# Current-voltage characteristics of nanoplatelet-based conductive nanocomposites

- Amirhossein Biabangard Oskouyi
^{1}, - Uttandaraman Sundararaj
^{2}and - Pierre Mertiny
^{1}Email author

**9**:369

https://doi.org/10.1186/1556-276X-9-369

© Oskouyi et al.; licensee Springer. 2014

**Received: **1 April 2014

**Accepted: **18 July 2014

**Published: **29 July 2014

## Abstract

In this study, a numerical modeling approach was used to investigate the current-voltage behavior of conductive nanoplatelet-based nanocomposites. A three-dimensional continuum Monte Carlo model was employed to randomly disperse the nanoplatelets in a cubic representative volume element. A nonlinear finite element-based model was developed to evaluate the electrical behavior of the nanocomposite for different levels of the applied electric field. Also, the effect of filler loading on nonlinear conductivity behavior of nanocomposites was investigated. The validity of the developed model was verified through qualitative comparison of the simulation results with results obtained from experimental works.

### Keywords

Nanocomposites Conductive nanoplatelets Current-voltage characteristics## Background

In recent years, the nonlinear electrical conductivity behavior of nanoparticle-modified polymers has received considerable attention by researchers, and several studies have been carried out to investigate the current-voltage characteristics of conductive nanocomposites. Even though several studies investigated the nonohmic conductivity behavior of insulator polymers filled with conductive spherical and stick-like inclusions [1–5], to the best of the authors' knowledge, all of the research in this field has been limited to experimental works. Experimental research devoted to the electric properties of nanoplatelet-based nanocomposites investigated the electrical conductivity of polymers with exfoliated graphite sheets with sizes varying from a few microns to several hundreds of a micron [6–10], which allows for only limited prediction of the conductivity behavior of nanocomposites with submicron size inclusions.

These limitations motivated the present authors to conduct a numerical study to investigate the current-voltage behavior of polymers made electrically conductive through the uniform dispersion of conductive nanoplatelets. Specifically, the nonlinear electrical characteristics of conductive nanoplatelet-based nanocomposites were investigated in the present study. Three-dimensional continuum Monte Carlo modeling was employed to simulate electrically conductive nanocomposites. To evaluate the electrical properties, the conductive nanoplatelets were assumed to create resistor networks inside a representative volume element (RVE), which was modeled using a three-dimensional nonlinear finite element approach. In this manner, the effect of the voltage level on the nanocomposite electrical behavior such as electrical resistivity was investigated.

## Methods

### Monte Carlo modeling

*eV*≈ 0), the tunneling resistivity is approximately proportional to the insulator thickness, that is, the tunneling resistivity shows ohmic behavior [11]. For higher voltages, however, the tunneling resistance is no longer constant for a given insulator thickness, and it has been shown to depend on the applied voltage level. It was derived by Simmons [11] that the electrical current density passing through an insulator is given by

where

*J*_{0} = *e*/2*πh*(*β* Δ*s*)^{2} and $A=\left(4\mathit{\pi \beta}\mathrm{\Delta}\mathit{s}/h\right){\left(2m\right)}^{\frac{1}{2}}$

*eV*≈ 0, Equation 1 can be simplified as [11]

*λ*of 1 eV, with respect to the normalized voltage eV/

*λ*. This graph indicates that a polymer only exhibits close to ohmic behavior when subjected to low electric fields, that is, the resistivity of the polymer is approximately constant in a small region near the ordinate axis (see inset in Figure 3), permitting the use of the linear approximation provided by Equation 2.

*λ*= 0.5 ev employing Equation 2 and illustrated in Figure 4. The tunneling resistance is drastically dependent on the insulator thickness, that is, tunneling resistance is sharply increasing as the insulator thickness is increasing. A cutoff distance can therefore be approximated at which tunneling resistors with length greater than this threshold do not appreciably contribute toward the overall conductivity of the nanocomposite. In [12] and [13], the cutoff distance was assumed to be 1.0 and 1.4 nm, respectively. It is expected that the resistivity of the insulator film is decreasing as the electrical field is increasing; so, when dealing with higher voltage levels, tunneling resistors with length greater than these cutoff distances may play a role in the nanocomposite conductivity. Hence, it was conservatively assumed in this study that tunneling resistors with length less than 4 nm contribute toward the nanocomposite conductivity.

In the first step of this work, a three-dimensional continuum percolation model based on Monte Carlo simulation was used to study the percolation behavior of an insulator matrix reinforced with conductive nanoplatelet fillers. Additional details on this modeling approach can be found in an earlier publication [14]. In the simulation, circular nanoplatelets are randomly generated and added to the RVE. The shortest distance between adjacent particles is calculated, and particles with distance between them shorter than the cutoff distance are grouped into clusters. The formation of a cluster connecting two parallel faces of the RVE is considered the formation of a percolation network that allows electric current to pass through the RVE, rendering it conductive.

### Finite element modeling

*σ*= 10

^{8}S/m for graphene), the electrical potential drop across the nanoplatelets was neglected. The tunneling resistors were modeled as nonohmic, which resistivity is governed by Equation 1. Employing appropriate finite element formulations, the governing equation of an electrical resistor can be written as

where *I*_{
ij
} is the electrical current passing between the *ith* and *jth* node; *k*_{
ij
} is the conductance of the resistor between nodes *i* and *j*; and *V*_{
i
} is the voltage of the *ith* node measured with respect to a node connected to ground. The system of the nonlinear equations governing the electrical behavior of the nanocomposite was obtained by assembling the governing equations for the individual elements. The resulting nonlinear system of equations was solved employing an iterative method.

## Results and discussion

### Modeling results

*λ*= 0.5 ev made conductive through the uniform dispersion of conductive circular nanoplatelets with a diameter of 100 nm. In the simulations, the size of the RVE was chosen to be nine times the diameter of the nanodisks, which was ascertained to be large enough to minimize finite size effects. In an earlier study [15], the authors showed that the Monte Carlo simulation results are no longer appreciably RVE-size dependent when the RVE size is about eight times the sum of

*2R*+

*d*

_{ t }, where

*R*and

*d*

_{ t }are the radius of the nanoplatelets and tunneling distance, respectively.The graph in Figure 5 depicts the effect of filler loading on nanocomposite conductivity. As expected, a critical volume fraction indicated by a sharp increase in nanocomposite conductivity, i.e., the percolation threshold, can be inferred from the graph.In the following, electric current densities passing through the nanocomposite RVE were computed for different electric field levels and filler volume fractions. As illustrated by Figure 6, the current density versus voltage curves were found to be nonlinear. The depicted electrical behavior of the conductive nanocomposite is thus clearly governed by the applied voltage in a nonohmic manner, which, as mentioned above, matches the expectation for a conductive nanocomposite at higher electric field levels.

*E*in order to compare the nonohmic behavior for nanocomposites with different filler loadings. Note that resistivity values were normalized with respect to a reference resistivity measured at

*E*= 0.8 V/cm. The results as displayed in Figure 7 indicate that the magnitude of the applied electric field plays an important role in the conductivity of nanoplatelet-based nanocomposites. The employed modeling approach predicts nanocomposite resistivity to be a nonlinear function of the applied voltage. Clearly, the nanocomposites exhibit nonohmic behavior where the resistivity decreases with increasing voltage. Interestingly, the results in Figure 7 also indicate a reduced drop in resistivity and decreased nonohmic behavior for nanocomposites with higher filler volume fraction, that is, nanocomposites with higher filler loadings are less sensitive to the applied electric field level.

### Comparison with experimental data

Graphene nanoplatelets were dispersed in acetone by sonication using a probe sonicater in an ice bath. In the following, epoxy was added to the mixture and sonication was repeated. The solvent was evaporated by heating the mixture on a magnetic stir plate and stirring with a Teflon-coated magnet. Remaining acetone was removed by using a vacuum chamber. The curing agent was added to the mixture and mixed with a high-speed mechanical shear mixer. The mixture was again degassed using the vacuum chamber and subsequently poured into a mold. A 2-h cure cycle was then performed at 120°C. Resulting samples were machined into circular disks with 30-mm diameter and 3-mm thickness. The sample volume resistivities were measured at different applied voltages employing a Keithley 6517A electrometer connected to a Keithley test fixture (Keithley Instruments, Cleveland, Ohio, USA).Data in Figure 8 depicting the resistivity behavior of the epoxy nanocomposite samples was normalized with respect to the resistivity measured at an applied voltage of 10 V. Samples with 1 and 1.25% graphene volume fraction exhibited high resistivity levels indicating a filler loading below the percolation threshold. For higher graphene volume fractions of 1.75 and 2.25%, measurements indicated that percolation was achieved, and resistivity was found to decrease with the increase of the applied electric field. As predicted by the preceding modeling work, sample resistivity was found to be less sensitive to the applied electrical field for higher filler loadings. Hence, modeling and simulation results are qualitatively in good agreement, indicating the validity of the assumptions undertaken for the numerical modeling. However, the data presented in Figures 7 and 8 also signify that further studies are warranted to establish a quantitative agreement between numerical and experimental results.

### Characterization of resistivity behavior

*P = V × I*can be described by an exponential expression:

where *α* is an index which generally varies between −1 and 0. The value of *α* is indicative of the nonlinearity of the current-voltage relationship, i.e., *α* = 0 corresponds to ohmic behavior, and *α* decreases with increasing nonlinearity of the current-voltage curve; *r* is a parameter relating to the resistivity of the nanocomposite when the electrical power passing through the sample is 1 W [16].

*α*as a function of filler volume fraction are provided in Figure 10. It is shown that

*α*values are increasing with rising filler volume fraction. A discontinuity in

*α*values can be observed in this graph for filler volume fractions of about 5%, which is associated with the percolation volume fraction. The behavior of data simulated herein is qualitatively congruent with results reported in [5] for carbon nanotube nanocomposites.

## Conclusions

In this study, the current-voltage behavior of conductive nanoplatelet-based nanocomposites was investigated. To this end, a numerical modeling approach was developed. The simulations predicted the resistivity of nanoplatelet-based nanocomposites to be strongly affected by the applied electric field. The nanocomposites exhibit nonohmic behavior, that is, resistivity is a nonlinear function of the applied electric field. Further, nanocomposite resistivity was ascertained to decrease with increasing voltage, while the degree of nonlinear behavior was found to decline with rising filler volume fraction. A good qualitative agreement was observed between simulations and experimental data, the latter of which was obtained employing measurements on nanographene/epoxy nanocomposites. The qualitative agreement between numerical and experimental studies encourages conducting a more comprehensive study to establish a quantitative agreement. The analysis further revealed that nanocomposite resistivity as a function of electrical power can be described by an exponential relation, where the exponent is a measure of the deviation from nonohmic behavior of the conductive nanocomposite.

## Nomenclature

*d*_{
t
}, tunneling distance

*e*, electron charge

*E*, applied electric field

*h*, Planck's constant

*I*, electrical current

*J*, quantum tunneling current density

*k*, conductance of tunneling resistor

*L*, dimension of representative volume element

*m*, electron mass

*P*, electric power

*r*, resistivity parameter

*R*, radius of circular nanoplatelets

*s*_{
1
}*, s*_{
2
}, limits of barrier at Fermi level

Δ*s = s*_{2} *− s*_{1}

*V*, voltage across insulator

*V*_{
f,
} filler volume fraction

*α*, nonlinearity factor

*β*, correction factor

*λ*, height of barrier for quantum tunneling

*ρ*, electrical resistivity

*σ*, electrical conductivity

## Declarations

### Acknowledgements

This research work was supported by the following organizations: Alberta Innovates-Technology Futures, ROSEN Swiss AG, and Syncrude Canada Ltd.

## Authors’ Affiliations

## References

- An S, Mahapatra DR: Quasi-static and dynamic strain sensing using carbon nanotube/epoxy nanocomposite thin films.
*Smart Mater Struct*2009, 18: 045013. 10.1088/0964-1726/18/4/045013View ArticleGoogle Scholar - Wichmann M, Buschhorn S, Gehrmann J, Schulte K: Piezoresistive response of epoxy composites with carbon nanoparticles under tensile load.
*Phys Rev B*2009, 80: 245437.View ArticleGoogle Scholar - Cattin C, Hubert P: Network formation and electrical conduction in carbon nanotube modified polydimethylsiloxane.
*Mater Res Soc Symp Proc*2012, 1410: 1–6.View ArticleGoogle Scholar - Ounaies Z, Park C, Wise KE, Siochi EJ, Harrison JS: Electrical properties of single wall carbon nanotube reinforced polyimide composites.
*Compos Sci Technol*2003, 63: 1637–1646. 10.1016/S0266-3538(03)00067-8View ArticleGoogle Scholar - Gorrasi G, Piperopoulos E, Lanza M, Milone C: Effect of morphology of the filler on the electrical behavior of poly(L-lactide) nanocomposites.
*J Phys Chem Solids*2013, 74: 1–6.View ArticleGoogle Scholar - Lin H, Lu W, Chen G: Nonlinear DC conduction behavior in epoxy resin/graphite nanosheets composites.
*Physica B*2007, 400: 229–236. 10.1016/j.physb.2007.07.015View ArticleGoogle Scholar - Celzard A, Furdin G, Mareche JF, McRae E: Non-linear current–voltage characteristics in anisotropic epoxy resin–graphite flake composites.
*J Mater Sci*1997, 32: 1849–1853. 10.1023/A:1018504906935View ArticleGoogle Scholar - Zheng Q, Song Y, Wu G, Yi X: Reversible nonlinear conduction behavior for high-density polyethylene/graphite powder composites near the percolation threshold.
*J Polym Sci Part B*2001, 39: 2833–2842. 10.1002/polb.10042View ArticleGoogle Scholar - Chen G, Weng W, Wu D, Wu C: Nonlinear conduction in nylon-6/foliated graphite nanocomposites above the percolation threshold.
*J Polym Sci Part B*2004, 42: 155–167. 10.1002/polb.10682View ArticleGoogle Scholar - He LX, Tjong SC: Zener tunneling in conductive graphite/epoxy composites: Dielectric breakdown aspects.
*Express Polym Lett*2013, 7: 375–382. 10.3144/expresspolymlett.2013.34View ArticleGoogle Scholar - Simmons G: Generalized formula for the electric tunnel effect between similar electrodes separated by a thin insulating film.
*J Appl Phys*1963, 34: 1793–1803. 10.1063/1.1702682View ArticleGoogle Scholar - Hu N, Karube Y, Yan C, Masuda Z, Fukunaga H: Tunneling effect in a polymer/carbon nanotube nanocomposite strain sensor.
*Acta Mater*2008, 56: 2929–2936. 10.1016/j.actamat.2008.02.030View ArticleGoogle Scholar - Bao WS, Meguid SA, Zhu ZH, Weng GJ: Tunneling resistance and its effect on the electrical conductivity of carbon nanotube nanocomposites.
*J Appl Phys*2012, 111: 093726. 10.1063/1.4716010View ArticleGoogle Scholar - Oskouyi AB, Mertiny P: Monte Carlo model for the study of percolation thresholds in composites filled with circular conductive nano-disks.
*Procedia Eng*2011, 10: 403–408.View ArticleGoogle Scholar - Oskouyi AB, Sundararaj U, Mertiny P: Tunneling conductivity and piezoresistivity of composites containing randomly dispersed conductive nano-platelets.
*Materials*2014, 7: 2501–2521. 10.3390/ma7042501View ArticleGoogle Scholar - Liu CH, Fan SS: Nonlinear electrical conducting behavior of carbon nanotube networks in silicone elastomer.
*Appl Phys Lett*2007, 90: 041905. 10.1063/1.2432283View ArticleGoogle Scholar

## Copyright

This article is published under license to BioMed Central Ltd. This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/4.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly credited.