scholarly journals Properties of Negatively Charged Ruthenium Clusters in Molten Sodium Chloride

2019 ◽  
Vol 123 (26) ◽  
pp. 16179-16185 ◽  
Author(s):  
Nazanin Rahimi ◽  
Eric W. McFarland ◽  
Horia Metiu ◽  
Henrik H. Kristoffersen
Keyword(s):  
Sodium Chloride ◽  
Ruthenium Clusters ◽  
Molten Sodium

scholarly journals Determination of the Average Molar Mass of the Vapour Above Molten Sodium Chloride by the Transpiration Method.

1979 ◽  
Vol 33a ◽  
pp. 407-412 ◽  
Author(s):  
Halvor Kvande ◽  
Oldrich Strouf ◽  
Pär Svanström ◽  
Elina Näsäkkälä ◽  
Eberhard Hoyer ◽  
...  
Keyword(s):  
Sodium Chloride ◽  
Molar Mass ◽  
Average Molar Mass ◽  
Molten Sodium ◽  
Transpiration Method

The structure of molten sodium chloride

1975 ◽  
Vol 8 (21) ◽  
pp. 3483-3490 ◽  
Author(s):  
F G Edwards ◽  
J E Enderby ◽  
R A Howe ◽  
D I Page
Keyword(s):  
Sodium Chloride ◽  
Molten Sodium

Self-diffusion in molten sodium chloride: a test of the applicability of the Nernst—Einstein equation

1957 ◽  
Vol 241 (1227) ◽  
pp. 554-567 ◽  
Keyword(s):  
Sodium Chloride ◽  
Einstein Equation ◽  
Diffusion Coefficients ◽  
Liquid Sodium ◽  
Einstein Relation ◽  
Transport Numbers ◽  
Self Diffusion ◽  
Capillary Method ◽  
Molten Sodium ◽  
The Individual

Self-diffusion coefficients of sodium and chlorine in molten sodium chloride have been determined by the capillary method with the aid of 22 Na and 36 Cl radio-tracers. The results can be represented by the expressions D Na = 8x 10 -4 exp (-4000/RT) and D Cl = 33 x 10 -4 exp (-8500/.RT). These values, when inserted in the Nernst-Einstein equation (A = (F 2 /RT) (D+ D-)), lead to a value of the equivalent conductance, A, which is about 40 % greater than that observed experimentally. The evidence that the diffusion coefficients of Na + and Cl - are similar in magnitude and that the activation energies are much smaller than the heat of vaporization of liquid sodium chloride, support the conclusions, derived from other evidence, that the free volume in the molten salt consists largely of holes, analogous to vacant lattice sites. On the basis of this model, the discrepancy in the Nernst-Einstein relation can readily be interpreted in terms of two diffusion mechanisms, one being normal vacancy diffusion of single ions, and the other a process in which no net charge is displaced in a unit step. It is suggested that the latter is the Seitz-Dienes mechanism of consecutive jumps of cation and anion in coupled vacancies. The interpretation mentioned enables the individual mobilities of Na + and Cl - ions to be determined, and hence their transport numbers can be calculated (t Na += 0.71, t Cl - = 0.29 at 935° C). The individual diffusion coefficients of the ions and of the coupled vacancies are in reasonable agreement with the Stokes-Einstein equation.

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