Strain-dependent electrical resistance of multi-walled carbon nanotube/polymer composite films

The strain-dependent electrical resistance characteristics of multi-walled carbon nanotube (MWCNT)/polymer composite films were investigated. In this research, polyethylene oxide (PEO) is used as the polymer matrix. Two representative volume fractions of MWCNT/PEO composite films were selected: 0.56 vol% (near the percolation threshold) and 1.44 vol% (away from the percolation threshold) of MWCNT. An experimental setup which can measure electrical resistance and strain simultaneously and continuously has been developed. Unique and repeatable relationships in resistance versus strain were obtained for multiple specimens with different volume fractions of MWCNT. The overall pattern of electrical resistance change versus strain for the specimens tested consists of linear and nonlinear regions. A resistance change model to describe the combination of linear and nonlinear modes of electrical resistance change as a function of strain is suggested. The unique characteristics in electrical resistance change for different volume fractions imply that MWCNT/PEO composite films can be used as tunable strain sensors and for application into embedded sensor systems in structures.

[1]  L. Onsager THE EFFECTS OF SHAPE ON THE INTERACTION OF COLLOIDAL PARTICLES , 1949 .

[2]  M. D. Hooven,et al.  Electrical engineering as it will be , 1956, Electrical Engineering.

[3]  G. V. Chester,et al.  Solid State Physics , 2000 .

[4]  J. Simmons Generalized Formula for the Electric Tunnel Effect between Similar Electrodes Separated by a Thin Insulating Film , 1963 .

[5]  John G. Simmons,et al.  Low‐Voltage Current‐Voltage Relationship of Tunnel Junctions , 1963 .

[6]  S. Redner,et al.  Introduction To Percolation Theory , 2018 .

[7]  I. Balberg,et al.  Excluded-volume explanation of Archie's law. , 1986, Physical review. B, Condensed matter.

[8]  Munson-McGee,et al.  Estimation of the critical concentration in an anisotropic percolation network. , 1991, Physical review. B, Condensed matter.

[9]  Charles M. Lieber,et al.  Probing Electrical Transport in Nanomaterials: Conductivity of Individual Carbon Nanotubes , 1996, Science.

[10]  H. Lezec,et al.  Electrical conductivity of individual carbon nanotubes , 1996, Nature.

[11]  Shiv P. Joshi,et al.  Design and structural testing of smart composite structures with embedded conductive thermoplastic film , 1999 .

[12]  P. Blanas,et al.  Composite piezoelectric sensors for smart composite structures , 1999, 10th International Symposium on Electrets (ISE 10). Proceedings (Cat. No.99 CH36256).

[13]  Work function of carbon nanotubes , 2000 .

[14]  H. Daniel Wagner,et al.  Single-wall carbon nanotubes as molecular pressure sensors , 2000 .

[15]  M. Shiraishi,et al.  Work function of carbon nanotubes , 2001 .

[16]  Zhengwei Pan,et al.  Work function at the tips of multiwalled carbon nanotubes , 2001 .

[17]  Dong Qian,et al.  Mechanics of carbon nanotubes , 2002 .

[18]  H. Wagner,et al.  Polarized resonance Raman spectroscopy of single-wall carbon nanotubes within a polymer under strain , 2002 .

[19]  Satish Nagarajaiah,et al.  Nanotube film based on single-wall carbon nanotubes for strain sensing , 2004 .

[20]  Tsu-Wei Chou,et al.  Strain and pressure sensing using single-walled carbon nanotubes , 2004 .

[21]  Huaqing Xie,et al.  Measuring the thermal conductivity of a single carbon nanotube. , 2005, Physical review letters.

[22]  M. Dresselhaus,et al.  Strain-induced interference effects on the resonance Raman cross section of carbon nanotubes. , 2005, Physical review letters.

[23]  T. Chou,et al.  Carbon Nanotube Networks: Sensing of Distributed Strain and Damage for Life Prediction and Self Healing , 2006 .

[24]  Deformation dependent electrical resistance of MWCNT layer and MWCNT/PEO composite films , 2007 .

[25]  Yuri S. Kivshar,et al.  Thermal conductivity of single-walled carbon nanotubes , 2009 .