quantitative analysis of water activity related to

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Communication Electrochemistry , 87(3), 139141 (2019) Quantitative Analysis of Water Activity Related to Hydration Structure in Highly Concentrated Aqueous Electrolyte Solutions Hideshi MAKI, a,b, * Ren SOGAWA, b Masaharu FUKUI, b Shigehito DEKI, b,and Minoru MIZUHATA b a Center for Environmental Management, Kobe University, 1-1 Rokkodai-cho, Nada-ku, Kobe 657-8501, Japan b Department of Chemical Science and Engineering, Graduate School of Engineering, Kobe University, 1-1 Rokkodai-cho, Nada-ku, Kobe 657-8501, Japan * Corresponding author: [email protected] ABSTRACT The measurements on the activity and solvation of H 2 O in hydrate melts and aqueous electrolyte solutions containing various metal chlorides were carried out by a vapor pressure measurement using a transpiration method and 1 H quantitative NMR ( 1 H qNMR). The electrolyte concentration dependence of the detection rate of H 2 O by 1 H qNMR reected the change of the hydration structure of the rst hydration shell, and the activity of H 2 O by the vapor pressure measurement clearly showed the change of the network structure of water including the rst and second hydration spheres. The correlation between the enthalpy and entropy of vaporization showed the existence of dierent kinds of water-cation interactions. © The Electrochemical Society of Japan, All rights reserved. Keywords : Activity Coecient, Hydration Structure, NMR, Hydrate Melt 1. Introduction Recently, the secondary batteries using aqueous electrolyte as an electrolytic solution have been extensively studied. 16 In the study of the secondary batteries using aqueous electrolyte, the attempts are made to ease desolvation, the extend of potential window from the viewpoint of equilibrium and reaction rate, and increase the electromotive force of the secondary batteries by reducing the activity of water using a concentrated electrolyte solution. 1,6,7 In this case, unlike the hydration structure of ordinary electrolytes, it is necessary to investigate the dynamic behavior of the solvent in a state which a sucient hydration sphere is not constructed, however the information about it is still not sucient. Therefore, in this study, the quantitative 1 H NMR ( 1 H qNMR) 811 method and the vapor pressure measurement were carried out using highly concentrated aqueous electrolyte solution and hydrate melts, and the activity of water, the ion hydration structure, the water-water and water-cation interactions were evaluated. 2. Experimental 2.1 Vapor pressure measurement using a transpiration method Samples were prepared in various concentration compositions from the reagent grade CaCl 2 , MnCl 2 , ZnCl 2 , and double-distilled water. Water vapor pressure of sample solutions was measured at various temperatures by using the transpiration method 1214 with a Karl-Fischer automatic titrator. From the equilibrium vapor pressure, P H2O , obtained by the above measurement, the activity of water, a H2 O , can be determined using the following equation: a H2O ¼ £ H2O X H2O ¼ P H2O =P ð1Þ where £ H2 O , X H2O , and P° is the activity coecient, of H 2 O, the mole fraction of H 2 O, and the vapor pressure of pure water, respectively. Furthermore, given that P° is the standard pressure, the standard Gibbs evaporation energy, ¦G V °, is G V ¼ RT ln P RT ln P H2O ¼RT lnðP H2O =P Þ¼ H V T S V ð2Þ where R, T , ¦H V ° and ¦S V ° is the gas constant and the temperature of sample solution, the standard vapor enthalpy, and the standard vapor entropy, respectively. 2.2 Quantitation of H 2 O using 1 H qNMR Samples were prepared in various concentration compositions from the reagent grade LiCl, NaCl, KCl, MgCl 2 , CaCl 2 and double- distilled water. 1 H qNMR spectra were observed on an INOVA 400 pulse FT-NMR spectrometer (Varian Inc., USA) at 20 « 0.5°C. 1 H qNMR analysis was carried out using the integrated intensities of 1 H NMR signals due to H 2 O molecules. 1 H NMR signal intensities of 20 sample solutions which have dierent mixing ratios of H 2 O and D 2 O (i.e., 0 < [H 2 O]/([H 2 O] + [D 2 O]) < 1) were measured as a calibration curve, and the calibration curve showed a high linearity with a correlation coecient of 0.9992 or more. 3. Results and Discussion The dependences of the activity coecient of H 2 O on the concentration compositions at various temperatures are shown in Fig. 1. For all sample solutions, £ H2 O decreased with decreasing molar ratio of H 2 O to electrolyte, r (i.e., [H 2 O]/C X (X = CaCl 2 , MnCl 2 , and ZnCl 2 )), however the decreases of £ H2O are not monotonous. In the CaCl 2 -H 2 O system, the decrease of £ H2 O becomes remarkable around r = 5.5, and it is nearly constant in r < 5. In the MnCl 2 -H 2 O system, the decrease of £ H2O was remarkable in r < 10. In the ZnCl 2 -H 2 O system, the decrease of £ H2 O becomes remarkable around r = 3, and it is nearly constant in r < 2.5. These suggest that the water-water and water-cation interactions becomes strong in the concentration region, and the network structure in solution changes. Furthermore, it should be noted that the previously reported electrical conductivity and its ³ Professor Emeritus, Kobe University, 1-1 Rokkodai-cho, Nada-ku, Kobe 657-8501, Japan Electrochemistry Received: November 13, 2018 Accepted: December 17, 2018 Published online: February 21, 2019 The Electrochemical Society of Japan https://doi.org/10.5796/electrochemistry.18-00087 139

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Communication Electrochemistry, 87(3), 139–141 (2019)

Quantitative Analysis of Water Activity Related to Hydration Structurein Highly Concentrated Aqueous Electrolyte SolutionsHideshi MAKI,a,b,* Ren SOGAWA,b Masaharu FUKUI,b

Shigehito DEKI,b,† and Minoru MIZUHATAb

a Center for Environmental Management, Kobe University, 1-1 Rokkodai-cho, Nada-ku, Kobe 657-8501, Japanb Department of Chemical Science and Engineering, Graduate School of Engineering, Kobe University,1-1 Rokkodai-cho, Nada-ku, Kobe 657-8501, Japan

*Corresponding author: [email protected]

ABSTRACTThe measurements on the activity and solvation of H2O in hydrate melts and aqueous electrolyte solutionscontaining various metal chlorides were carried out by a vapor pressure measurement using a transpiration methodand 1H quantitative NMR (1H qNMR). The electrolyte concentration dependence of the detection rate of H2O by1H qNMR reflected the change of the hydration structure of the first hydration shell, and the activity of H2O by thevapor pressure measurement clearly showed the change of the network structure of water including the first andsecond hydration spheres. The correlation between the enthalpy and entropy of vaporization showed the existenceof different kinds of water-cation interactions.

© The Electrochemical Society of Japan, All rights reserved.

Keywords : Activity Coefficient, Hydration Structure, NMR, Hydrate Melt

1. Introduction

Recently, the secondary batteries using aqueous electrolyte as anelectrolytic solution have been extensively studied.1–6 In the studyof the secondary batteries using aqueous electrolyte, the attempts aremade to ease desolvation, the extend of potential window from theviewpoint of equilibrium and reaction rate, and increase theelectromotive force of the secondary batteries by reducing theactivity of water using a concentrated electrolyte solution.1,6,7 In thiscase, unlike the hydration structure of ordinary electrolytes, it isnecessary to investigate the dynamic behavior of the solvent in astate which a sufficient hydration sphere is not constructed, howeverthe information about it is still not sufficient. Therefore, in this study,the quantitative 1H NMR (1H qNMR)8–11 method and the vaporpressure measurement were carried out using highly concentratedaqueous electrolyte solution and hydrate melts, and the activity ofwater, the ion hydration structure, the water-water and water-cationinteractions were evaluated.

2. Experimental

2.1 Vapor pressure measurement using a transpiration methodSamples were prepared in various concentration compositions

from the reagent grade CaCl2, MnCl2, ZnCl2, and double-distilledwater. Water vapor pressure of sample solutions was measured atvarious temperatures by using the transpiration method12–14 with aKarl-Fischer automatic titrator.

From the equilibrium vapor pressure, PH2O, obtained by theabove measurement, the activity of water, aH2O, can be determinedusing the following equation:

aH2O ¼ £H2O� XH2O ¼ PH2O=P

� ð1Þwhere £H2O

, XH2O, and P° is the activity coefficient, of H2O, themole fraction of H2O, and the vapor pressure of pure water,

respectively. Furthermore, given that P° is the standard pressure, thestandard Gibbs evaporation energy, ¦GV°, is

�GV� ¼ RT lnP� � RT lnPH2O

¼ �RT lnðPH2O=P�Þ ¼ �HV

� � T�SV� ð2Þ

where R, T, ¦HV° and ¦SV° is the gas constant and the temperatureof sample solution, the standard vapor enthalpy, and the standardvapor entropy, respectively.

2.2 Quantitation of H2O using 1H qNMRSamples were prepared in various concentration compositions

from the reagent grade LiCl, NaCl, KCl, MgCl2, CaCl2 and double-distilled water. 1H qNMR spectra were observed on an INOVA 400pulse FT-NMR spectrometer (Varian Inc., USA) at 20 « 0.5°C.1H qNMR analysis was carried out using the integrated intensities of1H NMR signals due to H2O molecules. 1H NMR signal intensitiesof 20 sample solutions which have different mixing ratios of H2Oand D2O (i.e., 0 < [H2O]/([H2O] + [D2O]) < 1) were measured as acalibration curve, and the calibration curve showed a high linearitywith a correlation coefficient of 0.9992 or more.

3. Results and Discussion

The dependences of the activity coefficient of H2O on theconcentration compositions at various temperatures are shown inFig. 1. For all sample solutions, £H2O

decreased with decreasingmolar ratio of H2O to electrolyte, r (i.e., [H2O]/CX (X = CaCl2,MnCl2, and ZnCl2)), however the decreases of £H2O

are notmonotonous. In the CaCl2-H2O system, the decrease of £H2O

becomes remarkable around r = 5.5, and it is nearly constant inr < 5. In the MnCl2-H2O system, the decrease of £H2O

wasremarkable in r < 10. In the ZnCl2-H2O system, the decrease of£H2O

becomes remarkable around r = 3, and it is nearly constant inr < 2.5. These suggest that the water-water and water-cationinteractions becomes strong in the concentration region, and thenetwork structure in solution changes. Furthermore, it should benoted that the previously reported electrical conductivity and its

³Professor Emeritus, Kobe University, 1-1 Rokkodai-cho, Nada-ku, Kobe657-8501, Japan

Electrochemistry Received: November 13, 2018Accepted: December 17, 2018

Published online: February 21, 2019

The Electrochemical Society of Japan https://doi.org/10.5796/electrochemistry.18-00087

139

activation energy for CaCl2 and ZnCl215,16 also show a remarkableincrease at almost the same r value as above.

To further thermodynamically consider the above results, ¦HV°and ¦SV° were determined from the temperature dependence of¦GV°. The Barclay-Butler plots,17–21 namely ¦SV° vs. ¦HV° plots,are shown in Fig. 2. For the CaCl2-, and ZnCl2-H2O systems, theseplots show clear discontinuous point, and the r values at thediscontinuous points are good agreement with those at the aboveinflection points in Fig. 1. It is obvious that the interaction betweenmolecules in the solution changes markedly at these inflectionpoints. Based on the r dependence of the Barclay-Butler correlation,three types of regions, namely RI, RII and RIII, were defined as inFig. 2. From the r and the hydration number of the ions, the variousinteractions for water, cations, and anions in the aqueous solution ineach region can be considered as advocated by Marcus and Hefter22

(a simplified illustrate is shown in Scheme 1): namely, (i) RI: Thewater-cation interaction becomes stronger in the vicinity of eachcation and anion, and the orientation of H2O molecule increases; (ii)RII: As a result of reduced free water, cations and anions begin toform contact ion pairs, hence the water-cation interaction decreases;(iii) RIII: Formation of contact ion pair becomes conspicuous, henceH2O molecules are not oriented to isolated ions and weakly interactto contact ion pair.

The dependence of the detected H2O ratios by 1H qNMR inLiCl-, NaCl-, KCl-, MgCl2-, and CaCl2-H2O systems on the r valueare shown in Fig. 3. Remarkably, it is obvious that the detected H2Oratios by 1H qNMR (filled circles in Fig. 3) is smaller than the H2Oamount (open circles in Fig. 3) calculated from the densitymeasurement of sample solution. The dashed line in Fig. 3 showsthe extrapolation of the electrolyte concentration dependence of thedetected H2O ratios by 1H qNMR in the dilute electrolyteconcentration region of 0.5mol L¹1 or less. Assuming that watermolecules in the first hydrated shell of cations cannot be detected by1H q NMR, the hydration number calculated from the slope of thisdashed line tended to agree with the literature value23,24 (Table 1).

This obviously suggests that the mobility of the water moleculesbound in the first hydration shell of cations are extremely restrictedand thus cannot be detected by 1H NMR. This is in contrast to theactivity measurement from vapor pressure which reflects the water-water and water-cation interactions, that is, the network structure ofwater including the first and second hydration spheres. On the otherhand, in the electrolyte concentration of 0.5mol L¹1 or more, thedetected H2O ratios by 1H qNMR shows an extraordinary changewith increasing electrolyte concentration, namely, they show thelocal minimum value and increase, then turn to decrease again(LiCl- and NaCl-H2O systems) or the decrease once becomes mildly(MgCl2- and CaCl2-H2O systems). These reversal and mitigation ofthe decrease in the detected H2O ratios with the increase in theelectrolyte concentration (CLiCl = 3mol L¹1, CNaCl = 2mol L¹1,CMgCl2 = 1mol L¹1, CCaCl2 = 1.5mol L¹1) is considered to beowing to the release of H2O which hydrated to the cation and theanion at the initial stage of the formation of contact ion pair. Such aphenomenon is thought to be remarkable in the case of “structure-making ion”23 which strongly attract water in the hydration shell.Indeed, in the system containing K+ ion which is “structure-breaking ion”, the decrease of the detected H2O ratios by 1H qNMRis monotonous. Furthermore, the hydration structure in theintermediate electrolyte concentration region (i.e., 0.5 < CLiCl <3mol L¹1, 0.5 < CNaCl < 2mol L¹1, 0.5 < CMgCl2 < 2.5mol L¹1,0.5 < CCaCl2 < 1.5mol L¹1) may be more destabilized than that in

(a) CaCl2-H2O system

[H2O] / CCaCl2

γ H2O

T / ˚C

(b) MnCl2-H2O system (c) ZnCl2-H2O system

γ H2O

γ H2O

[H2O] / CMnCl2[H2O] / CZnCl2

T / ˚C T / ˚C

9 8 78.5 7.5 6.5CCaCl2

/ mol L-1

10

CZnCl2/ mol L-1

11 9 812

CMnCl2/ mol L-1

6 5 4 3.5 3.24.55.5

Figure 1. Dependence of the activity coefficient of H2O on the concentration compositions at various temperatures in the CaCl2-, MnCl2-,and ZnCl2-H2O systems.

ΔHV˚/ kJ mol-1

ΔSV˚/

kJ m

ol-1

K-1

(a) CaCl2-H2O system (b) MnCl2-H2O system (c) ZnCl2-H2O system

r < 5.5

r > 5.5RI

RIII

ΔHV˚/ kJ mol-1ΔS

V˚/

kJ m

ol-1

K-1

r < 2.8

r > 2.8RII

RIII

ΔHV˚/ kJ mol-1

ΔSV˚/

kJ m

ol-1

K-1

RI7.0 < r < 23.6

r ≈ 5.5RII

Figure 2. Barclay-Butler relationships for the vaporization of CaCl2-, MnCl2-, and ZnCl2-H2O systems.

RI RII RIII

Scheme 1. Schematic representation of the various interactions forwater, cations, and anions in the aqueous solution.

Electrochemistry, 87(3), 139–141 (2019)

140

the Debye-Hückel region.22,25 The water release owing to theformation of contact ion pair which observed by 1H qNMR occurredin the much lower concentration region than the region where the gvalue reaches the inflection point. This study suggested that theformation behavior of contact ion pairs in highly concentratedaqueous electrolyte solution complicatedly may be changed withincrease of the electrolyte concentration. Furthermore, it is shownthat the possibility which the NMR signal intensity depends on thephysicochemical environment of atoms and molecules. This suggeststhat quantitative NMR can be used as a novel tool to estimate theactivity of observation chemical species. The findings obtained inthis study are useful for elucidating of the enlargement of potentialwindow of high concentration aqueous electrolyte solutions and thedevelopment of high voltage aqueous secondary batteries.6

4. Conclusions

In the measurements of £, ¦H ° and ¦S ° of H2O by vaporpressure measurement, the changes of the hydration structure in thehydration shell and the interaction between molecules as theincrease of the electrolyte concentration was shown. The activitymeasurement from vapor pressure reflected the change of thenetwork structure of water including the first and second hydrationspheres. In the 1H qNMR measurement, it was confirmed that aremarkable decrease in the detection rate of H2O molecules as theincrease of the electrolyte concentration. It can be regarded as aresult of a significant decrease of the H2O mobility in the hydration

shell, and this suggests the possibility which the activity of varioussolvent molecules can be determined by 1H qNMR method.Furthermore, the decrease in the detection rate of water moleculeswas not monotonous with the increase in electrolyte concentration,and showed the inflection point peculiar to ions. It can be consideredthat the solvation structure of water in the first hydration zonechanged by the formation of contact ion pair.

References

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2. D. Bin, Y. Wen, Y. Wang, and Y. Xia, J. Energy Chem., 27, 1521 (2018).3. N. Alias and A. A. Mohamad, J. Power Sources, 274, 237 (2015).4. C. Yang, J. Chen, T. Qing, X. Fan, W. Sun, A. Cresce, M. S. Ding, O. Borodin, J.

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Xu, Science, 350, 938 (2015).8. S. K. Bharti and R. Roy, Trends Anal. Chem., 35, 5 (2012).9. G. F. Pauli, T. Gödecke, B. U. Jaki, and D. C. Lankin, J. Nat. Prod., 75, 834

(2012).10. H. Maki, G. Sakata, and M. Mizuhata, Analyst, 142, 1790 (2017).11. H. Maki, Y. Okumura, H. Ikuta, and M. Mizuhata, J. Phys. Chem. C, 118, 11964

(2014).12. H. E. Bent and R. J. Francel, J. Am. Chem. Soc., 70, 634 (1948).13. W. Davis, Jr. and H. J. Bruin, J. Inorg. Nucl. Chem., 26, 1069 (1964).14. R. Prasad, V. Venugopal, and D. D. Sood, J. Chem. Thermodyn., 9, 765 (1977).15. S. Deki, M. Mizuhata, S. Nakamura, K. Nakamura, A. Kajinami, and Y. Kanaji,

J. Electrochem. Soc., 139, 996 (1992).16. M. Mizuhata, Y. Sumihiro, and S. Deki, Phys. Chem. Chem. Phys., 6, 1944 (2004).17. M. Barclay and J. A. Butler, Trans. Faraday Soc., 34, 1445 (1938).18. H. S. Frank, J. Chem. Phys., 13, 493 (1945).19. C. F. Wells, Inorg. Chim. Acta, 177, 127 (1990).20. A. R. Henn and W. Kauzmann, Biophys. Chem., 100, 205 (2002).21. G. Graziano, J. Phys. Chem. B, 109, 981 (2005).22. Y. Marcus and G. Hefter, Chem. Rev., 106, 4585 (2006).23. P. Sripa, A. Tongraar, and T. Kerdcharoen, J. Mol. Liq., 208, 280 (2015).24. H. Ohtaki and T. Radnai, Chem. Rev., 93, 1157 (1993).25. N. F. A. Vegt, K. Haldrup, S. Roke, J. Zheng, M. Lund, and H. J. Bakker, Chem.

Rev., 116, 7626 (2016).

(b) NaCl-H2O system

(e) CaCl2-H2O system

(a) LiCl-H2O system

CNaCl / mol L-1

CCaCl2/ mol L-1

CLiCl / mol L-1

(c) KCl-H2O system

CKCl / mol L-1

(d) MgCl2-H2O system

CMgCl2/ mol L-1

100 50 40 30 20 15 12 100 50 40 30 20 15 12

[H2O] / CLiCl [H2O] / CNaCl100 50 40 30 20 15 12

[H2O] / CNaCl

100 50 40 30 20 15 12

[H2O] / CMgCl2100 50 40 30 20 15 12

[H2O] / CMgCl2

Figure 3. Detected ratios of H2O by 1H qNMR in LiCl-, NaCl-, KCl-, MgCl2-, and CaCl2-H2O systems. ( ) Detected H2O amount by1H qNMR; ( ) calculated H2O amount from density measurements of sample solutions.

Table 1. Hydration number of cations which calculated from theslope of the dashed line in Fig. 3 and the literature value.22,23

Li+ Na+ K+ Mg2+ Ca2+

This study 5.4 6.5 7.8 7.5 8.8

Literature 4.223 5.423 6.323 6.024 7.623

Electrochemistry, 87(3), 139–141 (2019)

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