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Chapter 5 β Production of Few Layer Graphene in Organic Solvents Figure 5.13: πΌπ· βπΌπΊ ratio as a function of 1βγπΏγ for all the samples produced. The linear fit does coincide with the measured value of (πΌπ·βπΌπΊ)ππππhππ‘π which is also shown. The γπΏγ was estimated from AFM analysis for all the different samples produced under different conditions. The plot between πΌπ·βπΌπΊ vs 1βγπΏγ is shown in Figure 5.13. It has to be noted that all data from FLG/NMP and FLG/DMF were used for the plots. The linear relationship can be clearly seen between πΌπ·βπΌπΊ and 1βγπΏγ suggesting the observed increase in D band intensity is only due to the edges. Interestingly, the intercept of the straight line (~0.1) coincides approximately with the measured value of (πΌπ·βπΌπΊ)ππππhππ‘π (~0.08) suggesting that the sonication does not introduce any new basal plane defects in the graphene apart from pre-existing defects in the starting graphite powder.127 The slope of the graph is π = 0.14, which is comparable to literature values on the solvent exfoliated graphene by sonication (π = 0.17 62 and π = 0.26 61) and shear exfoliation (π = 0.17 127). These values can be used in Equation 5-1 such that πΏ can be estimated via Raman measurements. πΏπ ππππ = 0.14 Equation 5.2 πΌπ·βπΌπΊβ0.08 However, care should be taken when it comes to the (πΌπ·βπΌπΊ)ππππhππ‘π (~0.08) and the constant π (0.14) as it is shown to vary on the type of graphite used.127 Figure 5.14 shows the length data derived from the Equation 5-2 (πΏπ ππππ) and its correlation with πΏπ΄πΉπ for different sonication and centrifugation speeds used. It can be seen that the 150PDF Image | PRODUCTION AND APPLICATIONS OF GRAPHENE AND ITS COMPOSITES
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