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loop in which sodium was circulated<br />
have been completed. Samples from <strong>the</strong><br />
hoL, cold, and heat exchanger sections<br />
of <strong>the</strong> loop were examined. Corrosion<br />
was negligible, as shown in Table 11.13.<br />
FUNDAMENTAL CORROSION RESEARCH<br />
W. R. Grimes<br />
Materials Chemistry Division<br />
W. D. Manly<br />
Metallurgy Division<br />
The basic research needed for<br />
determining corrosion mechanisms has<br />
Initial weight, g<br />
2<br />
Initial area, in.<br />
Initial volume,<br />
3<br />
in.<br />
Initial density,<br />
3<br />
dcm<br />
Approximate<br />
weight of NaK, g<br />
Duration of<br />
heating, hr<br />
Final weight, g<br />
Weight loss<br />
In grams<br />
In per cent<br />
Final volume,<br />
3<br />
in.<br />
Approximate<br />
volume loss, x<br />
Weight loss per<br />
initial unit<br />
area, mg/in. 2<br />
PERIOlD ENDING DECEMBER IO, 1.952<br />
been continued. Examinations have<br />
been made of corrosion products from<br />
dynamic corrosion test by making use<br />
of chemical and physical means to<br />
determine identities of <strong>the</strong> products,<br />
and studies are continuing on high-<br />
temperature reactions of various<br />
liquids withstructural metals, <strong>the</strong>rmal<br />
stability of NiO and NiF,, and reactions<br />
of molten fluorides under applied<br />
potentials. The preparation of various<br />
complex interaction products of<br />
structural metals with fluorides and<br />
<strong>the</strong> characterization of <strong>the</strong>se compounds<br />
TABLE 11.12. SUMMARY OF BeO-NaK COMPATIBILITY TESTS<br />
1(a)<br />
0.625<br />
0.0313<br />
90<br />
6.4<br />
2<br />
1.5054<br />
0.625<br />
0.0313<br />
2.93<br />
82<br />
96<br />
1.3320<br />
0.1734<br />
11.5<br />
280<br />
--<br />
3(b)<br />
1 I 4196<br />
0.625<br />
0.0312<br />
2.80<br />
82<br />
129<br />
1.1047<br />
0.3149<br />
22.2<br />
500<br />
4(c )<br />
1.4049<br />
0.623<br />
0.0307<br />
2.80<br />
82<br />
203<br />
1.3653<br />
0.0396<br />
2.81<br />
0.0306<br />
leg1 igi bl e<br />
60<br />
RUN AND SAMPLE NO.<br />
5<br />
1.2287<br />
0.609<br />
0.0310<br />
2.60<br />
82<br />
174<br />
1.0896<br />
0.1391<br />
11.3<br />
Q. 0263<br />
15<br />
2 30<br />
1.2736<br />
0.455<br />
0. 0293(h)<br />
2.65<br />
a2<br />
2 12<br />
0.9384<br />
0.3352<br />
26.3<br />
”0. 028(h )<br />
3(h)<br />
7 40<br />
1. a437<br />
0.625<br />
Q.0378(h)<br />
2.98<br />
82<br />
2 12<br />
1.4335<br />
0.4102<br />
22.3<br />
0.031(h)<br />
19(h)<br />
67 0<br />
25.3124<br />
4.60<br />
0. 567<br />
2.72<br />
75<br />
29.9273<br />
(a)Temperature cycled from hoom temperature to<br />
1500+OF once and BOO to 1500 F five times; one (“Surface removed irregularly, leaving<br />
corner chipped off during test. “ditches” and rounded corners.<br />
‘b’Sample in two pieces at end of run; no o<strong>the</strong>r (f’Dense outer section of Be0 block (for<br />
pieces found.<br />
(C’Rotat,ed 14 hr; static 189 hr.<br />
density, see sec. 12, “Metallurgy and Ceramics”).<br />
‘g ) I rregu 1 ar semi w edge 6 hapes .<br />
(d)Porous inner section of Be0 block (for (h)Calculated for irregularly shaped samples;<br />
dens~ty~ see sec. 12. “Metallurgy and Ceramics”). values uncerteln.<br />
5.45<br />
0.640<br />
2.85<br />
75<br />
151