Open access peer-reviewed chapter

Molecular Interactions in Ionic Liquids: The NMR Contribution towards Tailored Solvents

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Mónica M. Lopes, Raquel V. Barrulas, Tiago G. Paiva, Ana S.D. Ferreira, Marcileia Zanatta and Marta C. Corvo

Submitted: May 8th, 2019 Reviewed: August 14th, 2019 Published: September 30th, 2019

DOI: 10.5772/intechopen.89182

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Abstract

Ionic liquids have been on the spotlight of chemical research field in the last decades. Their physical properties (low vapor pressure, thermal stability, and conductivity) and the possibility of fine tuning make them a versatile class of compounds for a wide range of applications, such as catalysis, energy, and material sciences. Ionic liquids can establish multiple intermolecular interactions with solutes such as electrostatic, van der Waals, or hydrogen bonds. The prospect of designing ionic liquid structures toward specific applications has attracted the attention to these alternative solvents. However, their rational design demands a molecular detailed view, and Nuclear Magnetic Resonance is a unique and privileged technique for this purpose, as it provides atomic resolution and at the same time enables the study of dynamic information. In this chapter, we provide an overview about the application of Nuclear Magnetic Resonance spectroscopy techniques as a methodology for the rational design of ionic liquids as solvents for small organic compounds, CO2 capture, and polymers such as cellulose focusing mainly in the last 10 years.

Keywords

  • ionic liquids
  • nuclear magnetic resonance spectroscopy
  • molecular interactions
  • chemical shift deviations
  • nuclear Overhauser effect
  • solute/solvent

1. Introduction

Ionic liquids (ILs) can be defined as ionic species that melt under 100°C. These materials are usually made from organic cations such as imidazolium, ammonium, pyrrolidinium, or phosphonium, and organic or inorganic anions such as chloride, bromide, tetrafluoroborate, or bis(trifluoromethylsulfonyl)imide ( Figure 1 ). Their physical properties, namely low vapor pressure, thermal stability, and conductivity grant them the status of alternatives to organic solvents in a wide range of applications, from catalysis and energy applications to material sciences. These properties are a direct consequence of the identity and interactions between the cations and the anions; however, the vast number of possible combinations hampers the tailoring of ILs as solvents for specific applications. In order to establish the desired structure-property relationships, a molecular understanding on structure and interactions is required. Nuclear Magnetic Resonance (NMR) techniques enable this study by allowing to probe both cations and anions through several nuclei (1H, 13C, 19F, 35Cl, 11B, 15N, and 31P). In addition, the use of chemical shift deviations, relaxation, NOE, and diffusion experiments allows advanced studies about cation-anion-solute interactions and consequently facilitates the design and IL applications.

Figure 1.

Common cation and anion structure of ILs. The abbreviations used in this chapter are described in Section 7.

As solvents, ILs can establish several attractive interactions that range from weak, nonspecific, and isotropic forces such as van der Waals, solvophobic, and dispersion forces, to strong interactions as Coulombic forces and anisotropic forces such as hydrogen bonds (H-bonds), halogen bonds, dipole-dipole, magnetic dipole, and electron pair donor/acceptor interactions. The diversity and strength of intermolecular forces in ILs are responsible for the local arrangements in bulk and interface [1].

NMR enables the study of structure and dynamics in ILs providing information that allows the rationalization of the solvation behavior [2, 3]. Thus, by obtaining the profile of IL molecular interactions, it is possible to select and optimize the cation and anion identity and their relation to solvated species. In particular, the use of multinuclear NMR experiments and homo and heteronuclear correlation protocols enables the in-situevaluation of cation-cation, cation-anion, anion-anion, and also IL-solute relationships.

In neat imidazolium ILs (ImILs), H-bonds are formed between the cation and the anion. This attractive force in which hydrogen nuclei are bound to electronegative atoms such as nitrogen, oxygen, or fluorine is mainly felt by the aromatic protons of the imidazolium cation (H2, H4, and H5) and establishes a regular network. When a H-bond is formed, the hydrogen’s electron density is pulled by an electronegative atom, leading to a deshielding of this nucleus and consequent positive chemical shift deviation (∆δ). If a H-bond is weakened or broken, the opposite occurs, leading to a negative ∆δ. The addition of a solute to the IL can establish additional H-bonds and also introduce perturbations to the regular network, either reinforcing the interaction between cation and anion (positive ∆δ) or weakening (negative ∆δ) ( Figure 2I ) [4, 5].

Figure 2.

NMR experimental techniques used to probe molecular interactions in ILs.

The nuclear Overhauser effect (NOE) is commonly used to study local structure in liquids and solutions. Considering the two nuclear spins, Iand S, the magnetization transfer through coupling of their magnetic dipole moments produces a cross-relaxation and a consequent NOE ( Figure 2II ). Increasing the internuclear distance (r), the cross-relaxation rate decays with 1/r6. Thus, a NOE is only felt if ris less than 4–5 Å. Although this theory still holds for intramolecular distances, a new concept was introduced by Gabl et al. to analyze intermolecular NOE in ILs. According to these authors, the distance rule is strongly dependent on the frequencies of the interacting nuclei and can instead vary with 1/r. Site-specific NOE should be interpreted cautiously as it can reflect the mean orientation of the ions over longer distances, rather than the local structure of distinct ion aggregates. Nevertheless, homonuclear (NOESY) and heteronuclear NOE (HOESY) studies have been widely used to analyze intermolecular interactions of solutes with ILs [6, 7, 8].

In ILs, the self-diffusion coefficients in solution can be measured through diffusion ordered spectroscopy (DOSY) providing a means to understand charge transport properties. In particular, using pulsed field gradient NMR (PFG-NMR), the spatial positions of the nuclei are encoded by magnetic field gradients, in which the signal intensity attenuation is correlated with the diffusion time (Δ) and the gradient-related parameters (g, δ) [9]. Multinuclear diffusion measurements can give access to anion and cation self-diffusion coefficients ( Figure 2III ); however, since ion-pair interactions take place on a timescale faster than the diffusion, the coefficients are a weighted average of charged and neutral species [10].

A deeper insight into atomic level interactions comes from NMR relaxation techniques ( Figure 2IV ). NMR spin-lattice (T1) and spin-spin (T2) relaxation measurements allow the study of reorientation dynamics in ILs and the analysis of inter- and intramolecular interactions [11, 12, 13].

Overall, probing intermolecular interactions in ILs through simple 1D NMR spectrum analysis (∆δ), or more complex relaxation phenomenon, NOE experiments, and diffusion provides an understanding of the interplay between ILs and solutes. The following sections highlight several examples where NMR techniques were used to tailor ILs.

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2. Interactions between ionic liquids and small organic molecules

The optimization of liquid-liquid extraction processes for small organic molecules with organic solvents usually requires high investment and large energy consumption due to unfavorable capacity and selectivity [14]. Since this process is common in many industrial areas, more sustainable procedures are required in order to reduce organic solvent volatiles. Usually, an efficient separation of azeotropic systems containing the mixtures of aromatic/saturated hydrocarbons or alcohols/aliphatic hydrocarbons is difficult to obtain because of similar boiling points and several possible azeotropes. In this field, ILs have been cited as an alternative solvent, since they can provide an enhanced solvation capability while having negligible vapor pressure [14, 15]. The efficiency of ILs for absorption of aromatic compounds is determined by the size and structure of both cations and anions, as well as the molecular structure of the aromatic compounds. This section will focus on IL-aromatic molecule interactions consisting of two main groups: (i) unsubstituted and (ii) substituted aromatic molecules.

2.1 Unsubstituted aromatic molecules

Kumar and Banerjee reported that smaller IL cations enhanced the extraction capability for aromatic compounds [16]. Later, Potdar et al. studied binary mixtures of [C2C1Im]+ with [C1SO4], [C2SO4], and [C1SO3] as counterions to extract benzene from hexane, measuring the equilibrium compositions by 1H NMR spectroscopy [14]. [C2C1Im][C2SO4] achieved higher selectivity and capacity than IL binary mixtures. The combination of two ILs could result in lower free volume than a single IL, and benzene molecules would be unable to penetrate the core of the solvent.

Other studies in 2014 by Dias et al. reported interactions between benzene and [C2C1Im][NTf2], through several NMR experiments, namely, 1D 1H and 13C spectroscopy and 2D 1H,1H-NOESY spectroscopy [17]. In the mixture of benzene with [C2C1Im][NTf2], H2 presented a lower chemical shift (more shielded) than neat IL, which indicated that the cation was positioned above and below the aromatic ring plane, and the anion was located in the same plane as benzene protons [17, 18]. Early works on the absorption of aromatic sulfur compounds by Su et al. studied the interaction between thiophene and [C4C1Im][PF6], [C4C1Im][BF4], and [C2C1Im][BF4], through 1D 1H, 19F, 11B, and 31P spectroscopy [19]. The ring current effect in neat thiophene was stronger than in neat [C4C1Im][PF6], because in the former, molecules were tightly packed, whereas in the IL, [C4C1Im]+ cations were separated by [PF6] anions. The bulky [PF6] prevented [C4C1Im]+ cations from coming close and reduced the aromatic current effect. In [C4C1Im][PF6]/thiophene mixture, an upfield shift in [C4C1Im]+ protons was explained as a result of the CH-π interaction between [C4C1Im]+ and thiophene aromatic ring. The trend of ∆δ indicated that [C4C1Im]+ was in the shielding cone of thiophene ring current and the thiophene was located near the deshielding zone of [C4C1Im]+ ring current. In addition, thiophene is not a good H-bond acceptor because the unpaired electrons of sulfur participate in the aromatic ring current and may carry a partial positive charge. The [PF6] anion was a potential hydrogen acceptor but introduced a downfield shift. The dilution of [C4C1Im][PF6] by a neutral molecule like thiophene was not expected to break apart the strong Coulombic interaction between [C4C1Im]+ and [PF6] ions significantly by a simple insertion between them. The electric field effect risen from the physical interaction between fluoro-based anions and cations or thiophene was not a dominant factor in determining the IL absorption capacity for thiophene. The upfield shift effect was strongest for the ring protons in the imidazolium cation followed by the methyl and methylene protons next to the nitrogen. The further away the protons were from the ring as in 1-butyl or 1-ethyl groups, the weaker the upfield shift effect became. Therefore, thiophene molecules must locate close to the ring of the IL’s imidazolium cation. The CH-π interaction between the acidic hydrogen of cation and thiophene was not as important as the π (imidazolium ring)-π (thiophene ring) interaction. Apparently, the aromatic ring current effect (π-π interaction) is the dominant factor to determine the ∆δ trend in these IL systems. The chain length of the imidazolium alkyl group and the size and character of anion affected the coordination number and geometric arrangement of thiophene molecules relative to IL’s cations and anions. The stacking structure of the cation and anion was tightest for the neat [C2C1Im][BF4], followed by [C4C1Im][BF4] and [C4C1Im][PF6]. Therefore, the negative charge of [BF4] anion in the [C2C1IM][BF4] was spread more around fluorine atoms and less around boron than those in the [C4C1Im][BF4] system. It also suggested that the [BF4] anion in the [C2C1Im][BF4] system is more basic and interacts more intimately with the imidazolium cation than in [C4C1Im][BF4]. The NMR results suggested that the partial positive charge in thiophene sulfur should direct the anions outside the thiophene plane. Overall, the aromatic ring current interaction between the imidazolium cations and the thiophene was responsible for the absorption of aromatic sulfur compounds in ILs [19].

Revelli et al. studied the interaction of thiophene with [C1C1Im][(C1O)PHO2] and [C4C1Im][SCN], using 1H and 31P NMR spectroscopy [15]. The dilution of [C4C1Im][SCN] by thiophene did not lead to a visible 1H ∆δ; therefore, thiophene did not break apart the strong Coulombic interactions between cation and anion. Indeed, phase equilibria of [C4C1Im][SCN]/thiophene system indicated that thiophene had low solubility in this IL. The acidic hydrogen atoms of the imidazolium cation formed weak H-bonds with the sulfur of thiocyanate anions. 1H NMR chemical shifts of the ring protons in neat thiophene were more upfield than those in neat [C4C1Im][SCN], indicating, as previously, that the aromatic ring current effect was stronger in neat thiophene than in neat [C4C1Im][SCN]. The bulky [SCN] anion prevented the [C4C1Im]+ cation from coming close, thus greatly reducing the aromatic current effect. Similar studies were made to unveil the interactions between thiophene and [C1C1Im][(C1O)PHO2]. The ∆δ of thiophene and [C1C1Im][(C1O)PHO2] followed the same trend as in [C4C1Im][SCN]. The chemical shifts of thiophene protons were more downfield when the thiophene is in a mixture of IL, although the IL proton chemical shifts were upfield. The 31P chemical shifts were measured at several molar ratios of thiophene in [C1C1Im][(C1O)PHO2], but no ∆δ was observed; hence, the interactions between thiophene and anion are weak. The most prominent features in the vicinity of thiophene are an excess of cations in the polar regions above and below the ring and an excess of anions around the equator of thiophene. In the end, [C4C1Im][SCN] is a promising IL to act as a solvent for desulfurization [15].

Kaintz et al. contributed to the measurements of solute diffusion in IL solutions through infinite dilution, since it eliminates solute-solute interactions. The authors studied the interactions between [CnC1Pyr][NTf2] (n= 3, 4, 6, 8, and 10) and [P6,6,6,14][NTf2] and naphthalene, anthracene, pyrene, and biphenyl, through pulsed field gradient 1H NMR. Within the selected set of aromatic solutes and pyrrolidinium ILs, no dependence was found on solute dipole moment. Neither was there any evidence that the polar/nonpolar domain formation in the higher homologs of the [CnC1Pyr][NTf2] series or in [P6,6,6,14][NTf2] influences diffusion of solutes as small as benzene. Through Stokes-Einstein predictions, it was possible to observe that self-diffusion in ILs is like self-diffusion in conventional solvents. However, the relation to solute/solvent size ratio was greater in ILs than in conventional solvents [10].

2.2 Substituted aromatic molecules

2.2.1 Polyphenols (Catechins)

Barrulas et al. gave an important contribution for the NMR study of interactions between ILs and small molecules [20]. The articles so far were not very complete in terms of the NMR experiments available, lacking always some proof of concept. Extracts from plants like matcha green tea have considerable significance as bioactive compounds with several pharmacological applications, namely polyphenols (being catechins the most prevalent). Nonetheless, the amount of these compounds in the extracts is typically very low. Consequently, green extraction techniques with higher efficiency for phenolic compounds are of paramount importance, in which ILs can be used as designer solvents. In order to rationalize the interactions, several model compounds were selected – naphthalene to study π-π stacking, veratrole, L-3,4-dihydroxyphenylalanine (L-DOPA) to understand the behavior of the phenol moiety toward H-bonds and hydrophobic interactions, and 1,2-dihydroxyanthraquinone (alizarin) in order to study all the interactions simultaneously. Several ILs were tested: [C4C1Im]Cl, [BzC1Im]Cl, [C2C1Im]Cl, [C4C1C1Im]Cl, [C2C1Im][OTf], [C2C1Im][TCM], [C2C1Im][DCA], and [C4C1Im][OTf]. The solutions resulting from the mixture of the ILs and the model compounds were tested through 1H-DOSY and 1H,1H-NOESY NMR experiments ( Figure 3 ). Both the IL cation and anion had an influence on the solvent behavior.

Figure 3.

2D 1H,1H-NOESY spectrum with 200 ms mixing time of [C4C1Im]Cl/naphthalene mixture [0.16:0.16 (M/M) in DMSO-d6] and main intermolecular interactions (adapted from Ref. [20]).

The best ILs for extracting matcha polyphenols were imidazolium derivatives with shorter alkyl sidechains and weakly basic anions such as [TCM], [DCA], and [OTf]. Finally, it was possible to locate π-π stacking and hydrophobic interactions in case of the cation and H-bond acceptor interactions in case of the anion [20].

2.2.2 5-Hydroxymethylfurfural

Nowadays, searching for new sources of green energy is crucial. Biomass is receiving attention, since the reserves are abundant, the price is low and is renewable. The preparation of 5-hydroxymethylfurfural (5-HMF) from biomass is a very interesting topic, since this compound is applied in the production of high value-added chemicals and biofuels [5, 21]. Thus, new high-efficiency reaction medium for the preparation of 5-HMF is needed, and ILs are suitable alternatives. Mixtures of 5-HMF and ILs with anion [NO3] and different cations [C4C1Im]+, [C4Py]+, [C4C1Pyr]+, [CnC1Pip]+, and [N1,1,1,H]+ were studied and presented strong intermolecular interactions. In order to unveil the chemical nature of such interactions, 1H NMR experiments were done for different ILs/5-HMF systems, and the ∆δ of each proton was estimated [5]. In [C4Py][NO3], the H-bond between the anion and the cation was mainly formed by O atom in [NO3] and H2, H5 atoms that were close to the N atom of the pyridine ring [5, 22]. Therefore, the upfield movement of H2 and H5 protons indicated that the input of 5-HMF into ILs weakens the H-bonding between anion and cation. With the addition of 5-HMF into ILs, the π-π interactions between pyridine rings became weaker and the shielding effect was strengthened, causing the protons of the alkyl chain in cation upfield shift. Based on 1H,1H-NOESY experiments, it was seen that the addition of 5-HMF induced the change of alkyl chain conformations, from gauche to trans. With the exception of [C4C1Pyr]+ and [CnC1Pip]+, [C4C1Im]+, [C4Py]+, and [N1,1,1,H]+ could form H-bonds with hydroxyl group in 5-HMF, and this capacity increased as follows: [C4Py]+ ≈ [C4C1Im]+ < [N1,1,1,H]+. 5-HMF could strongly bind IL anions, while the H-bond interaction of 5-HMF with the cation was much weaker. Also, the interactions between the carbonyl group of 5-HMF and the cation of ILs were also very weak. Therefore, the cation impacted the interaction of 5-HMF with ILs through its interaction with the anion [5].

2.2.3 Fluorinated derivatives of benzene

Dias et al. studied the interactions between mixtures of [C2C1Im][NTf2] with benzene (discussed in Subsection 2.1), fluorobenzene, 1,2-difluorobenzene, 1,4-difluorobenzene, 1,3,5-trifluorobenzene, 1,2,4,5-tetrafluorobenzene, pentafluorobenzene, and hexafluorobenzene through 1D 1H NMR and 13C NMR and 2D 1H,1H-NOESY NMR spectroscopy [17]. Relative to 1H NMR, it is important to highlight that proton H2 was the most interactive site (most acidic proton) of the imidazolium cation, which means that any perturbation in the polar network of the IL was felt at this position. In case of the benzene mixtures, the aromatic protons exhibited larger shielding shifts than their aliphatic counterparts; thus, in case of [C2C1Im][NTf2]/1,2-difluorobenzene mixtures, the H2 protons exhibited small shielding shifts as the aromatic molecule concentration increased. At higher concentrations, these turned into small deshielding shifts. The aliphatic protons showed intermediate shielding shifts, and the H4/H5 protons displayed the largest shielding shifts. In case of [C2C1Im][NTf2]/hexafluorobenzene mixtures, most shifts were deshielding through the order of H2 > H6−H8 > H4/H5. When the aromatic molecules are interspersed in the polar network of the IL, there is a competition between the interactions with the oxygen atoms of the [NTf2] anion (OBT) and the π electrons or fluorine atoms of the aromatic solute. The polar network was stronger at the H2−OBT contacts than at the H4/H5−OBT contacts. This led to a higher proportion of H4 and H5 protons interacting with the solute molecules, relative to H2 interactions. With 13C NMR, it was possible to observe that the carbon atoms attached to hydrogen atoms experienced small shielding shifts in the benzene mixtures that changed to larger deshielding shifts in mixtures with more fluorinated aromatic molecules. The carbon atoms linked to fluorine atoms experienced deshielding shifts in the hexafluorobenzene mixtures that became progressively larger shielding shifts in mixtures with less fluorinated aromatic molecules. 2D NOESY spectra of the equimolar mixtures of [C2C1Im][NTf2] with 1,4-difluorobenzene and pentafluorobenzene identified a cross-peak between the H8 protons of the IL and the protons of the aromatic molecule. Summing up, in benzene, the cations are mainly located above and below the aromatic plane, experiencing the diamagnetic influence of the aromatic electrons. As the aromatic ring becomes much more fluorinated, the cations migrate to the equatorial plane of the aromatic molecule, to a region of milder paramagnetic effect.

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3. Interactions between ionic liquids and CO2

NMR spectroscopy allows the direct measurement of CO2 solubility as well as the evaluation of intermolecular interactions and sorption mechanism [23, 24]. Since ILs exhibit the ability to tailor many of their physical and chemical properties, such as gas solubility, they have been extensively studied in CO2 sorption. Different sorption mechanisms can be observed according to the site and the strength of CO2/IL interaction. Therefore, according to the CO2 sorption mechanism, the ILs can be divided into three main groups: physisorption, chemisorption, and water sorption ( Figure 4 ).

Figure 4.

Summary of CO2-IL interactions observed by NMR experiments.

In general, CO2/anion interactions are preferential in comparison to CO2/cations; therefore, the classification of ILs in these three groups is mainly based on the anion functional group and respective IL properties. Non-basic nucleophilic anions capture CO2 through a noncovalent pathway, and these anions belong to the first group. Basic anions that can form covalent bonds with CO2 molecule belong to the second and third groups. Besides the functional groups of the anions and the mechanism of sorption, the main difference between ILs of the second and third groups is the products that are formed, since the third group reacts with the water existing in the IL.

Furthermore, the pressure and temperature may also affect CO2 solubilization. For lower pressure applications, the chemisorption is favored; meanwhile, increasing the pressure, physisorption becomes preferential. A smart selection of pressure and IL structure is essential to develop a higher CO2-philic material. It is important to mention that all CO2 capture mechanisms can occur simultaneously in a single IL. In this context, the NMR spectroscopy allows direct measurement of CO2 solubility, intermolecular interactions, and sorption mechanism and performs in situhigh pressure experiments. Therefore, the NMR is a powerful technique for designing ILs with high steric hindrance and low viscosity to capture CO2 efficiently and selectively [23].

3.1 Noncovalent interactions—physisorption

To design an efficient sorbent for CO2 capture, CO2 transport properties need to be understood. In physisorption, the surface area of IL attracts CO2 molecules by van der Waals forces. In this case, CO2 sorption occurs mainly in ILs containing nonbasic-nucleophilic anions, like fluorinated anions. Based on 3D structures of ImILs that create ion cage-like structures with void spaces capable of confining CO2, several NMR techniques were being used to study the capability of ImILs to absorb CO2 and understand IL/CO2 interactions.

Corvo and co-workers studied [C4C1Im][PF6], [C4C1Im][BF4], and other fluorinated ILs with slight changes in the aliphatic substituent as chain branching or elongation, such as [(iPr)C2C1Im][NTf2] and [C4C1Im][NTf2], respectively. The cation/anion, cation/cation, cation/CO2, and anion/CO2 interactions were analyzed through NOE, DOSY, and relaxation experiments, at 10 and 80 bar, combined with molecular dynamics (MD) simulations ( Figure 5 ) [24, 25].

Figure 5.

(A) 1H,19F-HOESY spectra with 400 ms mixing time of [(iPr)C2C1Im][NTf2]: (a) neat IL at 298 K; (b) mixed with 10 bar CO2 at 298 K; (c) neat IL at 313 K; (d) mixed with 80 bar CO2 at 313 K; (B) 13C,1H-HOESY spectrum of [(iPr)C4C1Im][NTf2], with 10 bar of 13CO2 at 298 K; (C) 13C ,1H-HOESY spectra (500 ms mixing time) of [C4C1Im][PF6], mixed with 13CO2 at 298 K and 11 bar; (D) 13C,19F-HOESY (400 ms mixing time) of [C4C1Im][PF6], mixed with 13CO2 at 298 K and 11 bar (adapted from Refs. [24,25]).

The comparison of 1H-1H NOE cross-peak intensity in the presence and absence of CO2 showed the direct cation/cation interactions. Cross-peaks between the methyl group and the methylene of the aliphatic chain are particularly informative because they reflect only intercationic interactions. From the NOESY data for neat IL and IL/CO2 solutions, it was possible to conclude that at 80 bar, the pattern of cation/cation interactions changes considerably with the correlations between protons of the methyl group H10 (NCH3) and the sidechain protons H7/8 almost absent from the spectra.

1H,19F-HOESY experiments showed essentially the cation-anion contacts. Due to the geometry of the anion, the [NTf2] in ImIL was near to the terminal methyl groups (RCH3 and NCH3) in linear and branched chain. After CO2 dissolution, the similarity on the cross-peak intensity from the 1H,19F-HOESY experiment indicated that the cation/anion contacts were mostly the same as in the neat ILs ( Figure 5a ). The main differences between the neat ILs and the IL/CO2 mixtures indicated the locations that were mostly affected by CO2 solvation. At 10 bar of CO2, the aromatic protons H4/H5 presented stronger correlations with the anion and also the methyl group NCH3. At 80 bar of CO2, the fluorine contacts with the nonpolar domains, specifically with the methylene protons and the methyl groups, decrease slightly. As Figure 5b demonstrates, in the 13C,1H-HOESY spectra of [(iPr)C2C1Im][NTf2]/CO2 mixture, CO2 was located around the methyl group RCH3 and the isopropyl methyl group, proving the direct cation-CO2 interactions. The HOESY experiments also indicate that increasing CO2 pressure may lead to the deformation of the ion cage structure of the ILs, accommodating more CO2 molecules.

13C,1H-HOESY and 13C,19F-HOESY experiments proved cation-CO2 and anion-CO2 interactions. Analyzing the 13C, 1H-HOESY spectra from the [C4C1Im][PF6], at 10 bar using 13C-labeled CO2 was possible to notice strong interactions between CO2 and the aromatic protons H4/H5, the methyl group RCH3 of alkyl chain and the methyl protons of NCH3 ( Figures 5b , c ). In the same way, the 13C,19F-HOESY experiment confirmed the existence of direct anion-CO2 interaction ( Figure 5d ).

By using 13C-T1NMR relaxation experiments, it was possible to conclude that at low pressure, the solubilization of CO2 has a minimum effect in the global mobility of the IL. Meanwhile, the opposite was observed for higher pressure (80 bar). Taking into consideration all the experimental data, it was possible to conclude that the physisorption of CO2 occurs in the cavities near methyl groups NCH3 and RCH3 and aromatic protons H4/H5 [24, 25].

Taking advantage of known physical sorption of CO2 in [C4C1Im][NTf2], Allen and Damodaran had chosen this IL to evaluate the diffusion of CO2 in ILs. Slice-selective inverse gated pulse field gradient technique was employed and demonstrated as an excellent alternative to study gas dynamic solvation under non-equilibrium conditions in a method similar to magnetic resonance imaging (MRI) [26].

3.2 Covalent bond—chemisorption

Many ILs have previously been reported as physical sorbents for CO2, under different pressures. More recent studies described the capability of ILs to interact through a chemical pathway with CO2, under low pressures. ILs that contain reactive functional groups, usually N or O moieties on the cation or the anion, can bond covalently with CO2, which results on the formation of carbamates or carboxylates, respectively. 1D and 2D NMR techniques can easily prove the chemical CO2-IL interactions.

3.2.1 Carboxylates

Due to the possibility of chemical sorption between CO2 and the 2-position of the imidazolium ring, ImILs with carboxylate anions have been intensely studied. In 2012, through the 13C NMR analysis, the chemical reaction and the formation of 1,3-dialkylimidazolium-2-carboxylate and acetic acid were reported for the first time, by Blath and co-workers and Danten and co-workers. Both proposed a mechanism of the CO2 absorption [27, 28, 29].

Danten and co-workers started their study with the comparison between the 13C NMR spectra of the pure IL with the CO2-IL mixture and observed a new signal ca. 155 ppm connected with the CO2.

The comparison of the 15N NMR spectra of the pure IL with the IL/CO2 mixture proved the carboxylation into imidazolium ring by the observation of two intense signals at 183.7 and 171.6 ppm assigned to the nitrogen atoms of the ring core. In the mixture, two additional resonance signals flanking each of the previous peaks were observed at 182.1 and 170.0 ppm, respectively ( Figure 6a ). The 2D 1H,15N-HMBC spectra of the mixture proved the correlation between the new signals and the secondary peak observed in the 1H NMR spectrum of the IL/CO2 mixture ( Figure 6b ).

Figure 6.

(a) 15N NMR spectra of the neat [C4C1Im][OAc] and [C4C1Im][OAc]/CO2 mixture; (b) correlation in 1H,15N-HMBC of [C4C1Im][OAc]/CO2 mixture; (c) 13C NMR spectra of the neat [C4C1Im][OAc] and [C4C1Im][OAc]/CO2 mixture; (d) 13C NMR INADEQUATE of [C4C1Im][OAc]/CO2 mixture (adapted from Ref. [28]).

To understand the favored chemical site among the three possibilities (C4/C5 and C2), the 2D spectrum using the INADEQUATE sequence was performed. The C2 signal of the [C4C1Im]+ cation (138.3 ppm) was not correlated with the two new peaks located at 155.3 and 141.6 ppm ( Figure 6d ). These two peaks were correlated showing the formation of a new species in which CO2 is covalently bonded to the C2 of the imidazolium ring ( Figure 6c ) [28, 29].

Another similar study lead by Kortunov, employing non-aqueous [C2C1Im][OAc], supported these conclusions. Once again, the presence of the signal at 155.3 ppm in the 13C NMR spectrum indicated the presence of the carboxylate complex. To reinforce this idea, the 1H,13C-HSQC and 13C DEPT-135 NMR experiments were executed, neither the new carbon peaks (141.5 and 155.1 ppm) have protons directly attached nor the new proton signal (15.7 ppm) has any carbon attached [30].

Other essential work using carboxylate anions has been published by Umecky and co-workers. The authors prepared task-specific ImILs with 2,4-pentanedionate and fluorine derivatives to use as CO2 chemical absorbents. The experiments were performed in neat IL and in dichloromethane solution (50 vol%) by bubbling CO2. A comparison of 1H NMR spectra among the fluorinated and carboxylate anions showed that the acidity of the hydrogen atom at the 2-position strongly influences the CO2 sorption capacity. The chemisorption of CO2 is governed not only by the anion basicity but also by the acidity of H2 and the possibility of its abstraction. By using 2D analysis (HMQC and HMBC), it was possible to prove the formation of a complex between [C2C1Im]+ and CO2. In those conditions, the influence of dissolved water and consequently the formations of the carbonate (CO3 2−) and bicarbonate (HCO3 ) were negligible [31].

Ether-functionalized ImILs were also capable of capturing the CO2 physically and chemically. The physisorption was proved by Seo et al. and the chemisorption by Sharma et al. Both studies were accomplished through 13C NMR and FTIR techniques. Sharma et al. proposed a mechanism for the formation of the carboxylic acid based on ca. 205 ppm signal in the 13C NMR [32, 33].

3.2.2 Amines

The use of ILs containing a basic amine group (task-specific ILs) to capture CO2 by chemical reactions was reported for the first time by Davis group [34]. After that, amine-based ILs have been the focus of many works, due to their highly efficient capacity on gas solubilization. Generally, the aqueous solution of primary and secondary amines reacts with CO2 yielding carbamates. On the other side, the reaction between CO2 and the tertiary amine depends on water amount in the system. The formation of carbamate and bicarbonate has been demonstrated; however, the reaction is still a critical point of discussion and merits further investigations [35, 36].

Combining the idea of low toxicity and high reactivity toward CO2, a series of choline-based amino acid ILs were reported by Bhattacharyya and Shah. DFT calculations, IR, and NMR spectroscopic techniques were employed to examine the mechanism of the CO2 interaction with ILs. The 1H, 13C, and 1H,1H-COSY NMR analysis of [N1,1,6,2O4][Lys] demonstrated the signals shifted during the sorption procedure. In 13C NMR spectrum, three new signals were observed: ca. 178 ppm attributed to carboxylate anion with a strong intermolecular hydrogen bonding; at 160.9 and 163.7 ppm attributed to the formation of carbamic acid and carbamate anion, respectively [37].

The CO2 dissolution and the ionic mobility by diffusion experiments of choline-based ILs [N1,1,6,2O4]+ with [Threo] and [Im] anions were investigated by the same group. Once again, the formation of carbamic acid and carbamate anion ([Threo]–CO2) was observed after CO2 capture, by the presence of characteristic peaks (160.4 and 164.0 ppm) in 13C NMR spectrum. In addition, the [Threo] alpha proton represented by a doublet at 3.11 ppm shifted to 3.43 ppm, whereas the beta protons at 3.94 ppm shifted to 4.16 ppm and the methyl proton from 1.20 to 1.29 ppm after CO2 reaction. By contrast, the 1H NMR spectrum of [N1,1,6,2O4][Im] did not show significant ∆δ after CO2 absorption. However, in the 13C NMR spectrum, a new signal at 160.8 ppm was observed and attributed to the formation of a carbamate specie. Both neat ILs demonstrated broadened signals in 1H NMR spectra, particularly after CO2 absorption. Using the diffusion decays of the stimulated spin echo, it was possible to observe that the diffusion of anion and cation was not affected by CO2. The diffusion behavior of both ILs before and after absorbed CO2 was also studied in a temperature range of 20–90°C. The diffusion of cations and anions changes by the same factor regardless of temperature. From the observed 1H diffusometry results, the mobility increased for [Im] IL after CO2 sorption and decreased for [Threo] anion. The authors explained this behavior based on the decrease in the aromaticity and electron density volume of the imidazolate by the formation of carbamate due to CO2 reaction [38].

Over the last few years, NMR techniques have proven that the reaction between CO2 and 1,3-dialkyl imidazolium cation is strongly dependent on the anion [27]. Chen et al. demonstrated that some functionalized ILs can interact physical and chemically with CO2, by studying the behavior of [aC2C1C1Im][BF4] with this gas. After CO2 capture, the 1H NMR spectrum showed duplicate signals and the 13C NMR spectrum showed two new peaks, proving that part of [aC2C1C1Im][BF4] interacts with CO2 chemically, producing carbamic acid IL-NHCOOH (ca. 163 ppm), and the remaining [aC2C1C1Im][BF4] interacts with CO2 physically (ca. 160 ppm) [39].

More recently, the influence of CO2 sorption in ion mobility in aqueous solution (50/50 wt%) of similar choline-based amino acid ILs was evaluated by Filippov et al. Similar to their previous work, they proposed a mechanism of CO2 sorption in IL containing amino acid anion (such as [Threo]) process by carbamic acid and carbamate anion formation, proved by the presence of the signal ca. 159 ppm. While the water diffusivity was not affected by the absorption of CO2, the increase in ion mobility upon CO2 chemisorption was demonstrated by employing 1H and 13C NMR diffusion experiments [40].

Brennecke’s group prepared a series of alkyl-phosphonium cation ILs with aprotic heterocyclic anions (AHAs) and studied the CO2 capture in dry and wet conditions. All anions correspond to a tertiary amine incorporated into a heterocyclic ring: indazolide, imidazolide, pyrrolide, pyrazolide, and triazolide-based anions. In dry conditions, they suggested a formation of carbamate species, via Lewis acid-base interaction. Comparing the 1H NMR chemical shifts of the dry with wet protonated-heterocyclic anions, they concluded that the [P6,6,6,14][2-CNPyr] did not suffer from the anion reprotonation in the presence of water and CO2, and the opposite trend was previously reported by them for [P6,6,6,14][Pro]. In that case, due to reprotonation and deactivation of the anion, the water reduced the CO2 molar capacity. Even though they did not discard the bicarbonate formation from CO2 and water, they believed that the amount of bicarbonate formed was not expected to be prevalent enough at such low CO2 pressure. For the [P6,6,6,14][2-CNPyr], the addition of 5 wt% of water increased the CO2 solubility, and the authors suggested a change in the IL-CO2 complex activity upon water addition. However, no 13C NMR spectra have been reported to confirm the theory [41, 42].

Based on the concept of preorganization, a novel CO2 sorption mechanism using [P4,4,4,2][Suc] was addressed by Huang et al. Through a combination of 13C NMR, FTIR, and quantum chemical calculations, they suggested an innovative structure organization with superior CO2 capacity resulting from the interaction between CO2 and the [Suc] anion [43]. Following this idea, the authors also published the tuning of those imide-based anion IL with phosphonium cations by the addition of the electron-donating group. By changing the CO2 sorption amount, several 1H NMR and 13C NMR spectra were acquired, and the cooperative interactions between anion and CO2 were reinforced. According to the authors, at the first stage, the absorption was dominated by N-CO2 interaction confirmed by the presence of a new signal ca. 159 ppm and by the shift of the signal from 195.6 to 188.0 ppm related to C〓O anions. The second stage of absorption mechanism was dominated by the additional O-CO2 interactions, as suggested by the shift of the same signal to 182.8 ppm. The physical interaction occurred at the last stage and is weaker than the first two. This was confirmed by 1H NMR spectrum through the shift of the signal from 1.23 to 1.30 ppm during the uptake of CO2, that indicates the physical hydrogen bond between methylene in the anion and oxygen atom of the CO2 (C-H-O) [44].

3.3 CO2 interaction in wet ionic liquids

Since most ILs are hygroscopic, dry ILs are extremely difficult to obtain. The presence of water in ILs can affect many properties, including CO2 sorption. In this field, a few groups started to evaluate the CO2 capture in wet ILs. Using analogous phosphonium-based ILs and experimental conditions, our group has demonstrated a different point of view of Huang et al. based on NMR analysis. Combining the 13C-{1H}, attached proton test (APT), phase-sensitive HSQC, HMBC, and 31P-{1H} NMR spectra, the degradation of [Suc] anion was proposed. The 13C-{1H} NMR spectra showed a second set of signals that did not correspond to the [P4,4,4,2]+ or [Suc] at 34.4, 35.4, 174.8, and 176.4 ppm. Those signals were observed at APT analysis and represent two CH2 groups and two C〓O, indicating IL degradation or contamination. Combined with the correlation between protons and carbons observed by HMBC and HSQC experiments, the analysis suggested the formation of 4-amino-4-oxobutanoate (anion from succinamic acid) resulting from the basic hydrolysis of the pyrrolidine-2,5-dione (SucH) during the synthesis of IL. Furthermore, the formation of bicarbonate by the reaction between CO2 and IL confined water was proposed due to the presence of the signal ca. 159 ppm. The same chemical shift was observed for [P4,4,4,2][HCO3] IL, reinforcing the idea of bicarbonate formation [45].

Davis and co-workers demonstrated that the CO2 capture is hugely impacted by the presence of water in a series of [N1,1,1,1] ILs having amino acid anions. Employing 1H and 13C NMR analysis, they demonstrated the formation of a carbamate only as transitory specie (ca. 163 ppm) for amino acid ILs. Indeed, when the amount of CO2 present in the system exceeds about 0.5 mol/mol of IL present, the carbamate complex was detected in trace amounts and the carbonate/bicarbonate capture emerged as predominant. Due to rapid proton exchange, carbonate and bicarbonate appear as a single peak ca. 159 ppm. The study also reported the CO2 sequestration in wet [N1,1,1,1][2-CNPyr]; in the 13C NMR spectrum, the migration correlated with proton sequestration, and the carbonate/bicarbonate peak was observed; however, the signal associated with carbamate formation was not observed, in opposition of Brennecke’s work [41, 42, 46].

Recently, Filippov et al. using solid-state 13C and 15N MAS NMR spectroscopy demonstrated the CO2 absorption in [N1,1,n,2OH][Threo] and [N1,1,n,2OH][Tau] aqueous solution (50 wt%) ILs. After CO2 reaction, a precipitated product appeared and was analyzed by ssNMR (13C and 15N), suggesting that the solid sediment is composed of neutral threonine (or taurine) in the zwitterionic forms. Therefore, they assigned the resonance line at 164.4 ppm to the formation of the carbamate anion and the resonance line at 160.6 ppm to the carbamic acid [47].

The confinement of a water molecule between the cation and the anion in ImILs was demonstrated through NOESY experiment by our research group. This water can react reversibly with CO2 to yield bicarbonate. The phenomenon occurred only with basic anions, such as [OAc] and [Im]. Whereas fluorinated anions, such as [BF4] and [NTf2], show only noncovalent interactions with CO2, and no significant contacts between water and cation could be detected. In the same work, 13C inverse-gated decoupled analysis was employed to quantify the CO2 capture by an aqueous solution of [C4C1C1Im][Im] and [C4C1C1Im][OAc]. The best system [C4C1C1Im][Im]/H2O (1/1000) presented a sorption capacity of 10 molCO2/molIL. Additionally, the comparison between the 1H,15N-HMBC NMR spectra of [C4C1C1Im][Im]/D2O (1/1000) neat and under 20 bar of CO2 reinforced the idea of bicarbonate formation instead of carbamate, since it was not observed any change in the chemical shift [48].

The formation of bicarbonate was demonstrated, once again, by Dupont and co-workers for bare ImILs under 10 bar of CO2. In this work, the water in the hygroscopic IL was enough for the signal related to HCO3 /CO3 2− species (ca. 160 ppm) to appear in 13C NMR. A description of interactions between ImIL and CO2 was demonstrated combining NMR spectroscopy with MD simulation. According to the ImIL structure, three types of CO2-IL interaction were described: physical sorption by the polar domains (halogenated anions); chemical sorption by reaction with cation and formation of [C4C1Im]-CO2 complex or by reaction with anion by carbamate formation (amino acid anions); and bicarbonate formation (hygroscopic basic anions). Another interesting result to point out in this work is [C4C1Im][Pro]-CO2 interaction. Through the contour map of 1H,13C-HMBC associated with 13C NMR studies, it was possible to understand the CO2 sorption mechanism and observe the pH dependence for this anion. Bubbling CO2 in neat IL, the 13C NMR signals suggested a reaction with the [Pro] anion and the formation of the carbamate (ca. 180 and 162 ppm) and bicarbonate (ca. 161 ppm), which was confirmed by 1H,13C-HMBC ( Figure 7 ). This work demonstrated that the sorption capacities of ImILs could be enhanced by the variation of cation-anion-CO2 and IL-CO2-water interaction, providing a helpful investigation to understand the structure-activity relation in IL materials for CO2 capture [49].

Figure 7.

Possible reaction of [C4C1Im][Pro] after bubbling CO2 and 1H,13C-HMBC NMR experiment (100 MHz, DMSO-d6capillary) (adapted from Ref. [49]).

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4. Interactions between ionic liquids and cellulose

Cellulose is a natural, renewable, and the most abundant polymer in nature [50]. The applications range from the papermaking industry and film manufacturing to pharmaceuticals. Cellulose’s poor solubility in common solvents is attributed to inter and intramolecular H-bonds, which limits its uses and imposes very harsh treatments like the Lyocell process (N-methylmorpholine N-oxide dissolution) and solvent systems such as LiOH/urea, dimethyl sulfoxide (DMSO)/[N4,4,4,4]F, and dimethylacetamide (DMAc)/LiCl.

ILs have been used successfully to dissolve cellulose either using pure ILs such as [C4C1Im]Cl and [C4C1Im][OAc] or using binary mixtures with organic solvents such as DMSO.

Although there are several strategies to dissolve this polymer, the dissolution process is still poorly understood. Alkali salts like LiOH or NaOH mixtures with urea are one of the most employed solvent systems. The dissolution and gelation of cellulose in 8 wt % NaOH/H2O with and without the addition of urea were studied using polarization transfer NMR techniques (PTNMR), INEPT, and CP [51]. It was revealed that the solvent containing urea is able to fully dissolve cellulose. The use of liquid state polarization technique (INEPT) and a solid-state polarization technique (CP) allowed the discrimination of liquid and solid states. It was noted by the authors that the presence of some signal in the fully dissolved urea/NaOH/H2O solution is due to the reorientation dynamics of a very viscous sample, leading to some CP transfer.

The dissolution of cellulose in LiOH/urea was studied using solid-state NMR (ssNMR), by using 13C CP/MAS NMR, 6Li CP/MAS NMR, 6Li single-pulse NMR, 2D heteronuclear 1H,13C, and 1H,6Li-(FSLG-HETCOR) [52]. Four existing forms of Li+ ions were detected. Some Li+ ions coordinate with cellulose chain, and a large population of Li+ ions in the form of Li+-OH-urea surrounds the Li+-cellulose chains, which prevent their self-aggregation. The ability to dissolve cellulose is likely determined by the coordination ability of alkali metal ions (Li+, Na+, K+).

XRD and NMR methods were used to study the low-temperature dissolving mechanism of chitin/chitosan in the alkali (LiOH, NaOH, and KOH) aqueous solvents [53]. Aqueous alkali showed different dissolving abilities based on the acetylation degree (AD) of chitin, namely, KOH > NaOH >> LiOH for AD between 0.94 and 0.74; KOH ≈ LiOH ≈ NaOH for AD between 0.53 and 0.25; and the inverse order, LiOH > > KOH > NaOH for AD lower than 0.25. By measuring the active species of cations in semi-frozen solutions using 7Li, 23N, and 39K NMR, differences from the stoichiometric quantities were obtained with a Na+/Li+ ratio higher than K+/Li+, which is the proposed explanation to the sodium higher destabilizing effect of chitosan at lower temperatures.

[CnC1Im][(C1O)PHO2] was used to dissolve and regenerate cellulose under mild conditions [54]. Requiring heating to 80°C and being able to dissolve up to 4 wt%, coagulation with water afforded cellulose as a transparent gel. NMR was used to monitor the dissolution process by measuring 31P and 13C chemical shift differences to the pure IL. PLM photographs show complete dissolution after 120 min of heating.

Minnick et al. studied the solubility of cellulose in mixtures of [C2C1Im][(C2O)2PO2] with aprotic solvents (DMSO, dimethylformamide, 1,3-dimethyl-2-imidazolidinone) and protic antisolvents (water, methanol, and ethanol), concluding that polar aprotic solvents/IL mixtures can improve the cellulose solubility, while polar solvents have the opposite effect [55]. The 1H ∆δ of the IL-cation imidazolium ring resonances presented downfield shifts for the aprotic solvents, while protic solvents have the opposite effect. The reduced shielding experienced by the IL in aprotic solvents can be attributed to the solvation of the cation, which decreases cation-anion interactions, resulting in an increase in anion availability to form more and stronger interactions with cellulose. The authors explained negative chemical shift variations of IL in protic solvents as a result of stronger IL-solvent interactions, which change/compete with the IL-cellulose interactions.

On the use of an organic solvent as co-solvent of cellulose, DMSO was used in conjunction with [CnC1Im]Cl to dissolve cellulose, using NMR relaxation measurements to study the dissolution process and co-solvation ability of DMSO [56]. At low concentration, DMSO improves the cellulose solvating ability of [CnC1Im]Cl by reducing the viscosity of the IL but weakens it at high concentration. T2 measurements on 1H and 1D spectra on 1H, 35Cl indicate that the tight association between the cation and the anion in the [CnC1Im]Cl network is loosened at low DMSO concentration. Neat [CnC1Im]Cl exhibits one population with smaller T2 having a slower rotational dynamics and another with a larger T2 and faster rotational dynamics. When DMSO concentration was increased, the [CnC1Im]Cl with slower rotational dynamics transfers to faster rotational dynamics by going through a coalescence step at 0.4 DMSO molar fraction. Analysis of Δδ allowed probing the ion clustering, by studying the imidazolium H-bond change with DMSO addition and by using 35Cl NMR to access the chlorine local environment. At 0.5 DMSO molar fraction, a turning point in 35Cl NMR shifts is also observed, in a similar way as in T2 relaxation. As imidazolium 1H shifts change due to the shielding effect, the higher concentration of DMSO breaks the IL H-bond network into small ion clusters that are incapable of dissolving cellulose.

NMR PFG-diffusion was used to study the dissolving process of microcrystalline cellulose in aqueous tetrabutylammonium hydroxide [N4,4,4,4][OH] at 40 wt% concentration [57]. From the molecular self-diffusion coefficients of microcrystalline cellulose (MCC) and [N4,4,4,4][OH], [N4,4,4,4]+ is involved in the dissolution of carbohydrates, binding in a 1.2 stoichiometry to glucose units based on diffusion measurements and mass relations. The binding might be due to electrostatic interactions between the deprotonated hydroxyl groups or to hydrophobic effects, which have been discussed in the literature as important in cellulose dissolution by using either NMR or other techniques, such as calorimetry and rheology [58, 59].

Another use of cellulose is to make physical composites by blending it with another polymer to reinforce the final material. To understand the molecular origin of the enhanced mechanical properties for a cellulose/Silk blend film (SF), ssNMR was used as the tool to investigate the conformational changes, intermolecular interactions between cellulose and silk, and the water organization [60]. ssNMR can be used to gain an insight into polymer’s molecular structure and dynamics, being able to identify its molecular constituents, structural morphology, and chain dynamics [61].

Cellulose/silk films were prepared by dissolution in [C4C1Im]Cl followed by precipitation with methanol. 2D 1H,13C-HETCOR NMR reveals the intermolecular H-bonding interactions between the NH groups of SF and the OH groups bonded to carbons C2 and C3 of cellulose. 2D WISE experiments measured the hydrophilic character of each carbon sites, based on the lineshape with increasing mixing times, water is more localized in the vicinity of cellulose chains than silk.

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5. Ionic liquids as co-solvents

ILs can be used as co-solvents in several applications, not only to increase the solubility of target species but also to tune the important physicochemical properties, such as conductivity and viscosity toward a more efficient industrial performance and operational conditions. In recent years, mixtures of ILs either with other ILs (IL/IL mixtures) [62, 63], molecular liquids (water, organic solvents) [64, 65, 66], or polymers [67] have gained such an interest that has been labeled as the fourth evolution of ILs [68]. IL mixtures do not fall in the definition of salt in solution, neither their physicochemical properties follow mixing behavior of molecular liquid mixtures, which create the need to develop new fundamental and structural/dynamic research.

In recent years, there has been an interest on mixtures of two or more ILs (IL/IL mixtures). This approach has been presented as a new strategy to tune the IL properties, with several studies showing that in most mixtures, physicochemical properties have close to ideal mixing behavior, due to a random ionic distribution (Coulombic interactions). However, non-ideal behavior has been reported, particularly for mixtures with very different constituents [69, 70]. These “anomalies” can be explained by the formation of nano-segregated phases due to strong ionic interactions [71], making the ionic distribution nonrandom. Therefore, in terms of nanostructure organization, IL mixtures show an increased degree of complexity compared to neat ILs, having to consider the different combinations of the several ions present in solution. NMR techniques have been particularly useful to enlighten these deviations from linearity. Matthews et al. analyzed binary mixtures of ILs with a common cation [C4C1Im]+ and different anions by 1H and 13C NMR chemical shift peak analysis [72]. Studying the full concentration range of IL/IL mixtures, they inferred that there is a preferential interaction of the cation with one of the anions. That was evident by the H2 1H NMR peak, which shows a preferential interaction with the stronger H-bond acceptor anion over the NMR timescale. From the 13C NMR, imidazolium ring C4 and C5 showed greater affinity for the weakest H-bond anions, which was not obvious in 1H NMR, suggesting that the weakest H-bond will occupy a position above the plane of the imidazolium, forming an anion-π interaction. These slightly preferential associations have a very small effect on the structural organization but can be the driving force for nonideal deviations observed for some ILs.

Marullo et al. used [BzC4Im][NTf2] with [Bz(F5)C4Im][NTf2] or [BzC4Im][BF4] or [N3,3,3,4][NTf2], as a function of the composition, as solvents for the Diels Alder reaction of 9-anthracenemethanol with N-ethylmaleimide [73]. The authors observed that the reactivity is affected by two main solvent parameters: the viscosity and the molecular organization. For IL/IL mixtures sharing the same cation, the kinetic rate was showed to be more affected by composition, correlating to structural modifications due to a more ordered local domain. For the anion shared IL/IL mixtures, they observed an unexpected result: changing the molar ratio of two cations with similar size and chemical nature produced a more profound effect on the reaction kinetics than IL mixtures ([BzC4Im]x[N3,3,3,4]1-x[NTf2]) with different size cations. 1H ∆δ showed that the imidazolium H2, H9, and H10 exhibit a significant upfield shift, in which H2 and H9 show two chemical shift domains, with a discontinuity point, [BzC4Im]0.4[N3,3,3,4]0.6[NTf2], corresponds to the maximum rate, to which the authors justified with the transition point between a typical aliphatic IL and an aromatic type IL.

One of the applications of ILs is in the field of tribology [74]. ILs can be used as a lubricant by itself or as an additive to increase commercially available oil efficiency. Combining low molecular weight polyethylene glycol (PEG) with orthoborate ILs allowed a decrease in the wear and friction properties for steel on steel contacts. Filippov et al. studied mixtures of PEG 200 with ImILs derived from [BMB] or [BOB] anions as function of concentration by diffusion NMR and ∆δ [75]. The chemical shift analysis showed that the presence of PEG affects the chemical shift of both the cations and the anions, with the protons of the imidazolium ring of the cation the most affected. For the anions, [BMB] showed two chemical shift domains in the PEG concentration range, suggesting that above 50% wt PEG, there is a modification on the interaction mode of PEG/IL, which is not visible for the ImIL derived from [BOB]. The diffusion experiments showed that for ImIL derived from [BMB], the cation and anion differ on their diffusion coefficient in all the concentration range, which suggested that in the mixture, the IL is partially dissociated, which agrees with the data obtained from impedance analysis.

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6. Conclusions

The combination of different NMR experiments allowed to observe the molecular panorama of cation-anion-solute interactions. The diversity of NMR techniques at our disposal allows gathering crucial information to rationalize the IL solvent behavior. Despite the notion that ILs are tailored solvents, their optimization is still seldom done on the basis of the fundamental knowledge of IL performance and the dissolution mechanisms. Instead, the trial and error approach often prevails.

The success of ILs as solvents depends on the strength and nature of the interactions that cations and anions can establish with the solute while maintaining their intrinsic interaction. Chemical shift deviation analyses identify the electronic perturbations in nuclei, either by making or breaking H-bonds or by inducing changes in the geometry. NOE experiments allow a more complete picture, probing solute structural organization within ILs; in this case, both strong and weak interactions can be identified. Relaxation studies are capable of sensing a shorter timescale and identifying even short-lived events that take place upon solubilization processes. Finally, diffusion studies in ILs provide the knowledge of solute behavior and respective associations and also cation/anion feedback in the presence of the solute. This information allows probing macroscopic properties, such as viscosity, which are intimately related to the desired application of ILs.

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Acknowledgments

This work was funded by FCT—Portuguese Foundation for Science and Technology, Portugal, under the projects PTDC/EPH-PAT/0224/2014, PTDC/QUI-QFI/31508/2017, POR Lisboa, and PTNMR (ROTEIRO/0031/ 2013; PINFRA/22161/2016), co-financed by FEDER through COMPETE 2020, Portugal, POCI, and PORL and FCT through PIDDAC (POCI-01-0145-FEDER-007688; UID/CTM/50025/2019; and UID/Multi/04378/2019). T.G.P. acknowledges FCT for the SFRH/BD/133447/2017 PhD fellowship.

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Conflict of interest

The authors declare no conflict of interest.

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Cations
[(iPr)C2C1Im]+1-methyl-3-isopentylimidazolium
[aC2C1C1Im]+1,2-dimethyl-(3-aminoethyl)imidazolium
[Bz(F5)C4Im]+1-(2,3,4,5,6-pentafluorophenyl)-3-butylimidazolium
[BzC1Im]+1-benzyl-3-methylimidazolium
[BzC4Im]+1-benzyl-3-butylimidazolium
[C1C1Im]+1,3-dimethylimidazolium
[C2C1Im]+1-ethyl-3-methylimidazolium
[C4C1C1Im]+1-butyl-2,3-dimethylimidazolium
[C4C1Im]+1-butyl-3-methylimidazolium
[C4C1Pyr]+1-butyl-1-methylpyrrolidinium
[C4Py]+1-butylpyridinium
[CnC1Im]+1-alkyl-3-methylimidazolium
[CnC1Pip]+1-butyl-1-methylpiperidinium
[CnC1Pyr]+, n = 3, 4, 6, 8, and 101-alkyl-1-methylpyrrolidinium
[N1,1,1,1]+tetramethylammonium
[N1,1,1,H]+trimethylammonium
[N1,1,n,2OH]+alkyldimethyl(2-hydroxyethyl)ammonium
[N3,3,3,4]+n-butyltriethylammonium
[P4,4,4,2]+tri-n-butylethylphosphonium
[P6,6,6,14]+trihexyl(tetradecyl)phosphonium
Anions
[BF4]−tetrafluoroborate
[BMB]−bis(mandelato)borate
[BOB]−bis(oxalato)borate
[2-CNPyr]−2-cianopyrrolide
[(C1O)PHO2]−methylphosphonate
[C1SO3]−methylsulfonate
[C1SO4]−methylsulfate
[C2SO4]−ethylsulfate
[DCA]−dicyanamide
[(C2O)2PO2]−diethyl phosphate
[Im]−imidazolate
[Lys]−lysinate
[NO3]−nitrate
[NTf2]−bis(trifluoromethylsulfonyl)imide
[OAc]−acetate
[OTf]−trifluoromethanesulfonate
[PF6]−hexafluorophosphate
[Pro]−prolinate
[SCN]−thiocyanate
[Suc]−succinate
[Tau]−taurine
[TCM]−tricyanomethanide
[Threo]−threonine
Techniques
COSY1H,1H-correlation spectroscopy
CPcross polarization
DFTdensity functional theory
DOSYdiffusion ordered spectroscopy
FSLG-HETCORfrequency-switched Lee-Goldburg—dipolar heteronuclear correlation
HMBCheteronuclear multiple bond correlation
HSQCheteronuclear single quantum coherence
HOESYheteronuclear nuclear Overhauser effect spectroscopy
INADEQUATEincredible natural abundance double quantum transfer experiment
INEPTinsensitive nuclei enhanced by polarization transfer
IRinfrared
FTFourier-transform
MASmagic angle spinning
MDmolecular dynamic
NMRnuclear magnetic resonance
NOEnuclear Overhauser effect
NOESYnuclear Overhauser effect spectroscopy
PFGpulsed field gradient
PLMpolarized light microscopy
PTNMRpolarization transfer NMR
ssNMRsolid state nuclear magnetic resonance
XRDX-ray diffraction

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Written By

Mónica M. Lopes, Raquel V. Barrulas, Tiago G. Paiva, Ana S.D. Ferreira, Marcileia Zanatta and Marta C. Corvo

Submitted: May 8th, 2019 Reviewed: August 14th, 2019 Published: September 30th, 2019