Ultrasonic Investigation of Molecular Interaction in Binary Liquid Mixture of Polyethylene Glycol with Ethanol
Commenced in January 2007
Frequency: Monthly
Edition: International
Paper Count: 32797
Ultrasonic Investigation of Molecular Interaction in Binary Liquid Mixture of Polyethylene Glycol with Ethanol

Authors: S. Grace Sahaya Sheba, R. Omegala Priakumari

Abstract:

Polyethylene glycol (PEG) is a condensation polymer of ethylene oxide and water. It is soluble in water and in many organic solvents. PEG is used to make emulsifying agents, detergents, soaps, plasticizers, ointments etc. Ethanol (C2H5OH) also known as ethyl alcohol is a well-known organic compound and has wide applications in chemical industry as it is used as a solvent for paint, varnish, in preserving biological specimens, used as a fuel mixed with petrol etc. Though their chemical and physical properties are already studied, still because of their uses in day to day life the authors thought it is better to study some more of their physical properties like ultrasonic velocity and hence adiabatic compressibility, free length, etc. A detailed study of such properties and some excess parameters like excess adiabatic compressibility, excess free volume and few more in the liquid mixtures of these two compounds with PEG as a solute and Ethanol as a solvent at various mole fractions may throw some light on deeper understanding of molecular interaction between the solute and the solvent supported by NMR, IR etc. Hence the present research work is on ultrasonics/allied studies on these two liquid mixtures. Ultrasonic velocity (U), density (ρ) and viscosity (η) at room temperature and at different mole fraction from 0 to 0.055 of ethanol in PEG have been experimentally carried out by the authors. Acoustical parameters such as adiabatic compressibility (β), free volume (Vf), acoustic impedance (Z), internal pressure (πi), intermolecular free length (Lf) and relaxation time (τ) were calculated from the experimental data. We have calculated excess parameters like excess adiabatic compressibility (βE), excess internal pressure (πiE) free length (LfE) and excess acoustic impedance (ZE) etc for these two chosen liquid mixtures. The excess compressibility is positive and maximum around a mole fraction 0.007 and excess internal pressure is negative and maximum at the same mole fraction and longer free length. The results are analyzed and it may be concluded that the molecular interactions between the solute and the solvent is not strong and it may be weak. Appropriate graphs are drawn.

Keywords: Adiabatic Compressibility, Binary mixture, Induce dipole, Polarizability, Ultrasonic.

Digital Object Identifier (DOI): doi.org/10.5281/zenodo.1092271

Procedia APA BibTeX Chicago EndNote Harvard JSON MLA RIS XML ISO 690 PDF Downloads 2740

References:


[1] A T Seshadri and B Subrahmanyam, "Excess compressibility and excess dielectric constant for a morpholine-n-butyl alcohol liquid mixture” Journal of Physics: Condens. Matter, volume 2, (1990),7353-7360.
[2] S Mohanan, V K Vadiyan and K V Kevian, "A study on specific optic impedance of materials”,Applied Physics Letters, volume 70, (1997) 805.
[3] K. Genuit, "Background and Practical Examples of Sound Design”, ActaAcustica united with Acustica, 83, 1997, 805-812.
[4] Mehra, Rita,Sajnani, Hema, "Acoustical studies in ternary electrolytic mixtures at 25, 30, 35, 40 and 45°C" , Indian J Pure & Appl. Phys. 38 (2000) 762-765.
[5] Ramana, G Venkata; Rajagopal, E; Murthy, N Manohara," Ultrasonic studies in dilute solution of water and nonelectrolytes", Indian Journal of Pure and Applied Physics 38 (2000) 10-14.
[6] Deepti Gupta, AnandPrakash, SubhashChaudhary,PankajSrivastava and Dheeraj Kumar, "Molecular Interactions in Binary Mixture of Propylamine with Non-polar Solvents”, Asian Journal of ChemistryVol. 20, No. 6 (2008), 4234-4238.
[7] P .S.Nikam, Hasan,T.B. Mehdi Pawar, A.B.Sawant, "Ultrasonic velocity and allied parameters of symmetrical tetraalkylammonium bromides in aqueous ethanol at 298.15 K”Indian Journal of Pure and Applied Physics 42 (2004) 172-178.
[8] F Dunn, P D Edmonds and E J Fry, "Absorption and Dispersion of Ultrasound in Biological Media’ in Biological Engineering”. H P Schcoal, Ed., Mcgraw-Hill Book co., New York, N.Y.,(1969)
[9] Poly (ethylene glycol) Chemistry: Biotechnical and Biomedical Application (Ed. J M Haris),Plesum, NewYork, (1992)
[10] R Lawrance, " Engineering Process for Bioseperations” Butter Worth – Heinemann, Woburn (1994)
[11] D S Soane, " Polymer Applications in Biotechnology Pretice Hall, Eagle Wood Cliffs (1992)
[12] G D Smith, D Y Yoon, R L Jaffe, R H Colby, R Krishnamoorti, L J Fetlers "Conformations and structures of PEG melts from Molecular Dynamics simulations and small Angle Neutron Scattering Experiments” J Macromolecules,29, 3462-3469 (1996)
[13] Theodore A Litovitz, Daniel Setle, " Dielectric and Ultrasonic relaxation in Glycerol” J. of Chemical Physics, 21(17), (1953)
[14] Tiwari K, Patra C &Chkaravorthy A, AcoustLett, 19(3),(1995),53.
[15] P.B.Thakor,P.Gajjar, A.R.Jani, "Temperature dependence of thermodynamic properties of liquid alkali metals”Indian Journal of Pure and Applied Physics 38 (2000) 811-814.
[16] Subramanjan Naidu P&Ravindra Prasad K, "Ultrasonic velocity and allied parameters in solutions of cypermethrin with xylene and ethanol",Indian J Pure & Appl. Phys. 42 (2004) 512.
[17] EzhilPavaiR .&KanappanA.N,"Ultrasonic studies on aqueous ternary electrolytes" ,Indian J Pure & Appl. Phys. 42 (2004) 934