Dissolution situations in the instant- and slow-cooling processes
The mixture of MCC (10 wt%) and NaOH-urea solution (90 wt%) was separately treated with instant- and slow-cooling processes from 26 to − 20°C. The NaOH-urea solution contained 7 wt% NaOH, 12 wt% urea and 81 wt% water. As shown in Fig. 1A, after instant cooling, the mixture still contained a large quantity of white solid (no freeze and thaw), and the mixture was slightly viscous, indicating low solubility of MCC. In contrast, as shown in Fig. 1B, the slow-cooling mixture was transformed into a very viscous and transparent solution (also no freeze and thaw). This slow-cooling process took 1.5 h. The small white spots in the solution were tiny bubbles rather than MCC. The optical microscopy images showed that the instant-cooling mixture contained many MCC granules (Fig. 1C), and 10 wt% MCC also could not be dissolved in the NaOH-urea solution with a freeze-thaw procedure from 26 to − 22°C (Fig. S2), even if the freeze procedure took 1.5 h. In contrast, the slow-cooling mixture was homogeneous without granules (Fig. 1D), showing the complete dissolution of 10 wt% MCC. The rationale for the criterion of cellulose dissolution by using optical microscopy is supported by many literatures (Chen, et al. 2020; Kostag and El Seoud 2019; Rosca, et al. 2005; Xu, et al. 2019). The optical and microscopic images directly demonstrated that the solubility of MCC could be improved through the regulation of cooling rate. It was confirmed that the cooling rate or thermal history affected the solubility of MCC.
The low efficiency of instant-cooling-dissolution method was also proven at other terminal temperatures. The MCC-NaOH-urea-water mixtures were instantly cooled from 26 to − 4, −6, − 8, −10, − 12, and − 14°C, separately, and the dissolution situations are shown in Fig. 2A‒F, respectively. In the microscopic images of all these samples, the edges of un-dissolved granules were clear, and a few cracks inside MCC granules were observed in Fig. 2C and E (− 8 and − 12°C). Regardless of the terminal temperature, the MCC solubility in these instant-cooling processes could not be improved to the high level of 10 wt%. In other words, the slow-cooling process exhibited a promotion effect on the cryogenic dissolution of MCC compared to all these instant-cooling processes.
Effects of thermal history and solvent composition on the MCC solubility
In this section, the slow-cooling conditions were further optimized for higher solubility. The maximum solubility was quantified on the basis of the facts that no granule was observed in this solution by optical microscopy, and more MCC would not be dissolved in this system. The solubility increased with the decrease of terminal temperature (Fig. 3A), implying that low temperatures were favorable to the dissolution process. The solubility reached a high level of ca. 10 wt% at ≤ − 14°C (terminal temperature). More importantly, as shown in Fig. 3B, with the same terminal temperature of − 14°C, higher solubility of 11.8 wt% was realized under the cooling-rate condition of − 0.286°C/min. The average cooling rate was calculated from the overall temperature decrease divided by cooling time. It reflects the slope of cooling curve (Fig. 4), which represents the thermal history of MCC dissolution. However, with the further decrease of cooling rate, the solubility declined to a small extent. A possible reason is that a proportion of urea was decomposed in the alkaline solution during the very long dissolution period, and the decreased urea concentration was unfavorable to the dissolution of MCC.
Table 1
Cellulose solubility values reported in the literatures and this paper
Cellulose type
|
Solvent
|
Temperature (°C)
|
Solubility (wt%)
|
Reference
|
Flax cellulose
|
NaOH, urea, and water
|
−12
|
2
|
(Tang, et al. 2019)
|
Dissolving pulp
|
LiOH, urea, and water
|
−12
|
4
|
(From, et al. 2020)
|
Spruce cellulose
|
H2SO4 (aq)
|
−20
|
5
|
(Huang, et al. 2016)
|
Dissolving pulp
|
1-ethyl-3-methylimidazolium diethyl phosphate (IL)
|
100
|
5
|
(Zhang, et al. 2019)
|
Microwave-treated cellulose/urea
|
NaOH/ZnO (aq)
|
−12
|
5.5
|
(Fu, et al. 2014)
|
MCC
|
LiOH, urea, and water
|
−12
|
6
|
(Yang, et al. 2011a)
|
Cotton linter pulp
|
NaOH, thiourea, and water
|
−8
|
6
|
(Weng, et al. 2004)
|
Cotton linter pulp
|
NaOH, urea, ZnO, and water
|
−13
|
8
|
(Yang, et al. 2011b)
|
Cotton linter pulp
|
Cuprammonium hydroxide (aq)
|
Not reported
|
8
|
(Jia, et al. 2014a)
|
MCC
|
Tetra(n-butyl)ammonium acetate (IL)
|
60
|
15
|
(Kostag and El Seoud 2019)
|
MCC
|
1-allyl-3-methylimidazolium methyl phosphonate (IL)
|
80
|
22
|
(Xu, et al. 2019)
|
MCC
|
NaOH, urea, and water
|
−14
|
14
|
This paper
|
Under the conditions of preferable terminal temperature and cooling rate, the effects of NaOH and urea contents in the solvent were investigated. As shown in Fig. 3C and D, low contents of NaOH and urea led to significantly low solubility values, demonstrating that both NaOH and urea were indispensible and involved in the interactions during dissolution. Under the preferable conditions (terminal temperature = − 4.7°C; cooling rate = − 0.3°C/min; 9 wt% NaOH and 12 wt% urea), the solubility reached a maximum of 14 wt%, which is the highest cellulose solubility reported in the studies using non-ionic-liquid solvents (Table 1). In addition, the operation conditions are relatively mild compared to those reported in the literatures, and the dissolution of MCC can be easily realized in winter (minimum operation temperature = − 14°C).
Crystal structure of the regenerated cellulose
According to the literatures (Isogai and Atalla 1998; Qi, et al. 2011; Ran, et al. 2010), after the dissolution of cellulose I, cellulose II can be precipitated through solvent-adding or heating. Therefore, in the case of complete dissolution, the diffraction peaks corresponding to cellulose I should not be detected in the XRD pattern of precipitated or regenerated cellulose (Lethesh, et al. 2020). As depicted in Fig. 5, diffraction signals at 2θ of 15.1, 16.5, and 23.0° were detected in the XRD pattern of pristine MCC (left inset), indicating a typical I-type crystalline form (Wang, et al. 2022). After the dissolution of 14 wt% MCC (maximum solubility in Section 3.2), white and loose solid was precipitated with the addition of absolute ethanol. Diffraction peaks at 2θ of 12.3, 20.2, and 22.2° were observed in the pattern of white solid (Wang, et al. 2022), indicating a II-type crystalline form. The absence of signals at 15.1 and 16.5° confirmed that the precipitated or regenerated solid did not contain cellulose-I crystals. Thereby, 14 wt% MCC was completely dissolved in the solvent (9 wt% NaOH, 12 wt% urea, and 79 wt% water) under the condition of appropriate thermal history, in accordance with the result of optical microscopy (right inset in Fig. 5). Although the intrinsic viscosity of cellulose could be taken as another index to the complete dissolution of MCC (Lethesh, et al. 2020), most of the solutions prepared in the present work were too viscous to be measured with a Ubbelohde viscometer due to their high concentrations. For instance, a 7 wt% solution could not flow in the viscometer within 12 h (Fig. S3).
DSC measurement
The reason for the effect of thermal history on MCC solubility was studied by DSC, in which the exotherm or endotherm during the dissolution processes with different cooling rates was measured. As shown in Fig. 6A, with the cooling rates of − 20 to − 0.5°C/min, no exothermic or endothermic peaks were observed. In contrast, when the cooling rate was decreased to − 0.3°C/min, an obvious exothermic phenomenon was observed at circa − 4.7°C, implying that the structures of components were altered or interactions took place. Under this cooling-rate condition, this exothermic phenomenon was not observed in the NaOH-water and cellulose-NaOH-water systems (Fig. 6B). The intense exothermic peak in the profile of cellulose-water system was attributed to the freeze of water in the absence of NaOH. Therefore, urea participated in the exothermic process, which merely occurred under this slow-cooling condition. This cooling rate (− 0.3°C/min) was close to the condition adopted in the experiment with the maximum solubility of 14 wt% (Fig. 3D). The saturated mass fraction of urea in water is as high as 28.6 wt% at 0°C (vs 12 wt% urea in the aqueous phase of sample), and thereby this exothermic phenomenon should not be ascribed to the supersaturation and crystallization of urea (Samuel and Yan 2003). Considering the principle that the formation of new bonds is an exothermic process, the cryogenic environment promoted the exothermic dissolution of cellulose through the generation of new bonds. Furthermore, according to the maximum solubility (14 wt%) and quantity of dissolved cellulose (13.2 wt%) in the sample, the heat was calculated to be 31.9 ± 1.6 J/g MCC based on the integral area of the exothermic peak. The exothermic phenomenon during the dissolution of cellulose indicated that the cryogenic environment was favorable to the interaction or reaction between the solvent and cellulose from the thermodynamic point of view. The efficient cryogenic dissolution of MCC (Fig. 1) can be explained from this point of view. In contrast, other well-known dissolution processes of substances (e. g. sucrose dissolved in water) are promoted at higher temperatures under most circumstances.
Reason for the high cellulose solubility under the slow-cooling condition
After the verification of the promotion effect of cryogenic environment on the dissolution of cellulose by DSC, the indispensability of slow cooling (Fig. 1) was explored from the aspect of diffusion and mass transfer of urea and NaOH. As shown in Fig. 7A, the viscosity of 5 wt% cellulose solution was evidently increased with the decrease of temperature. The fit result showed that the data points were consistent with an exponential relationship (the inset of Fig. 7A), which usually implies a drastic variation trend. The viscosity was increased from 0.4 (20°C) to 2.25 Pa · s (− 15°C). For comparison, the viscosity of viscous glycerol is 1.5 Pa · s (20°C). Under the instant-cooling conditions, the outer shells of MCC granules could be dissolved due to the thermodynamic factor. However, the viscosity of dissolved cellulose in the shell would be instantly increased at low temperatures in the instant-cooling process, and a viscous barrier would be generated over the granules. The diffusion of urea and NaOH into the cores of granules would be impeded by this barrier. In contrast, the viscosity of dissolved cellulose was slowly decreased in the slow-cooling process, so the urea and NaOH in the bulk could diffuse into the granules for complete dissolution of cellulose at higher temperatures. Meanwhile, because the high-temperature condition continued for a long time in the slow-cooling process, the dissolved cellulose with relatively low viscosity could diffuse into the bulk due to the low viscosity and high diffusion rate.
The diffusion coefficients of urea and OH− in this solution were calculated according to the Wilke-Chang equation (Rossi, et al. 2015; Wilke and Chang 1955). As depicted in Fig. 7B, from 20 to − 15°C, both diffusion coefficients were decreased by an order of magnitude. The diffusion rates of urea and OH− would be decreased proportionally under the same concentration-gradient condition according to the Fick’s law (Qin, et al. 2022). In the instant-cooling process, the duration of high-temperature dissolution was very short, so the high diffusion rates of urea and OH− merely took place in this short period. In contrast, the low viscosity and high diffusion rate could be maintained for a long time in the slow-cooling process, and thereby urea and OH− could smoothly diffuse into the cores of MCC granules for dissolution. Meanwhile, the dissolved cellulose could diffuse into the solution, so the viscous barrier that prohibited the diffusion of urea and OH− disappeared. In summary, due to the low viscosity and weak barrier effect of dissolved cellulose in the slow-cooling procedure, the efficient diffusion of solvent components ensured the smooth solvent-cellulose interaction and complete dissolution of MCC granules. Therefore, the cooling rate or thermal history does have an impact on the solubility of cellulose by controlling the diffusion rates of solvent and dissolved cellulose, and the speculation of this paper (thermal history affects the solubility) was confirmed.
Hydrogen bonds determined by Raman spectroscopy
For the understanding of the bonds and functional groups during the dissolution process, the cellulose dissolved in the 14 wt% solution was precipitated with ethanol, and the regenerated dry cellulose powders were measured by Raman spectroscopy. Figure 8 shows that the pristine MCC contained a large number of inter- and intra-chain hydrogen bonds corresponding to the bands at 1100 and 1120 cm− 1, respectively (Morssli, et al. 1991; Schenzel, et al. 2005). After the dissolution and regeneration procedures in the NaOH solution without urea (green profile), the intramolecularly and intermolecularly hydrogen bonds were shifted to a low-frequency zone by 15 cm− 1, approximately. More importantly, most of the intramolecularly hydrogen bonds were cracked, while a small portion of the intermolecularly hydrogen bonds were cracked. In contrast, both hydrogen-bond-related bands almost disappeared in the spectrum of cellulose dissolved in the solution of urea and NaOH (red profile). Before the Raman measurement, all the samples were rinsed with water thoroughly, and the intense bands corresponding to urea at 1525 and 1600 cm− 1 indicate that the urea molecules strongly interacted with the functional groups on the surface of regenerated cellulose (Mafy, et al. 2015; Shen, et al. 2020). Due to the strong interactions, the locations of bands were different from the values of pure urea (1525 vs 1468 cm− 1, 1600 vs 1622 cm− 1). Noticeably, the overlapping bands at 1525 and 1600 cm− 1 may be assigned to carbamate ions (possible decomposition of urea in the alkaline solution) according to the literature (Foo, et al. 2016), but the absence of bands at 1700–1770 cm− 1 excluded the possibility of carbamate existing on the regenerated cellulose (Ekin and Webster 2006; Lachenmeier 2005; Yadav, et al. 2021). These results indicate that the intramolecularly and intermolecularly hydrogen bonds in cellulose were cleavaged during its dissolution in the NaOH-urea-water system, and new bonds were formed between urea and cellulose. The crack of bonds is an endothermic process while the formation of bonds is exothermic. In the light of the obvious exothermic peak detected by DSC, it is rational to believe that new and stable bonds were generated between MCC, NaOH, and urea after the crack of original hydrogen bonds. And, the apparent exothermic phenomenon was observed by DSC (Fig. 6).
Cleavage and generation of hydrogen bonds
Solid-state 13C NMR spectroscopy is a powerful tool to study the properties of biomass carbon atoms (Amaral, et al. 2019). The numbering of anhydroglucose unit (AGU) in cellulose is based on a common law (Amaral, et al. 2019). As illustrated in Fig. 9, the resonance of C4 and C6 atoms, especially the latter, was shifted upfield. Kamide et al. reported that inter-molecule hydrogen bonds were generated at the hydroxyl groups neighboring C3 and C6 atoms in cellulose-I crystals, i. e. MCC (Kamide, et al. 1992). The Raman measurement result (Fig. 9) showed that the inter-molecule hydrogen bonds in MCC were cracked in the presence of urea, so the C3 and C6 atoms would be affected by the dissolution-regeneration process. The resonance of C2, C3, and C5 overlapped, so it is impossible to clearly analyze the change in C3 atom. Instead, the C4 atom was in the vicinity of C3 atom, and the shifted resonance (upfield) of C4 and C6 atoms could reflect the shielding effect of urea on the resonance of C4 and C6 atoms by forming hydrogen bonds with hydroxyl groups (Liu, et al. 2012; Radula-Janik, et al. 2013). In this section, the crack of original inter-molecule hydrogen bonds and formation of new hydrogen bonds are understood.
Status of elements on the surface of the regenerated cellulose
Figure 10A shows the XPS spectrum of regenerated cellulose. Only C, O, and N elements were detected, and the ratio of N on the surface was very low. The N 1s spectrum (Fig. 10B) shows that the binding energy was increased by 0.2 eV, which is attributed to the bonding between urea and cellulose (Raman result in Section 3.6). These new bonds are probably hydrogen bonds, because urea is well recognized as a strong hydrogen donor (Cai, et al. 2012; Li, et al. 2018b; Paul and Paul 2015; Singh, et al. 2011). The peak at 287.7 eV in the C 1s spectrum (Fig. 10C) is assigned to the C = O groups in the urea molecules binding with regenerated cellulose. Urea might decompose into carbamate in the alkaline solutions, so it is necessary to analyze the possibility of carbamate binding with regenerated cellulose. As depicted in Fig. 10C, the peak at 288.8 eV corresponds to the carboxyl group in pure ammonium carbamate. Its intensity is much lower than the peak at 287.7 eV in the spectrum of regenerated cellulose. Therefore, the peak at 287.7 eV should not be assigned to the carboxyl group in carbamate. In addition, the Raman result also denied the existence of carbamate on the surface of regenerated cellulose (Section 3.6). The C 1s binding energy (287.7 eV) of the urea over regenerated cellulose is evidently smaller than that (289 eV) of C = O in pure urea, indicating that the paired electrons in the oxygen atoms of cellulose were transferred to the proton and adjacent carbonyl groups in urea (Stevens, et al. 2020). This shift is so obvious (1.3 eV) that it can only be ascribed to the formation of chemical or hydrogen bonds. The peak at 286.4 eV is assigned to C–OH and C–O–C groups, which are the intrinsic moieties of cellulose (Titirici, et al. 2007). The XPS analysis result proved the strong hydrogen-bonding interaction between urea and regenerated cellulose.
DFT calculation and plausible dissolution mechanism
According to the results of Raman, XPS, and solid-state 13C NMR, the NH2 group in urea interacts with the O-containing functional groups in cellulose via hydrogen bonds during the dissolution process. The binding sites on the cellulose chain were theoretically probed by DFT calculations. The calculation and simulation results are illustrated in Fig. 11. The intramolecularly and intermolecularly hydrogen bonds in MCC are cracked by NaOH and urea, respectively, in the cryogenic dissolution process (Fig. 11A). After the dispersion of cellulose chains, urea remains on the chain. The poor dissolution effect of NaOH solution and almost intact inter-molecule hydrogen bonds of NaOH-dissolved cellulose (Fig. 8) indicate that the crack of inter-molecule hydrogen bonds by urea is the primary reason for the high solubility of MCC such as 14 wt%. Therefore, we focused on the interaction or binding between cellulose and urea in the DFT calculations, of which the results are illustrated in Fig. 11B. In the cryogenic dissolution process, a stable individual chain composed of urea and cellulose is generated, and urea and cellulose are linked by two hydrogen bonds. The change in Gibbs free energy (ΔG) was calculated to be − 39.2 kJ/mol urea. On the other hand, the Raman analysis result (Fig. 8) proved that most of the intramolecularly hydrogen bonds were cracked in the NaOH-water system, while the majority of intermolecularly hydrogen bonds were sound. The DSC measurement result showed that the slow-cooling process of MCC in the NaOH-water system did not exhibit an obvious exothermic effect (Fig. 6B), indicating that the thermal effect of crack of intramolecularly hydrogen bonds was too weak to be determined. Therefore, the crack of inter-molecule hydrogen bonds by urea was taken as the dominant exothermic contributor, and the isobaric heat measured by DSC (Fig. 6), − 10.4 kJ/mol urea, was taken as the enthalpy change (ΔH) during the interaction between urea and MCC. ΔH accounts for 26.5% of ΔG, implying that the heat during the urea-MCC interaction contributed to the spontaneity of MCC dissolution to a small extent. And, because TΔS accounts for 73.5% of ΔG, the dominant contributor is the increase of entropy (ΔS, chaos degree), which should be attributed to the dispersion and random distribution of those individual cellulose chains.