown in Figure 9.
Following the linear elastic deformation, plastic flow commences at a stress approximately equal to the yield stress, σ 0.2, defined as the stress corresponding to a strain of 0.002. During plastic deformation, an evident strain-hardening is observed, that is, the stress required increases with the development of plastic strain. The maximum strength of a conducting polymer film is approximate to that of aluminum thin film when the thickness is smaller than about 10 μm. It can be seen from Figure 9 that the strengths of Pth films varied with the thickness. That is, the tensile strength increases as the Pth film thickness decreases. The strengths of films are especially sensitive to the film thickness when the latter is less than about 10 μm. However, the strengths of films approach a constant value when the film thickness is more than about 20 μm. Especially, an evident change has been observed in σ0.2 when the thickness is more than about 20 μm. A film with the thickness of 4 μm possesses the highest strength. This is because the thin film/coating early stage of deposited nucleation process is strongly influenced by substrate so that the thickness forms a correspondingly compact structure, but with the increasing of thickness, this influence becomes smaller and smaller. Therefore, the defects and cracks easily occur at the relative thicker film/coating layer. This insufficiency of defects and cracks in film/coating layer can be improved by the appropriate synthesis methods [18,24,45,51,67,73–82].
The elastic (Young’s) modulus also varies pronouncedly with the thickness of film which is less than about 10 μm, but it approaches a constant when the thickness is more than about 10 μm. The relationship between elastic modulus and the thickness is shown in Figure 10. The main reason of this phenomenon seems to associate with the growth mechanism and its influence factors of the Pth films. When the thickness is less than 10 μm, the Pth mainly grows up in a stable manner on the base layer. But with increasing thickness, more and more agglomerated molecule groups are formed away from the base layer. Therefore, many micro-defects such as micro-cracks and micro-voids easily exist in the adjacent surface layer. At the same time, the binding energy of these agglomerated molecule groups becomes smaller and smaller because of the electrochemical influence or the influence of the metal substrate. Therefore, the microstructures of Pth films will change as the thickness increases. A thin film with the thickness of about 4 μm generally has a perfect microstructure with few defects.
In most applications, the film/coating-substrate structure appears in the components and devices. The estimation of the mechanical properties of the film/coating-substrate system has been investigated over the last several decades [41,98–102]. These mechanical properties of the film/coating-substrate structure refer to the many influencing factors such as internal stress, adherence force and the elastic properties of the thin film. Using either the static bending [41,98,100] or the vibrating reed technique [99,101] considering the integrated structure, the Young’s modulus Ef of film-substrate structure can be estimated by the vibrating method:
Though the determined curvature (or bending) method can estimate the stress in film/coating layers, the internal stress experimentally measured by the curvature of a sample has even more errors. Stoney’s linear formula is most commonly used, but, it may be inadequate owing to nonlinear effects that should not be ignored. For example, taking into account the case of a rectangular plate, the role of the different parameters controlling the geometrical nonlinear effects are examined, and then the one-to-one mapping that exists between the degree of nonlinearity and the parameter b2 / d s R (b,ds, R are the sample’s width, thickness and bending curvature, respectively) can be established . In estimations of the internal stress of film/coating through the curvature method, important nonlinear effects may affect the validity of Stoney’s formulae. Townsend et al.  and Fawcett et al.  modified Stoney’s formula and measured the Young’s modulus of thin films on thick substrates by a novel method. Stoney’s formula accepts that curvature may cause some errors, especially when the substrate is difficult to inflect. Therefore, this effect of flexural and torsional modes must be corrected by stress measurements for accurate determination of the thin film/coating substrate structure . Besides, with narrow cantilevers the frequency is very sensitive to curvature . The ratio of frequencies of the torsional and flexural modes mainly depends on the curvature. Thermal expansion and residual stress are two important mechanical parameters of conducting polymer coating-substrate structure or of microelectronics and microelectromechanical systems (MEMS). There are several problems in that the mismatch of thermal expansion between the thin film/coating and the substrate may lead to residual stresses in thin film or coating layer reported in literature . The residual stress will cause damage or deformation mismatch in thin film/coating- substrate structures . Fang et al.  found that the coefficient of thermal expansion (CTE) of thin films varied with the changing of the thickness on the micro scale. These results indicated that thickness of thin film/coating influenced not only the strength and Young’s modulus but also the CTE of thin film/coating layer. However, the thickness of thin film or coating layer is too thin, causing difficulties in determining these mechanical parameters by a general method. The novel methods for measuring mechanical properties are necessary, such as the bilayer microcantilever technique, the scratch and SEM in situ observation methods, etc.
5. Micro Cracking Behavior of Macromolecular Coating-Substrate Structure under Thermal-Mechanical Loadings
To estimate the thermal contribution of the film/coating-substrate structure in the equivalent stress formula, it should know an effective behavior of the different thermal expansion coefficient on the crack initiation or mechanical properties worsen. The cracking tests under thermal-mechanical loading were carried out from 30 °C to 100 °C. The applied thermal loading ratio is a 2.67 °C/min then holding 1 hour in the vacuum chamber of SEM using a specially designed servo-hydraulic testing system. The temperature control is by a thermoelectric couple and it has a precision of about ±1 °C. Given the fixed tension stress is 73 MPa for AISI 304 stainless steel substrate during the applied thermal loading, the relationship between the displacement increment Δℓ of free surface film/coating layer, temperature and linear thermal expansion coefficient can be defined as follows when the interface strain mismatch between the film/coating and substrate can be ignored:
Figure 11 shows the crack initiation development of a film/coating-substrate structure based on SEM in situ observation under different temperatures and holding times. To observe the crack initiation or propagation behavior, the special zone on free surface of polythiophene film/coating was chosen as a fixed observation zone, as shown in Figure 11a. Comparing the images in Figures 11a and 11b, it was seen that the effect of thermal-mechanical loading on the crack initiation near the interface of a molecular grain on the free film/coating surface is very obvious. It can be seen that the crack open displacement (COD) of 2.80 μm exists near the interface of the agglomerative molecular during the applied and held temperatures. At this moment, the estimated thermal stress reaches about 199.50 MPa, based on Equation (17). It can be deduced that this stress value is big enough to laniate the film compared with the failure strength as shown in Figure 9. Therefore, the estimated value by the Equation (17) is not reliable. However, if we assume there is a consistent deformation of both the film and substrate, it is possible to calculate the stress in the film layer via the elastic strain and Young’s modulus of substrate. The elastic strain is about 0.13% when the strength of the substrate is about 199.50 MPa. If the strain of the free surface of the film/coating layer is also about 0.13%, the interior stress in the film/coating layer at the strain of 0.13% is approximately equal to about 6–10 MPa, according to the stress-strain curves relation as shown in Figure 9. Therefore, the difference of stress values based on the estimation methods refers to rather complicated scientific issues, which should be studied further. However, the interface COD can reflect the fact that the maximum displacement trend is about 90° tilted to the applied mechanical loading direction, and another is that the crack occurs first at the maximum agglomerative molecular gain (its diameter is about 13.00 μm) in the view-scale as shown in Figure 11b. Figure 11c shows the crack propagation behavior, which is along a direction tilted about 90° with respect to the applied mechanical loading direction and the interface crack does not occur in another direction (the parallel applied mechanical loading direction) even if the thermal stress can be defined as 2-D or 3-D stress states. With an increased holding time at 100 °C, the COD increases quickly from 2.80 μm to 3.12 μm. It should noted that the size and shape (about 13.00 μm) of this molecular gain is almost unchanged compared with Figures 11a and 11c. The driving force for an interface crack at various depths a / d f (a is the crack depth, d f is the diameter of this grain) has been described by Hutchinson and Suo . These results indicated that the dimensionless stress intensity factor, where K is a stress intensity factor), depends only on the relative crack depth, a / d f, and Dundurs’ parameters , α and β as follows:
In addition, another feature was found during the tests, which is that the opened amount of the microcrack did not vary with an increase of the thermal and mechanical coupled loadings because the coating and substrate had been damaged at other points, such as the sample boundary. Therefore, other failure models may occur in the conducting polythiophene coating-substrate structure. Subsequently, this means that it is possible to improve the cracking resistance of conducting polythiophene coating when the agglomerative grain of the polymer is fine and small enough. Another defect was found in the vicinal fine regions and it is highly dependent on the processing conditions, not only the conductivity but also the thermal-mechanical properties of the conducting polythiophene coating-substrate structure .
The SEM in situ results showed that the characteristics of the crack initiation and propagation of conducting polythiophene coating appear to be complex. The failure models of the coating-substrate structure under thermal-mechanical loadings mainly represent that the thermal loading affects on the interface microcrack initiation and slight propagation in the vicinal greater agglomerative grain of polymer, and the macro-crack can be continuously formed at the interfaces of the agglomerated polymer grains in the coating layer.
6. Evaluation Method of Interface Adhesion Strength and Failure Stress of Coating-Substrate Structure
Most estimation methods of stress in film/coating-substrate structure were based on the Stoney formula  and its ramifications, which were based on the curvature radius R. This parameter R (R = (ℓ2 +δ2) / 2δ) can also be indirectly measured by δ displacement parameter in SEM in situ bending tests. In addition, Asaro  and Wang et al.  independently reported how to estimate failure stress in thin films. For example, it is shown that when the free surface of thin film is unstable or thin enough the following relationship exists:
Wang et al. [35–39] recently reported the cracking behaviors of thin Cu film-substrate structures. They discovered that unstable wave motion occurred in the surface film/coating layer and they obtained the relationship between the bending loadings and curvature displacements of thin film-substrate structures based on the SEM in situ observation tests. Therefore, according to the measurement parameters, the failure stress in thin films can be estimated based on different methods. For example, when the thin film thickness is 1 μm and the parameters of λc=20μm,G =46GPa, γ =1.83J / m2 ,νf =0.364 are substituted into Equation (19), the failure stress can be estimated. All estimation data of the failure stresses are listed in Table 2.
Therefore, Equation (19) provides a method of estimating failure stress for film-substrate structures which are thin enough, especially when the thickness of the thin film is less than 1 μm. The threshold value of estimating failure stress is closely related to the fracture process of the thin film-substrate structure or the cracking behavior of the thin film. Based on the fracture process of the thin film-substrate structure, the critical failure stress may be quantitatively estimated by the nano scratch and SEM in situ observation tests. It causes the more errors that other estimation methods of critical failure stress based on the curvature radius of the thin film-substrate structure or beam. That is, the effects of free surface stability, composite stress state and interfacial strength on the cracking behavior of thin film-substrate structure have to be considered when the thin film is thin enough. At the same time, these results are also suit for the polymer thin film/coating-substrate structures.
Understanding the mechanical behaviors of thin film/coating-substrate constructs is indispensable for the kinds of practical applications of thin film/coatings used in industry. The investigations on the mechanical properties, the cracking behavior and dependable influence factors of polymer film/coating substrate structures play a key role for their design and applications. These properties of polymers are strongly dependent on their microstructure, synthesis method and doping processing. In this work, there are not only the presently selected views of the mechanics analysis from the abundant literature, but also included the authors’ recent works. These results indicate that the following conclusions can be made:
The island by island nature of the electrochemical deposition behavior of conducting polymer has been validated by surface morphological analysis of different deposited states. Therefore, with the increase of film/coating thickness, these micro defects in the film/coating layer can directly affect the mechanical properties of conducting polymers, especially the Young’s modulus parameter. This is because the micro defects near the surface layer could not bear the applied loading. These cross-section areas will influence the estimated reliability of the nominal stress. In addition, these micro defects easily cause the stress concentration to occur early fracture. To obtain a conducting polymer film/coating without micro defects, the critical or effective thickness of conducting polymer film/coating layer is not than 5 μm closed to the substrate based on the three-electrode system when the total film thickness is about 65 μm.
By doping small amounts of nano particles, filler or ionic particles into the matrix, the mechanical properties of a polymer can be improved. One of the reasons is that the microstructure varies with the doping amount, but there is an optimal result. The high strength of thin film/coating on substrates can be attributed partly to the fine microstructures found in the conducting polymers. Further work is required to understand in more detail how to control the cracking behavior in small dimensions and how to improve the particle/filler size and texture.
The free surface cracking behavior of conducting polymer film/coating, taking into account the factors of temperature and holding time, can describe how cracks occur easily at the interface of greater agglomerated grains based on in situ SEM observations. The cracks’ main propagation direction is about 90° tilted to the mechanical loading direction. However, the increment of crack open displacement is about from 2.80 to 3.12 μm under a holding time 35 min at 100 °C. The effective difference of thermal distensibility between polymer and metal substrate on the crack proportion is still not obvious.
As the film/coating-substrate structure, the interested problem in engineering applications is how to estimate the failure model and critical failure stress in the film/coating, especially for thin coating layers. In general, the estimation methods of failure stress in coating layers are based on the Stoney formula and its ramifications. However, with the increasing of hardness difference of substrate and film/coating, the effective detection of curvature radius R becomes more and more difficult. In addition, as there is the stress gradient in a bent curvature, the estimation method of critical failure stress causes more errors based on the curvature radius. Therefore, the estimation method of failure stress for thin film/coating-substrate structures should be expressed combining the SEM in situ observation technology and scratch testing methods.
Investigations on the relationship between microstructure and mechanical of conducting polymer are insufficient up to the present, especially the studies on the relationship between the microstructure’s formation mechanism and cracking behavior. These behaviors can be described quantitatively to a certain extent.
The work was supported by the National Natural Science Founding of China (Grant No. 1077209, No. 50575228) and National Basic research Program of China through Grant Nos. 2004CB619304 and 2007CB936803.
- KorriYoussoufi, H; Garnier, F; Srivastava, P; Godilloy, P; Yassar, A. Toward bioelectronics: Specific DNA recognition based on an oligonucleotide-functionalized polypyrrole. J. Am. Chem. Soc 1997, 119, 7388–7389. [Google Scholar]
- Peng, H; Zhang, LJ; Soeller, C; Travas-Sejdic, J. Conducting polymers for electrochemical DNA sensing. Biomaterials 2009, 30, 2132–2148. [Google Scholar]
- Teles, FRR; Fonseca, LR. Applications of polymers for biomolecule immobilization in electrochemical biosensors. Mater. Sci. Eng. C-Biomimetic Supramol. Syst 2008, 28, 1530–1543. [Google Scholar]
- Cosnier, S. Recent advances in biological sensors based on electrogenerated polymers: A review. Anal. Lett 2007, 40, 1260–1279. [Google Scholar]
- Ramanavicius, A; Ramanaviciene, A; Malinauskas, A. Electrochemical sensors based on conducting polymer- polypyrrole. Electrochim. Acta 2006, 51, 6025–6037. [Google Scholar]
- Morita, M; Hashida, I. Enhanced electrochromic stability of polyaniline in polyaniline-matrix polymer composite films in aprotic medium. Macromol. Chem. Phys 1992, 193, 921–936. [Google Scholar]
- Chiu, HT; Lin, JS; Shiau, JN. The influence of dopant permeability on electrochromic performance of polypyrrole films. J. Appl. Electrochem 1992, 22, 522–527. [Google Scholar]
- De la Plaza, MA; Izquierdo, MC; de la Blanca, ES; Fuentes, IH. Electrosynthesis, electrochemical and structure of poly[bis(phenoxyphosphazene)]-poypyrrole doped composite film. Synth. Met 1999, 106, 121–127. [Google Scholar]
- Hay, JN; Khan, A. Review environmentally friendly coatings using carbon dioxide as the carrier medium. J. Mater. Sci 2002, 37, 4841–4850. [Google Scholar]
- Chiang, CK; Park, YW; Heeger, AJ; Shirakawa, H; Louis, EJ; MarDiarmid, AG. Electrical-conductivity in doped polyacetylen. Phys. Rev. Lett 1977, 39, 1098–1101. [Google Scholar]
- Diaz, AF; Kanazawa, KK; Gardini, GP. Electrochemical polymerization of pyrrole. J. Chem. Soc.-Chem. Comm 1979, 14, 635–636. [Google Scholar]
- Sato, M; Tanaka, S; Kaeriyama, K. Soluble conducting polythiophenes. J Chem Soc-Chem Comm 1986, 11, 873–873. [Google Scholar]
- Jen, KY; Miller, GG; Elsenbaumer, RL. Highly conducting, soluble, and environmentally-stable poly(3-alkylthiophenes). J Chem Soc Chem Comm 1986, 17, 1346–1347. [Google Scholar]
- Wei, Y; Focke, WW; Wnek, GF; Ray, A; MacDiarmid, AG. Synthesis and electrochemistry of alkyl ring-substituted polyanilines. J Phys Chem 1989, 93, 495–499. [Google Scholar]
- Roth, S. Conducting polymers and intercalation. Synth Met 1990, 34, 617–622. [Google Scholar]
- Kanatzidis, MG. Conductive polymers. Chem. Eng. News 1990, 68, 63. [Google Scholar]
- Roth, S; Filzmoser, M. Conducting polymers - 13 years of polyacetylene doping. Adv Mater 1990, 2, 356–360. [Google Scholar]
- Waltman, RJ; Bargon, J. Electrically conducting polymers—a review of the electropolymerization reaction, of the effects of chemical-structure on polymer film properties, and of applications towards technology. Can J Chem 1986, 64, 76–95. [Google Scholar]
- Diaz, AF; Lacroix, JC. Synthesis of electroactive conductive polymer-films—electrooxidation of heteroaromatic-compounds. New J Chem 1988, 12, 171–180. [Google Scholar]
- Adamcova, Z; Dempirova, L. Film-forming electropolymerization. Prog Org Coat 1989, 16, 295–320. [Google Scholar]
- Meerholz, K; Heinze, J. Electrochemical solid-state studies on oligomeric para-phenylenes as model compounds for conductive polymers. Angew Chem Int Ed 1990, 29, 692–695. [Google Scholar]
- Baker, GL. Progress toward processable, environmentally stable conducting polymers. Adv Chem Ser 1988, 218, 271–296. [Google Scholar]
- Patel, AO; Heeger, AJ; Wudl, F. Optical-properties of conducting polymers. Chem Rev 1988, 88, 183–200. [Google Scholar]
- Wang, XS; Xu, JK; Shi, GQ; Lu, X. Microstructure-mechanical properties relationship in conducting polypyrrole films. J Mater Sci 2002, 37, 5171–5176. [Google Scholar]
- Wang, XS; Feng, XQ. Effects of thickness on mechanical properties of conducting polythiophene films. J Mater Sci Lett 2002, 21, 715–717. [Google Scholar]
- Tourillon, G. Handbook of Conducting Polymers; Skotheim, TA, Dekker, Marcel, Eds.; CRC Press: New York, NY, USA, 1986; p. 294. [Google Scholar]
- Roncali, J. Conjugated poly(thiophenes)-synthesis, functionalization, and applications. Chem Rev 1992, 92, 711–738. [Google Scholar]
- Chan, HSO; Ng, SC. Synthesis characterization and applications of thiophene-based function polymers. Prog Polym Sci 1998, 23, 1167–1231. [Google Scholar]
- Francis, LF; McCormick, AV; Vaessen, DM; Payne, JA. Development and measurement of stress in polymer coatings. J Mater Sci 2002, 37, 4897–4911. [Google Scholar]
- Koufopoulos, T; Theocaris, PS. Shrinkage stresses in 2-phase materials. J. Compos. Mater 1960, 3, 308–320. [Google Scholar]
- Croll, SG. Adhesion loss due to internal strain. J Coat TechnolRes 1980, 52, 35–43. [Google Scholar]
- Hoffman, RW. Stress distributions and thin-film mechanical-properties. Surf Interface Anal 1981, 3, 62–66. [Google Scholar]
- Suhir, E. Calculated stresses in dual coated optical fibers. Polym Eng Sci 1990, 30, 108–117. [Google Scholar]
- Wang, XS; Deng, YH; Li, YQ. An experimental investigation of failure behaviors of conducting polythiophene coating films. J Mater Sci 2002, 37, 4743–4748. [Google Scholar]
- Huang, JG; Wang, XS; Meng, XK. SEM in situ study on deformation under three-point bending loading in Cu and Cu/Ni films. Mater Trans 2007, 48, 2795–2798. [Google Scholar]
- Li, Y; Wang, XS; Meng, XK. Buckling behavior of metal film/substrate structure under pure bending. Appl. Phys. Lett 2008, 92, 131902. [Google Scholar]
- Wang, XS; Yan, CK; Li, Y; Xue, YB; Meng, XK; Wu, BS. SEM in situ study on failure of nanocrystal metallic thin films and substrate structure under three point bending. Int J Fract 2008, 151, 269–279. [Google Scholar]
- Li, Y; Wang, XS; Fan, QS. Effects of elastic anisotropic on the surface stability of the film/substrate system. Int J Eng Sci 2008, 46, 1325–1333. [Google Scholar]
- Wang, XS; Li, Y; Meng, XK. An estimation method on failure stress of micro thickness Cu film-substrate structure. Sci China Ser E Technol Sci 2009, 52, 2210–2215. [Google Scholar]
- Baumert, B; Stratmann, M; Rohwerder, M. The deformation response of ultra-thin polymer films on steel sheet in a tensile straining test: The role of slip bands emerging at the polymer/metal interface. Zeitschrift Metallkunde 2004, 95, 447–455. [Google Scholar]
- Stoney, GG. Tension of electro-deposited films. Proc R Soc Lond 1909, 82, 172–175. [Google Scholar]
- Hoffman, RW. Physics of Non-Metallic Thin Films; Dupuy, CHS, Chachard, A, Eds.; Plenum: New York, NY, USA, 1976; p. 273. [Google Scholar]
- Corcoran, EM. Determining stresses in organic coatings using plate beam deflection. J Paint Technol 1969, 41, 635–640. [Google Scholar]
- Chiu, CC. Determination of the elastic-modulus and residual-stresses in ceramic coatings using a strain-gauge. J Am Ceram Soc 1990, 73, 1999–2005. [Google Scholar]
- Benabdi, M; Roche, AA. Mechanical properties of thin and thick coatings applied to various substrates .1. An elastic analysis of residual stresses within coating materials. J Adh Sci Tech 1997, 11, 281–299. [Google Scholar]
- Campbell, DS. Handbook of Thin Film Technology; Maissel, LI, Glang, R, Eds.; McGraw-Hill: New York, NY, USA, 1969; p. 12. [Google Scholar]
- Ohring, M. The Materials Science of Thin Films; Academic Press: New York, NY, USA, 1992; pp. 1–20. [Google Scholar]
- Qu, LT; Shi, GQ. Electrochemical synthesis of novel polypyrrole microstructures. Chem Commun 2003, 2, 206–207. [Google Scholar]
- Qu, LT; Shi, GQ; Chen, F; Zhang, JX. Electrochemical growth of polypyrrole microcontainers. Macromolecules 2003, 36, 1063–1067. [Google Scholar]
- Hoshikawa, T; Yamada, M; Kikuchi, R; Eguchi, K. Impedance analysis for dye-sensitized solar cells with a three-electrode system. J Electroanal Chem 2005, 577, 339–348. [Google Scholar]
- Ferreira, CA; Aeiyach, S; Aaron, JJ; Lacaze, PC. Electrosynthesis of strongly adherent polypyrrole coatings on iron and mild steel in aqueous media. Electrochim Acta 1996, 41, 1801–1809. [Google Scholar]
- Asavapiriyanont, S; Chandler, GK; Gunawardena, GA; Pletcher, D. The electrodeposition of polypyrrole films from aqueous-solutions. J Electroanal Chem 1984, 177, 229–244. [Google Scholar]
- Hillman, AR; Mallen, EF. Nucleation and growth of polythiophene films on gold electrodes. J Electroanal Chem 1987, 220, 351–367. [Google Scholar]
- Hamnett, A; Hillman, AR. An ellipsometric study of the nucleation and growth of polythiophene films. J Electrochem Soc 1988, 135, 2517–2524. [Google Scholar]
- Li, FB; Albery, WJ. A novel mechanism of electrochemical deposition of conducting polymers - 2-dimensional layer-by-layer nucleation and growth observed for poly(thiophene-3-acetic acid). Electrochem Acta 1992, 37, 393–401. [Google Scholar]
- Li, FB; Albery, WJ. Electrochemical deposition of a conducting polymer, poly(thiophene-3-acetic acid) - the 1st observation of individual events of polymer nucleation and 2-dimensional layer-by-layer growth. Langmuir 1992, 8, 1645–1653. [Google Scholar]
- Kontturi, K; Pohiakallio, M; Sundholm, G; Vieil, E. Potential controlled electrosynthesis of poly(thiophene-3-methanol): Application of the two-dimensional layer-by-layer nucleation and growth model. J Electroanal Chem 1995, 384, 67–75. [Google Scholar]
- Rohwerder, M; Michalik, A. The conducting polymer for corrosion protection-what makes the difference between failure and success. Electrochim Acta 2007, 53, 1300–1313. [Google Scholar]
- Freitas, JM; Duarte, ML; Darbre, T; Abrantes, LM. Electrochemical synthesis of a novel conducting polymer: The poly [(3-pyrrolyl)-octanoic acid. Synth Meth 2005, 155, 549–554. [Google Scholar]
- Akundy, GS; Rajagopalan, R; Iroh, JO. Electrochemical deposition of polyaniline-polypyrrole composite coatings on aluminum. J Appl Polym Sci 2002, 83, 1970–1977. [Google Scholar]
- Akundy, GS; Iroh, J. Polypyrrole coatings on aluminum—synthesis and characterization. Polymer 2001, 42, 9665–9669. [Google Scholar]
- Fleischmann, M; Thirsk, HR. Advances in Electrochemistry and Electrochemical Engineering; Delahary, P, Ed.; John Wiley & Sons: New York, NY, USA, 1963; p. 123. [Google Scholar]
- Harrison, JA; Thirsk, HR. Electroanalytical Chemistry; Bard, AJ, Ed.; Marcel Decker Inc: New York, NY, USA, 1971; p. 67. [Google Scholar]
- Johanson, U; Marandi, M; Tamm, T; Tamm, J. Comparative study of the behavior of anions in polypyrrole films. Electrochim Acta 2005, 50, 1523–1528. [Google Scholar]
- Yan, G; White, JR. Residual stress development in a bi-layer coating. Polym Eng Sci 1999, 39, 1856–1865. [Google Scholar]
- Wu, XQ; Wang, B. Thin Film Nucleation; Science Press: Beijing, China, 2001; pp. 7–20. [Google Scholar]
- Beck, F; Michaelis, R. Strongly adherent, smooth coatings of polypyrrole oxalate on iron. J Coat Technol Res 1992, 64, 59–67. [Google Scholar]
- Chainet, E; Billon, M. In situ study of polypyrrole morphology by STM: Effect of the doping state. J Electroanal Chem 1998, 451, 273–277. [Google Scholar]
- Zuo, JP; Wang, XS. A novel fractal characteristic method on the surface morpho; ogy of polythiophene films with self-organized nanostructure. J Phys E 2005, 28, 7–13. [Google Scholar]
- Cassugnol, C; Cavarero, M; Boudet, A; Ricard, A. Microstructure-conductivity relationship in conducting polypyrrole/epoxy composites. Polymer 1999, 40, 1139–1151. [Google Scholar]
- Lux, F. Models proposed to explain the electrical-conductivity of mixtures made of conductive and insulating materials. J Mater Sci 1993, 28, 285–301. [Google Scholar]
- Mano, V; Felisberti, MI; Matencio, T; De Paoli, MA. Thermal, mechanical and electriochemical behaviour of poly(vinyl chloride)/polypyrrole blends (PVC/PPy). Polymer 1996, 37, 5165–5170. [Google Scholar]
- Xu, JK; Wei, ZH; Du, YK; Pu, SZ. Facile electrosyntheses of high-strength and highly-conductive poly(1,12-bis(carbazolyl) dodecane) films. Mater Lett 2007, 61, 2486–2490. [Google Scholar]
- Wang, LX; Li, XG; Yang, YL. Preparation, properties and applications of polypyrroles. React Funct Polym 2001, 47, 125–139. [Google Scholar]
- Tjong, SC. Structural and mechanical properties of polymer nanocomposites. Mater Sci Eng R 2006, 53, 73–197. [Google Scholar]
- Somanathan, N; Wegner, G. Mechanical properties of conducting poly (3-cyclohexyl thiophene) films. Polymer 1996, 37, 1891–1895. [Google Scholar]
- Andreatta, A; Heeger, AJ; Smith, P. Electrically conductive polyblend fibers of polyaniline and poly-(para-phenylene terephthalamide). Polym Comm 1990, 31, 275–278. [Google Scholar]
- Moulton, J; Smith, P. Electrical and mechanical-properties of oriented poly(3-alkylthiophenes) .2. Effect of side-chain length. Polymer 1992, 33, 2340–2347. [Google Scholar]
- Wang, XS; Zhang, YH; Fu, SY; Feng, XQ. Effect of montmorillonte addition on mechanical characterizations of polyimide nanocomposite films. Acta Mech Solida Sin 2005, 18, 200–206. [Google Scholar]
- Pettarin, V; Frontini, PM; Pita Rodriguez, VJR; Dias, ML; Diaz, FV. Polyethlene/(organo-montmorilloite) composite modified with ethylene/methacrylic acid copolymert: Morphology and mechanical properties. Compos Pt A-Appl Sci Manuf 2008, 39, 1822–1828. [Google Scholar]
- Shah, RK; Krishnaswamy, RK; Takahashi, S; Paul, DR. Blown films of nanocomposites prepared from low density polyethylene and a sodium ionomer of poly(ethylrnr-co-methacrylic acid). Polymer 2006, 47, 6187–6201. [Google Scholar]
- Pacheco, EBA; Dias, ML. Reactive blending of poly(ethylene terephthalate) and ionmers: 1. The influence of processing conditions. J Polym Eng 2003, 23, 23–42. [Google Scholar]
- Jordan, J; Jacob, KI; Tannenbaum, R; Sharaf, MA; Jasiuk, I. Experimental trends in polymer nanocomposites—a review. Mater Sci Eng A 2005, 393, 1–11. [Google Scholar]
- Wang, XS; Li, YQ. Characterization of the fatigue surface microcrack growth in vicinal inclusion for powder metallurgy alloys. Acta Mech Soilida Sin 2003, 16, 327–333. [Google Scholar]
- Wang, XS; Liang, F; Zeng, YP; Xie, XS. SEM in situ observations to investigate the effects of inclusions on the low cyclic fatigue crack initiation and propagation of super strength steel. Acta Metall Sin 2005, 41, 1272–1276. [Google Scholar]
- Wang, XS; Zhang, LN; Xie, XS. An experimental investigation of the fatigue microcrack initiation and growth in surface inclusion for P/M Rene95 alloy. J Univ Sci Technol Beijing 2006, 13, 244–249. [Google Scholar]
- Zeng, YP; Fan, HM; Wang, XS; Xie, XS. Study on micro-mechanism of crack initiation and propagation induced by inclusion in ultra-high strength steel. Key Eng Mater 2007, 353–358, 1185–1190. [Google Scholar]
- Zhou, S; Murakami, Y; Beretta, S; Fukushima, Y. Experimental investigation on statistics of extremes for three-dimensional distribution of non-metallic inclusions. Mater Sci Technol 2002, 18, 1535–1543. [Google Scholar]
- Murakami, Y; Endo, M. Effects of defects, inclusions and inhomogeneities on fatigue-strength. Int J Fatigue 1994, 16, 163–182. [Google Scholar]
- Murakami, Y; Endo, M. Quantitative-evaluation of fatigue-strength of metals containing various small defects or cracks. Eng Frac Mech 1983, 17, 1–15. [Google Scholar]
- Kaynak, A; Rintoul, L; George, GA. Change of mechanical and electrical properties of polypyrrole films with dopant concentration and oxidative aging. Mater Res Bull 2000, 35, 813–824. [Google Scholar]
- Wang, XS; Zhang, JX; Zhu, SQ; Shi, GQ. Deformation measurement of conducting polythiophene thin films by an electronic speckle pattern interferometric method. Acta Mech Solida Sin 2002, 15, 30–35. [Google Scholar]
- Tang, HP; Wang, XS; Zhao, RQ; Li, Y. Investigation on thermo-mechanical behaviors of artificial muscles films. J Mater Sci 2008, 43, 3733–3737. [Google Scholar]
- Joenathan, C; Franze, B; Haible, P; Tiziani, HJ. Novel temporal fourier transform speckle pattern shearing interferometer. Opt Eng 1998, 37, 1790–1795. [Google Scholar]
- Huntley, JM. Random phase measurement errors in digital speckle pattern interferometry. Opt Lasers Eng 1997, 26, 131–150. [Google Scholar]
- Huang, PS; Jin, F; Chiang, FP. Quantitative evaluation of corrosion by a digital fringe projection technique. Opt Lasers Eng 1999, 31, 371–380. [Google Scholar]
- Yang, GB; Wu, K. Principles and research of a high accuracy digital image correlation measurement system. Opt. Eng 2007, 46, 051006. [Google Scholar]
- Djordjevich, A. Alternative to strain measurement. Opt Eng 2003, 42, 1888–1892. [Google Scholar]
- Harms, U; Kempen, L; Neuhäuser, H. Influence of stress in thin film modulus measurements by the vibrating reed technique. Thin Solid Films 1998, 323, 153–157. [Google Scholar]
- Mezin, A. Coating internal stress measurement through the curvature method: A geometry-based criterion delimiting the relevance of Stoney’s formula. Surf Coat Technol 2006, 200, 5259–5267. [Google Scholar]
- Mizubayashi, H; Yoshihara, Y; Okuda, S. The elasticity measurements of aluminum nm-films. Phys Stat Sol A Appl Res 1992, 129, 475–481. [Google Scholar]
- Nix, WD. Mechanical properties of thin films. Metall Trans A Phys Metall Mater Sci 1989, 20, 2217–2245. [Google Scholar]
- Townsend, PH; Barnett, DM; Brunner, TA. Elastic relationships in layered composite media with approximation for the case of thin films on a thick substrate. J Appl Phys 1987, 62, 4438–4444. [Google Scholar]
- Fawcett, N. A novel method for the measurement of Young’s modulus for thick-film resistor material by flexural testing of coated beams. Meas Sci Technol 1998, 9, 2023–2026. [Google Scholar]
- Fang, W; Wickert, JA. Determining mean and gradient residual stress in thin films using micromachined cantilevers. J Micromech Microeng 1996, 6, 301–309. [Google Scholar]
- Fang, W; Lo, CY. On the thermal expansion coefficients of thin films. Sens Act 2000, 84, 310–314. [Google Scholar]
- Hutchinson, JW; Suo, Z. Mixed mode cracking in layered materials. Adv. Appl. Mech 1991, 29, 63–191. [Google Scholar]
- Dundurs, J. Edge-bonded dissimilar orthogonal elastic wedges. J Appl Mech 1969, 36, 650–652. [Google Scholar]
- Asaro, RJ; Tiller, WA. Interface morpohology development during stress corrosion cracking: Part I, via surface diffusion. Met Trans 1972, 3, 1789–1996. [Google Scholar]
- Allen, HG. Stiffness and strength of 2 glass-fiber reinforced cement laminates. J Comp Mater 1971, 5, 194–207. [Google Scholar]
- Allen, HG. Analysis and Design of Structural Sandwich Panels; Pergamon Press: Oxford, UK, 1969. [Google Scholar]
|Electrolyte composition and temperature||IPA+5%BFEE|
|+5%DEG at 0 °C||+5%PEG1000 at 15 °C*||+5%PEG400 at 0 °C|
|Tensile strength (MPa)||60.30||30.10||62.60|
Notes:*The experiment was performed at 15 °C because of the low solubility of PEG1000 in IPA at lower temperatures.
© 2009 by the authors; licensee Molecular Diversity Preservation International, Basel, Switzerland. This article is an open-access article distributed under the terms and conditions of the Creative Commons Attribution license (http://creativecommons.org/licenses/by/3.0/).