| Literature DB >> 35424969 |
Huamei Yang1, Ju Jiang1, Bingzhe Zhang1, Wenyuan Zhang1, Weining Xie2, Jing Li1.
Abstract
Ionic liquids (ILs) have been investigated to dissolve and/or pre-treat cellulose by combining with a low viscous co-solvent. Dissolution and pretreatment of cellulose by ILs are dynamic processes of dissolution and precipitation, which would caused the physical and chemical changes (such as crystallinity and thermal stability) of un-dissolved cellulose residues. Hence, this study focused on the thermal behavior of un-dissolved cellulose (PCEL) after pre-treatment using [BMIM]HSO4/ethanol. Ethanol was used as a green and cheap co-solvent of 1-butyl-3-methylimidazolium hydrogen sulfate ([BMIM]HSO4) to pre-treat cellulose under different conditions. The pretreatment effect on thermal behavior of PCEL was investigated by thermogravimetric analysis and the distributed activation energy model. [BMIM]HSO4/ethanol pretreatment efficiently lowered the thermal stability of cellulose, and promoted the thermal decomposition at low temperature. The thermal behavior of PCEL can be adjusted by the [BMIM]HSO4 mass concentration. This journal is © The Royal Society of Chemistry.Entities:
Year: 2022 PMID: 35424969 PMCID: PMC8978641 DOI: 10.1039/d2ra00876a
Source DB: PubMed Journal: RSC Adv ISSN: 2046-2069 Impact factor: 3.361
Fig. 1Structure diagram of [BMIM]HSO4.
Fig. 2Viscosity of [BMIM]HSO4/ethanol with the [BMIM]HSO4 mass concentration changing from 0% to 100%.
Fig. 3TG and DTG curves of MCEL, [BMIM]HSO4 and PCELs: (a) and (b) for [BMIM]HSO4 mass concentration at 0–100%; (c) and (d) for pretreatment temperatures at 80–200 °C; (e) and (f) for pretreatment time for 1–16 h; (g) and (h) for solid–liquid mass ratio at 1 : 20–1 : 1.
Thermogravimetric parameters of MCEL, pure [BMIM]HSO4 and PCEL0%–PCEL100%
| Name |
|
|
|
|
|
|
|
|---|---|---|---|---|---|---|---|
| MCEL | 320.2 | 394.6 | — | — | 373.4 | 3.10 | 7.68 |
| [BMIM]HSO4 | 341.8 | 411.9 | — | — | 380.8 | 2.59 | 8.74 |
| PCEL0% | 320.8 | 394.3 | — | — | 377.9 | 2.44 | 10.59 |
| PCEL0.1% | 307.5 | 395.0 | — | — | 360.2 | 2.30 | 5.03 |
| PCEL1% | 273.6 | 394.7 | — | — | 352.4 | 1.70 | 6.35 |
| PCEL5% | 249.6 | 293.0 | 265.2 | 0.15 | 353.7 | 1.43 | 8.47 |
| PCEL10% | 244.4 | 388.1 | 275.1 | 0.43 | 342.4 | 1.28 | 9.35 |
| PCEL20% | 232.1 | 396.0 | 277.4 | 0.58 | 340.6 | 1.02 | 11.45 |
| PCEL40% | 321.9 | 369.1 | 277.8 | 0.57 | 340.2 | 1.00 | 13.45 |
| PCEL60% | 229.4 | 369.1 | 273.6 | 0.69 | 334.0 | 0.75 | 13.87 |
| PCEL100% | 313.3 | 401.4 | — | — | 369.5 | 2.13 | 6.31 |
T i is the temperature of thermal decomposition at which the main weightless zone begins.
T is the temperature of thermal decomposition at which the main weightless zone finishes.
T max1 and Tmax2 are the temperature corresponding to the first and second peak of DTG curve, respectively.
D max1 and Dmax2 are the weight loss rate corresponding to the first and second peak of DTG curve, respectively.
M r is the final residue amount after thermal pyrolysis.
Ultimate analysis of MCEL and PCEL0%–PCEL60%
| Name | N [%] | C [%] | H [%] | O |
|---|---|---|---|---|
| MCEL | 0.00 | 43.16 | 5.789 | 51.051 |
| PCEL0% | 0.00 | 43.16 | 5.789 | 51.051 |
| PCEL0.10% | 0.00 | 43.20 | 6.081 | 50.719 |
| PCEL1% | 0.00 | 43.24 | 6.084 | 50.676 |
| PCEL5% | 0.02 | 44.25 | 6.287 | 49.463 |
| PCEL10% | 0.03 | 44.10 | 6.303 | 49.597 |
| PCEL20% | 0.15 | 43.60 | 6.198 | 50.202 |
| PCEL40% | 1.62 | 43.96 | 6.200 | 49.840 |
| PCEL60% | 2.01 | 44.19 | 6.254 | 49.556 |
Calculated by the differences.
Fig. 4XRD patterns of MCEL and PCEL0%–PCEL60%.
Fig. 5SEM of MCEL and PCEL0%–PCEL60% at 140 °C: (a) 500 μm; (b) 10 μm.
Fig. 6The cumulative distribution of particle size of MCEL and PCEL0%–PCEL60% at 140 °C.
Fig. 7The calculated E of MCEL and PCEL0%–PCEL100% at 140 °C.