ORNL-1816 - the Molten Salt Energy Technologies Web Site
ORNL-1816 - the Molten Salt Energy Technologies Web Site ORNL-1816 - the Molten Salt Energy Technologies Web Site
ANP QUARTERLY PROGRESS REPORT Fig. 6.11. (a) As-Received ZrC. 150OOF for 100 hr. Unetched. 500X. loop sectionedafter a test may be seen in Fig.6.12. The hot legs of the loop were constructed of 0.5- in,-OD, 49-mi I-wall tubing, and the condenser section was of 0.25-in.-OD, 35-mil-wall tubing. The loop was loaded with 8 cm3 (approximately 12 9) of vacuum-distilled rubidium, which filled it to the level indicated in Fig. 6.12. A vapor- phase heat transfer system of this type will elimi- nate mass transfer in the vapor regions. However, the temperature gradients present in the liquid region might conceivably cause crystal deposition. The maximum attack occurred in the hot leg of the loopto adepth of lmil,as may be seen in Fig.6.13. The attack was intergranular, and one grain ap- peared to be ready to fall from the wall. A schematic diagram of the apparatus presently used to distill rubidium is shown in Fig. 6.14. r, 3 lb of rubidium has been purified, Since the addition of 8% sodium will reduce the melting point of rubidium to approximately 2OoF, tentative 0.001 0.002 0.003 0.004 0.005 0.006 0.007 0.008 I 0 5 (b) ZrC After Exposure to NaF-ZrF,-UF, (53.5-40-6.5 mole %) at plans call for an investigation of the corrosion properties of the sodium-rubidium eutectic. FUNDAMENTAL CORROSION RESEARCH G. P. Smith Meta I I urgy Di vi sion Mass Transfer in Liquid Lead J. V. Cathcart Metallurgy Division The results of previous tests3 indicated that a1 loys in which intermetallic compound formation was possible showed a marked increase in re- sistance to mass transfer in liquid lead as com- pared with the mass transfer obtained with their pure components. Comparable behavior was not observed in alloys such as Nichrome V in which 'J. V. Cathcart, ANP Quar. Prog. Rep. Sept. 10, 1954, ORNL-1771, p 100.
AT= 136OOF OPERATING TIME = 312 hr MAXIMUM CORROSION PENETRATION = 0 001 in. i6O0F NOTE EQUILIBRIUM LOOP SURFACE TEMPERATURES ARE GIVEN. - 0°F 4651 BOILER AND VAPOR SEPARATOR SECTION 30°F - 1 1 2 3 4 5 1 Fig. 6.12. Sectioned lnconel Loop After Ex- posure to Boiling or Vaporized Rubidium for 100 hr. During - the past quarter this hypothesis has been tested further, and, as in ,. PERlOD ENDING DECEMBER 70, 1954 The first loops in which the 50% Fe--50% Cr specimen was tested in liquid lead failed after 46 hr of operation with hot- and cold-leg Vempera- tures of 805 and 550°C, respectively. The second loop failed after only 30 hr of o and cold-leg temperatures of 805 and 5OO0C, re- spect ivel y. Microscopic examination showed clearly that a phase transformation took piece in the test specimens during the operation of the loops. As shown in Fig, 6.16, a narrow layer of a second phase formed at the outer surface of the hot-leg specimens, Hardness measurements yielded values of 162 and 1140 (DPH hardness scale) for the new and original phases, respectively. These values correspond closely to those expected for ferrite and sigma phases, The possibility that the new phase was ferritic was supported by the fact that it was magnetic and by a chemicctl analy- sis of the plugs formed in the loops. Siince the plugs were slightly richer in chromium than in iron, a decrease in the chromium content of the outer layers of the test specimens was indicated. The test temperature was close to the sigma-fo- ferrite transformation point, and therefore even a slight alteration in the original 50% Fe--50% Cr composition would produce an alloy in which only ferrite is stable at the temperature in question. A second alloy, 50% Mo-50% Fe, was a1 so tested. This alloy was chosen because an intermetallic compound predominates at the indicated compo- sition, Circulation of lead in this loop stopped after 520 hr with hot- and cold-leg temperatures of 805 and 5OO0C, respectively. Examination of this loop has not yet been completed; therefore, the results obtained will not be discussed other for loops containing their pure constituents. '
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ANP QUARTERLY PROGRESS REPORT<br />
Fig. 6.11. (a) As-Received ZrC.<br />
150OOF for 100 hr. Unetched. 500X.<br />
loop sectionedafter a test may be seen in Fig.6.12.<br />
The hot legs of <strong>the</strong> loop were constructed of 0.5-<br />
in,-OD, 49-mi I-wall tubing, and <strong>the</strong> condenser<br />
section was of 0.25-in.-OD, 35-mil-wall tubing.<br />
The loop was loaded with 8 cm3 (approximately<br />
12 9) of vacuum-distilled rubidium, which filled<br />
it to <strong>the</strong> level indicated in Fig. 6.12. A vapor-<br />
phase heat transfer system of this type will elimi-<br />
nate mass transfer in <strong>the</strong> vapor regions. However,<br />
<strong>the</strong> temperature gradients present in <strong>the</strong> liquid<br />
region might conceivably cause crystal deposition.<br />
The maximum attack occurred in <strong>the</strong> hot leg of <strong>the</strong><br />
loopto adepth of lmil,as may be seen in Fig.6.13.<br />
The attack was intergranular, and one grain ap-<br />
peared to be ready to fall from <strong>the</strong> wall.<br />
A schematic diagram of <strong>the</strong> apparatus presently<br />
used to distill rubidium is shown in Fig. 6.14.<br />
r, 3 lb of rubidium has been purified, Since<br />
<strong>the</strong> addition of 8% sodium will reduce <strong>the</strong> melting<br />
point of rubidium to approximately 2OoF, tentative<br />
0.001<br />
0.002<br />
0.003<br />
0.004<br />
0.005<br />
0.006<br />
0.007<br />
0.008<br />
I<br />
0<br />
5<br />
(b) ZrC After Exposure to NaF-ZrF,-UF, (53.5-40-6.5 mole %) at<br />
plans call for an investigation of <strong>the</strong> corrosion<br />
properties of <strong>the</strong> sodium-rubidium eutectic.<br />
FUNDAMENTAL CORROSION RESEARCH<br />
G. P. Smith<br />
Meta I I urgy Di vi sion<br />
Mass Transfer in Liquid Lead<br />
J. V. Cathcart<br />
Metallurgy Division<br />
The results of previous tests3 indicated that<br />
a1 loys in which intermetallic compound formation<br />
was possible showed a marked increase in re-<br />
sistance to mass transfer in liquid lead as com-<br />
pared with <strong>the</strong> mass transfer obtained with <strong>the</strong>ir<br />
pure components. Comparable behavior was not<br />
observed in alloys such as Nichrome V in which<br />
'J. V. Cathcart, ANP Quar. Prog. Rep. Sept. 10, 1954,<br />
<strong>ORNL</strong>-1771, p 100.