Open Access Article
Benjamin Pingreya,
James D. Edeb,
Christie M. Sayes
c,
Jo Anne Shatkinb,
Nicole Starkd and
You-Lo Hsieh
*a
aBiological and Agricultural Engineering, Chemical Engineering, University of California at Davis, Davis, CA 95616-8722, USA. E-mail: ylhsieh@ucdavis.edu; Tel: +1 530 752 0843
bVireo Advisors, LLC, PO Box 51368, Boston, MA 02130, USA
cEnvironmental Science, Baylor University, Waco, TX 76798-7266, USA
dUSDA Forest Service, Forest Products Laboratory, Madison, WI 53726-2398, USA
First published on 25th March 2024
Amphiphilic sulfated cellulose nanofibrils were synthesized with yields in excess of 99% by sulfation of dissolving pulp cellulose using chlorosulfonic acid in anhydrous N,N-dimethyl formamide followed by high-speed blending. The sulfation level was stoichiometrically tunable to between 1.48 and 2.23 mmol g−1. The optimized SCNF demonstrated the ability to act as an effective dispersant for graphene produced via exfoliation in aqueous media, allowing for the production of aqueous stabilized graphene with 3.9 ± 0.3 wt% graphite to graphene conversion and suspended solids comprised of 19.5 ± 1.5 wt% graphene. Graphene exfoliated with SCNF was observed to consist exclusively of mono- and bilayers, with 42% of sheets being monolayer. Furthermore, it was demonstrated that SCNF defibrillation and graphene exfoliation could be combined into a single one-pot process.
000 cm2 V−1 s−1, giving rise to a correspondingly high in-plane electrical conductivity.1 The thermal conductivity of graphene is on the order of 3000 W m−1 K−1; nearly an order of magnitude higher than that of copper.1 Monolayers of graphene possess a staggeringly high tensile modulus of 1 TPa, making it among the strongest materials ever measured.2 Despite these outstanding properties, graphene has yet seen widespread adoption, largely due to the difficulty of producing high quality graphene in monolayers consistently and in bulk.3
The simplest way to produce graphene sheets is by peeling them off of graphite using cellophane tape;1 a simple top-down mechanical method that produces some of the highest quality graphene sheets available. However, this method is neither high-yielding nor scalable, and is therefore nonviable for any form of bulk production. Alternative top-down mechanical shearing approaches have mainly involved liquid exfoliation of graphite or graphite oxide in organic4–6 or aqueous7–10 media. Graphite has been converted into graphite oxide and then ultrasonicated in N,N-dimethylformamide (DMF) into graphene oxide and subsequently reduced into graphene using hydrazine.10 Direct exfoliation of graphite via shearing is possible in organic liquids with surface energies close to that of graphene (ca. 70–80 mJ m−2),6 including DMF,11 N-methyl-2-pyrrolidone (NMP),5 and 1,2-dichloroethane.4 While these organic liquid exfoliation processes aid the dispersion of graphene, the use of organic solvents imposes hazards as well as additional processing steps and costs. In order to aqueously exfoliate graphite, the use of dispersants, such as poly(styrene sulfonate),7 porphyrins,8 sodium salts,9 and 1-pyrenebutyrate,10 is necessary to suspend graphene in water. These dispersants act by building up electrical double layers on graphene surfaces. In the cases of mono- or even few-layer graphene, the presence of significant quantities of dispersants is necessary, leading to low graphene concentration and a dramatic reduction in the conductivity of the resulting product. As an example, an aqueous dispersion of graphene containing 1-pyrenebutyrate was stable at a concentration of 0.1 mg mL−1, but yielded a low in-plane conductivity of only 2 S cm−1.10
We previously demonstrated that C6 carboxylated cellulose nanofibrils (CNFs) produced through TEMPO-mediated oxidation of rice straw cellulose coupled with high-speed blending12 were effective in facilitating the exfoliation of graphite into graphene and stabilize the resulting graphene at concentrations of up to 1 mg mL−1, all in aqueous media.13 The effectiveness of the TEMPO CNF was postulated to be a result of amphiphilicity on the nanofibrillar surfaces. The hydrophobic (200) crystalline planes of TEMPO CNF faced with carbon and axial hydrogen atoms could associate with graphene surfaces, acting similarly to cellophane tape used during manual exfoliation and helping with the shear force applied during blending to peel off graphene. Simultaneously, the nanocellulose's surface hydrophilic hydroxyl groups and charged carboxylates present on (110) planes allow hydrogen bonding to water and dispersing graphene as stable aqueous dispersions.
Although TEMPO CNF were effective in aiding exfoliation and dispersing the exfoliated graphene, the high cost of TEMPO itself raises the need for alternative nanocelluloses, given the diversity of cellulose chemistry and the potential effectiveness in facilitating graphene production. Of particular interest are sulfated nanocelluloses, which are both anionic like TEMPO CNF and can be easily produced through multiple sulfation routes. Sulfation of cellulose has been known for decades to produce water dispersibility and super absorbency imparted by hydrophilic sulfate groups.14 Aqueous sulfation of various craft pulps,15,16 cotton,17 and CNCs18 with sodium metaperiodate and sodium bisulfite has produced macroscopic sized sulfated cellulose,15,17 10–60 nm wide CNF,16 and 200–300 nm diameter spheres or 8 nm wide CNCs.18 Sulfation of freeze-dried CNF19 and cellulose powder20 with chlorosulfonic acid in DMF, on the other hand, produced sulfated CNF with less than 100 nm diameters19 or soluble sulfated cellulose.20 Sulfation of pulp cellulose with sulfamic acid and urea as a deep eutectic solvent generated 4 nm wide CNF, however, some extent carbamation was observed due to the use of urea.21 We previously established a straightforward and robust procedure for the direct production of sulfated cellulose nanofibrils (SCNF) from macroscale rice straw cellulose using chlorosulfonic acid in DMF followed by high-speed blending, to convert 94–97% cellulose into SCNF.22 These SCNF displayed evidence of amphiphilic surface behavior, analogous to TEMPO CNF, while possessing a wider range of tunable charges, ranging from 1.0 to 2.2 mmol of sulfate half-ester groups per gram of SCNF.
The current work aims to explore the stoichiometrically optimized sulfation of the most abundantly available cellulose feedstock, i.e., dissolving pulp, into SCNFs and the efficacy of SCNF for exfoliating and dispersing graphene in comparison to that of the TEMPO CNF demonstrated previously. The relationship between the sulfation levels of SCNFs and the exfoliation efficacy of graphite into graphene was examined by optimizing exfoliation conditions with mechanical blending to maximize graphene production. The effectiveness of SCNF at exfoliating graphite into graphene, the dimensions of graphene sheets, and the conductivity of films formed by vacuum filtration of aqueous graphene dispersions were assessed. Additionally, streamlining the defibrillation of sulfated cellulose into SCNF and the exfoliation of graphite to graphene by combining these two separate processes into one single, simultaneous blending step was investigated to reduce the total time and energy input for this aqueous exfoliation approach.
Each dialyzed SCell was defibrillated into SCNF by blending (30
000 rpm, 30 min) using a high-speed blender (Vitamix 5200) in 5 min increments with cooldown periods to prevent excessive heating. For the most highly sulfated SCell (1.5 HSO3Cl/AGU molar ratio, 60 min reaction time), a briefer 5 min blending was also performed. Each aqueous suspension was centrifuged (Eppendorf 5804R, 5000 rpm, 15 min) to collect the SCNF-containing supernatant. The yield of SCNF was determined by drying an aliquot of the supernatant to determine the concentration, multiplying by supernatant volume to get SCNF mass, and dividing this by the mass of purified SCell.
Atomic force microscopy (AFM) was used to determine nanofibril height and length. Each aq. SCNF sample was diluted to ca. 0.0001 wt% and 10 μL was deposited on a freshly cleaved mica disc and allowed to dry. Samples were scanned using an Asylum Research MFP-3D AFM in tapping mode with OMCL-AC160TS standard silicon probes with a nominal tip radius of 7 nm and force constant of 26 N m−1, 5 μm × 5 μm scan size in 512 × 512 pixels. The open-source software programs Gwyddion and ImageJ were utilized to determine the height and length of nanofibrils from collected scans.
Transmission electron microscopy (TEM) was used to determine the width of SCNF. A drop of SCNF dispersions at 0.01 wt% was deposited on glow-discharged TEM grids (300 mesh, coated with carbon/formvar) and blotted dry after 10 minutes. Samples were then repeatedly stained with 2 wt% uranyl acetate to enhance contrast. Micrographs were taken with a JEOL 2100F TEM equipped with a Schottky FEG electron source at an accelerating voltage of 200 kV. The widths of nanofibrils were determined using ImageJ. TEM micrographs for 30 min blended 2.23 mmol g−1 SCNF were unavailable, but widths are presumed similar to the 5 min blended sample of the same SCNF.
The crystallinity index (CrI) of SCNF and the dissolving pulp cellulose starting material were determined using X-ray diffraction (XRD). SCNF films approximately 10 μm thick were made by depositing approximately 10 mL of SCNF in a glass dish and drying it at 50 °C. The films were mounted on the stage of a Bruker D8 Advance Eco diffractometer with a Cu Kα radiation source using a very small amount of high-vacuum grease. Dissolving pulp cellulose was instead deposited on the stage as a powder, rather than being formed into a film. Scans were collected at 2θ values ranging from 5° to 40° with an angular increment of 0.03° and a scan time of 2.5 s per increment. Crystallinity was estimated from XRD using the Segal method.23
000 RPM for 30 min in 10 min increments with cooldown periods between. After blending, the mixture was allowed to cool to room temperature then centrifuged (Eppendorf 5804R, 5000 rpm, 15 min) to precipitate unexfoliated graphite and collect the aqueous SCNF/graphene supernatant.
Simultaneous SCell defibrillation and graphite exfoliation was also studied, consolidating both blending steps into one. This process proceeded through a procedure analogous to the one detailed above for SCNF and graphite, with 10 mg mL−1 of aqueous graphite and a 5 graphite/SCell mass ratio in the feed.
The dimensions of exfoliated graphene were assessed using AFM. Drops of diluted SCNF/graphene suspension (0.0005 wt%) were deposited on mica and AFM imaging was carried out through an identical procedure to that highlighted for the analysis of SCNF. The height and lateral dimensions of the exfoliated graphene sheets were determined using Gwyddion. If a graphene sheet was rectangular or oblong shaped, the shorter lateral dimension was measured.
SCNF/graphene films were made through vacuum filtration. 25 mL of 0.1 wt% aqueous SCNF/graphene were filtered for 24 h using polycarbonate filters with a diameter of 47 mm and a 0.6 μm pore size. The film conductivity (σ) was determined by measuring the electrical resistance (Rs) using the four-point probe method24 with colinear probes spaced 1 mm apart. The Rs was measured at several different locations on each film and averaged to calculate conductivity σ = 1/(t Rs)25 using thickness (t) measured by a digital micrometer.
The combination of chlorosulfonic acid treatment and blending led to a reduction in the crystallinity index (CrI) of dissolving pulp cellulose. The original cellulose had a CrI of 0.81, while all four batches of SCNF had a CrI of around 0.65, irrespective of the sulfation or blending conditions studied, as observed by the overlap in the normalized XRD peaks for SCNF (Fig. 2a). This reduction in CrI suggests that sulfation not only affects cellulose in the amorphous regions but also amorphous–crystalline interfaces or crystalline surfaces.
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| Fig. 2 SCNF: (a) crystallinity (CrI) by XRD; (b) cross-sectional model showing hydrophobic and hydrophilic crystalline planes. | ||
As AFM was conducted on freshly cleaved hydrophilic mica surfaces, the SCNF surfaces in contact with the imaging surface are presumed to represent hydrophilic surfaces (110 or 1
0 crystalline planes), whereas the edges could represent hydrophobic surfaces (200 crystalline planes) of SCNF cross-sections (Fig. 2b). Applying this simplified SCNF cross-sectional model and known nanofibril dimensions, it can be estimated the SCNF are more hydrophilic, as evidenced by the 2.1–2.7 W/T ratios. Given that the width and thickness did not vary dramatically between sulfation and blending conditions, these SCNFs have similar overall hydrophilic–hydrophobic proportions on their surfaces. The main difference between SCNF batches lies in the density of charged sulfate half-ester groups present on the hydrophilic surfaces. Therefore, SCNF are expected to have similar ability to interact with graphene (via similar proportions of exposed hydrophobic planes) but may exhibit varied charge-dependent aqueous dispersibilities. This SCNF series also provides a range of well represented C6 sulfated CNFs along with C6 and C2/C3 carboxylated CNFs by respective TEMPO and periodate–chlorite oxidation of the same dissolving pulp26 toward the development of a toolbox of safer by design substance evaluation tools linking the biological behavior of functionalized CNFs to their surface chemistries, charges, and dimensions.27
:
1 w/w graphite/SCNF) was conducted to assess the effect of each of the two variables of interest.
Using the least sulfated SCNF (1.48 mmol g; T: 1.2 nm, W: 3.2 nm; L: 693 nm), each aqueous mixture of graphite and SCNF was blended and then centrifuged to collect the supernatant containing the exfoliated graphene and the associated SCNF, with any un-exfoliated or large fragmented graphite remaining as precipitate. The first response examined was the graphene content in the graphene/SCNF supernatant. This serves as a measure of how efficiently SCNF could exfoliate and disperse graphene while also providing the graphene content in each graphene/SCNF dispersion. The second response of interest is the graphene yield, expressed as the wt% of graphene exfoliated from the starting graphite in the feed. The main effects plots (Fig. 3) show that the graphene content of the supernatant increased from 13.5 to 19.5 wt% as the graphite/SCNF feed ratio is increased from 2.5 to 5 initially, then leveled off at 19.6% with a further increase of graphite/SCNF feed ratio to 10 (Fig. 3a). At a 2.5 graphite/SCNF feed ratio, 4.8% graphite in the original feed was converted to graphene. The graphite to graphene conversion lowered to 3.9% and 2.1%, as the graphite/SCNF feed ratio increased from 2.5 to 5 and 7.5, respectively (Fig. 3a). This falls within expectations, as higher feed ratios see more graphite added to the system without any increase in SCNF.
The effect of aqueous graphite concentration on the graphene composition of the supernatant closely aligns with that of the graphite/SCNF feed ratio, with an initial increase in graphene content followed by a plateau (Fig. 3b). Interestingly, the conversion of graphite to graphene was improved by a small but statistically significant margin as graphite concentration was increased (Fig. 3b). The interaction plots for this experiment appear parallel, indicating no significant two-factor interaction between the graphite concentration and graphite/SCNF ratio variables (Fig. 4). Balancing both the graphene concentration in the supernatant and the graphite to graphene conversion, the optimal exfoliation condition for 1.48 mmol g−1 SCNF appeared to be a 5
:
1 graphite
:
SCNF feed ratio and a 10 mg mL−1 aqueous graphite concentration. These conditions led to the conversion of 3.9 ± 0.3 wt% of the starting graphite in the feed into graphene, with 19.5 ± 1.5 wt% of suspended solids being graphene.
Using the exfoliation conditions highlighted above, the effect of varying sulfated SCNFs on exfoliation was explored. At the 2.23 mmol g−1 level, the 5 minute blended sample was used to keep the nanofibrillar dimensions closer to the two lower charged SCNF. As SCNF charge increased from 1.48 to 1.81 and 2.23 mmol g−1, less graphene was exfoliated and suspended, with the concentration of graphene in the supernatant falling from 19.5 to 8.9 and 8.2 wt%, respectively (Fig. 5). As all three SCNF have similar width/thickness ratios or presumed proportions of hydrophobic-to-hydrophilic surfaces, the reduction in exfoliated/suspended graphene with increasing charge (hydrophilicity) may be taken as an indication that the hydrophobic interactions between graphene and SCNF were interfered by the increasing charges on the hydrophilic planes in this process.
Since both the defibrillation of sulfated cellulose (SCell) into SCNF and the exfoliation of graphite into graphene were carried out by the same shear force generated by high-speed blending and in aqueous media, the prospect of combining the two separate shearing processes into a single one-pot process was also examined. SCell was substituted for SCNF at the same conditions (10 mg mL−1 graphite, 5
:
1 feed ratio) for each charge level. It was found that the amount of graphite exfoliated increased as more highly charged SCell was utilized. Interestingly, this is the opposite trend compared to what was observed during the two separate defibrillation–exfoliation process when SCNF was utilized. In particular, the most charged 2.23 mmol g−1 SCell led to a much higher production of exfoliated graphene in the supernatant (12.2 wt%) than that by the two-step process (8.2 wt%) using SCNF with the same charge. It is reasonable to assume that the presence of graphite in the blending mixture may affect how SCell defibrillates into SCNF. Higher charged SCell may work better for this one-pot defibrillation–exfoliation due to the greater ease with which the SCell is defibrillated into SCNF. However, it is worth noting even the best forming one-pot trial with 2.23 mmol g−1 SCell still produced less graphene (12.2%, Fig. 5) than the ca. 19.5% graphene exfoliated under the same 5
:
1 feed ratio, 10 mg mL−1 graphite concentration utilizing 1.48 mmol g−1 SCNF (Fig. 3). While this process does save time and energy, it appears to come at the cost of lower efficiency. However, the robust sulfation and easy tuning of SCNF properties with this in mind may close this gap.
:
1 feed ratio) was further assessed. AFM of the dispersion shows visible graphene sheets amidst SCNF (Fig. 6a), with measured graphene sheet thickness ranging between 0.20 and 0.49 nm (Fig. 6b). Using the 0.335 nm monolayer thickness reported for graphene,28 all the graphene observed consisted of either monolayer or bilayers. Since the distribution of graphene sheet thicknesses does not appear bimodal, the relative abundance of mono- and bilayers was determined by setting a threshold as the cutoff point. Taking a conservative estimate that monolayers should have an AFM measured thickness of no more than 0.335 nm leads to the result that 42% of graphene sheets observed were monolayers, with the remaining 58% being bilayers. This result differs significantly from the layer distribution (determined by the same method) of graphene exfoliated using TEMPO CNF from rice straw (T: 1.7 nm, W: 2.6 nm; L: 990 nm), which consisted of approximately 5% monolayers, 19% bilayers, 26% triple layers, 47% with 4–9 layers, and 3% with 10+ layers.13 A possible explanation for this phenomenon is that the hydrophobic interactions between (200) planes on SCNF and graphite may be weaker compared to TEMPO, either due to the difference in the relative lesser proportion of the hydrophobic (200) planes (2.6 vs. 1.5 W/T ratio for TEMPO) or in the charge nature or level (1.48 vs. 1.33 mmol g−1 for TEMPO). Weaker hydrophobic interactions or lesser SCNF-graphite affinity is thought to lead to a gentler exfoliation process, wherein only lighter mono- and bilayers could be removed from the bulk graphene flakes under the same shear force during high-speed blending. This finding is significant, as monolayer graphene is generally considered more desirable than multilayer samples. The width of graphene sheets ranged from 76 to 353 nm, with the highest fraction of sheets having widths on the order of 150–200 nm (Fig. 6c). This are similar to the lateral dimensions measured for graphene exfoliated by TEMPO CNF, which had average sheet widths of 248 ± 121 nm.13 Even the finest of the sheets measured have widths many times larger than the radius of the AFM probe tip (nominally 7 nm), which means that height measurements of graphene sheets should be unaffected by the peak broadening and height reduction that is often observed when nanoscale features (such as SCNF themselves) are measured due to finite tip sharpness.29
The optimal graphene/SCNF dispersion with the highest 19.5 wt% graphene was vacuum fitrated to form free-standing films with an average thickness of 18.8 (±0.8) μm (Fig. 6d). The graphene/SCNF film showed moisture sensitivity, bending and curling when exposed to a humid environment and straightening again once in a lower humidity setting, similar to films made from graphene/TEMPO CNF.13 This behavior can be explained by the absorption of water molecules causing asymmetric expansion in SCNF on the side of the film exposed to moisture, leading to bending. The conductivity of the graphene/SCNF film was 0.60 ± 0.05 S cm−1, much lower than the in-plane conductivity of graphene or even graphite due to the very large amount of the non-conducting SCNF (ca. 80 wt%) still present in the film. To improve electric conductivity of such graphene/SCNF films, SCNF may be removed by leveraging the significant differential thermal or chemical stability of graphene relative to SCNF. SCNF may be reduced or even removed thermally by pyrolysis or chemically via dissolution with solvents like N-methylmorpholine N-oxide (NMMO) and/or other chemical reactions that could degrade or depolymerize cellulose and allow for its removal from the system. Ultimately, the potential to improve graphene quality must be weighed against the additional processes or post treatments. At the same time, the presence of SCNF in the graphene dispersion permits viscosity control to offer novel processing opportunities such as fiber spinning into high strength fibers as previously demonstrated.22 Furthermore, aqueous graphene/SCNF dispersions may be concentrated to increase viscosity or to form gel, allowing film formation or lamination by doctor blade coating.
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