TY - JOUR
T1 - Conduction transportation from graphene to an insulative polymer medium
T2 - A novel approach for the conductivity of nanocomposites
AU - Zare, Yasser
AU - Munir, Muhammad Tajammal
AU - Rhee, Kyong Yop
AU - Park, Soo Jin
N1 - Publisher Copyright:
© 2024 the author(s), published by De Gruyter.
PY - 2024/1/1
Y1 - 2024/1/1
N2 - Some models have been proposed for the electrical conductivity of graphene-filled nanocomposites, but they have not reflected the characteristics of an imperfect interphase surrounding the graphene nanosheets. In this article, the size and conductivity of an imperfect interphase are used to develop a model for conductivity of the graphene/polymer system. Also, "Y,"the degree of conduction transfer through an imperfect interphase, is expressed as graphene dimensions and interphase conductivity to define the effective converse aspect ratio and effective filler portion in the samples. The developed model for nanocomposite conductivity is examined by the experimental data of some samples. Furthermore, the influences of various factors on "Y,"percolation onset, and nanocomposite conductivity are investigated. Thin and large nanosheets, poor filler conductivity, and high interphase conductivity produce a high "Y."Likewise, "Y"and graphene volume portion (φ f) significantly govern the conductivity of samples. Y = 9 and φ f} = 0.03 yield the highest nanocomposite conductivity of 16 S/m, while Y < 2 or φ f} < 0.022 cannot improve the conductivity of samples.
AB - Some models have been proposed for the electrical conductivity of graphene-filled nanocomposites, but they have not reflected the characteristics of an imperfect interphase surrounding the graphene nanosheets. In this article, the size and conductivity of an imperfect interphase are used to develop a model for conductivity of the graphene/polymer system. Also, "Y,"the degree of conduction transfer through an imperfect interphase, is expressed as graphene dimensions and interphase conductivity to define the effective converse aspect ratio and effective filler portion in the samples. The developed model for nanocomposite conductivity is examined by the experimental data of some samples. Furthermore, the influences of various factors on "Y,"percolation onset, and nanocomposite conductivity are investigated. Thin and large nanosheets, poor filler conductivity, and high interphase conductivity produce a high "Y."Likewise, "Y"and graphene volume portion (φ f) significantly govern the conductivity of samples. Y = 9 and φ f} = 0.03 yield the highest nanocomposite conductivity of 16 S/m, while Y < 2 or φ f} < 0.022 cannot improve the conductivity of samples.
KW - conduction conveyance
KW - electrical conductivity
KW - graphene
KW - interface/interphase
KW - nanocomposite
KW - percolation threshold
UR - https://www.scopus.com/pages/publications/85213215501
U2 - 10.1515/ntrev-2024-0131
DO - 10.1515/ntrev-2024-0131
M3 - Article
AN - SCOPUS:85213215501
SN - 2191-9089
VL - 13
JO - Nanotechnology Reviews
JF - Nanotechnology Reviews
IS - 1
M1 - 20240131
ER -