In this section the three MCC precursors are first carbonized in tube furnace at temperature 800℃ to 1400℃ in nitrogen atomosphere, respectively, then measured and characterized.
Carbonization of sMCC
The carbon product, carbonized from sMCC at tempereture1400°C for 1 hour, is labeled as sMCC-C. A notable phenomenon is that the sMCC-derived carbon sMCC-C keeps the shape and architecture of its precursor sMCC. The SEM images of sMCC-C in Fig. 5 (a) and (b) are like dried petals of rose, very similar to its precursor sMCC in Fig. 1 (b).
(Fig. 5. SEM and TEM of sMCC-C)
A 10 nm resolution HRTEM image of sMCC-C is shown in Fig. 5 (c), in which a large patch of graphene 2D crystal is marked in a pink circle, and Fig. 5 (d) is a close view of the graphene 2D crystal. In Fig. 5 (e) a larger graphene 2D crystal is shown, where exquisite honeycomb-shaped hexagonal lattice can be seen clearly. Careful calculation reveals that the sides length of the hexagon is 0.142 nm. This is just the crystal structure of 2D graphene. The Raman spectrum of sMCC-C is shown Fig. 8, where the peak-D at 1339 cm-1, peak-G at 1564 cm-1, peak-2D at 2677cm-1, and peak-(D + G) at 2901 cm-1 indicate that there is a certain amount of graphene in sMCC-C, although not all particles in sMCC-C are 2D graphene.
The 2D graphene crystal converted from 2D cellulose crystal was firstly reported by Du’s research team 33, where the cellulose 2D crystal was produced through deep hydrolysis of bagasse fibrous cellulose in NaOH solution. In this study the cellulose 2D crystal is found from sugarcane pith, and is converted to graphene 2D crystal. A reasonable inference is that 2D graphene can be fabricated from 2D cellulose precursor, and this may open a new way for production of 2D graphene from sustainable microcrystal cellulose in very low cost.
Carbonization of bMCC The carbon product, carbonized from bMCC at tempereture1400°C for 1 hour, is labeled as bMCC-C that is fluff-like mass of soft and elastic. Figure 6 (a) is a SEM image of bMCC-C powder, and Fig. 6 (b) is a close-view of a bMCC-C particle, where the round shape is like its precursor bMCC in Fig. 3 (b).
(Fig. 6. Photo and SEM of bMCC-C)
Figure 6 (c) is a HRTEM image of bMCC-C, where is filled with multi layers of graphene microcrystals distributing in different directions. In Fig. 6 (c) there is no visible graphene 2D crystal, very different from sMCC-C in Fig. 5. Another HRTEM image of bMCC-C is shown in Fig. 6 (d), where the particles of graphene microcrystal (GMC) are even smaller than that in Fig. 6 (c), only a few nm and a few layers. In a research article of Du’s team 45, GMC (graphene microcrystal) fabricated from lignin was reported that is a type of hard carbon like glass and ceramic 29,46–48, however, the GMC derived from bMCC is soft and elastic. A comparison between bMCC-derived GMC (labeled as b-GMC) and lignin-derived GMC (labeled as l-GMC) is shown in Fig. 10, we will discuss it more detailed in theoretical analysis section.
Carbonization and activation of sMCCs
Spherical carbon or carbon dot 49,50 is usually fabricated from sugar, starch, and relative feedstocks 51–53. In this study the sMCCs sugar, hydrolyzed from sugarcane pith, is used to fabricate the sphere carbon. The saccharified sMCCs precursor with residual phosphoric acid is put in graphite crucibles, carbonized in a tube furnace in nitrogen atmosphere at tempereture 800°C for 1 hour, where phosphoric acid plays the role of activation reagent. The produced carbon is washed using DI water to neutral, then dried. As fabricated sphere carbon is labeled as sMCCs-C. Figure 7 (a) and (b) are the SEM images of sMCCs-C, where the sphere carbon particles are in diameter 5 to 20 microns.
(Fig. 7: Sphere carbon sMCCs-C)
The sphere carbon sMCCs-C is porous carbon that was activated by phosphoric acid in the carbonization reaction. The specific surface area (SSA) of sMCCs-C is 1973 m2/g, and the total pore volume is 1.1653 ml/g, measured by using BET (Brunauer-Emmett-Teller) gas adsorption method. The curve of pore-volume vs pore-size is shown in Fig. 7 (c), in which the micro pore volume is 73.5% and the mesoporous pore volume is 24.4%, a good porous carbon for supercapacitor 20–22.
Characterization and theoretical analysis In this study the 2D graphene is derived from 2D cellulose of sMCC and the graphene microcrystal (GMC) is derived from bMCC. The HRTEM images in Fig. 5 are the direct evidence of sMCC-derived 2D graphene, and the HRTEM images in Fig. 6 are the direct evidence of bMCC-derived GMC. However, not all ingredients in sMCC-C and bMCC-C are graphene. Raman spectroscopy is a powerful tool for characterization of graphene and relative materials. The Raman spectrums of sMCC-C and bMCC-C are shown in Fig. 8 (a) and (b), respectively, where the peak-D at 1339 cm-1, peak-G at 1564 cm-1, peak-2D at 2677cm-1, and peak-(D + G) at 2901 cm-1 indicate that there is a certain amount of graphene in the MCC-derived carbon products, althou not all carbon particles are graphene.
(Fig. 8: Raman spectrums)
An explanation for the chemical reaction from cellulose 2D crystal to graphene 2D crystal is as follows. The carbonization reaction of cellulose 2D crystals follows the mechanism of "in situ carbonization" and "nearby recombination". According to this mechanism, the 6-carbon glucose monomers of 2D cellulose lost water molecules at high temperature, recombine into benzene rings, and form the 2D crystal structure of graphene on the basis of the precursor’s 2D crystal structure,
(2D cellulose)(C6H10O5)n → (2D graphene) (C6)n + 5n(H2O).
From theoretical viewpoint, cellulose 2D crystal is very unstable, because large amount of unbonded hydrogen bond elements (donors and receptors) are exposed on the surface. Fortunately, in the center of sugarcane tube the highly concentrated sucrose solution saturate the hydrogen bond elements and makes the cellulose 2D crystal stable, consequently large amount of 2D microcrystal cellulose exists in sugarcane pith.
Following the same reaction mechanism the cabbage leaves like cellulose microcrystals of bamboo pith are converted to graphene microcrystal (b-GMC) keeping the shape of its precusor bMCC. The bMCC derived b-GMC is soft and elastic, very different from the lignin-derived l-GMC 45, the latter is very hard, like glass and ceramic. The XPS spectrum of carbon atoms in bMCC is shown in Fig. 9 (a), where the sub-peak-1 centered on 285.2 nm is of carbon sp3 atoms, and the sub-peak-2 centered on 286.8 nm is of carbon atoms bonded by oxygen atoms. Figure 9 (b) is the XPS spectrum of carbon atoms of bMCC-C. An interesting phenomenon is that in the sub-peak-1 of Fig. 9 (a) almost all carbon atoms of bMCC are in sp3 electron state (285.2 nm), however, in Fig. 9 (b) most carbon atoms of bMCC-C are in sp2 electron state (284.7 nm). It means that during carbonization reaction most carbon atoms of bMCC are converted their electron state from sp3 in cellulose to sp2 in graphene, and the other carbon atoms are in an amorphous form, keeping their sp3 electron state.
(Fig. 9: XPS spectrums)
The XPS spectrums of lignin and lignin-derived carbon are shown in Fig. 9 (c) and (d), respectively. Based on the XPS spectrum of lignin in Fig. 9 (c), 72.7% carbon atoms are in sp2 state and 27.3% carbon atoms are in sp3 state. And based on the XPS spectrum of lignin-derived carbon (l-GMC) in Fig. 9 (d), the percentages of sp2 and sp3 carbon atoms are around 73% and 27%, respectively, almost the same as the bMCC-derived b-GMC. In the lignin-derived l-GMC the sp2 graphene microcrystals are chemically bonded by sp3 carbon atoms, forming the sp2-sp3 hybrid hard graphene microcrystal, like glass and ceramic. On the other hand, in bMCC-derived b-GMC the sp3 carbon atoms are in amorphous form, and the sp2 graphene microcrystals are piled together without chemical bond conections. Figure 10 is a comparison of bMCC-derived b-GMC and lignin-derived l-GMC, and Fig. 10 (e) is a model structure of l-GMC, where the pink circles are the sp3 carbon atoms that join the graphene microcrystal units by chemical bonds.