# Two-Dimensional FTIR as a Tool to Study the Chemical Interactions within Cellulose-Ionic Liquid Solutions

Authors: Kalyani Kathirgamanathan; Warren J. Grigsby; Jafar Al-Hakkak; Neil R. Edmonds
Journal: International Journal of Polymer Science
 (2015)

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## Abstract

In this study two-dimensional FTIR analysis was applied to understand the temperature effects on processing cellulose solutions in imidazolium-based ionic liquids. Analysis of the imidazolium ionνC2–H peak revealed hydrogen bonding within cellulose solutions to be dynamic on heating and cooling. The extent of hydrogen bonding was stronger on heating, consistent with greater ion mobility at higher temperature when the ionic liquid network structure is broken. At ambient temperatures a blue shifted νC2–H peak was indicative of greater cation-anion interactions, consistent with the ionic liquid network structure. Both cellulose and water further impact the extent of hydrogen bonding in these solutions. The FTIR spectral changes appeared gradual with temperature and contrast shear induced rheology changes which were observed on heating above 70°C and cooling below 40°C. The influence of cellulose on solution viscosity was not distinguished on initial heating as the ionic liquid network structure dominates rheology behaviour. On cooling, the quantity of cellulose has a greater influence on solution rheology. Outcomes suggest processing cellulose in ionic liquids above 40°C and to reduce the impacts of cation-anion effects and enhance solubilisation, processing should be done at 70°C.


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## Body

## 1. Introduction

The use of ionic liquids for cellulose solubilisation and media for cellulose chemical modification emerged over a decade ago [1]. Since this time a range of ionic liquids have been evaluated to dissolve cellulosic precursors and prepare cellulose fractions, gels, and various regenerated cellulose materials. More recently the application of ionic liquids to dissolve cellulose has progressed to use in pretreatment and isolation of lignocellulosic fractions and feedstocks [2]. Alongside the extensive work on cellulose solubilisation and regeneration, studies have evaluated the processing of ionic liquids containing cellulose typically undertaken as solutions or on gel formation. This has included the rheological properties of the cellulose/ionic liquid solutions which have practical applications for equipment design and processing [3, 4]. There are many considerations for cellulose/ionic liquid solution properties including viscosity and chemical stability. Cellulose/ionic liquid solution rheology properties are dependent on cellulose concentration and degree of polymerization together with the frequency and shear rate [5, 6]. Typically studies have revealed cellulose solutions to be shearing thinning and dependent on temperature [5, 7–9]. However, cosolvents or water content can also influence cellulose solution rheology behaviours [10, 11].The chemistry of cellulose dissolution and processing in ionic liquids has been subject to significant investigation [1]. Hydrogen bonding determines the structures and properties of room-temperature ionic liquids where connections between hydrogen bonds form a network within the liquid [12, 13]. Hydrogen bonding within the ionic liquid is important to cellulose dissolution as well as the structure and resulting physical properties of the solution or gel. Interactions between the anion and cellulose play an important role in cellulose solvation [1, 14]. Furthermore, hydrogen bonding and solvation efficiency can determine chemical interactions in ionic liquids and cellulose solutions [15]. We have become interested in processing cellulose in ionic liquids to generate novel nanoscale architectures which require control of cellulose solution properties [16]. The purpose of the current paper is to relate the practical aspects of processing cellulose/ionic liquid solutions to the chemistry and hydrogen bonding networks within these solutions. Primarily we investigate the influence of temperature on solution chemistry and rheology behaviours. Through the use of two-dimensional infrared correlations we relate how the presence of cellulose and water sorption impact these properties. Ultimately the goal is to establish preferred conditions to dissolve and process cellulose in ionic liquids as well as outcomes potentially contributing to understandings of cellulose dissolution by ionic liquids.


## 2. Methodology

### 2.1. Materials

The ionic liquids 1-butyl-3-methylimidazolium chloride (BMIMCl) and 1-ethyl-3-methylimidazolium acetate (EMIMOAc) were obtained from Sigma Aldrich. Each was dried and distilled under vacuum prior to use. Allyl chloride and N-methylimidazole were obtained from Aldrich and freshly distilled prior to their use. The cellulose used was a Whatman high purity microcrystalline cellulose powder which was poly-dispersed with a molar mass distribution range between 1 × 104 and 3 × 106 and further defined elsewhere [16]. Postprocessing molecular weight analysis was not undertaken given differing conditions were employed (N2, air).


#### 2.1.1.
1-Allyl-3-methylimidazolium Chloride (AMIMCl) Synthesis

Allyl chloride (200 mL) was added to N-methylimidazole (100 mL) in a round bottomed flask as described by Zhang et al. [14]. The mixture was then refluxed under nitrogen for 24 h with stirring. After cooling any unreacted materials were removed by extraction with ethyl acetate. The residual product was vacuum distilled to give pure AMIMCl as an amber liquid (yield 62%).m/z calculated: 158.5, found: 158.05. Refractive index: 1.547, lit. value: 1.5465. 1H NMR δ 3.63 (N–CH3), 4.89 (N–CH2–CH), 5.28 (N–CH2–CH=CH2), 6.01 (N–CH2–CH=CH2), 7.8-7.7 (C4H, C5H), 9.40 (C2H) ppm. 13C NMR δ 36.0 (N–CH3), 50.9 (N–CH2CH), 120.5 (N–CH2CH=CH2), 122.4 (C5), 123.9 (C4), 132.0 (N–CH2–CH=CH2), 136.8 (C2).


### 2.2. Cellulose Dissolution

Prior to cellulose dissolution, cellulose and each ionic liquid were further dried in a vacuum oven at 65–70°C overnight. Cellulose (2–10% w/w) was then weighted into a flask containing ionic liquid. Dissolution of each solution was then carried out by stirring in a sealed flask at elevated temperature (70–90°C) using an oil bath. Cellulose dissolution was monitored by light microscopy until no more fibrous material was observed. Cellulose solutions were then stored at 35°C in a vacuum oven prior to use.


### 2.3. Rheology

Oscillatory and steady shear measurements were carried out using a Universal Dynamic Rheometer (UDS 200, Paar-Physica, Germany) equipped with an air cooled peltier heating element using a parallel plate geometry (MP 30, 25 mm, 0°) with a gap distance of 0.5 mm. Temperature sweep studies employed a strain of 1% and an angular frequency of 10 Hz. Heating or cooling was undertaken at a rate of 1°C/min.


### 2.4. Fourier Transform Infrared Spectroscopy (FTIR)

FTIR spectra were acquired employing a Thermo Electron Nicolet 8700 FTIR spectrometer. A total of 32 scans were collected in the 650 cm−1 to 4000 cm−1 range with a resolution of 4 cm−1. Variable temperature spectra were collected using a Spectra-Tech Thermal ARK accessory fitted with a ZnSe crystal trough plate which was flushed with dry air. For heating or cooling spectra, the sample was heated at a rate of 5°C/min and allowed to equilibrate at the set temperature for 5 minutes prior to spectra acquisition.


#### 2.4.1. Two-Dimensional Correlation Analysis

A baseline correction was performed for all spectra in defined wavenumber ranges before calculation of the 2D correlation. A reference spectrum was chosen as the average spectrum of all the spectra selected for correlation analysis. A generalised two-dimensional correlation analysis was performed using the 2D spectral correlation analysis solution of the OMNIC spectroscopic software (version 1.1.0, Thermo Electron Cooperation Spectra Corr). In the 2D contour maps, the red coloured regions are defined as the positive correlation intensities with blue-coloured region the corresponding negative correlation intensities.


## 2.1. Materials

The ionic liquids 1-butyl-3-methylimidazolium chloride (BMIMCl) and 1-ethyl-3-methylimidazolium acetate (EMIMOAc) were obtained from Sigma Aldrich. Each was dried and distilled under vacuum prior to use. Allyl chloride and N-methylimidazole were obtained from Aldrich and freshly distilled prior to their use. The cellulose used was a Whatman high purity microcrystalline cellulose powder which was poly-dispersed with a molar mass distribution range between 1 × 104 and 3 × 106 and further defined elsewhere [16]. Postprocessing molecular weight analysis was not undertaken given differing conditions were employed (N2, air).


### 2.1.1.
1-Allyl-3-methylimidazolium Chloride (AMIMCl) Synthesis

Allyl chloride (200 mL) was added to N-methylimidazole (100 mL) in a round bottomed flask as described by Zhang et al. [14]. The mixture was then refluxed under nitrogen for 24 h with stirring. After cooling any unreacted materials were removed by extraction with ethyl acetate. The residual product was vacuum distilled to give pure AMIMCl as an amber liquid (yield 62%).m/z calculated: 158.5, found: 158.05. Refractive index: 1.547, lit. value: 1.5465. 1H NMR δ 3.63 (N–CH3), 4.89 (N–CH2–CH), 5.28 (N–CH2–CH=CH2), 6.01 (N–CH2–CH=CH2), 7.8-7.7 (C4H, C5H), 9.40 (C2H) ppm. 13C NMR δ 36.0 (N–CH3), 50.9 (N–CH2CH), 120.5 (N–CH2CH=CH2), 122.4 (C5), 123.9 (C4), 132.0 (N–CH2–CH=CH2), 136.8 (C2).


## 2.1.1.
1-Allyl-3-methylimidazolium Chloride (AMIMCl) Synthesis

Allyl chloride (200 mL) was added to N-methylimidazole (100 mL) in a round bottomed flask as described by Zhang et al. [14]. The mixture was then refluxed under nitrogen for 24 h with stirring. After cooling any unreacted materials were removed by extraction with ethyl acetate. The residual product was vacuum distilled to give pure AMIMCl as an amber liquid (yield 62%).m/z calculated: 158.5, found: 158.05. Refractive index: 1.547, lit. value: 1.5465. 1H NMR δ 3.63 (N–CH3), 4.89 (N–CH2–CH), 5.28 (N–CH2–CH=CH2), 6.01 (N–CH2–CH=CH2), 7.8-7.7 (C4H, C5H), 9.40 (C2H) ppm. 13C NMR δ 36.0 (N–CH3), 50.9 (N–CH2CH), 120.5 (N–CH2CH=CH2), 122.4 (C5), 123.9 (C4), 132.0 (N–CH2–CH=CH2), 136.8 (C2).


## 2.2. Cellulose Dissolution

Prior to cellulose dissolution, cellulose and each ionic liquid were further dried in a vacuum oven at 65–70°C overnight. Cellulose (2–10% w/w) was then weighted into a flask containing ionic liquid. Dissolution of each solution was then carried out by stirring in a sealed flask at elevated temperature (70–90°C) using an oil bath. Cellulose dissolution was monitored by light microscopy until no more fibrous material was observed. Cellulose solutions were then stored at 35°C in a vacuum oven prior to use.


## 2.3. Rheology

Oscillatory and steady shear measurements were carried out using a Universal Dynamic Rheometer (UDS 200, Paar-Physica, Germany) equipped with an air cooled peltier heating element using a parallel plate geometry (MP 30, 25 mm, 0°) with a gap distance of 0.5 mm. Temperature sweep studies employed a strain of 1% and an angular frequency of 10 Hz. Heating or cooling was undertaken at a rate of 1°C/min.


## 2.4. Fourier Transform Infrared Spectroscopy (FTIR)

FTIR spectra were acquired employing a Thermo Electron Nicolet 8700 FTIR spectrometer. A total of 32 scans were collected in the 650 cm−1 to 4000 cm−1 range with a resolution of 4 cm−1. Variable temperature spectra were collected using a Spectra-Tech Thermal ARK accessory fitted with a ZnSe crystal trough plate which was flushed with dry air. For heating or cooling spectra, the sample was heated at a rate of 5°C/min and allowed to equilibrate at the set temperature for 5 minutes prior to spectra acquisition.


### 2.4.1. Two-Dimensional Correlation Analysis

A baseline correction was performed for all spectra in defined wavenumber ranges before calculation of the 2D correlation. A reference spectrum was chosen as the average spectrum of all the spectra selected for correlation analysis. A generalised two-dimensional correlation analysis was performed using the 2D spectral correlation analysis solution of the OMNIC spectroscopic software (version 1.1.0, Thermo Electron Cooperation Spectra Corr). In the 2D contour maps, the red coloured regions are defined as the positive correlation intensities with blue-coloured region the corresponding negative correlation intensities.


## 2.4.1. Two-Dimensional Correlation Analysis

A baseline correction was performed for all spectra in defined wavenumber ranges before calculation of the 2D correlation. A reference spectrum was chosen as the average spectrum of all the spectra selected for correlation analysis. A generalised two-dimensional correlation analysis was performed using the 2D spectral correlation analysis solution of the OMNIC spectroscopic software (version 1.1.0, Thermo Electron Cooperation Spectra Corr). In the 2D contour maps, the red coloured regions are defined as the positive correlation intensities with blue-coloured region the corresponding negative correlation intensities.


## 3. Results and Discussion

In this study cellulose was dissolved in ionic liquids with concentrations varying from 1 to 10% w/w. Of the three ionic liquids used, cellulose solutions prepared with 1-butyl-3-methylimidazolium chloride (BMIMCl) tended to have relatively higher viscosity than using 1-allyl-3-methylimidazolium chloride (AMIMCl) with 1-ethyl-3-methylimidazolium acetate (EMIMOAc) solutions proving to be the least viscous. Cellulose concentrations up to 7% were used in rheology assessments, but, practically, lower concentration cellulose solutions were easier to handle and process as noted by others [5, 17, 18]. The cellulose solutions were also prepared to avoid moisture sorption, but rheology and infrared evaluations were conducted in ambient conditions to mimic typical processing environments. This led to the hygroscopic cellulose solutions and respective ionic liquids readily adsorbing moisture during analyses.


### 3.1. Rheology of Ionic Liquids and Cellulose Solutions

Rheological behaviours of ionic liquids and cellulose solutions were assessed by oscillatory shear experiments. Shear behaviour profiles of AMIMCl solutions with varying cellulose content are given in Figure1. In these profiles, sample solutions were analysed by initially cooling from 100°C to minimise any effects of solution hygroscopicity on rheology. Analysis revealed the 2% cellulose solution had very low storage modulus (G′) at 100°C which was observed to increase atca. 40°C followed by a minor G′ increase with further cooling to 20°C. On cooling the 4% cellulose solution, two transitions were observed with the first atca. 65°C followed by a second atca. 45°C. At 7% cellulose content, the solution has greater storage modulus at high temperatures and, on cooling, an increase was observed at 50°C with the profile being similar to both 2% and 4% solutions on further cooling to 20°C. On heating, all samples have relatively similar G′ profiles toca. 60°C where each exhibited a transition onset with significant loss in G′ between 70 and 100°C. This transition was observed at 77°C, 86°C, and 96°C for the 2%, 4%, and 7% cellulose solutions, respectively. Pure AMIMCl did not show these shear behaviours on cooling or heating. Interestingly, a 2% cellulose solution prepared with 1-butyl-3-methylimidazolium chloride (BMIMCl) showed comparable shear behaviour as that observed with AMIMCl (see Supplementary Material available online at http://dx.doi.org/10.1155/2015/958653).Figure 1
Effect of cellulose concentration of storage modulus with temperature for AMIMCl solutions on cooling (a) and heating (b). Pure AMIMCl (black), 2% cellulose (green), 4% cellulose (red), and 7% cellulose (blue) solutions.
(a)
(b)A dependency of cellulose content in AMIMCl solution shear behaviour was also evident in viscosity profiles of these solutions (Figure2). Unsurprisingly, higher cellulose content gave greater viscosity [5, 17, 18] with this more distinguished at higher temperature. On cooling from 100 to 20°C, samples show a steady, consistent viscosity increase. However, on heating, samples initially have comparable viscosities, but above 50°C viscosity was distinguished by higher cellulose content. This shear thinning viscosity behaviour is consistent with reportedly pseudoplastic AMIMCl solutions at 10–25% cellulose content [17]. However, discontinuities in viscosity profiles are also evident in Figure 2 which can be related to temperature transitions observed in rheology profiles (Figure 1). On cooling below 50°C the discontinuity was associated with an increase in viscosity evident across the three cellulose solutions, but not with pure AMIMCl. Similarly, on heating above 50°C each solution showed an abrupt increase in viscosity compared to pure AMIMCl. This discontinuity was at 55°C for the 2% cellulose solution compared to 70°C for 7% cellulose content, consistent with the observed onset of the transition and shear behaviours on heating (Figure 1).Figure 2
Viscosity profiles for cellulose in AMIMCl solution on cooling (a) and heating (b). Pure AMIMCl (black), 2% cellulose (green), 4% cellulose (red), and 7% cellulose (blue) solutions.
(a)
(b)Rheology evaluation of EMIMOAc cellulose solutions also revealed shear behaviour dependencies with temperature and cellulose content (Figure3). On cooling 4% and 7% cellulose solutions there appeared minimal effect on rheological behaviours above 50°C. Cooling below 40°C gave an increase in G′ with transitions observed at 25°C and 35°C for the 4% and 7% solutions, respectively. On heating, both solutions show a decrease in G′ aboveca. 40°C with a significant loss in G′ between 55°C (4%) and 70°C (7%) which was comparable to that observed for AMIMCl solutions (Figure 1). In contrast, the 2% cellulose EMIMOAc solution maintained a relatively static G′ profile on cooling to 20°C, being similar to the behaviour of pure EMIMOAc. This was similarly the case on heating both pure EMIMOAc and the 2% cellulose solution. Also perhaps an emerging influence of moisture on rheology profiles is evident in Figure 3. Cooling EMIMOAc solutions revealed decreases in G′ values consistent with ionic liquid hygroscopicity with water known to impact EMIMOAc rheological properties [11].Figure 3
Effect of cellulose concentration of storage modulus with temperature for EMIMOAc solutions on cooling (a) and heating (b). Pure EMIMOAc (black), 2% cellulose (green), 4% cellulose (red), and 7% cellulose (blue) solutions.
(a)
(b)


### 3.2. FTIR Spectroscopy Analysis

To assess the effect of temperature on ionic liquid networks and observed rheological properties, infrared analysis was used to gain insights into the extent of hydrogen bonding. FTIR spectra were acquired for cellulose solutions at key temperatures between 20 and 100°C on first heating and then cooling samples (Figure4). Generally, for each cellulose solution, the spectra were relatively similar to that obtained for the respective pure ionic liquid (Supplementary Material). The spectrum of 2% cellulose in AMIMCl solution shows key peaks at 3050, 2965, 1570 and 1165 cm−1 attributable to νC2–H, νC–H methyl, νC–N, and δC–H, respectively [15]. These peaks, representative of the imidazolium ion, were also common to BMIMCl and EMIMOAc solutions. Other relevant identifying peaks include 3100 (νC–H), 1645 (νC=C), and 1420 cm−1 (δCH). Peaks attributable to cellulose such as the key cellulose νC–O–C peak at 1020 cm−1 were difficult to determine, perhaps reflective of the low concentration in the ionic liquid [19].Figure 4
FTIR spectra of 2% cellulose solutions in AMIMCl (a) and EMIMOAc (b) solutions. Spectra obtained on heating (—) from 25°C to 100°C and then on cooling (- - -) to 25°C. 25°C (black), 40°C (blue), 70°C (green), and 100°C (red).
(a)
(b)Analysis of cellulose in AMIMCl spectra revealed theνC2–H (3050 cm−1) and alkyl (νC–H, 2980 cm−1) peaks were dynamic on both heating and cooling (Figure 4). Each temperature step in Figure 4 was selected to encompass temperatures incorporating rheological transitions evident in Figure 1. With the νC2–H peak sensitive to hydrogen bonding [15], Figure 4 provides evidence for changes in the extent of imidazolium ion hydrogen bonding with temperature. An increase in hydrogen bonding causes the lengthening of the C2–H bond with the νC2–H stretching peak moving to lower wavenumbers (red shift). In contrast, other AMIMCl (cellulose solution) peaks between 700 and 1700 cm−1 including the allyl group (1645 and 1420 cm−1) remain relatively unaffected on heating or cooling. In comparing the relative intensity changes of imidazolium ion peaks to that observed with the pure ionic liquid (Supplementary material), these appear relatively less than observed for the cellulose solution. Despite attempts to exclude moisture, evident in Figure 4 were spectra showing the strong νO–H stretching band (3500–3200 cm−1) to be dynamic on both heating and cooling. This reflects sample hygroscopicity, where the νO–H peak was indicating water loss on heating with water sorption evident on cooling. A comparison of FTIR obtained with pure AMIMCl also revealed similar hygroscopicity with water sorption also evident on both heating and cooling. Analysis of the BMIMCl cellulose solution revealed spectral changes of the imidazolium ion peaks were similar to AMIMCl, but the νO–H absorption was observed to increase both on heating and cooling (Supplementary Material).Infrared spectroscopic evaluation of the EMIMOAc cellulose solution revealed spectral changes were relatively more responsive to heating and cooling than AMIMCl solution (Figure4). Imidazolium ion νC–H peaks at 2990 and 2970 cm−1 decrease in intensity with higher temperature. Furthermore, this change in peak intensity was relatively greater with the cellulose solution than for pure EMIMOAc (Supplementary Material). Dynamic EMIMOAc peaks were also observed between 700 and 1650 cm−1 attributable to the acetate anion (1590 and 1380 cm−1). Analysis of the broad νO–H peak revealed the presence of water to remain relatively static on heating but increase in intensity upon cooling, which was similarly the case for pure EMIMOAc (Supplementary Material).Infrared analysis revealed imidazolium ion peaks in both AMIMCl and EMIMOAc cellulose solutions to be dynamic on heating and cooling. There were changes to both peak shifts and intensities indicating that temperature was influencing the hydrogen bonding networks within both ionic liquids. Furthermore, when compared with pure ionic liquids the presence of cellulose appeared to also impact the relative intensity of these changes. However, the presence of water also proved to complicate this interpretation, with water known to influence hydrogen bonding and cellulose dissolution in ionic liquids [11]. To further distinguish temperature and water influences on ionic liquid hydrogen bonding two-dimensional correlation spectroscopy (2D FTIR) analysis was undertaken. Synchronous and asynchronous spectra generated from simulated spectra gave positive (red) and negative (blue) correlation squares for FTIR peak (band) shift and intensity changes (Figures 5 to 7 and Supplementary Material). Typically, both heating and cooling spectra of pure ionic liquids and cellulose solutions by 2D FTIR show strong cross peaks associated with νO–H and νC2–H peaks, evident as correlation squares (Figure 5).Figure 5
Two-dimensional FTIR correlation analysis for 2% cellulose in AMIMCl solution. Asynchronous spectrum on heating. Spectral range from 2700 to 3600 cm−1.Two-dimensional correlation FTIR analysis revealed the synchronous spectrum of the cellulose solution in AMIMCl during heating (Figure6) was similar to the synchronous spectrum of pure AMIMCl during cooling (Supplementary Material). On heating, the cellulose solution has a broad, in-phase autopeak for νO–H (3600 to 3200 cm−1) and νC2–H peaks. The autocorrelation peak (νC2–H) was at 3072 cm−1 for the cellulose solution whereas in the pure AMIMCl cooling spectrum it was at 3093 cm−1. This indicated water and potentially cellulose even at 2% concentration was influencing hydrogen bonding of the imidazolium ion within the solution. Moreover, other νC–H peaks were also impacted in the cellulose solution, whereas for pure AMIMCl only the νC–H at 2937 cm−1 peak was affected (Supplementary Material). In the case of spectra obtained on cooling (Figure 5), the synchronous spectrum of this cellulose solution was similar to that for heating perhaps reflective of temperature effects and similar water content observed on heating and cooling (Figure 4). However, any alkyl νC–H cross peaks with the νO–H region (3500 to 3100 cm−1) were not developed for this solution during cooling.Figure 6
Two-dimensional FTIR correlation analysis of cellulose in AMIMCl solution. Synchronous spectrum on heating (a) and cooling (b). Spectral range 2700 to 3600 cm−1.
(a)
(b)Figure 7
Two-dimensional FTIR correlation analysis of cellulose in EMIMOAc solution. Full spectrum range (400 to 4000 cm−1) synchronous spectra on heating (a) and cooling (b).
(a)
(b)In the corresponding asynchronous heating spectrum for the cellulose AMIMCl solution (Figure5), out of phase cross peaks were developed for the νC–H alkyl vibrations and imidazolium νC4–H and νC5–H peaks with νO–H. This indicated the intensities of two spectral features change out of phase with each other and that these differing functional groups were experiencing different effects from heating. No asynchronous cross peaks were observed between νO–H and νC2–H peaks. This contrasts the asynchronous spectrum of pure AMIMCl which showed cross peaks between νO–H and νC2–H (Supplementary Material). In this latter case, the cross peaks observed between νO–H and νC2–H were observed in both the pure AMIMCl synchronous and asynchronous spectrums indicating these two changes were not occurring simultaneously, but were either delayed or accelerated. These results were suggestive of both water and temperature influencing imidazolium ion hydrogen bonding with the asynchronous correlations suggesting the presence of cellulose may also impact hydrogen bonding networks given emergence of C4–H and C5–H cross peaks.Two-dimensional correlation spectroscopy of the EMIMOAc cellulose solution revealed positive cross peaks at 3089 and 2981 cm−1 and a relative absence of interaction with the νO–H region in the synchronous spectrum on heating (Figure 7, Supplementary Materials). No cross peaks were observed in the asynchronous spectrum of the heating spectra in this region. This suggests water was not contributing to any imidazolium ion hydrogen bonding differences in EMIMOAc solution on heating. In contrast, on cooling, autopeaks were observed for 3080 cm−1 and the νO–H region with an absence of any correlation peak at 2981 cm−1. This was also the case for pure EMIMOAc in which there was a strong autopeak at 3070 cm−1 and the νO–H region compared to a reduced prominence of the 2978 cm−1 peak. Unlike the cellulose solution, the asynchronous cooling spectrum of pure EMIMOAc (Supplementary Material) has cross peaks at 3030 cm−1 and 2960 cm−1 with the 3330 cm−1 band indicative of water interactions. Collectively, this shows, on cooling, that water also had an effect on hydrogen bonding within EMIMOAc solution. Moreover, this was consistent with the increasing presence of water in this sample on cooling (Figure 4).With the presence of an acetate anion, the carbonyl absorption of EMIMOAc was also analysed by 2D FTIR to determine the extent of any cation-anion hydrogen bonding in EMIMOAc solution (Figure7). Analysis of the cellulose solution revealed cross peaks of the anion (1500–1600 cm−1) with νC–H and νO–H peaks which increase on heating and lessen during cooling. Similarly, for pure EMIMOAc the band at 1602 cm−1 was correlated with the νO–H peak but was decreasing with both the νC2–H (3030 cm−1) and νC–H (2960 cm−1, alkyl) peaks (Supplementary Material). These results suggest that the anion is interacting with the cation C2H and methyl group during heating, but only with the C2H on cooling. Figure 7 shows contrasting behaviour of this carbonyl absorption during cooling together with a cross peak between the νO–H and νC2–H at 3086 cm−1. This provides evidence that the acetate carbonyl (1602 cm−1) is hydrogen-bonded with water and also involved in hydrogen bonding with the imidazolium νC2–H, particularly at lower temperatures consistent with network structure formation [20]. In comparing 2D FTIR analysis for the cellulose solution and pure EMIMOAc, their similarity suggests, at 2%, the cellulose content may not impact hydrogen bonding networks within the ionic liquid. This finding was also consistent with the 2% cellulose content having no impact on the rheology profile (Figure 3).


### 3.3. Discussion

It was evident in FTIR analysis that temperature together with water sorption due to ionic liquid hygroscopicity was influencing the interactions and hydrogen bonding of the imidazolium cation. Water can play a significant role in cellulose dissolution in ionic liquids in addition to impacting hydrogen bonding networks in the ionic liquid [11, 21]. In this study 2D FTIR has revealed temperature can also influence hydrogen bonding networks within the ionic liquids which may manifest in observed rheology profiles. A shift in the νC2–H peak is an indication to the extent of hydrogen bonding [15] with C2–H bond lengthening contributing a red shift to lower wavenumbers. For cellulose in AMIMCl solution the νC2–H absorption was at 3072 cm−1 during heating, but increased to 3093 cm−1 on cooling (Figure 4). This was similarly the case in BMIMCl solution with the νC2–H absorption at 3040 cm−1 on heating and increasing to 3087 cm−1 on cooling (Supplementary Material). This indicated hydrogen bonding of imidazolium ion C2–H was stronger on heating consistent with greater ion mobility at higher temperature. At ambient temperature, there were more cation-anion interactions with the νC2–H frequency blue shifted. Also consistent with heating and cooling effects were other νC–H peak changes indicating the alkyl groups have greater rotational and vibrational freedom at higher temperature when the ionic liquid network structure is broken. FTIR results suggest the higher water contents on cooling enabled water to interact more contributing to a weaker imidazolium-anion interaction and νC2–H peak shift. Furthermore, the presence of cellulose in AMIMCl solution also induced changes in the imidazolium νC–H absorptions which were not observed in the pure ionic liquid. 2D FTIR suggests cellulose may have minimised the water influence on hydrogen bonding, given differences observed between out of phase cross peaks on heating and cooling (Figure 6).With EMIMOAc, theνC2–H peak of pure EMIMOAc was at 3030 cm−1 during heating and blue shifted to 3070 cm−1 during cooling suggesting temperature similarly influenced the extent of imidazolium cation hydrogen bonding as established for AMIMCl. However, cellulose in EMIMOAc solution contributed to a narrower range in the νC2–H peak shift (3080–3089 cm−1) indicating a relatively minimal influence on νC2–H hydrogen bonding due to temperature. Moreover, results show the anion to be interacting with C2H together with other imidazolium C–H and methyl groups. Potentially this indicates differences in the extent of interactions between the imidazolium ion and acetate and chloride anions in cellulose solutions with EMIMOAc and AMIMCl, respectively. The νOH peak also contributed a dominant influence on hydrogen bonding due to water sorption on cooling.FTIR spectra show a gradual change in imidazolium ion hydrogen bonding between 25 and 100°C, on both heating and cooling. At lower temperatures there were closer interactions between cations and anions indicative of a network structure in the ionic liquids. The shear applied to the ionic liquid solutions was sufficient to break this network, with this observed as transitions under shear at key temperatures in Figures1 and 3. These transitions resulted in significant inflexions in rheology storage modulus values which were not distinguished by FTIR at these temperature steps, perhaps as FTIR was undertaken without solution shear. Furthermore, there was a rheological hysteresis evident between heating and cooling. With decreasing temperature there is apparent super cooling and gel formation [1] leading to slower network organisation within the liquid, observed below 40°C. However, on heating, initially the ionic liquid network structure is greater and the effect of shear not evident until a higher temperature (50–70°C), being common to both ionic liquids (Figures 1 and 3). The presence of cellulose increases the ionic liquid viscosity (Figure 2), but has minimal effect on initial heating (Figures 1 and 3) as the ionic liquid network structure is dominant. Only on cooling and gel formation was the presence and quantity of cellulose observed to impact rheology. Moreover, given the impact of cellulose observed by 2D FTIR it can be expected cellulose plays an increasing role in hydrogen bonding in AMIMCl at higher concentrations whereas in EMIMOAc any impact of cellulose was observed at ≥4% concentration.


## 3.1. Rheology of Ionic Liquids and Cellulose Solutions

Rheological behaviours of ionic liquids and cellulose solutions were assessed by oscillatory shear experiments. Shear behaviour profiles of AMIMCl solutions with varying cellulose content are given in Figure1. In these profiles, sample solutions were analysed by initially cooling from 100°C to minimise any effects of solution hygroscopicity on rheology. Analysis revealed the 2% cellulose solution had very low storage modulus (G′) at 100°C which was observed to increase atca. 40°C followed by a minor G′ increase with further cooling to 20°C. On cooling the 4% cellulose solution, two transitions were observed with the first atca. 65°C followed by a second atca. 45°C. At 7% cellulose content, the solution has greater storage modulus at high temperatures and, on cooling, an increase was observed at 50°C with the profile being similar to both 2% and 4% solutions on further cooling to 20°C. On heating, all samples have relatively similar G′ profiles toca. 60°C where each exhibited a transition onset with significant loss in G′ between 70 and 100°C. This transition was observed at 77°C, 86°C, and 96°C for the 2%, 4%, and 7% cellulose solutions, respectively. Pure AMIMCl did not show these shear behaviours on cooling or heating. Interestingly, a 2% cellulose solution prepared with 1-butyl-3-methylimidazolium chloride (BMIMCl) showed comparable shear behaviour as that observed with AMIMCl (see Supplementary Material available online at http://dx.doi.org/10.1155/2015/958653).Figure 1
Effect of cellulose concentration of storage modulus with temperature for AMIMCl solutions on cooling (a) and heating (b). Pure AMIMCl (black), 2% cellulose (green), 4% cellulose (red), and 7% cellulose (blue) solutions.
(a)
(b)A dependency of cellulose content in AMIMCl solution shear behaviour was also evident in viscosity profiles of these solutions (Figure2). Unsurprisingly, higher cellulose content gave greater viscosity [5, 17, 18] with this more distinguished at higher temperature. On cooling from 100 to 20°C, samples show a steady, consistent viscosity increase. However, on heating, samples initially have comparable viscosities, but above 50°C viscosity was distinguished by higher cellulose content. This shear thinning viscosity behaviour is consistent with reportedly pseudoplastic AMIMCl solutions at 10–25% cellulose content [17]. However, discontinuities in viscosity profiles are also evident in Figure 2 which can be related to temperature transitions observed in rheology profiles (Figure 1). On cooling below 50°C the discontinuity was associated with an increase in viscosity evident across the three cellulose solutions, but not with pure AMIMCl. Similarly, on heating above 50°C each solution showed an abrupt increase in viscosity compared to pure AMIMCl. This discontinuity was at 55°C for the 2% cellulose solution compared to 70°C for 7% cellulose content, consistent with the observed onset of the transition and shear behaviours on heating (Figure 1).Figure 2
Viscosity profiles for cellulose in AMIMCl solution on cooling (a) and heating (b). Pure AMIMCl (black), 2% cellulose (green), 4% cellulose (red), and 7% cellulose (blue) solutions.
(a)
(b)Rheology evaluation of EMIMOAc cellulose solutions also revealed shear behaviour dependencies with temperature and cellulose content (Figure3). On cooling 4% and 7% cellulose solutions there appeared minimal effect on rheological behaviours above 50°C. Cooling below 40°C gave an increase in G′ with transitions observed at 25°C and 35°C for the 4% and 7% solutions, respectively. On heating, both solutions show a decrease in G′ aboveca. 40°C with a significant loss in G′ between 55°C (4%) and 70°C (7%) which was comparable to that observed for AMIMCl solutions (Figure 1). In contrast, the 2% cellulose EMIMOAc solution maintained a relatively static G′ profile on cooling to 20°C, being similar to the behaviour of pure EMIMOAc. This was similarly the case on heating both pure EMIMOAc and the 2% cellulose solution. Also perhaps an emerging influence of moisture on rheology profiles is evident in Figure 3. Cooling EMIMOAc solutions revealed decreases in G′ values consistent with ionic liquid hygroscopicity with water known to impact EMIMOAc rheological properties [11].Figure 3
Effect of cellulose concentration of storage modulus with temperature for EMIMOAc solutions on cooling (a) and heating (b). Pure EMIMOAc (black), 2% cellulose (green), 4% cellulose (red), and 7% cellulose (blue) solutions.
(a)
(b)


## 3.2. FTIR Spectroscopy Analysis

To assess the effect of temperature on ionic liquid networks and observed rheological properties, infrared analysis was used to gain insights into the extent of hydrogen bonding. FTIR spectra were acquired for cellulose solutions at key temperatures between 20 and 100°C on first heating and then cooling samples (Figure4). Generally, for each cellulose solution, the spectra were relatively similar to that obtained for the respective pure ionic liquid (Supplementary Material). The spectrum of 2% cellulose in AMIMCl solution shows key peaks at 3050, 2965, 1570 and 1165 cm−1 attributable to νC2–H, νC–H methyl, νC–N, and δC–H, respectively [15]. These peaks, representative of the imidazolium ion, were also common to BMIMCl and EMIMOAc solutions. Other relevant identifying peaks include 3100 (νC–H), 1645 (νC=C), and 1420 cm−1 (δCH). Peaks attributable to cellulose such as the key cellulose νC–O–C peak at 1020 cm−1 were difficult to determine, perhaps reflective of the low concentration in the ionic liquid [19].Figure 4
FTIR spectra of 2% cellulose solutions in AMIMCl (a) and EMIMOAc (b) solutions. Spectra obtained on heating (—) from 25°C to 100°C and then on cooling (- - -) to 25°C. 25°C (black), 40°C (blue), 70°C (green), and 100°C (red).
(a)
(b)Analysis of cellulose in AMIMCl spectra revealed theνC2–H (3050 cm−1) and alkyl (νC–H, 2980 cm−1) peaks were dynamic on both heating and cooling (Figure 4). Each temperature step in Figure 4 was selected to encompass temperatures incorporating rheological transitions evident in Figure 1. With the νC2–H peak sensitive to hydrogen bonding [15], Figure 4 provides evidence for changes in the extent of imidazolium ion hydrogen bonding with temperature. An increase in hydrogen bonding causes the lengthening of the C2–H bond with the νC2–H stretching peak moving to lower wavenumbers (red shift). In contrast, other AMIMCl (cellulose solution) peaks between 700 and 1700 cm−1 including the allyl group (1645 and 1420 cm−1) remain relatively unaffected on heating or cooling. In comparing the relative intensity changes of imidazolium ion peaks to that observed with the pure ionic liquid (Supplementary material), these appear relatively less than observed for the cellulose solution. Despite attempts to exclude moisture, evident in Figure 4 were spectra showing the strong νO–H stretching band (3500–3200 cm−1) to be dynamic on both heating and cooling. This reflects sample hygroscopicity, where the νO–H peak was indicating water loss on heating with water sorption evident on cooling. A comparison of FTIR obtained with pure AMIMCl also revealed similar hygroscopicity with water sorption also evident on both heating and cooling. Analysis of the BMIMCl cellulose solution revealed spectral changes of the imidazolium ion peaks were similar to AMIMCl, but the νO–H absorption was observed to increase both on heating and cooling (Supplementary Material).Infrared spectroscopic evaluation of the EMIMOAc cellulose solution revealed spectral changes were relatively more responsive to heating and cooling than AMIMCl solution (Figure4). Imidazolium ion νC–H peaks at 2990 and 2970 cm−1 decrease in intensity with higher temperature. Furthermore, this change in peak intensity was relatively greater with the cellulose solution than for pure EMIMOAc (Supplementary Material). Dynamic EMIMOAc peaks were also observed between 700 and 1650 cm−1 attributable to the acetate anion (1590 and 1380 cm−1). Analysis of the broad νO–H peak revealed the presence of water to remain relatively static on heating but increase in intensity upon cooling, which was similarly the case for pure EMIMOAc (Supplementary Material).Infrared analysis revealed imidazolium ion peaks in both AMIMCl and EMIMOAc cellulose solutions to be dynamic on heating and cooling. There were changes to both peak shifts and intensities indicating that temperature was influencing the hydrogen bonding networks within both ionic liquids. Furthermore, when compared with pure ionic liquids the presence of cellulose appeared to also impact the relative intensity of these changes. However, the presence of water also proved to complicate this interpretation, with water known to influence hydrogen bonding and cellulose dissolution in ionic liquids [11]. To further distinguish temperature and water influences on ionic liquid hydrogen bonding two-dimensional correlation spectroscopy (2D FTIR) analysis was undertaken. Synchronous and asynchronous spectra generated from simulated spectra gave positive (red) and negative (blue) correlation squares for FTIR peak (band) shift and intensity changes (Figures 5 to 7 and Supplementary Material). Typically, both heating and cooling spectra of pure ionic liquids and cellulose solutions by 2D FTIR show strong cross peaks associated with νO–H and νC2–H peaks, evident as correlation squares (Figure 5).Figure 5
Two-dimensional FTIR correlation analysis for 2% cellulose in AMIMCl solution. Asynchronous spectrum on heating. Spectral range from 2700 to 3600 cm−1.Two-dimensional correlation FTIR analysis revealed the synchronous spectrum of the cellulose solution in AMIMCl during heating (Figure6) was similar to the synchronous spectrum of pure AMIMCl during cooling (Supplementary Material). On heating, the cellulose solution has a broad, in-phase autopeak for νO–H (3600 to 3200 cm−1) and νC2–H peaks. The autocorrelation peak (νC2–H) was at 3072 cm−1 for the cellulose solution whereas in the pure AMIMCl cooling spectrum it was at 3093 cm−1. This indicated water and potentially cellulose even at 2% concentration was influencing hydrogen bonding of the imidazolium ion within the solution. Moreover, other νC–H peaks were also impacted in the cellulose solution, whereas for pure AMIMCl only the νC–H at 2937 cm−1 peak was affected (Supplementary Material). In the case of spectra obtained on cooling (Figure 5), the synchronous spectrum of this cellulose solution was similar to that for heating perhaps reflective of temperature effects and similar water content observed on heating and cooling (Figure 4). However, any alkyl νC–H cross peaks with the νO–H region (3500 to 3100 cm−1) were not developed for this solution during cooling.Figure 6
Two-dimensional FTIR correlation analysis of cellulose in AMIMCl solution. Synchronous spectrum on heating (a) and cooling (b). Spectral range 2700 to 3600 cm−1.
(a)
(b)Figure 7
Two-dimensional FTIR correlation analysis of cellulose in EMIMOAc solution. Full spectrum range (400 to 4000 cm−1) synchronous spectra on heating (a) and cooling (b).
(a)
(b)In the corresponding asynchronous heating spectrum for the cellulose AMIMCl solution (Figure5), out of phase cross peaks were developed for the νC–H alkyl vibrations and imidazolium νC4–H and νC5–H peaks with νO–H. This indicated the intensities of two spectral features change out of phase with each other and that these differing functional groups were experiencing different effects from heating. No asynchronous cross peaks were observed between νO–H and νC2–H peaks. This contrasts the asynchronous spectrum of pure AMIMCl which showed cross peaks between νO–H and νC2–H (Supplementary Material). In this latter case, the cross peaks observed between νO–H and νC2–H were observed in both the pure AMIMCl synchronous and asynchronous spectrums indicating these two changes were not occurring simultaneously, but were either delayed or accelerated. These results were suggestive of both water and temperature influencing imidazolium ion hydrogen bonding with the asynchronous correlations suggesting the presence of cellulose may also impact hydrogen bonding networks given emergence of C4–H and C5–H cross peaks.Two-dimensional correlation spectroscopy of the EMIMOAc cellulose solution revealed positive cross peaks at 3089 and 2981 cm−1 and a relative absence of interaction with the νO–H region in the synchronous spectrum on heating (Figure 7, Supplementary Materials). No cross peaks were observed in the asynchronous spectrum of the heating spectra in this region. This suggests water was not contributing to any imidazolium ion hydrogen bonding differences in EMIMOAc solution on heating. In contrast, on cooling, autopeaks were observed for 3080 cm−1 and the νO–H region with an absence of any correlation peak at 2981 cm−1. This was also the case for pure EMIMOAc in which there was a strong autopeak at 3070 cm−1 and the νO–H region compared to a reduced prominence of the 2978 cm−1 peak. Unlike the cellulose solution, the asynchronous cooling spectrum of pure EMIMOAc (Supplementary Material) has cross peaks at 3030 cm−1 and 2960 cm−1 with the 3330 cm−1 band indicative of water interactions. Collectively, this shows, on cooling, that water also had an effect on hydrogen bonding within EMIMOAc solution. Moreover, this was consistent with the increasing presence of water in this sample on cooling (Figure 4).With the presence of an acetate anion, the carbonyl absorption of EMIMOAc was also analysed by 2D FTIR to determine the extent of any cation-anion hydrogen bonding in EMIMOAc solution (Figure7). Analysis of the cellulose solution revealed cross peaks of the anion (1500–1600 cm−1) with νC–H and νO–H peaks which increase on heating and lessen during cooling. Similarly, for pure EMIMOAc the band at 1602 cm−1 was correlated with the νO–H peak but was decreasing with both the νC2–H (3030 cm−1) and νC–H (2960 cm−1, alkyl) peaks (Supplementary Material). These results suggest that the anion is interacting with the cation C2H and methyl group during heating, but only with the C2H on cooling. Figure 7 shows contrasting behaviour of this carbonyl absorption during cooling together with a cross peak between the νO–H and νC2–H at 3086 cm−1. This provides evidence that the acetate carbonyl (1602 cm−1) is hydrogen-bonded with water and also involved in hydrogen bonding with the imidazolium νC2–H, particularly at lower temperatures consistent with network structure formation [20]. In comparing 2D FTIR analysis for the cellulose solution and pure EMIMOAc, their similarity suggests, at 2%, the cellulose content may not impact hydrogen bonding networks within the ionic liquid. This finding was also consistent with the 2% cellulose content having no impact on the rheology profile (Figure 3).


## 3.3. Discussion

It was evident in FTIR analysis that temperature together with water sorption due to ionic liquid hygroscopicity was influencing the interactions and hydrogen bonding of the imidazolium cation. Water can play a significant role in cellulose dissolution in ionic liquids in addition to impacting hydrogen bonding networks in the ionic liquid [11, 21]. In this study 2D FTIR has revealed temperature can also influence hydrogen bonding networks within the ionic liquids which may manifest in observed rheology profiles. A shift in the νC2–H peak is an indication to the extent of hydrogen bonding [15] with C2–H bond lengthening contributing a red shift to lower wavenumbers. For cellulose in AMIMCl solution the νC2–H absorption was at 3072 cm−1 during heating, but increased to 3093 cm−1 on cooling (Figure 4). This was similarly the case in BMIMCl solution with the νC2–H absorption at 3040 cm−1 on heating and increasing to 3087 cm−1 on cooling (Supplementary Material). This indicated hydrogen bonding of imidazolium ion C2–H was stronger on heating consistent with greater ion mobility at higher temperature. At ambient temperature, there were more cation-anion interactions with the νC2–H frequency blue shifted. Also consistent with heating and cooling effects were other νC–H peak changes indicating the alkyl groups have greater rotational and vibrational freedom at higher temperature when the ionic liquid network structure is broken. FTIR results suggest the higher water contents on cooling enabled water to interact more contributing to a weaker imidazolium-anion interaction and νC2–H peak shift. Furthermore, the presence of cellulose in AMIMCl solution also induced changes in the imidazolium νC–H absorptions which were not observed in the pure ionic liquid. 2D FTIR suggests cellulose may have minimised the water influence on hydrogen bonding, given differences observed between out of phase cross peaks on heating and cooling (Figure 6).With EMIMOAc, theνC2–H peak of pure EMIMOAc was at 3030 cm−1 during heating and blue shifted to 3070 cm−1 during cooling suggesting temperature similarly influenced the extent of imidazolium cation hydrogen bonding as established for AMIMCl. However, cellulose in EMIMOAc solution contributed to a narrower range in the νC2–H peak shift (3080–3089 cm−1) indicating a relatively minimal influence on νC2–H hydrogen bonding due to temperature. Moreover, results show the anion to be interacting with C2H together with other imidazolium C–H and methyl groups. Potentially this indicates differences in the extent of interactions between the imidazolium ion and acetate and chloride anions in cellulose solutions with EMIMOAc and AMIMCl, respectively. The νOH peak also contributed a dominant influence on hydrogen bonding due to water sorption on cooling.FTIR spectra show a gradual change in imidazolium ion hydrogen bonding between 25 and 100°C, on both heating and cooling. At lower temperatures there were closer interactions between cations and anions indicative of a network structure in the ionic liquids. The shear applied to the ionic liquid solutions was sufficient to break this network, with this observed as transitions under shear at key temperatures in Figures1 and 3. These transitions resulted in significant inflexions in rheology storage modulus values which were not distinguished by FTIR at these temperature steps, perhaps as FTIR was undertaken without solution shear. Furthermore, there was a rheological hysteresis evident between heating and cooling. With decreasing temperature there is apparent super cooling and gel formation [1] leading to slower network organisation within the liquid, observed below 40°C. However, on heating, initially the ionic liquid network structure is greater and the effect of shear not evident until a higher temperature (50–70°C), being common to both ionic liquids (Figures 1 and 3). The presence of cellulose increases the ionic liquid viscosity (Figure 2), but has minimal effect on initial heating (Figures 1 and 3) as the ionic liquid network structure is dominant. Only on cooling and gel formation was the presence and quantity of cellulose observed to impact rheology. Moreover, given the impact of cellulose observed by 2D FTIR it can be expected cellulose plays an increasing role in hydrogen bonding in AMIMCl at higher concentrations whereas in EMIMOAc any impact of cellulose was observed at ≥4% concentration.


## 4. Conclusion

Oscillatory shear experiments reveal a dependency of temperature and cellulose content on rheology profiles of AMIMCl, BMIMCl and EMIMOAc cellulose solutions which also manifest in viscosity profiles on heating and cooling. Use of two-dimensional FTIR shows dynamic hydrogen bonding between the imidazolium cation and anion on heating and cooling which was also impacted by the presence of cellulose and moisture sorption. A red shift of the imidazoliumνC2–H peak on heating indicated hydrogen bonding of the cation was stronger consistent with greater ion mobility and loss of the ionic network structure with temperature. These FTIR spectral changes appeared gradual with temperature and contrast shear induced rheology changes which were observed on heating above 70°C and cooling below 40°C. The presence of cellulose increases ionic liquid solution viscosity, but this was not distinguished in solution rheology on initial heating as the ionic liquid network structure dominates. On cooling, the quantity of cellulose has a greater influence on solution rheology with this also expected to influence the processing of cellulose solutions at temperature. Practically, the results of this study suggest the processing of cellulose in ionic liquids to be undertaken above 40°C and, to reduce the impacts of cation-anion effects and enhance ionic liquid solubilisation, processing should be done at 70°C.



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*Source: 958653-2015-11-01.xml*