scholarly journals Corrigendum to “The partial molal volume and compressibility of Tris and Tris–HCl in water and 0.725 m NaCl as a function of temperature,” [Deep-Sea Res. I 104 (2015) 41–51]

2016 ◽  
Vol 114 ◽  
pp. 160-161
Author(s):  
Carmen Rodriguez ◽  
Fen Huang ◽  
Frank J. Millero
2017 ◽  
Vol 5 (10) ◽  
pp. 160-167
Author(s):  
Yasmin Akhtar

Densities, ultrasonic velocities and viscosities of L- Valine and L- Phenylalanine in aqueous sodium bromide (0.00, 0.025 and 0.05) m solutions have been determined experimentally at 308 and 313 K. The results obtained from density ultrasonic velocity and viscosity measurement have been used to calculate the apparent molal volume, фv, apparent molal, adiabatic compressibility ф Ks, partial molal volume ф0v at infinite dilution, partial molal adiabatic compressibility ф0Ks at infinite dilution, transfer volume ∆ф(tr), experimental slopes Sv and SKs,Falkenhagen coefficient A and  Jones-Dole B coefficient. The results are discussed in terms of the dehydration effect of the sodium bromide upon the amino acids and weak solute- solute and strong solute- solvent interactions. The properties of these amino acids in water and water + sodium bromide solution systems are discussed in terms of the charge, size and hydrogen bonding effect.


2017 ◽  
Vol 27 (4) ◽  
Author(s):  
Ahmed Mohammed Abbas ◽  
Zainab Wajdi Ahmed ◽  
Alaa Fadhil Sulaiman ◽  
Issam AbdalKreem AbdalLatif

In this study binary and ternary solutions are prepared by using the sodium acetate concentrations (0.1, 0.125, 0.2, 0.25, 0.4, 0.5, 0.8, 1 M) in water and acetone –water mixtures .The important parameters such as apparent molal volume, the partial molal volume transfer,  apparent  molal compressibility, free energy of activation of viscous flow and thermodynamic activation parameter (enthalpy and entropy) determined of sodium acetate in water , 20%, 40% ,60% and 80% V/V acetone –water mixtures at 298.15K, 303.15K, and 308.15K from density and viscosity measurements espectively. The limiting apparent molal volumes and experimental slopes were derived from the Masson equation, have been interpreted in terms of solute–solvent and solute–solute interactions  respectively. The viscosity data were analyzed using theJones–Dole equation and the derived parameter B - coefficient has also been interpreted in terms of solute–solvent interactions in the solutions. 


1999 ◽  
Vol 14 (10) ◽  
pp. 4111-4118 ◽  
Author(s):  
Wei-Lung Wang ◽  
J. R. Chen ◽  
Sanboh Lee

The solvent-induced stresses in glassy polymers were investigated. The mass transport accounts for case I, case II, and anomalous transport. Case I transport is attributed to the concentration gradient, whereas case II transport is attributed to stress relaxation. Anomalous transport is the mixture of case I and case II. Both one-side and two-side mass transports with the boundary condition of constant surface concentration are considered. The stresses and longitudinal displacement arising from the mass transport are formulated based on the linear elasticity theory. The maximum stress is always located at the surface at the initial time. The stresses are a function of the partial molal volume, Young's modulus, and Poisson's ratio. From the longitudinal displacement data, the partial molal volume was determined.


1987 ◽  
Vol 65 (12) ◽  
pp. 2810-2814 ◽  
Author(s):  
Henryk Piekarski

Heat capacities and densities of dilute solutions of formamide, acetone, tetrahydrofuran, ethylene glycol, 2-methoxyethanol, and 2-ethoxyethanol in N,N-dimethylformamide were determined at 298.15 K. Apparent molal heat capacities and volumes for these solutes in DMF were calculated and compared with the analogous data for other substances in DMF solution as well as with the data concerning solutions in methanol and water. Heat capacities of cavity formation (ΔCcav) in DMF were calculated on the basis of the Scaled Particle Theory. ΔCcav appeared to be linearly correlated with the standard partial molal volume of corresponding solutes in DMF. Similar dependences were also found for aqueous and methanolic solutions of the non-electrolytes.


1992 ◽  
Vol 50 (2) ◽  
pp. 35-37
Author(s):  
Hugo Patino ◽  
Ernst A. Kemper ◽  
Jean L. Miller ◽  
Walter L. Michener

1993 ◽  
Vol 48 (11) ◽  
pp. 1073-1080
Author(s):  
B. A. Bilal ◽  
E. Müller

Abstract The equilibrium constant, partial molal volume, entropy and enthalpy of the formation of HSO4- ion in aqueous solutions have been determined up to 473 K and 975 bar at the ionic strengths 1 = 0 as well as in NaCl solutions having I = 1, 0.5 and 0.1 mol kg-1 At 473 K, for instance, the thermodynamic formation constant K0 decreases by ≈ 0.75 log units from saturation pressure to 975 bar. The corresponding decrease of the apparent formation constant Q at I = 1 m is ≈ 0.6 log units. The increased dissociation at higher pressure leads to a decrease of the partial molal volume and entropy due to the resulting higher electrostriction in the system.


1968 ◽  
Vol 90 (17) ◽  
pp. 4527-4533 ◽  
Author(s):  
Norio. Ise ◽  
Tsuneo. Okubo

1972 ◽  
Vol 50 (18) ◽  
pp. 2951-2962 ◽  
Author(s):  
J. D. Riddell ◽  
D. J. Lockwood ◽  
D. E. Irish

Laser Raman and infrared vibrational spectra of solutions of NaNO3 in deuterium oxide reveal the presence of both [Formula: see text] ion pairs and solvated nitrate ions. The degree of association has been measured. The concentration quotients are remarkably independent of concentration and almost equal to the thermodynamic association constant, 0.060 ± 0.006 kg mol−1 at 25.0 °C. The latter quantity was obtained by an extrapolation procedure, taking account of the activity coefficients. Values are reported for the activity coefficient of the ion pair. Interpretation is also considered in terms of a place-exchange equilibrium involving the solvent. Vibrational assignments are made to the two forms of nitrate ion present. Density, partial molal volume, conductance, and viscosity data are also presented and discussed in terms of the reported constitution.


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