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ORNL-2106 - the Molten Salt Energy Technologies Web Site

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2.3. PHYSICAL PROPERTIES OF MOLTEN MATERIALS<br />

P R E SS UR E -C OM P OS Ill ON -1 EM P E R At UR E<br />

RELATIONS FOR THE SYSTEMS<br />

KF-ZrF, AND RbF-ZrF,<br />

S. Cantor<br />

Among <strong>the</strong> important guiding principles in <strong>the</strong><br />

search for improved or modified fuel mixtures are<br />

predictions regarding <strong>the</strong> changes in properties<br />

that will occur as a result of <strong>the</strong> substitution of<br />

one species of ion for ano<strong>the</strong>r in an o<strong>the</strong>rwise<br />

similar melt. To a very considerable extent <strong>the</strong>se<br />

predictions can be based on a determination of<br />

how <strong>the</strong> activity coefficients of <strong>the</strong> constituents<br />

change with composition. One of <strong>the</strong> easiest<br />

activities to measure, and a fairly important one<br />

to know, is <strong>the</strong> activity of ZrF, in mixtures with<br />

alkali fluorides at compositions such that <strong>the</strong><br />

vapor is essentially pure ZrF,. Mixtures con-<br />

taining 45 mole % or more ZrF, produce a vapor<br />

which, for practical purposes, is pure ZrF,, and<br />

<strong>the</strong> activity of ZrF, is readily obtained from <strong>the</strong><br />

toto t vapor pressure, Accordingly, measurements<br />

are being made of <strong>the</strong> pertinent vapor pressures<br />

in alkali fluoride-ZrF, systems. It has been<br />

found that <strong>the</strong> volatility of <strong>the</strong> ZrF, varies in-<br />

versely with <strong>the</strong> size of <strong>the</strong> alkali cation. This<br />

is a consequence of <strong>the</strong> more pronounced com-<br />

plexing of ZrF, in <strong>the</strong> presence of <strong>the</strong> alkali<br />

cations, which have less attraction for fluoride<br />

ions. Lithium fluoride represents <strong>the</strong> case of an<br />

outstandingly strong attraction of a cation for<br />

ratio of <strong>the</strong> lithium i<br />

vapor pressures fr<br />

C. J. Barton, ANP Q<br />

P Quar. Prog. Rep.<br />

,K. A. Sense et al.. Vapor Pressures of <strong>the</strong> Sodium<br />

Fluoride-Zirconium Fluoride System and Derived Jnfor-<br />

mation, BMI-1064 (Jan. 9, 1956).<br />

F. F. Blankenship G. M. Watson<br />

E. R. Van Artsdalen<br />

PERIOD ENDING JUNE 10, 7956<br />

termined by <strong>the</strong> Rodebush-Dixon method that has<br />

been used for o<strong>the</strong>r ZrF mixtures at <strong>ORNL</strong>.<br />

This method depends on Ae “valve” action of<br />

<strong>the</strong> salt vapor above a liquid held at constant<br />

temperature; <strong>the</strong> valve action is manifested by a<br />

differential manometer which registers <strong>the</strong> re-<br />

sistance to flow of inert gas through a region<br />

occupied by <strong>the</strong> refluxing salt vapor. The<br />

“valve” becomes suddenly much more definite<br />

in effect when <strong>the</strong> inert gas pressure is lowered<br />

to a value corresponding to <strong>the</strong> salt vapor pressure.<br />

An absolute manometer is used to measure <strong>the</strong><br />

pressure at which this occurs.<br />

The System KF-ZrF,<br />

The vapor pressure experiments initiated pre-<br />

viously on <strong>the</strong> system KF-ZrF were continued.’<br />

The Rodebush-Dixon method,46 previously de-<br />

scri bed,S,7 was employed.<br />

In <strong>the</strong> present study <strong>the</strong> temperature determi-<br />

nations were carried out potentiometrically by<br />

using calibrated platinum-platinum-rhodium <strong>the</strong>r-<br />

mocouples. Pure ZrF, was prepared by subliming<br />

hafnium-free ZrF, at 72OOC under a vacuum.<br />

Translucent crystals were <strong>the</strong>n hdnd-picked from<br />

<strong>the</strong> sublimate. Spectrochemical analyses for ten<br />

possible metallic contaminants showed, in every<br />

case, less of <strong>the</strong> impurity than of <strong>the</strong> available<br />

standard. Potassium fluoride was purified by<br />

heating <strong>the</strong> reagent-grade product to 50°C above<br />

<strong>the</strong> melting point, cooling it slowly, and selecting<br />

clear fragments of <strong>the</strong> fused salt.<br />

6W. H. Rodenbush and A. L. Dixon, Phys. Rev. 26,<br />

851 (1925).<br />

7R. E. Moore and C. J. Barton, ANP Quar. Prog. Rep.<br />

Sept. 10, 1951, <strong>ORNL</strong>-1154, p 136.<br />

111

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