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A C T A U N I V E R S I T A T l S L O D Z I E N S I S _____________ FOLIA CHIHICA 2, 1983________

Stefania. TanimMka-Oaińeka, flytuuzrd Gvoohoueki, B artłom iej Pateas •SPECTROSCOPIC INVESTIGATIONS

OF AQUEOUS NONELECTROLYTE SOLUTIONS

The observation of changes of water combination band (v( ^ * + V 2 ) [l] under the influence of organic solventa (ethylene gly­ col, glycerol, acetone, DMSO, dioxane, DMF) over the whole concen­ tration range was carried out.

' INTRODUCTION

Analysing, in our previous works [1, 2] the changes of wa­ ter spectra parameters caused by the temperature effect on the electrolytes dissolved in it or by monohydric alcohol we have chosen combination band (Vj 3 + V 2> of -OH groups as particul­

arly suitable for the Investigations, The changes of half width of this band seemed to fit the criterion of ordering and disor­ dering influence on water structure.

Examining water-alcohol mixtures we have also observed that ^ t h e band intensity as the function of composition seems to po- £^int to the changes of some interactions in the solution.

0 g| The combination band of water chosen by us was also examin­ ed by S i d o r o v a [3] and K o c h n e v [4]. Observ­ ing the wave number changes of combination band (Vj 3 + Vj) with

the composition change of water-alcohol systems, S i d o r o ­ v a et al. [3 ] came to the conclusion on ordering influence of small portions of monohydric alcohols on water structure si­ milar to those in our works.

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34 S. Taniewaka-OalAska, R. Grochowaki, B. PaJrec*

... ... ... . ... .. . .... — — ... ... . ....

The interpretation of the effect of ions on water structure led however to incompatible conclusions relative to the crite­ ria accepted by the mentioned authors and by us.

In this work we present spectroscopic investigations of aqueous solutions of some organic substances often used both in science and technology as solvents.

EXPERIMENTAL

, Measurements were carried out using a Unicam SP-700 spectro­ meter [1, 2] at the temperatur 25°C. The cell path length was 0,2 mm. Stability -0,5°C.

RESULTS AND DISCUSSION

Ethylene glycol-water

The absorotion in maximum (intensity) dependence of water combination band (Vj 3 + Vj) in binary mixture on ethylene gly­ col content E » f(x) (x is the mole per cent of organic sol­ vent) is expressed by the line with inflexion points (fig. 1).

These points make it possible to divide the whole range of the investigated mixture into four regions: 1:0-7 mol. S, II: 7-32 mol. %, III: 32-54 mol. %, IV: 54-100 mol. % of ethylene gly­ col. The observed changes of the E = f(x) function course sug­ gest certain differences in properties of the mixture relative to the concentration of the components.

The course of relation of the half-width: (Wt /2) of the discussed band and the mixture composition is also illustrated by the broken line (fig. 2) the inflexion points of which di­ vide the whole composition range into four regions. They cor­ respond exactly to the regions indicated by the absorption con- centrational relation course.

In the 1st region a slight decrease of the half-width in relation to its value in pure water can be observed. In an

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ear-Fig. 1. The dependence of water combination band absorption in maximum on the concentration of organic in mixturesi 1 - water-ethylene glycoli 2 - water- -glycerolj 3 - water-acetonf 4 - water-DMSO> 5 ~ water-dioxane, 6 - water- -DMF. The dependence of absorption in maximum of the first overton-op band on the concentration of organic solvent in mixtures: 4' waterDMSOj 5'

-water-dioxane

lier paper [1] the influence of the temperature changes on the bands of combination vibrations of the OH-group of water has

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Fig- 2. The course of dependence of half-width of water combination band on the concentration of organic solvent in mixtures: I - water-ethylene glycol) 2 - water-glycerolj 3 - water-aceton; 4 - water-DMSO; 5 - water-dioxaney 6 water-DMF. The dependence of half-width of the first overtone - OD band on the concentration of organic solvent in mixtures: 4' - water-DMSO; 5' -

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been investigated. It has been noticed that the half-width may be accepted as the index of "ordering" and "disordering“ influ­ ence on the water structure. The above criterion has been suc- cesfully applied to the influence of electrolyte and monohydric alcohols on water structure. Taking into consideration the abo­ ve results it may be assumed that the addition of glycol breaks the structure of water in the system. It reveals in the dec­ rease of the half width of the investigated band over the whole composition range. K r e s t o v [5] has interpreted the re­ lations between argon apparent heat capacity in the discussed system and the mixed solvent composition and he has drawn the conclusion, that glycol exerts destructive effect on water structure.

The acidity functions for water-organic series led B o y e r et al. {6] to the conclusion that the addition of diols to wa ­ ter causes the disturbance of the threedimentional water clath- rate compounds. The analysis of the. relation that holds bet­ ween wave number < max variations of the investigated band and

the investigated mixture composition (fig. 3) may lead to op­ posite conclusions. The discussed function is in the 1st region a monotonously decreasing curve.

According to S i d o r o v a [3,7] the decrease of the wave number of the OH - groups combination band shows that wa­ ter structure is ordered by the added component. Investigating the wave number concentrational variations in water-glycol mix­ tures, K o c h n e v £41 has obtained the coursé of function similar to that of ours. According to the author the drastic wave number decrease in the first region substantiates the or­ dering influence of nonelectrolyte as it is in the case of mono­ hydric alcohols. In the Il-nd range a drastic decrease of the half - width can be observed which substantiates, assuming the above mentioned critérium [1 1, the increasing destructive influ­ ence of glycol on water structure with the concentration growth.

In this range the occurance of 2 s 1 water-glycol associa­ tes is probable. Above the 1-st region the wave number - con­ centration function has the form of a less rapidly decreasing curve in the whole composition range, which is rather

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diffi-Fig. 3. The course of dependence of wave number V of water combination band on the concentration of organic solvent in mixtures: 1 - water-ethylene gly­ col; 2 - water-glycerolj 3 - water-aceton; 4 - water-DMSO; 5 - water-dioxa- ne; 6 - water-DMF. The dependence of wave number V of the first overtone - OD band on the concentration of organic solvent in mixtures: 4' - water-DMSO;

5' - water-dioxane

cult to explain now. Investigating the viscosity and density of water-glycol mixtures, I r a n y [8] has observed an in­ crease of viscosity starting with 30 mol. % contents.

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The course of these relations may hint at a change of pro­ perties between water-like structure solution and associated structure. At about 25 mol. % of ethylene glycol the maximum of water-ethylene glycol f9] mixing heat occurs. In the Ill-rd region a less drastically decreasing half-width is observed. It can be assumed that the shift from 2 * i to 1 s 1 associated

structure occurs.

In the IV-th region, above 50 mol. % as the concentration of the organic substance grows, we have probably to do with the glycol-likc structure.

Above the concentration of 60 mol. ft the diol value of electrolyte solutions activity coefficients is water-glycol mixtures decreases drastically [1 0].

Basing on the results of free energy of transfer of alcali metal chlorides from water to water-glycol mixtures W e l l s [11] has observed that in the range of 75 mol. ft of organic solvent the stabilization of "extra" water icebergs by ethylene glycol OH-group occurs.

Glycerol-water

Alike in water-glycol systems the relation between the intensity of water combination band and glycerol concentration E » f(x) is expressed by line (fig. l) with three Inflexion points. These points allow to distinguish three water-glycerol mixture composition ranges. They are as follows: I-st range 0-6 mol. ft of glycerol, Il-nd 6-24 %, Ill-rd 24-52% and IV-th 52-100 mol. ft of glycerol.

The observed changes of the discussed curve course hint, similarly to the case of ethylene glycol-water mixture, at the existance of certain differances in the mixture structure depending on the changes of the component concentration. The division of the whole composition range of glycerol-water mix­ ture may be performed on the basis of the dependence of half - width changes of the investigated band on glycerol content

(fig. 2).

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slope alike in the case of water-glycol mixture. It may be assumed that this slope substanciates a faintly disturbing ef­ fect of glycerol on water structure. The acid functions deter­ mined by B a y o r et al. (6) for the water-organic series

lead to a similar conclusion. According to the authors, the ad­ dition of trioles causes destruction of three dimensional wa­ ter clathrates. Calorimetric and densymetric measurements have led P a o 1 a and B e 1 1 e a n Cl21 to the conclusion that in water-glycerol solutions there exists much smaller or­ dering than in pure water. According to these authors the ef­ fect of glycerol on water structure is comparable to that of urea.

A different conclusion may be drawn from the analysis of Vmax wave number of the combination band changes relative to the glycerol concentration. Basing oh S i d o r o v a ' s opi­ nion [3, 7] the decreasing values of this function in compa­ rison to the value for pure water show the ordering effect of the added substance on water structure.

Examining the relation between the apparent thermal capa­ city of argon and the mixed solvent composition, Krestov came to a similar conclusion. In the discussed system the author has observed a similar course of changes of Cp values as it is in the case of monohydric alcohols, which in his opinion order wa­ ter- structure.

I > o g w i n i e n k o and P 1 u t a [13] have measured KI solution heat in water-glycerol mixtures. The heat isotherms of KI dissolving in the above mentioned system display the shift from type II, occuring only in aqueous solutions, to the cha­ racter typical for nonaqueous solvents (i-st type). This shift corresponds to about 8 mol. % of glycerol content, near the

value corresponding to the mixture composition in the first inflexion point of E * f(x) function.

It may be assuaied that starting from the given composition in water-glycerol mixture, water structure is obviously distur­ bed and this process intensifies, with the organic solvent con­ centration growth.

In the Il-nd range a drastic slope of half-width can be ob­ served. According to the previously expressed opinion it may

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substantiate a more intensive breaking of water-like structure of a solution by glycerol molecules.

In the above mentioned solution both density and viscosity [14] of tha discussed system change their values drastically. It provides a strong argument for a distinct change of struc­ ture and properties of mixture.

When the glycerol content reaches 25 mol. % the occurance of 1 s 3 type glycero1-water associates is probable.

The relation between the wave number and concentration both in this range and in the two remaining ones is represented by a monotously decreasing curve.

Examining the standard SEM of glycerol-water and electro­ lyte system within the range at 0 - 2 0 mol. % of glycerol

K h o o [153 has noticed some structural changes. According to this author the addition of trioles to water at first causes the growth of the structural order (about 1 2%) and the further quantities cause structure breaking in relation to water. A slight slope of the half - value width can be observed in the Ill-rd range. The occuring Inflexion at 52 mol. % of glycerol concentration, alike in water-monohydric alcohol systems [16] suggests the possibility of shifting of 1 : 3 associates into 1 : 1 agregates. The IV-th and the last of the ranges is pro­ bably the region of passing from mixed associates structure to glycerol-like structure.

Acetone-water

The intensity and half-width dependence of combination band (\?i 3 + Vj) of OH group of water on acetone concentration is expressed by the lines tl, 3] with four inflexion points, which make it possible to distinguish four characteristic regions i. e. Is 0-6 mol. %, II: 6-28 mol. %, Ills 28-50 mol. %, IV: 50-

- 1 0 0 mol. % of acetone.

In the first region a drastic decrease of half-width in comparison to a minimum decrease in glycol and glycerine sys­ tems can be observed.

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[1] it can be assumed that the addition of acetone causes water structure breaking in the investigated system.

A similar supposition is formulated by K r e s t o v [51 who interpreted the dependence of apparent heat capacity of ar­ gon on the acetone-water mixture composition and has drawn the conclusion about acetone distructlve influence on water struc­ ture. According to our and Kochnev's results, the wave number values rapidly decrease in the discussed region (fig. 3). In S i d o r o v a ' s e t a l . opinion [3, 7] this course proves the ordering effect of this substance on water structure. A no­ ticed inflexion of the function of half-width of C - 0 acetone band at about 8 mol. % of organic solvent 1. e. near observed

by us (6 mol. %) [17J. According to the author this course of

function may be associated with a change of specific nonelec­ trolyte molecule-water interactions.

In the Il-nd region a less drastic decrease of half - width can be obseved (fig. 2). The wave number value in this range increases with acetone concentration. It can be assumed that acetone molecule having two free electrone pairs may form 1 : 2

type associates with two water molecules (which is substantia­ ted by the second characteristic inflexion) (fig. 2). The pos­ sibility of existence of such type of complex is also suggest­ ed by spectroscopic works of F o x [18] and N a b i e r u- c h i n [19] .

In the discussed concentration range maximum of viscosity and ultrasound velocity [2 0],* diffusion activation energy 1 2 1] and maximum of proton relaxation time of acetone [2 2] could be

found.

In the Ill-rd region half-width decreases quite rapidly. The shift from 1 : 2 into 1 : 1 water-acetone agregates is possible in this region. This supposition is in accordance with N a b i e r u c h i n [19] and K e c k i s [23] opinion.___

Above 50 mol. % of acetone concentration the region of aqueous solutions of acetone begins.

Its properties become similar to those of pure acetone when the concentration of nonelectrolyte grows.

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DMSO - water

The intensity dependence of (Vx 3 + V 2> water combination band on DMSO concentration E = f(x) in a binary mixture is ex­ pressed by the line (fig. l) with the inflexion points. These points make it possible to divide the whole area of the in­ vestigated mixture . into three regions. Is from 0 to 30 mol. %, lit from 30 to 53 mol. % and Ills from 53 to 100 mol. % of or­ ganic solvent. The observed changes of E = f(x) function course suggest certain differences in properties of the mixture relat­ ive to the component concentration. The course of relation of the half-width (v,i/2) curve of the discussed band vs. the mix­ ture composition is also idustrated by the line (fig. 2). The inflexion points of this curve divide the whole composition area into three regions. They correspond exactly to the regions indicated by the absorption relation course.

In the I-st region a drastic change of the half-value width in relation to its volue in pure water can be observed.

The density measurements of this system also [24] suggest the destabilization of structure and hydrogen bonds breaking by DMSO molecules which occur in threedimentional water network.

Basing on the data concerning partial molal entropy and the heat of hydrogen solution in the discussed - mixture, S v-m o n s [25] suggests the occurance of 3 : 1 , 2 : 2 water- DMSO associates. The viscosimetric investigations by C o w i e and T o p o r o v s k i [26] and M i l e s [27), spectro­ scopic and calorimetric works by F o x and W h i t t i n g - h a m [28] and K e 1 m [29] electrochemical works by El - H a r a k a n y [30], L i n d e b e r g e ' s magnetic nuc­ lear resonance [31] provide a strong argument for the existance of such associates.

The analysis of the relation between changes of v max wave number of the examined band and the mixture composition allows to conclude that DMSO affects water structure. This function' is a curve decreasing from pure water values up to the concentr­ ation of about 30 mol. % of DMSO. According to S i d o r o v a

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trolyte on water structure. The discrepancies arising through the analysis of the changes of half-value width and wave number of the combination band (Vj/j + made us perform a series of spectroscopic measurements for DMSO - H 20 system within the concentration range 0-6 mol. % of organic solvent. He have ex­ amined the dependence of intensity« half-value and wave num­ ber on DMSO concentration for the first 2 band.

O H

Intensity and half-width decrease with the concentration growth (fig. 1, 2), while the value of wave number slightly in­

creases (fig. 3). The interpretation of the above mentioned parameters along the accepted criteria [1, 3, 7] allows us to conclude that nonelectrolyte exerts a distructive influence on water structure.

The viscosimetric and dielectric investigations of water- -DMSO system carried out by K e s s l e r et al. [32] have shown, however, the stabilizing influence of organic solvent on water structure below 15 mol. % of DMSO concentration. This sug­ gestion is confirmed by S a f f o r d [33], who has examined the discussed system by x - rays. According to him a small portion of DMSO added to water causes water structure ordering.

On the other hand B r i n k and F a l k [34] invest­ igating the discussed system in infra-red came to the conclus­ ion that a small mole per centage of DMSO does not bring about any changes in three dimentlonal water network.

In the mixtures of about 30 mol. % DMSO concentration (the first inflexion on E “ f(x) and Wj^ 2 ■ f(x) functions) cha­

racteristic spheres on entropy activation curves [35] and viscosity curves occur [36]. In this region the deviation [37] of dielectric constant from additivity shows maximum [37].

In the Il-nd range, where DMSO content varies from [30] to 53 mol. %, the values decrease less drastically (fig. 2), while the wave number is constant and independent of the com­ position till 100 mol. % of DMSO.

It may be assumed that with the DMSO concentration the shift of 1 : 2 type DMSO-water associates into 1 : 1 associates takes place. It is also suggested by spectroscopic investigat­ ions carried out by K e 1 m [29]. In the Ill-rd range,above 50 mol. % of DMSO concentration a moderate slope of half-width can be observed (fig. 2).

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In this region the dimethylsulfooxide-water solutions occur. With the growth of concentration of organic solvent their pro­ perties become similar to these of pure DMSO.

Dloxane-water

The dependence of concentration and half-width of the com­ bination band (Vt 3 + V 2 ) of OH-water groups on dioxane concen­ tration is expressed by the lines with three inflection points (fig. 1, 2). These points allow to distinguish three /character­ istic regions i. e. Is 0-16 mol. %, II: 16-41 mol. % and III: above 41 mol. % to 100 mol. % of dioxane.

In the I-st range a drastic decrease of half-width can be observed in comparison to its value in pure water which sub­ stantiates the destructive influence of dioxane on water struct ture [1]. This suggestion is confirmed by K r e s t o v [5] who interpreting the apparent heat capacity of argon in the dis­ cussed mixture on the mixed solvent composition concludes that dioxane affects water destructively. The analysis of the rela­ tion wave number «• f(x) of the given band (fig. 3) may

m a x

lead to different conclusions. The discussed function is at first presented as a curve decreasing to the value correspond­ ing to 16 mol. % of dioxane which may suggest, in accordance with S i d o r o v a ' s opinion [3, 7], the ordering effect on the of water structure.

. In order to account for divergent interpretations of half- - width and wave number, we have performed a series of spectro­

scopic measurements for dioxane - D^O system.

Considering the changes of stretching vibrations more cha­ racteristic for structure observations than deformation vibrat­ ions we have chosen the overtone band instead of the combinat­ ion band.

The intensity of the first overtone OD band and half-width decrease rapidly with the organic solvent Concentration growth (fig. 1, 2) while the values of wave number grow (fig. 3). The interpretation of the discussed parameters provides a strong argument for the destabilising influence of dioxane on three dimensional water structure.

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Basing on the Arhenius activation energy changes C 1 e- m e t t [381 expresses the opinion about the ordering inflic­ ence of dioxane. The excess mixing entropy of the discussed system, which shows minimum at about 2 0 mol. % of organic sol­ vent confirms this opinion. According to C l e m e t t [391 mentioned concentration of dioxane is the border between dio­ xane solutions in water and water clathrates in dioxane.

Within this concentration range S h k o d i n [401 has obtained maximum of viscous flow activation energy in the func­ tion of composition. Analysing spectroscopy data of water-dio- xane and D20-dioxane systems, N a b i e r u c h i n [41] claims that hydrogen bonds in water strengthen on adding small ammounts of dioxane. Near the characteristic point i. e. at about 2 0 mol. % of dioxane in the discussed mixture the dielec­ tric constant shows minimum, the self-diffusion activation energy shows maximum (421 and the minimum of maxing heat oc­ curs [431.

The half-width gradually decreases in the Il-nd and Ill-rd regions, and the wave number value in these regions grows with the growth of nonelectrolyte concentration.

C l e m e t t [441 expresses the opinion that in the range of greater nonelectrolyte concentrations water occurs in the form of clusters which disappear when the organic solvent con­ tent is below 70 mol. % because dioxane molecules become more effective in destroying the hydrogen bonds in water.

The investigations of this system in infra-red have shown that 4.7 /t band, characteristic for pure water disappears when nonelectrolyte concentration exceeds 70 mol. % [451, This ob­ servation is confirmed by the work of N a b i e r u c h i n

[191 who claims that the appearing water globules break when lioxane concentration is above 80 mol. %, which is the result of hydrogen bonds weakening.

DMF-water

The functions of density and half-wldth of (Vj 3 + V 2) OH- -group of water combination band in relation to DMF concentrat­ ion are illustrated by the lines with characteristic regions on

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them: Is 0-5%, II: 5-15 mol. %, III: 15-30 mol. % and IV: 30-100 mol. % of DMF concentration.

In the first range a drastic decrease Of half-width in the relation to this value for pure water can be observed, From the change of this parameter it follows that DMF exerts a des­ tructive influence on hydrogen bonds forming water network.

The analysis of V„_„ wave number changes of the examined

lU cL X

band in relation to water-DMF mixture composition leads to difr- ferent conclusion. The decrease of this function in the dis­ cussed region hints at ordering influence of nonelectrolyte on water structure. Near the first inflexion point (4 mol. % of DMF> Cu and Bi null potential in water-DMF mixtures shows mi­ nimum [46].

The second region is characteristic of its drastic dec­ rease of half-width with the growth of nonelectrolyte concen­ tration, while wave number slightly decreases exhibiting mini­ mum at about 15 mol. % of MDF concentration.

Different conclusions follow from the analysis of both these parameters. On the grounds of half-width it can be stated that the breakiftg of water structure is gradually strengthened by the penetrating influence of DMF molecules or by water-dimethyl- formamide agregates formation.

On the other hand the interpretation of wave number changes allows to assume that a further slight stabilization of water­ like structure takes place.

According to K e s s l e r [32] who has investigated the discussed system by viscosimetric and dielectric methods the stabilization of water structure occurs in the solutions con­ taining less than 15 mol. % of DMF.

L a r i n o v [47] has observed density maximum in the solution of the above mentioned concentration.

N a m o t o and E n d o [48] have observed maximum of ultrasounds diffusion and minimum of adiabatic compressibility coefficient in such mixtures [491.

In the Ill-rd region there is a less drastic change of half- -width and wave number grows continuously with nonelectrolyte, concentration growth. In this region the breaking of "water- -like" structure probably takes place and what is suggested by

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spectroscopic works [50], the formation of DMF.ZHjO associates is probable.

S h a k h p a r o n o v assumes that DMF - water system has a clathrate type structure [5lJ in a small amide contents ran­ ge. In the mixture containing about 25 mol. % of DMF all free interstitial spaces of water are filled. According to the aut­ hor the structure of such a solution is more stable« which is substantiated, among others, by the minimum of isothermic com­ pressibility in the discussed mixture.

Basing on the results of dielectric research, K e s s l e r [52] came to the conclusion that that up to 30 mol. * DMF in the mixture with water causes stabilization of water structure.

Maximum of viscosity in water-dimethylformamide system oc­ curs at the mentioned above.concentration [47, 53, 54]. A dif­ ferent opinion on the effect of DMF on water structure was ex­ pressed by F r a t i e l l o [553. He has investigated the discussed system by magnetic nuclear resonance method. Accord­ ing to M m organic solvent disorders water structure. The mea­ surements of DMF with water mixing heat, vapour pressure and osmotic pressure of water-DMF mixtures [56, 57] carried out by G e 1 1 e r et al. point at the presence of DMF hydrates.

The authors express the opinion that the discussed hydrates have DMF.nHjO composition, where n * 2 i 4. The existance of DMF.2H2 0 hydrates is confirmed also by the results of crio-

scopic works carried out by B o u g a r d and J a d o t [58]. Above 30 mol. * in the discussed mixture the IV-th region beg­ ins In which a slight change of half-value width can be ob ­ served. It may substantiate the differences in the mixture pro­ perties caused by the concentration change of the components.

From the literature data if follows that,in the IV-th region 1. e. above 50 mol. * of DMF the formation of H20.2DMF [50, 59,

60] associates as the result of strong interactions among water and DMF molecules is possible.

On the other hand, in the region of considerable DMF con­ tents the ordering of molecules characteristic for pure DMFt occurs.

As the presented material indicates the opinions . on non­ electrolyte influence on water structure depend on the exper­ imental method used.

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Different kinds of parameters characterizing the influence of solute on Solvent structure (breaking» ordering of structure) obtained by spectroscopic method lead very often to incompatible conclusions.

It seems to us that the half-width is a good criterion def­ ining the structural changes taking place in the solution.

Our view is confirmed by spectroscopic investigations of temperature and electrolyte effect on water structure [1, 2).

The criterion of "half-width" seems possible to apply due to its agreement in many systems with thermodynamic character­ istics.

The thermodynamic investigations of the change of entropy according to the opinion of F r a n k , W e n [61] and M i s h ­ c h e n k o [62] serve as the best criterion of the effect of ions on the water structure.

r e f e r e n c e s

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termodynamiki i stroeniya vodnykh i nevodnykh rastvorov elektrolitov, Leningrad (1968).

Institute of Chemistry University of łódi

Stefania Taniewska-Oaiiiska, Ryszard Grochowski, Biwtłonlej Pałecz

SPEKTROSKOPOWE BADANIA WODNYCH ROZTWORÓW NIEELEKTROLITOW

W niniejszej pracy ustalono spektroskopowe zależności natężenia, szero­ kości połówkowej oraz częstości pasma kombinowanego (Vj ^ + V,,) wody w mie­ szaninach z rozpuszczalnikami organicznymi: glikolem etylenowym, gliceryną, acetonem, DHSO, dioksanem i DMF. Pomiary przeprowadzono w całym zakresie stężeń w temperaturze 25°C. Otrzymane wartości parametrów zanalizowano pod kątem wpływu nieelektrolitów na strukturę wody. Przyjęto szerokość połówkową jako kryterium porządkującego lub zakłócającego działanie substancji rozpu­ szczonej na wodę. Omawiane rozpuszczalniki organiczne wpływają destrukcyjnie na strukturę wody w całym zakresie składów. Aceton, dioksan, DMF wykazują silniejsze tendencje do niszczenia trójwymiarowej siatki wiązań wodorowych w wodzie niź glikol etylenowy, gliceryna, DMSO.

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