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Origins of Heat Evolution in Mixing Water and Dimethyl Sulfoxide

著者 Mizuno Kazuko, Sumikama Takashi, Tarnai Yoshinori, Tani Masahiko

著者別表示 炭竈 享司

journal or

publication title

43rd International Conference on Infrared, Millimeter, and Terahertz Waves (IRMMW‑THz)

page range 1p.

year 2018‑09‑09

URL http://doi.org/10.24517/00053806

doi: 10.1109/IRMMW-THz.2018.8509894

Creative Commons : 表示 ‑ 非営利 ‑ 改変禁止 http://creativecommons.org/licenses/by‑nc‑nd/3.0/deed.ja

(2)

H

Origins of Heat Evolution in Mixing Water and Dimethyl Sulfoxide

Kazuko Mizuno

1,3

, Takashi Sumikama

2

, Yoshinori Tamai

1

, and Masahiko Tani

3

1

Graduate School of Engineering, University of Fukui, Fukui, 910-8507 Japan

2

WPI Nano Life Science Institute, Kanazawa University, Kakuma-machi, Kanazawa 920-1192 Japan

3

Research Center for Development of Far-Infrared Region, University of Fukui, Fukui, 910-8507 Japan Abstract—Dimethyl sulfoxide (DMSO) is one of small

amphiphiles composed of both hydrophobic and polar groups.

DMSO and water mix uniformly accompanied by intense heat evolution but molecular reasons of the negative molar excess enthalpy and entropy remain ambiguous since the 1940s. We present an interpretation on the origins, based on our results of IR and NMR measurements and simulations. Our interpretation can shed new light on the roles of water molecules in biological systems.

I. INTRODUCTION

eat evolutions observed on mixing water and a small amphiphile like alcohols have been related to self- association among water molecules through hydrogen(H-) bondings among water molecules around hydrophobic groups, which were considered to be stronger enough than those formed in bulk water [1]. Such the “Hydrophobic hydration”

has been the most widely used model of the water until thermodynamic, nuclear magnetic resonance (NMR) and simulation studies of aqueous solutions of clathrate-formers suggest that clathrate hydration is a more realistic model for hydrophobic hydration [2].

We have been skeptical about the interpretation of

‘hydrophobic hydration’, because roles of electronegative atoms like O and N of polar groups in amphiphiles solved in water in inter- and intramolecular polarization were not taken into consideration. We have been carrying out measurements of infrared (IR) and NMR spectra of aqueous binary mixtures of alcohols, ketones, and furans with varying compositions [3].

In this work, we measured the

1

H-chemical shift of water protons via NMR; and ν(Ο−D) stretching vibration spectra of HOD and ν(Η−Ο−H) bending vibration spectra of water in IR, and ν(C−H) stretching vibration spectra of the methyl groups, with varying the compositions via FTIR.

II. RESULTS.

We summarize in Fig. 1, the changes of chemical shifts for the water protons, the protons, and the carbons in DMSO caused by increasing water content. From the curves on Left column (A), mixing water with DMSO causes weakening of the H-bond donating strength of the Ο−H groups in water, which is contrary to the picture described by hydrophobic hydration.

The origin of the blue shift of ν(C−H) induced by a weak H- bond, C ─ H … OH

2

, was interpreted in terms of (1) polarization of the C ─ H bond, and (2) re-hybridization of the three C - H sp

3

orbitals followed by their contraction, where blue-shift of ν(C─H) vibration band occurs due to increase of the electron density in the C ─ H bond [3].

Fig. 1. Left column: Chemical shifts for the (A)

1

H protons of the water, (B)

1

H protons of the methyl groups in DMSO, and (C)

13

C carbons of the methyl groups in DMSO, in binary aqueous mixtures of DMSO with respect to concentration and temperature. Center column: Molar absorption spectra for the bending vibration band of the water in differing concentrations of binary mixtures of DMSO. Right column: Changes of O-D stretching vibration frequency, ν (O-D), in (HDO + H

2

O + DMSO) mixtures, and the bending vibration frequency ν (H-O-H) for the water in the binary mixtures with DMSO.

We have found that the heat evolution comes from the difference in the ease of localization of the oxygen electrons between C ─H•••OH

2

(a weak H-bond [3]) and in O─H•••OH

2

(the conventional H-bond). In the former, oxygen electrons cannot delocalize easily due to weak H-bonding; the accumulation of other electrons and friction among them results in heat evolution. Whereas in the latter, the formation of O─H•••OH

2

(the conventional H-bond), delocalization of the oxygen electrons can occur more easily.

Roles of water molecules in the interaction between or among the two types of H-bonds are not well understood, even though many kinds of amphiphiles exist in both animals and plants as biological reactors. Our results emphasize that weak hydrogen bonds play important roles in biological systems.

R EFERENCES

[1]. F. Franks, “HYDRATION AND THE EFFECT OF HYDROGEN BONDING SOLUTES ON THE STRUCTURE OF WATER,” Annals of the New York Academy of Science, vol. 125, pp. 277-289, 1965.

[2]. F. Franks, “Water: A Matrix of Life,” Royal Society of Chemistry, 2000.

[3]. K. Mizuno, S. Imafuji, T. Ochi, T. Ohta, and S. Maeda, “Hydration of the CH groups in dimethyl sulfoxide probed by NMR and IR,” Journal of Physical Chemistry B, vol. 104, pp. 11001-11005, November, 2000.

[4]. I. V. Alabugin, M. Manoharan, S. Peabody, and F. Weinhold, “Electronic basis of improper hydrogen bonding: A subtle balance of hyperconjugation and rehybridization,” Journal of the American Chemical Society, vol. 125, pp.

5973-5987, April 2003.

Fig. 1. Left column: Chemical shifts for the (A)  1 H protons of the water, (B)  1 H  protons of the methyl groups in DMSO, and (C)  13 C carbons of the methyl  groups in DMSO, in binary aqueous mixtures of DMSO with respect to  concentration and temperatu

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