IJNT INTERNATIONAL JOURNAL OF NANOMATERIALS AND TECHNOLOGY Volume 2, Number 1, January-June 2011, pp. 11-15, ISSN: 0976-6138 International Science Press MWCNT/EPOXY AND CB/EPOXY NANOCOMPOSITES: PROCESSING USING TWIN SCREW EXTRUSION AND CHARACTERISATION FOR ELECTRICAL CONDUCTIVITY Jeena J.K., H.N. Narasimha Murthy*, M. Krishna, Sreejith M. 1 and K.S. Rai2 1 Department of Mechanical Engineering R.V. College of Engineering, Bangalore-560059, Karnataka, India. 2 Department of Polymer Science, Mysore University, Karnataka, India. Abstract: Research efforts are concentrated on improving the electrical conductivity of polymers and one potential method is to disperse nanofillers such as multi-walled carbon nanotubes (MWCNT), carbon nanopowder (CB) into them. This paper is aimed at processing of the nanocomposites based on a space grade Epoxy (AV138M, structural adhesive) and two nanofillers namely MWCNT and CB using co-rotating twin screw extruder. Specimens with up to 31 vol % MWCNT and 45 vol % CB were fabricated and were characterised for volume resistivity and surface resistivity as per ASTM D257 using Keithley Model 6517. Dispersion of CB and MWCNT resulted in increase in electrical conductivity of the neat resin. The volume conductivity increased by 1.0 E-10 S/cm in both the cases of 31 vol % MWCNT and 45 vol % CB loading. With the achieved values of volume conductivity the structural adhesive transitioned from totally insulative (E-14 S/cm) to dissipative range (E-4 S/cm). SEM and AFM were used to examine the dispersion of the fillers. The effect of nanofillers on the glass transition temperature was studied using DSC. Tg increased by 10o in case of MWCNT (31 vol %) and 4oC in CB (45 vol %) loading into epoxy. Keywords: Nanocomposites, Electrical Conductivity, Theoretical prediction, SEM, AFM. 1. INTRODUCTION Epoxy based polymers are widely used in applications ranging from microelectronics to aerospace. Their insulating nature can cause accumulation of electrostatic charge on their surface, causing local heating and premature degradation to the electronic components or space structures. They can be made electrically and thermally conducting by the addition of various types of nano-reinforcements. In recent years, researchers have paid much attention on exploiting the unique properties of MWCNT and CB [1-5]. The main issue in preparing nanocomposites is the uniform dispersion of fillers in the polymer matrix. Because of the high aspect ratio and van der Waals attractive force, MWCNTs form bundles or agglomerates. To overcome the difficulty of dispersion, mechanical/physical methods such as ultrasonication, high shear mixing, surfactant addition, etc have been used. However, successful dispersion remains elusive. In twin screw extrusion, the high shear stresses break up the large agglomerates and disperse CNT throughout the matrix and extensional flow prior to solidification serves to further untangle the nanofillers and align them * Corresponding Author: hnmdatta@yahoo.com in the direction of extension. CNTs are loaded up to 20 wt % in polymers using screw extruder [6, 7]. Studies show that the levels of nanofiller loading required to achieve percolation threshold (appreciable increase in electric conductivity) varies widely, ranging from less than 1 to over 14% [1, 3]. In the present work co-rotating twin screw extruder has been used to obtain high shear mixing necessary to disentangle the nanofillers and disperse them in a high viscous epoxy matrix. The main objective of this work is to process MWCNT/Epoxy and CB/Epoxy nanocomposites using twin screw extruder and characterize them for electrical conductivity, glass transition temperature and study the dispersion of nanofillers using SEM and AFM. 2. EXPERIMENTAL 2.1 Materials The epoxy matrix used in this study consists of modified Bisphenol-A based two component epoxy [Structural Adhesive-Araldite AV138M with modified Polyamine Hardener HV998, (Huntsman, Hindustan Ciba- Geigy Ltd.)]. The details of the nanofillers used in the experiments are provided in Table 1. 12 International Journal of Nanomaterials and Technology Table 1 Specification of the Nanofillers Material Description Properties Suppliers (M/s) MWCNT CVD Grown Length: 1-3 µm Nanovatec NanoGrade: AP60- Diameter: 60-90 nm technology Division 80/90 Purity > 90% of Chemapol Industries, Mumbai CB ISAF N 220 24 to 33 nm with > 95% Purity Philips Carbon Black Ltd, Kolkata 2.2 Nanocomposite Preparation For dispersing the nanofillers in high viscous epoxy matrix, a co-rotating twin-screw extruder (OMEGA 20, M/s STEER Engineering, Bangalore). The mixture of nanotube and the prepolymer was fed in to the extruder. A detailed process study was conducted to arrive at the levels of the process parameters (Speed: 150 to 200 rpm, temperature: 60 to 75 C, residence time 2 to 3 min) for extrusion. The speed was matched with that required to process materials such as grease which is as viscous as the epoxy used in this study (50,000 to 100,000 mPaS). Mixing was done in two passes to ensure good dispersion. The MWCNT/prepolymer melt was collected from the extruder; the curing agent (Hardener: HV998) was added and was allowed to cure under room temperature for one week. The same procedure was followed for preparing CB/AV138M composites. Temperature Range: 25°C to 700°C). 5 mg sample was sealed in hermetic Aluminium crucible. To obtain the curing heat flow pattern of the composite, a dynamic scanning experiment was conducted from room temperature to 150°C at 20°C per minute. 3. RESULTS AND DISCUSSION 3.1 Electrical Conductivity Results In Fig. 1 and 2, the volume and surface conductivity results are plotted as a function of the filler volume fraction. The volume conductivity increased by 1.0 E-10 S/cm in both the cases of 31 vol % MWCNT and 45 vol % CB loading. The electrical properties of the nanocomposites depends on the size and shape of the filler, matrix properties, preparation method, filler properties, dispersion of the filler within matrix and interaction between compounds, etc. 2.3 Electrical Resistivity Measurement Volume and surface resistance of the samples were measured according to ASTM D257 using Keithley 6517A model 8009 Resistivity Test Fixture. The specimens were copper plated for better contact after subjecting to humidity conditioning at 95%RH and 37°C. The corresponding resistivity is calculated using the formulae: 22.9 R σv = (1) t ρs = 53.4 R where σ v and ρ s are the volume and surface resistivities respectively, R is the corresponding resistance in ohms, 22.9 and 53.4 are constants for the apparatus. The volume and surface conductivities are calculated from the resistivity values obtained from the above equations. Fig. 1: Variation of Electrical Conductivity with MWCNT Volume Fraction 2.4 Morphological Characterization SEM (JEOL JSM 840A, Japan) and Atomic Force Microscope (Nanosurf Easy Scan, Sinsil, Switz) were used to study the dispersion of the nanofillers into epoxy. 2.5 Differential Scanning Calorimetry Glass transition temperature, Tg of the specimens were obtained using DSC (Model-Mettler DSC-823, Fig. 2: Variation of Electrical Resistivity with CB Volume Fraction In order to achieve electrical conductivity similar to MWCNT/epoxy composite, greater amount of CB (45vol %) was needed due to their spherical shape which is more difficult to make interactions between particles 13 MWCNT/Epoxy and CB/Epoxy Nanocomposites: Processing using Twin Screw Extrusion ... and particles. A high aspect ratio (330) and high conductivity [10 4Ω–1cm–1(S/cm)] of MWCNTs enable them to make better reinforcing effect in epoxy compared to CB. Systems composed of an insulating material and a conductive filler experience an insulator-conductor transition at the electrical percolation threshold. The electrical percolation threshold is the minimal volume fraction of fillers so that a continuing conductive network exists in the composite. Above this volume fraction, the electrical conductivity of the composite is relatively high. Below the electrical percolation threshold, the compound essentially behaves as an insulator. In order to determine the critical volume concentration or percolation threshold, the volume conductivity data was fitted to power law in terms of volume fraction of nanofillers. The power law is described by the equation below: σpc = A(v – vc)t (3) Where σpc the conductivity of the composite, v is the volume fraction of nanofiller in the composite, vc is the critical volume fraction (volume fraction at percolation) A and t are fitted constants. Theoretical predictions of the critical exponent, t ranges from 1.5 to 2.0 while experimental values between 1.3 and 3.1 have been reported [1, 10–12]. Table 2 Power Law Equation Parameters Parameter MWCNT/AV138M CB/AV138M vc 0.025 0.075 t 2.71 2.49 A 2.88 × 10–3 3.10 × 10–4 3.2 Morphological Characterization 3.2.1 Scanning Electron Microscopy (SEM) The SEM of the nanocomposite specimens are presented in Fig. 3. The geometric parameters of the MWCNT used in the study (length: 1 to 3 µ, dia: 60 to 90 nm) are comparable with that shown by the scanning electron micrographs Fig. 3(a). The formation of filler network of MWCNT in epoxy are observed in Fig. 3(b) (12vol % MWCNT) and 3(c) (31vol % MWCNT). The same is more evident in Fig. 3(c) which is substantiated by the increase in conductivity values corresponding to the extent of filler loading. Fig. 3(d) shows the dispersion of CB in epoxy. The presence of CB agglomerates is observed in the micrographs corresponding to 45 vol % of the filler, which is the reason for higher levels of loading of CB compared to MWCNT for achieving the required levels of conductivity. The value of percolation threshold is very sensitive to the polymer type and aspect ratio of the reinforcement. In nanocomposites the interfacial area which is inversely proportional to the filler diameter will play fundamental role for electrical contact and also for mechanical properties through load transfer between the filler and the matrix [13]. The volume conductivity data of MWCNT/epoxy and CB/epoxy has been analyzed using the power law model. The plot of log σ versus log (ν – νc) is shown as inset of Fig. 1. and 2. Theoretically the value of A should approach the conductivity of the nanofillers. The experimental values of A (Table 2) were found to be lower than the expected values for both MWCNT and CB composites. This may be due to lack of physical contact between the nanofillers caused by the contact resistance between the adjacent nanofillers, which decreases the effective conductivity of the nanofillers. Moreover, in these composites, conducting fillers are separated by the insulating polymers that act as a potential barrier, so that it is likely that the electrical conductivity is limited by hopping and/or tunneling of the charge carriers between conductive fillers [14]. Fig. 3: SEM of MWCNT/CB/epoxy Composites. (a) MWCNT, (b) 12vol% MWCNT/epoxy, (c) 31vol% MWCNT/Epoxy, (d) 45vol% CB/epoxy 3.2.2 Atomic Force Microscopy (AFM) The compositional mapping with AFM is often used for observation of multiple phases. The phase contrast is related to the inherent properties of the two phases. The brighter areas in the image can be attributed to the greater force experienced by the cantilever tip when in contact with the filler (tubular or spherical). The matrix is in amorphous state and hence appears dark in the images. Figure 4(b) shows greater proportion of brighter spots indicating greater amount of MWCNT (31vol %) compared to 12vol % in Fig. 4(a). Greater levels of 14 International Journal of Nanomaterials and Technology connectivity are observed in Fig. 4(c) and (d) which corresponds to 45vol% of CB. Fig. 4: AFM of MWCNT/CB/epoxy Composites. (a) 12vol% MWCNT/epoxy, (b) 31vol% MWCNT/epoxy, (c) 12vol% CB/epoxy, (d) 45vol% CB/epoxy 3.3 DSC Differential Scanning Calorimeter was used to determine the Tg, using the measurement of heat flow verses change in temperature. Figure 5 shows the variation of glass transition temperature with increase in nanofiller content in the composite. The Tg increased with increase in MWCNT and a maximum of 100 increase was achieved with 31vol % loading. Similar behaviour was also observed in CB/epoxy composites. But, the increase in Tg was very low with respect to CB loading i.e. only 40 for loading of 45 vol %. The addition of nanofillers enhanced the thermostability of the composites which may be due to the reduction in the mobility of the epoxy polymer chains around the nanofillers by strong interfacial interactions. Greater increase in Tg in case of MWCNT is attributed to its greater thermal stability and superior thermal properties compared to that of CB. Fig. 5: Glass Transition Temperature (Tg) Verses the Nanofiller Content 4. CONCLUSIONS Co-rotating twin screw extruder as a process for dispersing nanofillers such as MWCNT and CB into thermosets was demonstrated. The process parameters can be standardized based on the matrix and the filler systems. Dispersion of the nanofillers resulted in increase in the volume conductivity and the surface conductivity of epoxy. The volume conductivity increased by 1.0 E10 S/cm in both the cases of 31 vol % MWCNT and 45 vol % CB loading. The increase in surface conductivity was 1.0 E -9 S for the same levels of the loading of the fillers. The increase in conductivity is due to the interfacial interaction between the carbon surface and the polymer. The measured conductivity was described by a percolation-like power law equation with a percolation threshold of 0.025 and 0.075 volume fractions for MWCNT and CB respectively. DSC measurements showed increase in Tg of the nanocomposites. Predispersion of the nanofillers in suitable solvents using ultrasonication prior to screw extrusion will be explored for more effective dispersion and to achieve the resulting properties. ACKNOWLEDGEMENTS The authors are grateful for the financial support provided by the Indian Space Research Organisation (ISRO), Bangalore (Sanction No. 10/3/547 dated 10-102005, Sanction Order No 9/2/125/2005 II dated 08-032006, Principal Investigator: Dr. H N Narasimha Murthy). REFERENCES [1] Z. Ounaies, C. Park, K.E. Wise, E.J. Siochi, J.S. Harrison, “Electrical Properties of Single Wall Carbon Nanotube Reinforced Polyimide Composites”, Composite Science and Technology, 63, 1637-1646 (2003). [2] Florian H. Gojny, Malte HGW, Bodo Fiedler, Ian A.K., Wolfgang Bauhofer, Alan Windle, Karl Schulte, “Evaluation and Identification of Electrical and Thermal Conduction Mechanisms in Carbon Nanotube/epoxy Composites”, Polymer, 1-10 (2006) [3] “Analysis of Correlation between Percolation Concentration and Elongation at Break in Filled Electroconductive Epoxy- based Adhesives”, Novak I, Krupa, Chodak, European Polymer Journal, 39(3), 585-592, (8), (2003). [6] Nahass, Paul R., Friend, Hausslein, Robert W., “Conductive Silicone and Methods for Preparing Same”, 5591382, U.S. (1994). [7] Thostenson, Eric T., “Conductive Thermosets by Extrusion”, 20070176319, U.S (2007). [8] Kin-tak Lau, Mei Lu, and Kin Liao, “Improved Mechanical Properties of Coiled CNTs Reinforced Epoxy Nanocomposites”, Composites Part A: Applied Science and Manufacturing, 37, (10), 1837-1840. [9] Young Seok Song, and Jae Ryoun Youn, “Influence of 15 MWCNT/Epoxy and CB/Epoxy Nanocomposites: Processing using Twin Screw Extrusion ... Dispersion States of CNTs on Physical Properties of Epoxy Nanocomposites”, Carbon, 43(7), 1378-1385, (2005). [10] Yu-Hsuan et al, “Investigation of the Dispersion Process of SWNT / SC -15 Epoxy Resin Nanocomposites”, Elsevier, Materials Sci & Engg, A (385) 2004. List of Abbreviations and Symbols MWCNT :- Multiwalled Carbon nanotube CB :- Carbon Black sν :- Volume Resistivity ρs :- Surface Resistivity σpc [12] Weber M., Kamal M.R., “Estimation of the Volume Resistivity of Electrically Conductive Composites”, Polymer Composites, 18(6), 711-725 (1997). :- Volume Conductivity composite ν :- Volume fraction of the filler [13] N.K Srivastava, and R.M. Mehra, “Study of Electrical Properties of Polystyrene/Foliated Graphite Composite”, Dept of Electronic Science, University of Delhi South Campus, New Delhi, India. νc :- Critical volume fraction Tg :- Glass Transition Temperature [11] Erik T. Thostenson, and Tsu-Wei Chou, “Aligned Multiwalled Carbon Nanotubereinforced Composites: Processing and Mechanical Characterization”, Journal of Physics D: Applied Physics, 35 (16), L77-L80 (2002). [14] S. Battacharya, V.K. Sachdev, R.P. Tandon, “Electrical Properties of Graphite Filled Polymer Composites”, 2nd National Conference Mathematical Techniques: Emerging Paradigms for Electronics and IT Industries, September 26-28, 2008. of polymer