2019
DOI: 10.1016/j.carbon.2018.12.114
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Structural and electrochemical properties of babassu coconut mesocarp-generated activated carbon and few-layer graphene

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Cited by 68 publications
(30 citation statements)
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“…Particularly, the (002) and (100) peak of HBFC-1 and HBFC-2 shifts to lower angle as compared with HBFC-3 and HBFC-4 samples, suggesting the larger interlayer distance of HBFC-1, HBFC-2 samples due to the much thinner carbon nanosheets. 42 Moreover, the (002) diffraction peaks can be distinguished in HBFC-1, due to the strong etching effect on the lamellar crystal structure by activation. This suggests that a disturbed structure in amorphous carbons is caused due to the randomly oriented hexagonal carbon layers, which is beneficial for increasing the specific surface area.…”
Section: Resultsmentioning
confidence: 99%
“…Particularly, the (002) and (100) peak of HBFC-1 and HBFC-2 shifts to lower angle as compared with HBFC-3 and HBFC-4 samples, suggesting the larger interlayer distance of HBFC-1, HBFC-2 samples due to the much thinner carbon nanosheets. 42 Moreover, the (002) diffraction peaks can be distinguished in HBFC-1, due to the strong etching effect on the lamellar crystal structure by activation. This suggests that a disturbed structure in amorphous carbons is caused due to the randomly oriented hexagonal carbon layers, which is beneficial for increasing the specific surface area.…”
Section: Resultsmentioning
confidence: 99%
“…Supercapacitors play an important role in electrochemical energy storage device due to their high energy density, longevity, and good stability [1][2][3]. They can be divided on the basis of energy storage principle into the electric double-layered capacitors (EDLCs) and pseudocapacitors [4].…”
Section: Introductionmentioning
confidence: 99%
“…Gr nanosheets were grown vertically on the Ta current collector to form a 3D mesh structure with multilevel pores, which provide this working electrode with an electroactive area ( A eff = 10.36 cm 2 ), which is 10.36 times larger than its geometric area (1 cm 2 ) (Figure S3). The electroactive area ( A eff ) was calculated using the Randles–Sevcik equation I P = 2.69 × 10 5 n 3/2 A eff D 1/2 ν 1/2 c , where n is the number of transferred electrons (here, n = 1), D is the diffusion coefficient (7.6 × 10 –6 cm 2 s –1 ), and c is the initial concentration of the redox probe. Specifically, A eff was calculated by substituting n , D , c , and the slope of the I p – v 1/2 curve (Figure S3c) into the Randles–Sevcik equation.…”
Section: Resultsmentioning
confidence: 99%