QUANTITATIVE RAMAN SPECTROSCOPY
20220364997 · 2022-11-17
Assignee
Inventors
Cpc classification
G01J3/44
PHYSICS
Y02P70/62
GENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
D01F2/00
TEXTILES; PAPER
International classification
Abstract
Disclosed is a method for quantification of water and/or one or more ionic liquid components in an ionic liquid (IL)/water (H2O) mixture. The method includes obtaining one or more Raman spectra for the IL/H2O mixture, and using a quantitative calibration model with the one or more Raman spectra to quantify water and/or one or more ionic liquid components in the IL/H2O mixture.
Claims
1. A method for quantification of water and/or one or more ionic liquid components in an ionic liquid (IL)/water (H.sub.2O) mixture, the method comprising: obtaining one or more Raman spectra for the IL/H.sub.2O mixture; and using a quantitative calibration model with the one or more Raman spectra to quantify water and/or one or more ionic liquid components in the IL/H.sub.2O mixture.
2. The method according to claim 1, wherein the ionic liquid is a protic ionic liquid.
3. The method according to claim 2, wherein the ionic liquid is or comprises: a non-imidazolium based protic ionic liquid.
4. The method according to claim 3, wherein using a quantitative calibration model involves univariate calibration, which is based on finding a relationship between a single spectral variable, peak intensity, peak area and/or peak shift, and an analyte concentration.
5. The method according to claim 4, comprising: determining H.sub.2O concentration in the IL/H.sub.2O mixture utilizing a linear relationship between H.sub.2O peak area and an H.sub.2O mass fraction in the IL/H.sub.2O mixture.
6. The method according to claim 5, comprising: determining a base concentration in the IL/H.sub.2O mixture utilizing a non-linear relationship between peak intensities and the base concentration.
7. The method according to claim 6, wherein the non-linear relationship is described with a power law model.
8. The method according to claim 6, wherein using a quantitative calibration model involves: using multivariate calibration.
9. The method according to claim 8, wherein the multivariate calibration utilizes partial least squares (PLS) regression.
10. The method according to claim 9, comprising: simultaneously determining an acid, base and H.sub.2O content and/or H.sub.2O concentration and A:B ratio in the IL/H.sub.2O mixture.
11. The method according to claim 10, comprising: quantifying one or more ionic liquid degradation products.
12. The method according to claim 11, wherein the quantifying of one or more ionic liquid degradation products involves: utilizing partial least squares (PLS) regression.
13. The method according to claim 12, wherein the quantifying of one or more ionic liquid degradation products involves: dividing the one or more Raman spectra into two or more subintervals.
14. A method comprising: quantifying water and/or one or more ionic liquid components in an ionic liquid (IL)/water (H.sub.2O) mixture according to the method of claim 1; and monitoring and/or controlling a process using the IL/H.sub.2O mixture.
15. The method according to claim 14, comprising: quantitative monitoring of an A:B ratio and/or H.sub.2O content for process control.
16. A method comprising: quantifying water and/or one or more ionic liquid components in an ionic liquid (IL)/water (H.sub.2O) mixture according to the method of claim 1; and producing Lyocell-type man-made cellulosic fibers based on cellulose pulp dissolution in an IL, dry-jet wet spinning of a solution in a H.sub.2O bath and a subsequent solvent recovery step, in which the IL and H.sub.2O are separated.
17. The method according to claim 16, comprising: solvent purification based on a quantification of one or more ionic liquid degradation products.
18. The method according to claim 1, wherein the ionic liquid is or comprises: a non-imidazolium based protic ionic liquid.
19. The method according to claim 1, wherein using a quantitative calibration model involves univariate calibration, which is based on finding a relationship between a single spectral variable, peak intensity, peak area and/or peak shift, and an analyte concentration.
20. The method according to claim 1, wherein using a quantitative calibration model involves: using multivariate calibration.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
[0051] The accompanying drawings, which are included to provide a further understanding and constitute a part of this specification, illustrate examples and together with the description help to explain the principles of the disclosure. In the drawings:
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[0091] Like references may be used to designate equivalent or at least functionally equivalent parts in the accompanying drawings.
DETAILED DESCRIPTION
[0092] The detailed description provided below in connection with the appended drawings is intended as a description of examples and is not intended to represent the only forms in which the example may be constructed or utilized. However, the same or equivalent functions and structures may be accomplished by different examples.
[0093] The disclosed methods may be used for an ionic liquid. In an embodiment, the ionic liquid is or comprises a protic ionic liquid. In an embodiment, the ionic liquid is or comprises a non-imidazolium and/or a superbase-based ionic liquid. In an embodiment, the ionic liquid is or comprises an amidine- or guanidine-based protic ionic liquid. In an embodiment, the ionic liquid is or comprises a DBN-based and/or TBD-based ionic liquid.
[0094] The DBN-based ionic liquid may comprise a 1,5-diazabicyclo[4.3.0]non-5-enium cation of the formula (I),
##STR00001##
wherein
R.sub.1 is selected from the group consisting of hydrogen, linear and branched C.sub.1-C.sub.6 alkyl, C.sub.1-C.sub.6 alkoxy, C.sub.1-C.sub.10 alkoxyalkyl and C.sub.6-18 aryl groups, which optionally are substituted with one or more substituents selected from hydroxy and halogen,
and
an anion selected from halides, such as fluoride, chloride, bromide and iodide; pseudohalides, such as cyanide, thiocyanide, and cyanate; a carboxylate, preferably formate, acetate, propionate, or butyrate; an alkyl sulphite, an alkyl sulphate, a dialkyl phosphite, a dialkyl phosphate, a dialkyl phosphonites, and a dialkyl phosphonate.
[0095] The DBN-based ionic liquid may also comprise a 1,5-diazabicyclo[4.3.0]non-5-enium cation of formula (I) above, where R.sub.1 is H, and the anion is a carboxylate anion, preferably formate, acetate, propionate or butyrate.
[0096] In an embodiment, the DBN-based ionic liquids is or comprises [DBNH][CO.sub.2Et] and/or [DBNH][OAc].
[0097] The TBD-based ionic liquid may comprise a cationic 1,5,7-triazabicyclo[4.4.0]dec-5-enium [TBDH]+moiety and an anion selected from the group according to Formula a), Formula b) and Formula c),
##STR00002##
wherein each of R, R2, R3, R4, R5, R7, R8, R9 and R10 is H or an organyl radical and X— is selected from the group consisting of halides, pseudohalides, carboxylates, alkyl sulphite, alkyl sulphate, dialkylphosphite, dialkyl phosphate, dialkyl phosphonites and dialkyl phosphonates.
[0098] All embodiments may be used in any combination with each other.
1. Materials and Methods
1.1. Materials
[0099] Samples of 1.5-Diazabicyclo[4.3.0]non-5-ene (DBN) (CAS no. 3001-72-7; purity 99.0% in mass) and acetic acid (HOAc) (CAS no. 64-19-7; purity 99.8% in mass) were purchased from Fluorochem and SigmaAldrich, respectively, and were used without further purification.
1.2. Sample Preparation
1.2.1. Water-Free ILs
[0100] [DBNH][OAc] was prepared by the slow and controlled addition of an equimolar amount of HOAc to DBN. The mixture was stirred and cooled in the beginning at 25° C. to divert the exothermic reaction enthalpy. When approaching the equimolar amounts in the mixture, the system was heated at 70° C. to avoid the crystallization of the IL. The system was kept for another hour at this temperature under mixing to ensure the reaction runs until completion. The water content of the synthesized IL is lower than 0.5 wt. %.
[0101] This IL sample was analyzed by .sup.1H NMR to determine its A:B ratio. The other samples were prepared by mixing the initial IL with known amounts of HOAc or DBN to reach the target A:B ratio. These samples were then mixed for homogenization and analyzed again by .sup.1H NMR for final determination of A:B ratio. The prepared samples were in the A:B molar ratio range of 0.4-1.98.
1.2.2. IL/H.SUB.2.O Mixtures
[0102] IL/H.sub.2O mixtures were prepared by dilution of the water-free IL samples with water. A 1 mg precision electronic scale was used during the dilution process to adjust the IL/H.sub.2O mixture to the target concentration. The covered IL concentration range was large enough to simulate concentrated and diluted samples (1.25-90 wt. % of IL in IL/H.sub.2O mixtures) with different molar A:B ratios (0.4-1.98). The IL/H.sub.2O mixtures were divided into calibration and validation sets for the model calibration and validation procedures. As each sample can be represented by its A:B ratio and IL concentration, the sample subsets are shown in
[0103]
1.3. 1H NMR Measurements
[0104] Water-free IL samples were characterized by .sup.1H NMR. Samples were loaded into standard 5 mm NMR tubes and dissolved in DMSO-d6. The spectra were acquired at 23° C. using a Bruker 400 MHz Ultra Shield NMR instrument (Bruker, Billerica, Mass., USA). NMR spectra were collected following the standard zg30 sequence with eight transients and an acquisition time of 2.56 s. All of the spectra are referenced to tetramethylsilane. The ACD/1D NMR Processor software was used for the treatment of the raw data. The A:B ratios were calculated by considering the ratio between the area of peaks related to the acid and to the base, respectively.
1.4. Raman Spectra Acquisition
[0105] The samples were analyzed with an Alpha 300 R confocal Raman microscope (WITec GmbH, Germany) at ambient conditions. Nearly 100 μL of the IL/H.sub.2O mixture were spread on a microscope concavity slide and covered with a cover glass. The Raman spectra were obtained by using a frequency doubled Nd:YAG laser (532.35 nm) at a constant power, and a Nikon 20× (NA=0.95) air objective. The Raman system was equipped with a DU970 N-BV EMCCD camera behind a 600 lines/mm grating. The excitation laser was polarized horizontally. After fixing the focus using the microscopy mode, each single spectrum was acquired as an average of 32 scans with an integration time of 0.1 s/scan. The baseline of the spectra were corrected with WITec Project 1.94 (WITec GmbH, Germany) using a 2.sup.nd order polynomial equation.
[0106] In total, 75 spectra were collected, with at least two replicates for each sample. The calibration set comprises 54 spectra and the validation set comprises 21. The samples and spectra of the two sets were prepared and collected independently on different days.
1.5. Calibration Methods Development for the Determination of the Acid, Base and H.SUB.2.O Concentration in the IL/H.SUB.2.O Mixtures
1.5.1. Univariate Calibration
[0107] Univariate calibration is the simplest approach to build a quantitative calibration model. It is based on finding relationships between single Raman spectral variables (peak intensity, peak area, peak shift) and the analyte concentration. A Matlab® (The Mathworks, Inc. Natick, Mass., United States) routine was created for the Raman spectra analysis, correlation identification and calculation of the calibration models parameters.
[0108] The fit quality is assessed through the coefficient of determination (R.sup.2) and the Root Mean Square Error of Calibration (RMSEC) and Prediction (RMSEP) which are expressed as:
where y.sub.l.sup.onl and ŷ.sub.l.sup.onl denote the measured and predicted values, respectively, and N the number of samples in the calibration data set, and
where y.sub.l.sup.val and ŷ.sub.l.sup.val denoted the measured and predicted values, respectively, and K the number of samples in the validation data set.
[0109] Although univariate calibration can work successfully in some cases, it sometimes fails in giving good results when dealing with complex Raman spectra that show for instance overlapping bands or unexpected shifts over the calibration range. In those cases, a multivariate approach would be more appropriate for calibration model building [19][20].
1.5.2. Multivariate Calibration: Partial Least Squares Regression (PLS)
[0110] When building calibration models using spectroscopic data and multivariate analysis, one usually encounters two main problems: there are typically much more spectral variables than samples, and there is a high variable collinearity encountered in most of the spectral data. This makes classical multiple linear regression (MLR) based on the original spectral variables either impossible or highly unstable.
[0111] A robust alternative to MLR is Partial Least Squares (PLS) regression. PLS projects data (spectral intensities in our case) in a new space with a smaller number of new variables. Those new variables are called components or Latent Variables (LVs). PLS calculates the LVs in a way that the covariance between the X block (spectral intensities), and the Y block (concentration of the different species) is maximized.
[0112] The LVs are mutually orthogonal, which suppresses problems related to matrix inversion when calculating the model coefficients. The reduction of the space dimension in addition to the mutual orthogonality of the LV makes PLS especially suitable for building predictive models out of spectroscopic data. A very good explanation of the principles of PLS is given in reference [21].
[0113] During the calibration procedure, the collected spectra are placed as rows in a X matrix (independent block), with n rows and k columns. Each row represents a spectrum and each column a single wavelength. The variables that we aim to predict are placed in a Y matrix (dependent block), with n rows and m columns. Each row represents one sample and each column a single variable.
[0114] Briefly, in PLS there are outer relations for which the X and Y blocks are decomposed into scores and loadings matrices:
X=TP′+E
Y=UQ′+F′
Where:
[0115] T and U represent respectively the score matrices for the X and Y blocks. [0116] P′ and Q′ represent respectively the score matrices for the X and Y blocks. [0117] E and F′ represent respectively the matrices of residuals for the X and Y blocks after the projection onto a defined number of LV.
There is also an inner relation between the scores, linking both blocks
U=BT
where B is the matrix containing the regression vectors.
A mixed relation can be written as:
Y=TBQ+F,
where ∥F∥ is to be minimized.
[0118] This mixed relation ensures the ability to use the model parameters for future prediction from a test set.
[0119] In the present study, the X block contains the Raman spectra of each sample and the Y block the weight fractions of acid, base, and H.sub.2O in each sample.
[0120] The number of LVs, the fit quality, and model validation were investigated through the evaluation of the R.sup.2 coefficient, RMSEC and RMSEP.
[0121] Data analysis and model building were performed with Matlab® and the Matlab® PLS Toolbox (Eigenvector Research, Inc. Manson, United States) software packages.
2. Results and Discussion
2.1. .SUP.1.H NMR of Water-Free IL Samples
[0122] The NMR spectra of the water-free ILs as well as the corresponding A:B ratio are shown in
[0123] As expected, only mixed peaks can be observed instead of peaks that represent molecular and ionic species separately. For the rapid exchange system, the observed .sup.1H chemical shift is assumed to be the weighted average of the molecular and ionic species.
[0124] One can notice a shift of the of the different peaks related to HOAc, DBN, and their ionized forms to the high ppm values when increasing the A:B ratio. These shifts can be directly linked to the different shielding/deshielding effects experienced by the protons when changing the A:B ratio.
[0125]
[0126] For instance, when the A:B ratio is increased, protons belonging to the acid methyl group (1.6-1.8 ppm) are shifted downfield. This is probably due to a higher hydrogen-bonding network between these protons and the oxygen atoms of the carboxylate group in neighboring free acetic acid molecules. This reduces the shielding around these protons and make them resonate at higher frequency.
[0127] The position of the methyl group singlet is linearly correlated to the A:B ratio, with a noticeable increase of the slope starting from A:B=0.85 denoting higher proton deshielding beyond this value. Similar linear relationships and slope change over the investigated A:B range were found for the equivalent protons bonded to C3 and C9 in DBN/DBNH.sup.+. The change of slopes is, however, different. The slopes were pronounced below A:B=1.1 and decreased markedly beyond this value, which means that the proton deshielding decreases markedly beyond this value. These results are illustrated in the supplementary materials. The different chemical shifts can be used to calculate the IL ionicity as explained in [22].
[0128] The A:B ratios were calculated by taking the ratio of the integral area of methyl group singlet (acid) to the sum of the integrated areas of the different multiplets (base). The area of the triplet observed in the range of ≈3.27-3.95 ppm, corresponding to the two hydrogen bonded to C9 was taken as a reference. The estimated relative error for the calculation of the A:B ratio was less than 5%.
2.2. Raman Spectroscopy
2.2.1. Raman Spectra of the Acid, Base, and IL
[0129] The area normalized Raman spectra of DBN, HOAc and IL (A:B=1.05) are presented in
[0130]
[0131] To the best of our knowledge, the assignment of the specific Raman bands for DBN has not been presented in the literature. The band assignment herein is based on Raman spectral tables [24] [25]. The peak at 313 cm.sup.−1 and 732 cm.sup.−1 could originate from C—C vibrations. The peak at 518 cm.sup.−1 could be attributed to C—N vibrations. The peak at 1650 cm.sup.−1 could be ascribed to C═N stretching, while the peaks at 1452 cm.sup.−1 and 2850 cm.sup.−1 could be ascribed to CH.sub.2 vibrations. Interestingly, the peaks at 313 cm.sup.−1, 518 cm.sup.−1, and 732 cm.sup.−1 do not overlap with peaks of HOAc, and would probably be good candidates to build a calibration model.
[0132] The Raman spectra of IL (A:B=1.05) display a complex pattern in which we can distinguish some features from the spectra of HOAc and DBN, respectively. One can note, for instance, that the peaks at 313, 518, and 732 cm.sup.−1 show a decrease in intensity compared to the pure base without any noticeable change in the shape or in the peak position, which confirms again their potential use for calibration. Some other overlapping peaks, for instance between 800-1000 cm.sup.−1 or between 2800-3200 cm.sup.−1, are more complex to interpret and results from the overlaps/shifts of the peaks from HOAc and DBN. A noticeable shift of the DBN peak related to —CH.sub.2 vibrations from 2850 cm.sup.−1 in the pure base to 2880 cm.sup.−1 in the IL is observed. Ionization and interactions between the molecular and ionized HOAc and DBN are probably behind those shifts.
2.2.2. Raman Spectra of Water-Free A/B Mixture with Excess of Base or Acid
[0133]
[0134] Indeed, for the nearly equimolar composition, once the proton exchange occurs when the acid and base are mixed, a great proportion of the molecules become ionized, the two double bonds become delocalized, and no “real” C═O or C═N vibration can be seen in the Raman spectra of the IL. When there is an excess of acid or base, those bands are more prominent due the presence of the neutral molecules.
[0135] It is also worth-mentioning here that in the case of protic IL like [DBNH][OAc], a chemical equilibrium takes place between ionized and neutral species (the equilibrium constant is directly linked to the so called ionicity of the IL). This may then explain why the band intensities of the double bonds do not vanish completely even in nearly equimolar composition (presence of neutral species) [4].
[0136]
[0137] The excess of base or acid in the mixtures affects also the spectrum in the high wave number region (2200-3200 cm.sup.−1). At low A:B ratio (excess base), the area in the range 2800-2900 cm.sup.−1 increases with the appearance of a shoulder at low wave numbers, and most probably related to molecular vibrations in the free base, while at high A:B ratios the area in the range 3000-3100 cm.sup.−1 increases mostly due to the presence of the molecular acid.
2.2.3. Effect of Water on the Raman Spectra of ILs as a Function of the A:B Ratio
[0138] So far, we showed that an excess of acid or base induces noticeable changes in the Raman spectra of A/B mixtures. In this section, we discuss the effect of water dilution of IL. The spectra of the different A:B ratio water-diluted IL samples (50 wt. % of water) are shown in
[0139] Dilution with water caused indeed noticeable changes in the Raman spectra compared to the water-free ILs. A broad band ascribed to the different O—H vibrations modes in the water molecule appeared in the wave number range of 3000-3700 cm.sup.−1, in addition to another peak ascribed to a bending vibration mode of water near to 1595 cm.sup.−1 [26]. The peak at around 1650 cm.sup.−1 attributed to the C═N vibration in the free base drastically decreased in the presence of water (probably due to ionization) and is only visible for samples with low A:B ratios. The peaks at 1600 cm.sup.−1 and 1700 cm.sup.−1 related to the free acid molecules are also visible in diluted samples with high A:B ratios. Here also, chemical equilibria define the ionization extent of the different molecules.
[0140]
[0141] Drastic changes were also reported for the IR and NMR spectra of Imidazolium-based ionic liquids having different anions upon the introduction of water due to interactions between the IL and H.sub.2O molecules [27].
2.2.4. Raman Spectra of the IL/Water Mixtures
[0142] The Raman spectra of the different IL/H.sub.2O samples are shown in
[0143] Although the presence of water caused noticeable changes in the Raman spectra of IL, its scattering does not noticeably interfere with the scattering resulting from the IL molecules.
[0144]
2.2.5. Univariate Calibration Approach for the Determination of H.SUB.2.O Concentration in IL/H.SUB.2.O Mixtures
[0145] To predict the H.sub.2O concentration in a H.sub.2O/IL mixture, the intensity variation in the range of 2200-3800 cm.sup.−1 can be exploited. Although there is a small overlap between the peaks ascribed to IL and H.sub.2O in the of 3000-3200 cm.sup.−1 region, the respective signals are still relatively well separated.
[0146] We developed a quite simple method for the calibration. In our spectral treatment procedure, the spectral range was first narrowed to the 2200-3800 cm.sup.−1 region. The raw spectra were then area-normalized. The peak areas related to IL and H.sub.2O are defined as follows:
IL.sub.peak area=∫.sub.2200.sup.3010Idϑ
H.sub.2O.sub.peak area=∫.sub.3010.sup.3800Idϑ
[0147] The graphical representation of the H.sub.2O peak area H.sub.2O.sub.peak area as a function of the H.sub.2O concentration is shown in
[0148]
[0149] A significant linear relationship is obtained between H.sub.2O.sub.peak area and the H.sub.2O mass fraction in the IL/H.sub.2O mixture. Some discrepancies at equivalent H.sub.2O mass fraction are observed for samples with different A:B ratios. Indeed, some of the spectral features change in the 2200-3010 cm.sup.−1 region, especially at low and high A:B ratios as discussed previously. These variations can be seen specifically for the samples with 50 wt. % of water, were the covered A:B range was the largest one.
[0150] Altogether, these changes do not dramatically affect the model. The RMSEC and RMSEP were 2.234 wt. % and 2.257 wt. %, respectively. These values are reasonable, considering the simple procedure and the large concentration range from 10 wt. % to 98.75 wt. % of H.sub.2O content. The prediction error is comparable that reported by Viell at al. [12] who quantified H.sub.2O in H.sub.2O/IL mixtures using mid-infrared (mid-IR) spectroscopy using advanced spectral treatment methods. The prediction error reported in their study was lower than 2.3 wt. % over the entire concentration range. Models parameters and fit quality metrics for the prediction of the water concentration in IL/H.sub.2O mixtures are given in Table 1.
TABLE-US-00001 TABLE 1 Models parameters and fit quality metrics for the prediction of the water concentration in IL/H2O mixtures. Raman RMSEC, RMSEP, peak water water Model: ƒ(x) = ax + b range, cm.sup.−1 R.sup.2 wt. % wt. % a b 3010-3800 0.991 2.234 2.257 0.008976 0.05309 (0.008734, 0.009218) (0.03843, 0.06774)
2.2.6. Univariate Calibration Approach for the Determination of the Base Concentration in IL/H.SUB.2.O Mixtures
[0151] The Raman scattering intensity from the IL components (acid and base) increases with IL concentration in the IL/H.sub.2O mixtures as depicted in
[0152] The relationship between the peak intensities and the base concentration is, however, not linear. The reasons behind this non-linearity over the base concentration range are not clear. Polynomial models can be used to approximate a complex nonlinear relationship, as they are just the Taylor series expansion of the unknown nonlinear function. However, we found that the observed relationships could be well described with simple power law models, which we adopted for the calibration equation.
[0153]
[0154] As depicted in
[0155] For both peaks, the RMSEC and RMSEP were lower than 2 wt. %, which is again a quite reasonable value regarding the covered range. Nevertheless, using the peak at 2890 cm.sup.−1 would result in a better model sensitivity, as the intensity range is larger over the same covered base concentration range.
TABLE-US-00002 TABLE 2 Models parameters and fit quality metrics for the prediction of the base concentration in IL/H.sub.2O mixtures. Raman RMSEC, RMSEP, shift, Base Base Model: ƒ(x) = ax.sup.b cm.sup.−1 R.sup.2 wt. % wt. % a b 743 0.991 1.566 1.086 0.1209 0.6763 (0.1101, 0.1317) (0.6517, 0.7008) 2890 0.985 1.944 1.840 0.2992 0.6957 (0.2673, 0.3311) (0.6665, 0.725)
[0156] So far, the univariate calibration showed a good potential for the quantification of water and base in IL/H.sub.2O mixtures. Nevertheless, it showed also limitations, as we were not able to predict the acid concentration in the IL/H.sub.2O mixtures using single spectral features. The acid concentration can be still obtained by difference to 100% assuming that only water, acid and base are present in the solution.
[0157] Using multivariate calibration can greatly improve the calibration model quality and performance, as it utilizes all the information in the spectra and not only focuses on a single variable. In the next section, we will discuss the potential of one of the multivariate calibration methods, namely the PLS regression.
2.2.7. PLS Regression for the Simultaneous Determination of the IL Components and H.SUB.2.O Content in IL/H.SUB.2.O Mixtures
[0158] Preprocessing is a very important step when performing multivariate data analysis. In our attempts to build the PLS calibration model, we tested several spectra preprocessing methods and evaluated them in the light of the model fit quality. The retained preprocessing strategy includes base line correction, smoothing (10 points moving window), area normalization and mean centering of the raw spectra (X block). The Y block data were mean centered.
[0159] The number of the model LVs was selected based on the minimization of the RMSECV and a visual inspection of the LVs. A model with four LVs leads to a very good fitting with more than 99% of explained variance in both X and Y blocks.
[0160] The measured and predicted values of acid, base, and H.sub.2O concentrations for the calibration and validation data sets are shown in
[0161]
[0162] The PLS calibration approach was clearly successful in predicting simultaneously the acid, base, and H.sub.2O contents in IL/H.sub.2O mixtures. The PLS model statistics are shown in Table 3.
TABLE-US-00003 TABLE 3 PLS model statistics for the prediction of acid, base, and H.sub.2O contents in the H.sub.2O/IL mixtures. Base, wt. % Acid, wt. % Water, wt. % Concentration range 0.86-62.81 0.39-33.17 10-97.75 RMSEC, wt. % 1.137 0.634 1.175 RMSEP, wt. % 0.908 0.441 1.037 R.sup.2 Calibration 0.995 0.994 0.997 R.sup.2 Prediction 0.996 0.996 0.998
[0163] The RMSEs are reasonable regarding the relatively wide covered range for the three variables. It has to be noted that, some of the validation set samples have acid, base, and H.sub.2O concentrations from the calibration set samples, which also reflects a good model prediction ability.
[0164] Those results are, to the inventors' best knowledge, the first in the literature to show the potential of Raman spectroscopy in combination with Chemometrics for a fast and quantitative determination of the Il components and H.sub.2O contents in IL/H.sub.2O mixtures. The applicability of this method can be extended to a wider range of processes involving IL/H.sub.2O mixtures [6]-[9].
2.2.8. Discussion on the PLS Calibration Model
[0165] The percent variance captured by the PLS regression model for the X and Y blocks are given in Table 4. LV1 and LV2 explain already nearly 99% of the variance in the data. The latent variable LV1 explains the greatest part of the variance, respectively 96.53% and 93.14% in the X and Y blocks.
TABLE-US-00004 TABLE 4 Percent variance captured by the PLS regression model Latent X-Block explained Y-Block explained variable variance, % variance, % 1 96.53 93.14 2 2.31 2.86 3 0.53 3.24 4 0.38 0.40
[0166] The score plot based on the two first LVs as well as the loadings plots for the four LVs are shown in
[0167] The positive peaks in the LV1 loading spectrum show an almost complete signal of the water peak. The negative peaks constitute an almost reversed spectrum of a water-free IL. From our previous discussion, we can deduce that the LV1 is mainly explaining variation of IL (respectively water) concentration in the mixture.
[0168] This observation is confirmed when looking at the LV1-LV2 score plot, where the scores are colored with water concentration in the mixture. The samples with IL concentration close to the mean concentration (around 40 wt. %) have a score value of zero because the data are mean centered. We can see that samples with negative scores on LV1 have IL concentrations below this average, while samples with positive scores on LV1 have lower IL concentration than this average.
[0169] From the loading plot of LV2, one can already see that this latent variable is not related to H.sub.2O concentration in the sample, since the loading values for LV2 are close to zero in the wavenumber region corresponding to the O—H vibrations.
[0170] The LV2 loadings show positive and negative peaks. A closer look reveals that the negative peaks corresponds to vibrational frequencies of chemical bonds found in the base and the positive peaks occur at the vibrational frequencies of the acid (see previous discussion on peak assignment). This is confirmed on the score plot, where the samples were found to be separated along LV2 according to the A:B ratio.
[0171] The same applies for LV3 and LV4 which would explain variation in the A:B ratio rather than concentration as the respective loadings showed features related to molecular vibrations in A and B. Both LVs would also explain in part the presence of molecular acid and/or base in the sample, as some of the spectral features related to them appear on the loadings plot.
[0172] Altogether, LV2, LV3 and LV4 are related to the variation of A:B ratio in the mixture, while LV1 explains the variation of IL concentration in it.
[0173]
[0174] Part 2: quantification of ionic liquid degradation products and improvement of prediction performance through interval PLS.
[0175] The liquid stream composition may change as the ionic liquid, such as 1.5-diazabicyclo[4.3.0]non-5-ene (DBN), can undergo a degradation such as a reversible hydrolysis into a degradation product, such as 1-(3-aminopropyl)-2-pyrrolidone (APP) which also forms 1-(3-aminopropyl)-2-pyrrolidonium acetate ([APPH][OAc]) with acetic acid (
[0176]
[0177] Some examples for quantifying an ionic liquid degradation product are provided. In an embodiment, the degradation product may be a hydrolysis product, such as APP, and while some of the examples are provided for this particular degradation product, any other degradation products may be applicable as well.
3. Material and Methods
3.1. Raw Materials
[0178] Samples of DBN (CAS no. 3001-72-7; purity≥99.0% in mass) and HOAc (CAS no. 64-19-7; purity≥99.8% in mass) were purchased from Fluorochem and Sigma-Aldrich, respectively, and were used without further purification.
3.2. Experimental Procedures
3.2.1. Sample Preparation
[0179] The [DBNH][OAc] stock solution was synthetized using the procedure described in (Guizani et al. 2020). 1-(3-aminopropyl)-2-pyrrolidonium acetate ([APPH][OAc]) was synthetized by the University of Helsinki. The stock solution of [APPH][OAc] contained partly DBN. Both stock solutions used for the sample preparation were characterized using capillary electrophoresis, NMR and Karl Fisher titration for the determination of the initial AcOH, DBN, APP and H.sub.2O concentrations. Their specifications are given in Table 8 in the Electronic Supplementary Information (ESI).
[0180] Out of those stock solutions and distilled H.sub.2O, forty samples (each weighing more than 3 g) with defined compositions were prepared gravimetrically using an electronic weighing scale with a precision of 0.1 mg. These forty samples can be classified into four categories as a function of the water contents (˜0 wt. %, ˜25 wt. %, ˜50 wt. % and ˜75 wt. %). The concentrations ranges for the four individual molecular constituents are given in Table 5. The composition of the forty samples is illustrated in
TABLE-US-00005 TABLE 5 Concentration ranges for AcOH, DBN, APP and H.sub.2O in the prepared mixtures Molecule AcOH DBN APP H.sub.2O Concentration range, wt. % 7.5-32.6 2.7-67.4 0-58.4 0.1-75.2
3.2.2. Refractometry
[0181] The reader may legitimately wonder if other, simpler inline methods could be considered instead of Raman spectroscopy. We asked ourselves similar questions while screening alternative analytical methods. Refractometry is widely applied for inline process monitoring and control, and is suitable to quantify the IL concentration in aqueous mixtures (Liu et al. 2008) (Kaneko et al. 2018). Therefore, we considered it as a serious alternative that should be investigated and conducted refractive index (RI) measurements on the set of forty samples in order to assess its potential. The RI was measured with a Peltier heated Abbe refractometer (Abbemat 300, Anton Paar, Austria) at 293.15 K.
3.2.3. Raman Spectroscopy
[0182] Samples were analyzed with an Alpha 300 R confocal Raman microscope (Witec GmbH, Germany) at ambient conditions. Nearly 100 μL of the sample were spread on a microscope concavity slide and covered with a cover glass. The Raman spectra were obtained by using a frequency doubled Nd:YAG laser (532.35 nm) at a constant power of 30 mW, and a Nikon 20× (NA=0.4) air objective. The Raman system was equipped with a DU970 N-BV EMCCD camera behind a 600 lines/mm grating. The excitation laser was polarized horizontally. After fixing the focus using the microscopy mode, each single spectrum was acquired as an average of 32 scans with an integration time of 0.5 s/scan. In total, forty spectra were collected for the forty mixtures.
3.3. Data Analysis
[0183] Data analysis and plotting were performed with Matlab® (The Mathworks, Inc.)
3.3.1. Exploratory Data Analysis: Principal Components Analysis (PCA)
[0184] The spectra were first baseline corrected using a second order polynomial and then area normalized. PCA was done on the pre-processed mean centered spectra. For more details on PCA the reader is invited to read specialized literature (Brereton 2003) (Geladi 2003) (Geladi et al. 2004).
3.3.2. Partial Least Squares Regression (PLS)
[0185] The PLS1 algorithm is used in this study to generate a model for each of the component in the sample set. The same pre-processing method as described for PCA was adopted for the PLS modelling. The decomposition into latent structures is done by maximizing the co-variance between the samples preprocessed spectra and their specific analyte mean-centered concentrations using the NIPALS algorithm (Geladi and Kowalski 1986).
[0186] The model validation and selection of the adequate number of latent variables for the PLS model was done using model cross-validation procedure based on the leave-one-out method. The root-mean square error of cross validation, RMSECV, was used as quantitative measure for the selection of the model LVs. It was calculated using the following formula:
where y.sub.i and ŷ.sub.i denote the measured and predicted values, respectively, and n the number of samples in the data set.
4. Results and Discussion
4.1. The Limitations of Refractometry
[0187] Refractometry was first considered regarding its simplicity and the proven applicability in analyzing mixtures of ILs and water (Liu et al. 2008) (Kaneko et al. 2018). Hence, we would like to discuss our choice of further developing the Raman analytical method in the light of results we got from refractometry. The evolution of the RI for the forty samples is shown in
[0188] The RI evolves linearly with the IL mass fraction and the trends are very similar in the presence or absence of APP. Samples measured at similar water content but with large difference in APP content do not show any significant difference in the RI value, though some spread in the RI values can be seen at low dilution levels. Altogether, those results show that refractometry is very limited in probing the extent of DBN hydrolysis to APP and that an alternative more sensitive analytical method is needed.
[0189]
4.2. Raman Spectra of the Liquid Mixtures
[0190] The pre-processed Raman spectra of the different mixtures are shown in
[0191]
Effects of H.SUB.2.O Addition
[0192] The spectra of the four APP-free samples having different water contents are shown in
[0193] In APP-free samples, the peaks at 464 and 518 cm.sup.−1 originate from the C—N—C bending/deformation modes in DBN. The peak around 740 cm.sup.−1 originated most probably from the C—C vibrations in DBN. The two prominent peaks at ˜920 and ˜2930 cm.sup.−1 were ascribed to the C—C and C—H stretching bands in AcOH, respectively. The peaks at ˜2890 and ˜2980 cm.sup.−1 would be attributed to —CH.sub.2 in phase and out of phase stretching in DBN. In the water free sample, the medium intensity band at ˜1650 cm.sup.−1 was safely attributable to the C═O stretching band from AcOH.
[0194] Upon addition of water, the scattering intensity in the 280-3000 cm.sup.−1 region decreased notably due to the dilution effect. Conversely, the broad peak related to the OH vibrations in the water molecule ˜3100-3700 cm−.sup.1 increased markedly when increasing the water content. It is well known that the Raman scattering from an analyte can show a strong dependence on the molecule's environment (Kauffmann and Fontana 2015). Thus, in addition to the intensity change due to the concentration of the analyte, band shift and shape modifications result from the change in the molecule's environment.
Interactions of the analytes with water molecules via hydrogen bonding are expected upon addition of water. Those would explain partly some modifications other than the intensity decrease in the spectra of the diluted samples. For instance, the C═O stretching band shifted down to ˜1600 cm.sup.−1 which was most likely due to the structural modifications of the solutions in the presence of water (Nakabayashi et al. 1999; Gofurov et al. 2019). Further, upon addition of H.sub.2O, the band at ˜900 cm.sup.−1 vanished, which might indicate the absence of specific AcOH structures (dimers or trimers) that were only present in the water-free IL. At higher frequencies, the reader can notice a marked intensity decrease in the 2800-2870 cm−.sup.1 region, reflecting modifications in the vibrational modes of DBN in the presence of water.
[0195]
Effects of APP Addition
[0196] The Raman spectra of APP-free samples and IL samples with APP/DBN=4.47 mol/mol are shown in Figure for both cases of nearly water-free mixtures and mixtures with 75 wt. % of water. The reader can notice that there were noticeable changes in the spectra upon the variation of the APP/DBN ratio regardless of the water content. To cite a few, the bands at ˜464 and ˜516 cm.sup.−1 decreased markedly upon the addition of APP. Those probably originated from the C—N—C bending/deformation modes in DBN which is absent in APP, even if there is still one C—N—C bond system remaining in APP. In the high-frequency region, the bands at ˜2890 and ˜2980 cm.sup.−1 attributed to —CH.sub.2 in phase and out of phase stretching in DBN, decreased markedly upon the addition of APP.
[0197] Upon the addition of APP, the peak around ˜1640-1675 cm.sup.−1 got broader and was thought to represent the overlapped contributions from C═O in the ketone group in APP, and the C═O of the carboxylic acid group in the AcOH. A clear shift in the wavenumber range was seen when adding water to the organic mixture as discussed previously. The scattering intensity increased in the region of 332-340 cm.sup.−1 and was assigned to the vibrational modes of δ C—C present in the aliphatic amino-propyl chain of APP.
[0198]
[0199] The observed changes in the spectral features due to the variation of the APP/DBN ratio and H.sub.2O contents encouraged the development of a quantitative analysis using the Raman spectra.
4.3. Principal Component Analysis (PCA)
[0200] PCA is a method for data reduction and visualization. It is in the core of chemometrics and is commonly used for an exploratory multivariate data analysis and unsupervised pattern recognition. In PCA, the dimensionality of the data set is reduced by transforming the original spectral data set into a smaller data set composed by few uncorrelated variables (PCs), which retain most of the variation present in all the original variables. The aim is to identify the direction of greatest variability in the data and interpret them in terms of the underlying chemistry.
[0201] PCA was performed on the pre-processed (background corrected, area normalized and mean-centered) data (see
[0202] The scores and loadings of the first three PCs are shown in
[0203] PC2 and PC3 separated the samples within each group according to the proportion of DBN in the sum of DBN and APP. PC2 and PC3 indicated also some interesting features. In PC2, the water-free samples and the samples with the highest water content had negative scores and are separated from the less extreme samples having respectively 25 wt. % and 50 wt. % H.sub.2O and positive scores. In PC3, the spread in scores became narrower as the dilution increased, and the shape of the scores for the different samples was very similar to the shape of DBN wt. % in the mixture as shown in
[0204]
4.4. Partial Least Squares Regression (PLS) for the Quantification of DBN, APP, AcOH and H.SUB.2.O in the Liquid Mixtures
4.4.1. PLS Model Based on the Entire Spectra
[0205] The PLS model was built on thirty-nine samples after discarding sample N35, which showed some signal anomalies and for which the background correction was unsuccessful resulting in a high Q residual and a clear outlier behavior when included in the models. The results from the PLS regression are shown in Table 6. As the PLS1 algorithm was adopted for the regression, each component was modeled separately. This choice was motivated by the fact that PLS1 regression results in a lower error than PLS2 with which all components are modeled simultaneously (Brereton 2003).
[0206] The number of chosen LVs varied between 3 and for the different models. Each of the models captured more than 96% of the variability in the predictor (spectra) and more than 99% of the variability in the response (concentrations).
TABLE-US-00006 TABLE 6 PLS regression results: explained variances and RMSECVs X Y Compo- var var RMSEC, RMSECV, Range, nent LVs % % wt. % wt. % R.sup.2 wt. % AcOH 3 98.7 99.9 0.20 0.23 0.999 7.5-32.6 DBN 4 99.1 99.7 1.73 2.09 0.992 2.7-67.4 APP 5 99.6 99.8 0.81 1.15 0.998 0-58.4 H.sub.2O 3 96.9 99.9 0.68 0.64 0.999 0.1-75.2
[0207] The RMSECV for the AcOH, DBN, APP and H.sub.2O were 0.23 wt. %, 2.09 wt. %, 1.15 wt. % and 0.64 wt. %, respectively. The model showed a better predictability for AcOH and H.sub.2O than for DBN and APP, although the results were still in a good range for the two last molecules.
[0208]
4.4.2. Enhancing the PLS Model Prediction Performance Through Variable Selection
[0209] The purpose of variable selection is to obtain a model that is easier to understand, and which has better predictive performances. In searching for the best variable selection procedure, one might be tempted to try all possible combinations of the predictor variables in order to select the best one. However, this turns out to be prohibitive due to the large number of variables and causes a high risk of overfitting when the number of variables is higher than the number of samples (Andersen and Bro 2010). Both, conditions are encountered when dealing with spectroscopic data. Therefore, the purpose here is not to search for the best model, but for a better one, in terms of prediction and understanding.
[0210] With this regard, we adopted a simple method in which the spectral range was divided into 10 subintervals and PLS models were determined based on all possible interval combinations. The algorithm calculated the RMSEC for all combinations and chose the combination that resulted in the lowest RMSEC. The results are shown in
[0211]
[0212] The best cases for lowest RMSEC were found between those two extremes. They are summarized in Table 7 with the optimal number of subintervals and the corresponding lowest RMSEC. The reader can notice that with this simple procedure, the model calibration errors can be further reduced.
TABLE-US-00007 TABLE 7 PLS regression results: explained variances and RMSECVs RMSEC RMSEC No. of intervals for before iPLS, after iPLS, minimum Component wt. % wt. % RMSEC AcOH 0.20 0.14 3 DBN 1.73 0.76 2 APP 0.81 0.52 3 H.sub.2O 0.68 0.41 7
FURTHER EXAMPLES
[0213] A. Sample Preparation
TABLE-US-00008 TABLE 8 Specifications of the original [APPH][OAc] and [DBNH][OAc] stock solutions [APPH][OAc] [DBNH][OAc] Weight fractions stock solution stock solution H.sub.2O (KFT), wt. % 0.97% 0.05% APP+, wt. % of dry 63.0% 0.0% DBN+, wt. % of dry 12.1% 75.4% HOAc, wt. % of dry 24.9% 24.6% [APPH][OAc], wt. % of dry 83.9% 0.0% [DBNH][OAc], wt. % of dry 16.1% 100%
[0214]
[0215] B. Raman Spectroscopy Analysis
[0216]
[0217]
[0218] C. PCA
[0219]
[0220]
[0221] D. PLS Models [0222] a. AcOH
[0223]
[0224]
[0225]
[0226]
[0228]
[0229]
[0230]
[0231]
[0233]
[0234]
[0235]
[0236]
[0238]
[0239]
[0240]
[0241]
[0242] The different functions discussed herein may be performed in a different order and/or concurrently with each other.
[0243] Any range or device value given herein may be extended or altered without losing the effect sought, unless indicated otherwise. Also, any example may be combined with another example unless explicitly disallowed.
[0244] Although the subject matter has been described in language specific to structural features and/or acts, it is to be understood that the subject matter defined in the appended claims is not necessarily limited to the specific features or acts described above. Rather, the specific features and acts described above are disclosed as examples of implementing the claims and other equivalent features and acts are intended to be within the scope of the claims.
[0245] It will be understood that the benefits and advantages described above may relate to one embodiment or may relate to several embodiments. The embodiments are not limited to those that solve any or all of the stated problems or those that have any or all of the stated benefits and advantages. It will further be understood that reference to ‘an’ item may refer to one or more of those items.
[0246] The term ‘comprising’ is used herein to mean including the method, blocks or elements identified, but that such blocks or elements do not comprise an exclusive list and a method or apparatus may contain additional blocks or elements.
[0247] Numerical descriptors such as ‘first’, ‘second’, and the like are used in this text simply as a way of differentiating between parts that otherwise have similar names. The numerical descriptors are not to be construed as indicating any particular order, such as an order of preference, manufacture, or occurrence in any particular structure.
[0248] Although the invention has been the described in conjunction with a certain type of apparatus and/or method, it should be understood that the invention is not limited to any certain type of apparatus and/or method. While the present inventions have been described in connection with a number of examples, embodiments and implementations, the present inventions are not so limited, but rather cover various modifications, and equivalent arrangements, which fall within the purview of the claims. Although various examples have been described above with a certain degree of particularity, or with reference to one or more individual embodiments, those skilled in the art could make numerous alterations to the disclosed examples without departing from the scope of this specification.
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