Thermodynamic study of CdCl 2 in 2-propanol (5 mass %) + water mixture using potentiometry

Similar documents
ALE 26. Equilibria for Cell Reactions. What happens to the cell potential as the reaction proceeds over time?

Physical Chemistry Laboratory I CHEM 445 Experiment 2 Partial Molar Volume (Revised, 01/13/03)

Solutions. Definitions pertaining to solutions

E o and the equilibrium constant, K

Study of Energy Eigenvalues of Three Dimensional. Quantum Wires with Variable Cross Section

Grade 3 Mathematics Course Syllabus Prince George s County Public Schools

[1 & α(t & T 1. ' ρ 1

Quantum Mechanics for Scientists and Engineers. David Miller

Unit -2 THEORY OF DILUTE SOLUTIONS

MATH Midterm Examination Victor Matveev October 26, 2016

2. Before we answer the question, here are four important terms relating to redox reactions and galvanic cells.

Electrochemistry Redox Half-Reactions

Every gas consists of a large number of small particles called molecules moving with very high velocities in all possible directions.

A New Method for Finding an Optimal Solution. of Fully Interval Integer Transportation Problems

CHAPTER 19 ELECTROCHEMISTRY

Multi-objective Programming Approach for. Fuzzy Linear Programming Problems

Chapter 3.1: Polynomial Functions

Author. Introduction. Author. o Asmir Tobudic. ISE 599 Computational Modeling of Expressive Performance

Study in Cylindrical Coordinates of the Heat Transfer Through a Tow Material-Thermal Impedance

Volume 8, ISSN (Online), Published at:

Axial Temperature Distribution in W-Tailored Optical Fibers

BIO752: Advanced Methods in Biostatistics, II TERM 2, 2010 T. A. Louis. BIO 752: MIDTERM EXAMINATION: ANSWERS 30 November 2010

5.80 Small-Molecule Spectroscopy and Dynamics

Markov processes and the Kolmogorov equations

, the random variable. and a sample size over the y-values 0:1:10.

Experimental and Theoretical Investigations of PAN Molecular Weight Increase in Precipitation Polymerization as a Function of H 2 O/DMSO Ratio

ENGI 4421 Central Limit Theorem Page Central Limit Theorem [Navidi, section 4.11; Devore sections ]

Sound Absorption Characteristics of Membrane- Based Sound Absorbers

A unified brittle fracture criterion for structures with sharp V-notches under mixed mode loading

D.S.G. POLLOCK: TOPICS IN TIME-SERIES ANALYSIS STATISTICAL FOURIER ANALYSIS

Electrostatics. . where,.(1.1) Maxwell Eqn. Total Charge. Two point charges r 12 distance apart in space

A Study on Estimation of Lifetime Distribution with Covariates Under Misspecification

K [f(t)] 2 [ (st) /2 K A GENERALIZED MEIJER TRANSFORMATION. Ku(z) ()x) t -)-I e. K(z) r( + ) () (t 2 I) -1/2 e -zt dt, G. L. N. RAO L.

are specified , are linearly independent Otherwise, they are linearly dependent, and one is expressed by a linear combination of the others

The Molecular Diffusion of Heat and Mass from Two Spheres

Difference of 2 kj per mole of propane! E = kj

Fourier Series & Fourier Transforms

Optical dispersion characterization of NiO thin films prepared by nebulized spray technique

The Excel FFT Function v1.1 P. T. Debevec February 12, The discrete Fourier transform may be used to identify periodic structures in time ht.

MATHEMATICS 9740/01 Paper 1 14 Sep hours

5.1 Two-Step Conditional Density Estimator

Rates and Mechanisms of Chemical Reactions

Review for cumulative test

Dynamic Response of Second Order Mechanical Systems with Viscous Dissipation forces

A Simplified Nonlinear Generalized Maxwell Model for Predicting the Time Dependent Behavior of Viscoelastic Materials

Journal of Hazardous Materials

ENGI 4421 Central Limit Theorem Page Central Limit Theorem [Navidi, section 4.11; Devore sections ]

Examination No. 3 - Tuesday, Nov. 15

Secondary aluminium-iron (III) chloride batteries with a low temperature molten salt electrolyte

Fourier Method for Solving Transportation. Problems with Mixed Constraints

Mean residual life of coherent systems consisting of multiple types of dependent components

The Acoustical Physics of a Standing Wave Tube

WEST VIRGINIA UNIVERSITY

Transference Numbers of Sodium Chloride in Formamide + Water Mixtures at K from Potential Difference Measurements #

General Chemistry 1 (CHEM1141) Shawnee State University Fall 2016

Ch. 1 Introduction to Estimation 1/15

A Hartree-Fock Calculation of the Water Molecule

Claude Elysée Lobry Université de Nice, Faculté des Sciences, parc Valrose, NICE, France.

Spontaneous and stimulated emission tuning characteristics. of a Josephson junction in a microcavity

Estimation of Thermodynamic Properties and Ionic Equilibria of Cobalt Chloride Solution at 298 K

Lecture 18. MSMPR Crystallization Model

DIFFERENT PHYSICAL PROPERTIES OF FEW AMINO ACIDS FOR FIVE DIFFERENT TEMPERATURES IN AQUEOUS SODIUM ACETATE SOLUTION

Cold mirror based on High-Low-High refractive index dielectric materials

cannot commute.) this idea, we can claim that the average value of the energy is the sum of such terms over all points in space:

L. A. P. T. Quick Look at Slow and Fast Light

THE MATRIX VERSION FOR THE MULTIVARIABLE HUMBERT POLYNOMIALS

On natural cubic splines, with an application to numerical integration formulae Schurer, F.

Chapter 5. Root Locus Techniques

Journal of Applied and Computational Mechanics, Vol. 3, No. 1, (2017), DOI: /jacm

Copyright 1978, by the author(s). All rights reserved.

Energy 43 (2012) 19e29. Contents lists available at SciVerse ScienceDirect. Energy. journal homepage:

Matching a Distribution by Matching Quantiles Estimation

ALL INDIA TEST SERIES

Anisotropic discs loaded by parabolically distributed pressure

Design and Implementation of Cosine Transforms Employing a CORDIC Processor

Chapter 8 Reduction and oxidation

Comparative analysis of bayesian control chart estimation and conventional multivariate control chart

Unifying the Derivations for. the Akaike and Corrected Akaike. Information Criteria. from Statistics & Probability Letters,

MODIFIED LEAKY DELAYED LMS ALGORITHM FOR IMPERFECT ESTIMATE SYSTEM DELAY

An Investigation of Stratified Jackknife Estimators Using Simulated Establishment Data Under an Unequal Probability Sample Design

Intermediate Division Solutions

Chemistry 20 Lesson 11 Electronegativity, Polarity and Shapes

Control Systems. Controllability and Observability (Chapter 6)

Department of Chemistry University of Texas at Austin

Partial Molar Volumes of Aluminium Chloride, Aluminium Sulphate and Aluminium Nitrate in Water-rich Binary Aqueous Mixtures of Tetrahydrofuran

COWLES FOUNDATION FOR RESEARCH IN ECONOMICS YALE UNIVERSITY

Optimum Sizing of a PV-Battery-Diesel Hybrid System for Remote Consumers

6.3 Testing Series With Positive Terms

Find this material useful? You can help our team to keep this site up and bring you even more content consider donating via the link on our site.

Find this material useful? You can help our team to keep this site up and bring you even more content consider donating via the link on our site.

October 25, 2018 BIM 105 Probability and Statistics for Biomedical Engineers 1

EXPERIMENT OF SIMPLE VIBRATION

Identical Particles. We would like to move from the quantum theory of hydrogen to that for the rest of the periodic table

AP Statistics Notes Unit Eight: Introduction to Inference

Review of Important Concepts

UC A-G Chemistry. Gorman Learning Center (052344) Basic Course Information

Pipe Networks - Hardy Cross Method Page 1. Pipe Networks

DESIGN, PRODUCTION, AND APPLICATION OF A STAND FOR TESTING FRICTION OF THE BEARINGS

Copyright Paul Tobin 63

A NEW METHOD OF THRUSTER CONTROL IN POSITIONING OF SHIPS BASED ON POWER CONTROL

Transcription:

Thermdyamic study f CdCl 2 i 2-prpal (5 mass %) + water mixture usig ptetimetry Reat Tmaš, Ađelka Vrdljak UDC: 544.632.4 Uiversity f Split, Faculty f Chemistry ad Techlgy, Teslia 10/V, HR-21000 Split, Cratia Summary The ptetial differece (pd) measuremets (E) are reprted fr galvaic cell withut liquid jucti: Cd(Hg) (l, satd.)cdcl 2 () i ZAgCl(s)Ag(s) at differet temperatures ad varius CdCl 2 mlalities () i aqueus mixture f 2-prpal (ctaiig 5 mass % 2-prpal), Z. Frm these values ad usig literature data fr staility cstats f the chlrcadmium cmplexes, the values f the stadard pd f the cell were taied at each temperature. These values served t calculate the stadard thermdyamic quatities fr the cell reacti, ad als mea mlal activity cefficiets f CdCl 2. The crrespdig thermdyamic results are discussed ad cmpared with literature data. Keywrds: thermdyamic prperties, cadmium chlride, 2-prpal + water mixed slvet, ptetimetry. Itrducti Ptetimetric methd usig a galvaic cell withut liquid jucti was fud t e a attractig experimetal techique fr studyig the thermdyamic prperties f electrlyte slutis i aqua-rgaic mixed slvets. This paper is a extesi f ur systematic ivestigati thermdyamic prperties f CdCl 2 i varius aqua-rgaic slvets usig ptetimetry. Specifically, i previus wrks y ur grup, the ahaviur f the CdCl 2 has ee studied i water mixtures with alchl c-slvet: ctaiig 10, 30, ad 50 mass % 2-prpal (Višić Mekjavić, 1993) r 2-methylprpa-2-l (tert. utal) (Tmaš et al., 2000), ad als with 5, 10, ad 15 mass % 2-utal (Tmaš et al., 2005). We have recetly pulished data the thermdyamic prperties f CdCl 2 i 2- methylprpa-2-l (5 mass %) + water mixture (Z) usig a flw ptetimetric methd (Tmaš et al., 2011). Namely, the ptetial differece (pd) measuremets have ee carried ut the fllwig galvaic cell: Cd(Hg) (l, satd.)cdcl 2 () i ZAgCl(s)Ag(s) (1) Crrespdig authr: rtmas@ktf-split.hr 41

i the temperature rage (293.15 K t 313.15 K) at 5 K itervals, fr differet CdCl 2 mlalities (). I this wrk, aalgus ivestigatis were perfrmed i 2-prpal + water mixture f the same ctet (ie., Z = 5 mass % 2-prpal), i rder t determie the thermdyamic quatities f the cell reacti, ad the stichimetric mea mlal activity cefficiets f CdCl 2. The results frm this study are cmpared with similar systems. Withi the ptetimetric data aalysis, the ccetratis f all iic species was calculated (Višić Mekjavić, 1989) usig data fr the thermdyamic staility cstats f chlrcadmium cmplexes i water medium, ad fr 10 mass % 2-prpal (Višić et al., 1993). Materials ad methds CdCl 2 H 2 O ad 2-prpal were p.a. purity (Merck). Befre use, 2-prpal ad water were distilled. Slvet mixture (Z) ad ccetrated electrlyte sluti i Z (stck sluti) were prepared y weight usig CdCl 2 H 2 O, water ad 2-prpal. The mlality ( max. ) f the stck sluti f CdCl 2 i Z was 0.0503 ml kg 1, with salt mass fracti, w = 0.01002. Desity f Z was measured usig scillatig U-tue desimeter (At Paar, mdel DMA 4500 M) with precisi f 1 10 5 g cm 3 (Bald et al., 2013). I rder t ctiuusly tai the pd (E i ) f the cell (1) at differet mlalities ( i ) f CdCl 2, we chage electrlyte ccetratis y addig a stck sluti i Z (mass, m i ) t a cell ctaiig a apprpriate mass f slvet mixture (m Z ). The mlality f CdCl 2 i the cell (1) after i th additi ( i ) is give y the expressi (Zhag et al., 1993): where M is the mlar mass f cadmium chlride. m w M i i / i m m 1 (2) w The preparati f electrdes, descripti f the cell, ad f the equipmet fr pd measuremets, ad the measurig prcedure itself were explaied earlier (Tmaš et al., 2011). Results ad discussi The ptetimetric results (E i ) fr the cell (1) i 5 mass % 2-prpal (Z) at the differet CdCl 2 mlalities ( i ) ad at all peratig temperatures (T) are cmpiled i Tale 1. Z i 42

Tale 1. Experimetal data fr cadmium chlride i Z at differet temperatures 10 3 / ml kg 1 E / V 10 3 / ml kg 1 E / V T = 293.15 K T = 298.15 K 4.123 0.77699 4.224 0.77757 7.686 0.75940 7.800 0.76027 10.732 0.75037 10.720 0.75144 13.358 0.74445 13.390 0.74539 15.672 0.74023 15.724 0.74126 17.720 0.73704 17.784 0.73804 19.525 0.73450 19.610 0.73570 21.150 0.73250 21.151 0.73368 22.528 0.73082 22.641 0.73206 23.862 0.72940 23.894 0.73066 25.098 0.72823 25.122 0.72948 26.129 0.72721 26.232 0.72841 27.160 0.72631 27.177 0.72751 28.030 0.72552 28.117 0.72669 28.920 0.72490 28.998 0.72594 T = 303.15 K T = 308.15 K 4.161 0.78030 4.193 0.78143 7.699 0.76154 7.730 0.76344 10.755 0.75667 10.732 0.75417 13.382 0.74650 13.399 0.74810 15.684 0.74244 15.664 0.74382 17.730 0.73930 17.674 0.74057 19.530 0.73671 19.545 0.73803 21.107 0.73480 21.170 0.73597 22.559 0.73305 22.633 0.73428 23.878 0.73173 23.943 0.73288 25.049 0.73053 25.146 0.73169 26.175 0.72941 26.245 0.73066 27.194 0.72851 27.241 0.72977 28.100 0.72771 28.162 0.72896 28.953 0.72691 29.010 0.72822 43

Tale 1. (Ctiued) 10 3 / ml kg 1 E / V T = 313.15 K 4.151 0.77440 7.682 0.76502 10.710 0.75575 13.346 0.74958 15.626 0.74545 17.667 0.74226 19.477 0.73965 21.106 0.73758 22.565 0.73593 23.866 0.73453 25.066 0.73328 26.179 0.73218 27.183 0.73127 28.108 0.73042 28.971 0.72964 The values f E frm Tale 1 were used t calculate the stadard mlal pd ( E ) fr the cell reacti: Cd(s) + 2 AgCl(s) 2 Ag(s) + Cd 2+ (Z) + 2Cl (Z) (3) accrdig t the relati, RT 2 2 3RT 1/2 1/2 E E l( (Cd )/ )( (Cl )/ ) l(10) A ( I/ ) /(1 a0b ( I/ ) ) 2F F 3RT 3RT l1 M Z Σx(X) E l(10) C I / (4) 2F 2F This relati was taied usig a cmiati f the Nerst equati ad the Deye- Hückel equati fr the mea activity cefficiet. Here I detes iic stregth, ad = 1 ml kg 1. The fllwig data are eeded t slve Eq. (4): 44

a) a value fr the i-size parameter (a 0 ); a 0 = 0.45 m (Višić et al., 1993), ) the mlar mass ad mass fracti f water ad f 2-prpal; these data are used t determie the mea mlar mass (M) f ivestigated mixed slvet Z, c) Deye-Hückel cstats (A, B ); these cstats were calculated usig literature data fr the relative permittivity, r (Åkerlöf, 1932) ad the desity, d (frm the preset study) f the slvet Z: the prperties ( r, d) at differet temperatures are give i Tale 2. d) the equilirium mlalities f all iic species, give y the term x (X), as well as the cell pd (E) fr each cadmium chlride mlality. Determiati f the E ca e perfrmed either y extraplati f E' frm Eq. (4) t zer iic stregth r y the least-squares methd. T calculate (Cd 2+ ), (Cl ), ad (f the remaiig iic species) fr each mlality f CdCl 2, it is ecessary t csider the cmplexati reacti i ivestigated mixed slvet Z (Višić Mekjavić, 1989): Cd 2+ + Cl (2 ) CdCl ( = 1, 2 i 3) (5) Iasmuch as the iterative prcedure has ee descried i detail i ur previus papers (Tmaš et al., 2004 ad 2011), ly a shrt ulie will e prvided here. Namely, fr a give cadmium chlride mlality, the stichimetric iic stregth f the sluti is first calculated as I = 3 d, ad the ccetrati staility cstats, K, fr the cmplex frmig reactis (5) are estimated at this iic stregth usig ext relati: lk 2 1/2 1/2 Δz Ac ( I/ c ) /(1 Bca0 ( I/ c ) ) lk (l10)δ CI/ c (6) These staility cstats are the served t calculate the ccetrati f each iic species. Iitial ccetratis thus taied are used t calculate the ew iic stregth ad staility cstat values. The treatmet is repeated util a satisfactry cstacy f K values is taied. I Eq. (6) C is a empirical cstat, c = 1 ml dm 3, ad 2 Δz = (2 ) 2 4, where z is the charge f each iic species. The parameters C ad (thermdyamic staility cstat) were determied experimetally fr water medium, ad fr 10 mass % 2-prpal (Višić et al., 1993). Fr the preset study, C ad K, are iterplated frm literature data; values at differet temperatures fr mixed slvet Z are reprted i Tale 2. K 45

The taied equlirium ccetratis f all iic species were the expressed as mlalities, ad usig Eq. (4) the stadard mlal pd, E, ad its stadard deviati were determied usig the least-squares methd. These values are listed i Tale 3. Regressi aalysis shwed that depedece f E T ca e adequately fitted y the secd-rder plymial. E ( T) ct 2 a T (7) Tale 2. Parameters f Eq. (6) i Z at differet temperatures T / K 293.15 298.15 303.15 308.15 313.15 K 1 121 123 128 132 136 K 2 517 575 610 644 678 409 448 448 507 537 K 3 ΔC 1 0.192 0.191 0.189 0.187 0.185 ΔC 2 0.375 0.380 0.379 0.379 0.379 ΔC 3 0.477 0.475 0.467 0.459 0.452 r 76.74 74.96 73.21 71.50 69.78 d / g cm 3 0.98962 0.98840 0.98692 0.98522 0.98330 Tale 3. Stadard ptetial differece ( E ) f cell (1) i Z at differet temperatures T / K E ± (E ) / V 293.15 0.56840 ± 0.00009 298.15 0.56579 ± 0.00008 303.15 0.56405 ± 0.00016 308.15 0.56149 ± 0.00012 313.15 0.55893 ± 0.00008 The plymial cefficiets a, ad c, taied y fittig Eq. (7) t the experimetal results are preseted i Tale 4, tgether with their stadard deviatis. Tale 4. Adjustale cefficiets a, ad c f Eq. (7) i system CdCl 2 Z a / V 0.5157 ± 0.282 10 4 / V K 1 7.824 ± 4.32 10 6 c / V K 2 2.057 ± 1.75 46

Frm the first derivate f Eq. (7), accrdig t relati r S = d E /dt = z F ( + 2 ct), (z = 2) (8) the stadard etrpy ( r S ) f the cell reacti (3) i Z is taied. The stadard Gis eergy ( r G ) is calculated accrdig t the expressi, Δ rg zfe (9) while the stadard ethalpy ( r H ) ca e calculated frm the relatiship, r H = r G + T r S (10) The stadard thermdyamic quatities fr the cell reacti (3) i Z at 298.15 K are give i Tale 5. The data fr water medium are, fr cmparisi, listed i the same tale. The deviatis were calculated frm the stadard deviati fr E. Tale 5. Stadard thermdyamic quatities fr the cell reacti (3) i water medium ad slvet Z at 298.15 K mass % r G / kj ml 1 r H / kj ml 1 r S / J K 1 ml 1 0 (Višić Mekjavić, 1993) 110.66 ± 0.02 134 ± 5 78 ± 10 5 (preset study, Z) 109.18 ± 0.01 129 ± 13 65 ± 25 As see frm Tale 5 the stadard Gis eergy fr th slvets has the egative sig, which prves that the cell reacti (3) is sptaeus. The values fr the stadard ethalpy ad etrpy chage are als egative. It ca e see that the cell reacti (3) is exthermic ad lead t decrease i etrpy. It ca als e see that the sptaeity ( r G ) f reacti (3) decreaces with addig 2-prpal i water. The same was reprted fr the aqueus mixtures with 5 mass % 2-uta, 2-utal, r t-utal (Tmaš et al., 2004, 2005, ad 2011). I this wrk, the stichimetric mea mlal activity cefficiet ( ) f cadmium chlride i Z was calculated usig the data fr E ad E f the cell (see Tales 1 ad 3), accrdig t the Nerst equati fr the cell reacti (3): RT/2F) l 4( / ) E E ( γ (11) 3 47

prvided that chlrcadmium cmplexes were t frmed i the sluti. Tale 6 shws the taied values f CdCl 2 i 5 mass % 2-prpal (Z) at each mlality ad at differet temperatures. Values f fr cadmium chlride i 5 mass% 2-prpal (Z) were t fud i literature. Tale 6. Stichimetric mea mlal activity cefficiets ( ± ) f CdCl 2 i Z at differet temperatures (CdCl2) / ml kg 1 T / K 0.003 0.005 0.007 0.009 0.010 0.015 0.020 293.15 0.697 0.599 0.542 0.503 0.487 0.432 0.397 298.15 0.691 0.594 0.535 0.495 0.479 0.423 0.387 303.15 0.678 0.583 0.527 0.489 0.474 0.419 0.381 308.15 0.672 0.577 0.525 0.485 0.469 0.413 0.377 313.15 0.665 0.570 0.520 0.479 0.462 0.410 0.368 Accrdig t the values give i Tale 6, activity cefficiets decrease with icreasig CdCl 2 mlality, as well as decrease with icreasig tempertaure. This result is expected frm Deye-Hückel thery. A crrespdig ehaviur has ee fud i ur earlier studies f the same electrlyte i aqueus kete (Tmaš et al., 2004) ad aqueus alchls (Tmaš et al., 2005 ad 2011) at the same mass fractis. Whe cmparig the values frm preset study with thse fr water medium (Višić Mekjavić, 1993), it ca e see that these values are higher i water. Oviusly, this is related t the degree f cmplexati. Aalgy was estalished with aqueus mixtures with 5 mass % 2-utae, 2-utal, ad t-utal (Tmaš et al., 2004, 2005, ad 2011). Furthermre, values f fr cadmium chlride at the same mass fracti (Z = 5 mass %) are similar; certai differeces are due t ifluece f relative permittivity ad ature f rgaic cmpet i the mixed slvet. Cclusis The preset ivestigati f thermdyamic prperties f cadmium chlride i aqueus mixture with 5 mass % 2-prpal (Z) ca e summarised as fllwig: Fr the preset system CdCl 2 i Z, was determied stadard mlal ptetial differece fr the cell reacti at differet temperatures: this value decreases with a icrease i the temperature. At cstat temperature, the mea mlal activity cefficiet f cadmium chlride decreases with a icrease i the mlality f sluti. At fixed mlality, the mea mlal activity cefficiet f cadmium chlride decreases with a icrease the temperature. The cell reacti is sptaeus, exthermic ad leads t reduced i etrpy. 48

Refereces Åkerlöf, G. (1932): Dielectric cstats f sme rgaic slvet water mixtures at varius temperatures, J. Am. Chem. Sc. 54 (11), 4125-4139. Bald, A., Kiart, Z., Tmaš, R. (2013): Vlumetric studies f aqueus slutis f msdium salts f sme aliphatic dicarxylic acids at 298.15 K. A ew methd f data aalysis, J. Ml. Liq. 178, 94-98. Tmaš, R., Višić. M., Mekjavić, I. (2000): Thermdyamics f cadmium chlride i t-utal water mixtures (w t-buoh = 10%, 30%, ad 50 %) frm electrmtive frce measuremets, Crat. Chem. Acta 73 (2), 423-433. Tmaš, R., Tmiić, I., Višić, M., Skl, V. (2004): Thermdyamics f Cadmium Chlride i 2- Butae + Water mixtures (5, 10, ad 15 Mass%) frm Electrmtive Frce Measuremets, J. Sluti Chem. 33 (11), 1397-1410. Tmaš, R., Tmiić, I., Višić, M., Skl, V. (2005): Thermdyamic study f cadmium chlride i aqueus mixtures f 2-utal frm ptetial differece measuremets, J. Sluti Chem. 34 (8), 981-992. Tmaš, R., Skl, V., Bškvić, P. (2011): Thermdyamic prperties f CdCl 2 i tert. utal (5 mass %) + water mixture. I Prceedigs: Iteratial Scietific ad Prfessial Cferece 13 th Ružička Days, Vukvar, Septemer 2010, Šuarić, D. (Ed.), Osijek, pp. 95-106. Višić, M., Mekjavić, I. (1989): Thermdyamics f the cell: Cd(s)+Hg CdCl 2 (aq, m)agclag, J. Chem. Thermdyamics 21 (2), 139-145. Višić, M., Jadrić, A., Mekjavić, I. (1993): The staility cstats f cadmium chlride cmplexes i 2-prpal water mixtures (0, 10, 30 ad 50 mass per cet) frm electrmtive frce measuremets, Crat. Chem. Acta 66 (3-4), 489-498. Višić, M., Mekjavić, I. (1993): Thermdyamics f the cell: Cd(Hg) satd. CdCl 2 (m)agclag i (10, 30 ad 50 Mass per Cet) 2-Prpal Water Mixtures, Crat. Chem. Acta 66 (3-4), 479-488. Zhag, L., Lu, X., Wag, Y., Shi, J. (1993): Determiati f activity cefficiets usig a flw emf methd. 1. HCl i methal water mixtures at 25, 35 ad 45C, J. Sluti Chem. 22 (2), 137-150. 49