CONDUCTOMETRIC INVESTIGATIONS ON OXALIC ACID IN 2-PROPANOL + WATER MIXTURES AT , , AND K

Similar documents
EFFECT OF DIELECTRIC CONSTANT ON THE SOLVATION OF SODIUM CITRATE

What is electrochemistry?

Chapter 7 Electrochemistry 7.2 Conductivity and its application

JCHPS Special Issue 1: January Page 47

Ultrasonic study of molecular interaction in binary liquid mixtures of n-hexane with alcohols

Journal of Chemical and Pharmaceutical Research

GAUTENG DEPARTMENT OF EDUCATION SENIOR SECONDARY INTERVENTION PROGRAMME. PHYSICAL SCIENCE Grade 11 SESSION 11 (LEARNER NOTES)

ELEC NCERT. 1. Which cell will measure standard electrode potential of copper electrode? (g,0.1 bar) H + (aq.,1 M) Cu 2+ (aq.

Conductometric Study of Sodium Chloride in Aqueous 2- methylpropan-2-ol of Mass Fraction 0.10, 0.30, 0.50, 0.70, 0.80 and 0.90

McMillan Mayer theory for solvent effects in inhomogeneous systems: Calculation of interaction pressure in aqueous electrical double layers

Electrical Conductivity of Sodium Chloride and Potassium Chloride in Water Soluble Polymers at Different Temperatures

ln P 1 saturation = T ln P 2 saturation = T

Apparent molal volumes of alcohols in aqueous solutions at different temperatures

I affirm that I have never given nor received aid on this examination. I understand that cheating in the exam will result in a grade F for the class.

Electrical conductivity of s-acetylthiocholine halides and perchlorate in 2-propanol at 25 C

Characteristics of Low-Temperature Plasmas Under Nonthermal Conditions A Short Summary

The Thermal Dependence and Urea Concentration Dependence of Rnase A Denaturant Transition

Measuring Temperature with a Silicon Diode

5.60 Thermodynamics & Kinetics Spring 2008

Supporting Online Material

Developed Correlations for Prediction of The Enthalpies of Saturated Vapor Liquid Coexisting Phases

Molar mass, M, of the empirical formula C 4 H 9 : M 4M 9M g/mol g/mol g/mol

PHY 171. Lecture 14. (February 16, 2012)

CHARACTERIZING THE KINETICS OF HETEROGENEOUS EXO- THERMIC REACTIONS

Chapter 4: Hypothesis of Diffusion-Limited Growth

Transport Properties for Aqueous Sodium Sulfonate Surfactants

International Journal of Pharma and Bio Sciences

SF Chemical Kinetics.

CHEM 481 Assignment 3 Answers

Phys463.nb. Many electrons in 1D at T = 0. For a large system (L ), ΕF =? (6.7) The solutions of this equation are plane waves (6.

(From the Gates Chemical Laboratory, California Institute of Technology, Pasadena.)

International Journal of Pharma and Bio Sciences

Example A1: Preparation of a Calibration Standard

V.N. Shilov a, *, A.V. Delgado b, F. Gonzalez-Caballero b, C. Grosse c

ENTHALPIES OF COMBUSTION AND FORMATION OF ISOMERS OF THE AMINO-BENZOIC ACID

Chapter 2 General Properties of Radiation Detectors

Solidification of Porous Material under Natural Convection by Three Phases Modeling

Electrical conductivity enhanced dielectric and piezoelectric properties of ferroelectric 0-3 composites

1 The properties of gases The perfect gas

EFFECT OF SOLVENT ON THE CONDUCTANCE OF TETRAMETHYL AMMONIUMM BROMIDE IN AQUEOUS N, N- DIMETHYL FORMAMIDE

Study of Excess Properties of Binary and Ternary Mixtures of Trichloroethene, Ethanoic Acid, and N,N-Dimethylformamide at Different Temperatures

Chemistry Department Al-kharj, October Prince Sattam Bin Abdulaziz University First semester (1437/1438)

Journal of Chemical and Pharmaceutical Research, 2012, 4(3): Research Article

Modelling of the Through-air Bonding Process

CHAPTER 16 KINETICS: RATES AND MECHANISMS OF CHEMICAL REACTIONS

U ms = U mf (gD c ) 0.5

Electrochemical Characterisation of the Ce(IV) limiting carbonate complex

Evaluation of apparent and partial molar volume of potassium ferro- and ferricyanides in aqueous alcohol solutions at different temperatures

Miscibility of Poly(vinylidene fluoride) and Cellulose Acetate Blends in Dimethyl Formamide

Model Fitting. CURM Background Material, Fall 2014 Dr. Doreen De Leon

Apparent molar volume of sodium chloride in mixed solvent at different temperatures

THERMAL ENDURANCE OF UNREINFORCED UNSATURATED POLYESTERS AND VINYL ESTER RESINS = (1) ln = COMPOSITES & POLYCON 2009

Quantifying the Blue Shift in the Light Absorption of Small Gold Nanoparticles

Colligative Properties of Helical Polyelectrolytes

Einstein Classes, Unit No. 102, 103, Vardhman Ring Road Plaza, Vikas Puri Extn., Outer Ring Road New Delhi , Ph. : ,

Conductometric Study of Complex Formation Between Cu (II) Ion and 2-hydroxyimino-3-(2'-hydazonopyridyl)-butane (HL)

Density and structure of undercooled liquid titanium

School of Chemistry, University of Nottingham, University Park, Nottingham, NG7 2RD, United Kingdom

Thermodynamics of Dissociation and Micellization of Carboxylates of Dysprosium in Organic Solvent

P (t) = P (t = 0) + F t Conclusion: If we wait long enough, the velocity of an electron will diverge, which is obviously impossible and wrong.

21. Practice Problem (page 556) What is the volume of 5.65 mol of helium gas at a pressure of 98 kpa and a temperature of 18.0 C?

Uniaxial compressive stress strain model for clay brick masonry

Genetic Algorithm Search for Stent Design Improvements

Virtual physics laboratory for distance learning developed in the frame of the VccSSe European project

SITARAM K. CHAVAN * and MADHURI N. HEMADE ABSTRACT INTRODUCTION

Geometric part of uncertainties in the calculation constant of the primary four electrode conductivity cell

1. Which two values of temperature are equivalent to the nearest degree when measured on the Kelvin and on the

Fluorescence studies of the excited-state proton transfer in substituted 3-hydroxychromones in supersonic jet

Effect of Polymer Solutions on Efflux Time for Two Exit Pipe System

COMPLEXES OF Ti(IV) AND Zr(IV) WITH SOME BIDENTATE SCHIFF BASES DERIVED FROM ISATIN

1.1 Heat and Mass transfer in daily life and process/mechanical engineering Heat transfer in daily life: Heating Cooling Cooking

Electronic Supplementary Information Proton Conductivity in Mixed-Conducting BSFZ Perovskite from Thermogravimetric Relaxation

CFD SIMULATION OF A MEMBRANE DISTILLATION MODULE CHANNEL

Recommended Reading. Entropy/Second law Thermodynamics

SHORT COMMUNICATION. Ultrasonic Studies of Amino Acids in Aqueous Sucrose Solution at Different Temperatures

ME 300 Thermodynamics II Exam 2 November 13, :00 p.m. 9:00 p.m.

CHAPTER 2 THERMODYNAMICS

IC1001 Kick-Off Meeting - 1

ESTIMATION OF UHMWPE CRYSTALLINITY DEGREE VARIATION. 1. Differential Scanning Calorimetry (DSC) in tests on polymers

T Madhu Mohan*, S Sreehari Sastry* & V R K Murthy**

Daniel López Gaxiola 1 Student View Jason M. Keith

Experimental studies on equivalent thermal properties of particle-reinforced flexible mould materials

ESTIMATING AND FORMING CONFIDENCE INTERVALS FOR EXTREMA OF RANDOM POLYNOMIALS. A Thesis. Presented to. The Faculty of the Department of Mathematics

Solvent Extraction Research and Development, Japan, Vol. 22, No 1, (2015)

AP Physics Thermodynamics Wrap-up

Physical Chemistry I for Biochemists Chem340. Lecture 32 (4/4/11)

Effective zero-thickness model for a conductive membrane driven by an electric field

Tables of data and equations are on the last pages of the exam.

Dielectric Relaxation Studies of Binary Mixtures of Ethanol and Chlorobenzene in Benzene Solution from Microwave Absorption Data

Molecular Speeds. Real Gasses. Ideal Gas Law. Reasonable. Why the breakdown? P-V Diagram. Using moles. Using molecules

DETERMINATION OF ADSORTION LAYERS ON SILICON SORPTION ARTIFACTS USING MASS COMPARISON

General Physical Chemistry I

Possible experimentally observable effects of vertex corrections in superconductors

Thermally Activated Asymmetric Structural Recovery in a Soft Glassy Nano-Clay Suspension

Feature Extraction Techniques

Kinetic Molecular Theory of. IGL is a purely empirical law - solely the

Catalytic and Viscometric Behavior of HClO 4 -H 2 O System

Classical systems in equilibrium

Indra Bahadur and Nirmala Deenadayalu*

The Solar Radio Microwave Flux Leif Svalgaard, May 2009

Transcription:

CONDUCTOMETRIC INVESTIGATIONS ON OXALIC ACID IN -PROPANOL + WATER MIXTURES AT 98.5, 0.5, 08.5 AND.5 K Shivakuar H R, Siju N Antony, Surekha M Prof & Head, Associate Professor, Departent of Cheistry KVG College of Engineering ( Affiliated to Visvesvaraya Technological University, Belgau, Sullia, D.K, Karnataka State, ( India Associate Professor, Departent of Cheistry, MVJ College of Engineering ( Affiliated to Visvesvaraya Technological University, Belgau, Bangalore, Karnataka State, ( India ABSTRACT Electrical conductivity of oxalic acid has been easured in -propanol + water ixtures covering the approxiate range of dielectric constant 7.0 ε 49.6 at 98.5, 0.5, 08.5 and.5 K. The conductance data have been analysed by using Shedlovsky equation to obtain liiting olar conductance, association constant and Walden product. The liiting olar conductance and Walden product values were found to decrease with increase in x pr (ole fraction of -propanol. Oxalic acid is found to be a structure breaker in the solvent edia explored. The results obtained fro the study were used to elicit the nature of ionion and ion-solvent interactions. Keywords: Liiting Molar Conductance, Walden Product, -Propanol, Oxalic Acid I. INTRODUCTION Investigations on transport property of an electrolyte and the effect of ion solvation on it in various aqueous and partial aqueous edia have received uch attention in recent years, since it gives valuable inforation regarding ion-ion and ion-solvent interactions [-5]. In continuation of our works on electrolytes in -propanol + water ixtures, we have chosen oxalic acid as the electrolyte due to its ability to for stable coplexes with various etal ions, and its substantial iportance in any industrial, geological, and biological systes [6]. Moreover, it is a weak electrolyte and is expected to for hydrogen bonds with both water as well as - propanol. Oxalic acid on dissociation gives oxalate ion and hydrogen ion. The forer is a structure breaker [7] and the latter is a kosotrope capable of breaking hydrogen bonds. However, oxalic acid is reported to show structure breaking properties in soe water + organic solvent ixtures [8]. In contrast to other dicarboxylic acids, conductance of oxalic acid in aqueous ediu at 98.5 K was repeatedly easured by Ostwald [9], Collie [0], and the ost extensive easureents by Darken []. Darken incorporated a sall correction in the deterined conductances considering the second dissociation of the acid. Using Quint-Viallard conductivity equation Lee and Wheaton further analysed Darken s conductance data. With an exception of Darken s work, other reports were of liited value and hence Barthel et al [6] ade systeatic and precise easureents of electrical conductivities of dilute aqueous oxalic acid solutions in the teperature range 98.5-08.5 K. 76 P a g e

However, conductoetric investigations on oxalic acid in -propanol + water ixtures are not reported in the literature. -Propanol + water ixtures are of special interest due to the clathrate-like structures present in the []. II. METHODOLOGY Oxalic acid (Merck, AR Grade, triply distilled water (specific conductance 0-6 ho c - and -propanol purified by using standard procedure [8] were used for preparing M oxalic acid stock solutions in different - propanol + water ixtures. These solutions were further diluted to obtain solutions of desired concentrations. Conductance easureents were ade using a digital icroprocessor based conductivity eter Systronics India Liited. All the easureents were ade in a therostat aintained at the desired teperature with an accuracy of ±0. C III. RESULTS AND DISCUSSION. Liiting Molar Conductance ( (Model-08, Molar conductance of oxalic acid in -propanol + water ixtures were calculated using the specific conductance obtained fro a direct reading digital conductivity eter at (98, 0, 08 and K. The resulted olar conductance values were analysed by Shedlovsky odel [], a variant of Fuoss-Kraus odel, which includes corrections for inter ionic effects on ionic obilities and for ionic activity coefficients. Shedlovsky equation used for deterining liiting olar conductance and association constant K a is given below: S C Sf K a ( where C 4 C S ; 5 8.040 ( T 8.5 ( T ; where log f 6.840 ( C /( T 8 50.40 R( C /( T S and e R q kt ; f is the ean activity coefficient, estiated fro the extended Debye-Huckel equation; R is ion size paraeter which is equal to the Bjerru s critical distance q; k is Boltzann s constant and T is the teperature in Kelvin. The Shedlovsky plots are presented in Fig. and values obtained are given in TABLE. 77 P a g e

Fig. : Plot of /SΛ (oh c - ol Vs CΛ Sƒ ± for oxalic acid in -propanol + water ixtures at Different Teperatures As expected the liiting olar conductance values are quite large ainly due to the presence of highly conducting hydrogen ions. The anoalously large obility of proton in aqueous ediu is often explained in ters of Grotthus echanis and quantu echanical tunneling [4]. The increase in dissociation and ionic obility caused the liiting olar conductance to show sharp increase with increase in teperature. A sharp decline in liiting conductance is noticed with increasing x pr. Various factors such as decrease in dielectric constant, increased viscosity of solvent ixture [], increased basicity, destruction of tetrahedral-like structure of water and increased solvated ion size ust have played a critical role in reducing the conductance. It is also known that the anoalous conductivity of proton declines with increasing alcohol content [5]. Liiting conductance is not reported beyond 0.67 ole fraction of -propanol due to poor linearity of the Shedlovsky plot. 78 P a g e

Table : Experiental olar conductance at infinite dilution ( : ho c ol - for oxalic acid in -propanol + water ixtures at different teperatures obtained fro Shedlovsky odel T (K x pr 0.0000 0.057 0.056 0.67 98.5 65 40 08 66 0.5 68 446 9 06 08.5 7 475 67.5 797 5 404 58. Association Constant (K a Association constants calculated fro the Shedlovsky odel is given in TABLE. Association is expected to predoinate over dissociation since the electrolyte under consideration is weak. Except for x pr = 0.057, association constant is found to increase with increase in teperature suggesting the endotheric nature of the syste. Siilar behavior is reported for tartaric acid in water + ethanol/ethanol systes [6]. The trends in the variation of K a with respect to ole fraction of -propanol is rather ausing. The initial addition of -propanol to water is found to reduce the association constant as against the usual increasing trend with declining dielectric constant. Thus the coputed K a values at x pr = 0.057 and x pr = 0.056 are lower than expected. The iniu K a values noticed at x pr = 0.057 can be explained on the basis of changes in water structure induced by the sall quantities of -propanol added. Water is a highly associated solvent due to the presence of hydrogen bonds that helps in the foration of polyeric aggregates of water. Hence pure water can stabilize the ion-pairs by foring chain structure around it [7]. On adding sall aounts of -propanol, depolyerisation of water chain occurs and hence ion-pairs are less stabilized. Larger K a values found at at x pr = 0.67 is due to the predoinating influence of decrease in dielectric constant favouring association. Table : Experiental values of K a for oxalic acid in -propanol + water ixtures at different teperatures T (K x pr 0.0000 0.057 0.056 0.67 98.5 74.99 64. 74.9 9.4 0.5 8.5 60.0 77.9 68.9 08.5 87.6 59.4 77.97 57.59.5 95.59 6.8 8.65 77.98. Walden Product Walden product was calculated for oxalic acid in different copositions of -propanol + water ixtures at four different teperatures using the forula: 79 P a g e

Walden product = ( where ɳ is the viscosity coefficient of solvent ixture. The linear plot of Walden product versus teperature provided in Fig. is having negative slope indicating structure breaking behavior of oxalic acid in aqueous as well as in -propanol + water ixtures. The Walden product is found to decrease with increasing x pr and consequently solvation is strengthened in that direction. The oentous deviation fro Walden rule with increasing ole fraction of -propanol ay be a consequence of change of ion solvation and of the solvent structure [8]. Fig. : Plot of walden product (S c ol - poise vs teperature (K for oxalic acid in - IV. CONCLUSIONS propanol + water ixtures The sharp decline in conductance with respect to increase in -propanol content in the solvent ixture is explained on the basis of different factors influencing ionic conductance. The endotheric nature of the syste is evident fro the K a values for different systes at different teperatures. The structure breaking character is established fro the variation of Walden product with teperature. V. ACKNOWLEDGEMENTS The financial support for this investigation given by Visvesvaraya Technological University, Belgau, India under the grant Ref. No. VTU/Aca/00-/A-9/9 dated 7 th Deceber 00 is gratefully acknowledged. REFERENCES []. H. R. Shivakuar and Siju N. Antony, Conductoetric studies of potassiu thiocyanate in -propanol + water ixtures, Asian Journal of Cheistry,, 00, 549-5498. []. J. Gregorowicz, A. Bald, A. Szejgis and A. Chielewska, Gibbs energy of transfer and conductivity properties of NaI solutions in ixtures of water with butan--ol at 98.5 K, and soe physicocheical properties of ixed solvent, Journal of Molecular Liquids, 84, 000, 49-60. 80 P a g e

[]. L. P. Safonova and A. M. Kolker, Conductoetry of electrolyte solutions, Russian Cheical Review, 6, 99, 959-97. [4]. H. R. Shivakuar, Siju N. Antony and M. Surekha, Acoustic investigations on benzoic acid in water + ethanol ixtures in the teperature range 9.5 to.5 K, International Journal of Science Technology and Manageent, 4, 05, 856-870. [5]. J. I. Bhat and T. N. Sreelatha, Study of transport behaviour of Bi(NO in water + DMF/DMSO, Indian Journal of Cheistry, 4A, 00, 46-467. [6]. M. Bester-Rogac, M. Tosic, J. Barthel, R. Neueder and A. Apelblat, Conductivity studies of dilute aqueous solutions of oxalic acid and neutral oxalates of sodiu, potassiu, cesiu, and aoniu fro 5 to 5 C, Journal of Solution Cheistry,, 00, -8. [7]. Y. Marcus, Ions in water and biophysical iplications: Fro chaos to cosos (Springer 0. [8]. H. R. Shivakuar, Siju N. Antony and M. Surekha, Thero-acoustical behaviour of oxalic acid in - propanol + water ixtures, International Journal of Cheistry, 6, 05, 754-764. [9]. W. Ostwald and W. Nernst, About free ions in oxalic acid solutions by conductivity study, Zeitschrift für Physikalische Cheie, 8, 889, 9-94. [0]. J. N. Collie and T. Tickle, LXVI The salts of diethylpyrone, and the quadrivalence of oxygen, Journal of Cheical Society Transactions, 75, 899, 70-77. []. L. S. Darken, The ionization constants of oxalic acid at 5 C fro conductance easureents, Journal of Aerican Cheical Society, 6, 94, 007-0. []. H. R. Shivakuar and Siju N. Antony, Thero-acoustical investigations on potassiu thiocyanate in - propanol + water ixtures, International Journal of Pure and Applied Cheistry, 6, 0, 65-7. []. T. Shedlovsky, The coputation of ionization constants and liiting conductance values fro conductivity easureents, Journal of the Franklin Institute, 5, 98, 79-74. [4]. J. O. M. Bockris and A. K. N. Reddy, Modern electrocheistry (Vol., New York, 970. [5]. B. E. Conway, J. O. M. Bockris and H. Linton, Proton conductance and existence of the H O + ion, Journal of Cheical Physics, 4, 956, 84-850. [6]. J. I. Bhat and H. R. Shivakuar, Conductoetric studies on solvation behaviour of tartaric acid in various solvent ixtures, Journal of Molecular Liquids,, 004, 0-08. [7]. N. H. El-Haay, A. I. Kawana, M. F. Aira and El-Sisy, Electrical conductivity and ion-pair foration of s-acetylthiocholine halides and perchlorate in ethanol-water at 5 C, International Journal of Phara and Biosciences, 6, 00, -. [8]. J. Doench and J. Miro, Electrical conductance of sodiu broide in foraide-water ixtures, Monatshefte für Cheie, 9, 988, 77-90. 8 P a g e