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ORNL-4191 - the Molten Salt Energy Technologies Web Site

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o<strong>the</strong>rs, but all three stringers in <strong>the</strong> reactor are<br />

bound toge<strong>the</strong>r. The new stringers for <strong>the</strong> reactor<br />

core specimens and <strong>the</strong>ir controls are all pinned at<br />

<strong>the</strong> joints with 0.040-in.-diam Hastelloy N in order<br />

to eliminate <strong>the</strong> pin deformation problem.<br />

Studies of <strong>the</strong> deposition of fission products on<br />

<strong>the</strong> graphite and <strong>the</strong> Hastelloy N are being conducted<br />

by <strong>the</strong> Reactor Chemistry Division. For<br />

<strong>the</strong>ir work, <strong>the</strong>y used <strong>the</strong> graphite specimens from<br />

<strong>the</strong> bottom, middle, and top of <strong>the</strong> reactor core<br />

specimen stringer, plus matching controls and<br />

selected Hastelloy N samples from <strong>the</strong> stringer and<br />

basket. The results of <strong>the</strong>ir examinations are reported<br />

in Chap. 9.<br />

The remaining graphite samples are being measured<br />

for dimensional changes. Tests of <strong>the</strong> types<br />

outlined in ref. 3 will be made when <strong>the</strong> dimensional<br />

measurements are completed.<br />

The results of <strong>the</strong> examination of <strong>the</strong> Hastelloy N<br />

tensile specimens from <strong>the</strong> core position and from<br />

outside <strong>the</strong> reactor vessel are reported in detail in<br />

Sect. 16.2.<br />

We have begun to expose samples in <strong>the</strong> MSRE<br />

core that are of interest for future molten-salt reactors<br />

and thus have extended <strong>the</strong> scope of <strong>the</strong>se<br />

studies beyond surveillance of <strong>the</strong> MSRE. In <strong>the</strong><br />

specimens just removed, <strong>the</strong> tensile specimen rods<br />

were made of heats of Hastelloy N modified to yield<br />

increased resistance to radiation damage. One of<br />

<strong>the</strong> rods had an addition of 0.52 wt % Ti, and <strong>the</strong><br />

o<strong>the</strong>r had 0.42 wt % Zr. Besides evaluating <strong>the</strong><br />

radiation resistance of <strong>the</strong>se modified alloys, we<br />

should also be able to obtain data on <strong>the</strong>ir corrosion<br />

resistance in <strong>the</strong> MSRE environment.<br />

The alloy modification study was continued in <strong>the</strong><br />

new stringer, RS3, just returned to <strong>the</strong> MSRE. One<br />

of <strong>the</strong> tensile specimen rods had an addition of 0.5<br />

wt % Ti and 2 wt % W; <strong>the</strong> o<strong>the</strong>r had an addition of<br />

0.5 wt % Hf.<br />

The graphite samples included <strong>the</strong> anisotropic<br />

MSRE graphite (grade CGB), graphitized-pitch<br />

impregnated grade CGB graphite, isotropic graphite,<br />

pyrolytic graphite, and a joint of isotropic graphite<br />

brazed to molybdenum with a 60 Pd-35 Ni-5 Cr<br />

(wt %) alloy. Th.is test of <strong>the</strong> brazed joint with<br />

radiation and in flowing salt should supplement <strong>the</strong><br />

data on corrosion of such joints in static salt without<br />

radiation that are discussed later in this<br />

section. Since <strong>the</strong> radiation dose received in <strong>the</strong><br />

3MSR Program Semiann. Progr. Rept. Aug. 31, 1965,<br />

<strong>ORNL</strong>-3872, p. 89.<br />

200<br />

MSRE is small compared with what will be en-<br />

countered in an MSBR, <strong>the</strong> primary purpose for in-<br />

cluding various grades of graphite is to extend <strong>the</strong><br />

study of fission product behavior with <strong>the</strong>se grades.<br />

The principal objective of this program is to en-<br />

sure <strong>the</strong> safe operation of <strong>the</strong> MSRE. We are,<br />

<strong>the</strong>refore, continuing to retain 65% or more of <strong>the</strong><br />

space in <strong>the</strong> assembly for exposure of <strong>the</strong> MSRE<br />

grades of Hastelloy N and graphite (see Table<br />

16.1).<br />

16.2 MECHANICAL PROPERTIES OF THE MSRE<br />

HASTELLOY N SURVEILLANCE SPECIMENS<br />

H. E. McCoy<br />

The results of tensile tests run on <strong>the</strong> first group<br />

of specimens removed from <strong>the</strong> MSRE were reported<br />

previously. These specimens were removed after<br />

7823 Mwhr of reactor operation, during which <strong>the</strong>y<br />

were held at 1190 k 18'F for 4800 hr and accumu-<br />

lated a <strong>the</strong>rmal dose of 1.3 x 10'' neutrons/cm2.<br />

The creep-rupture tests on <strong>the</strong>se specimens have<br />

now been completed, and <strong>the</strong> results are summarized<br />

in Table 16.2. The times to rupture for <strong>the</strong> surveil-<br />

lance specimens and <strong>the</strong> controls are compared in<br />

Fig. 16.3. The rupture life is reduced greatly as a<br />

result of <strong>the</strong> neutron exposure. However, Fig. 16.4<br />

shows that <strong>the</strong> minimum creep rate is not appreciably<br />

affected. Although <strong>the</strong> reduction in <strong>the</strong> rupture life<br />

is large, it is quite comparable with what we have<br />

observed for specimens irradiated to comparable<br />

doses in <strong>the</strong> ORR in a helium environment. This<br />

point is illustrated in Fig. 16.5. The superior rup-<br />

ture life of heat 5081 is evident. The fracture<br />

strain is <strong>the</strong> parameter of greatest concern, since<br />

<strong>the</strong> rupture life does not appear to be reduced<br />

greatly by irradiation at low stress levels. The<br />

fracture strains for <strong>the</strong> various heats of irradiated<br />

material are compared in Fig. 16.6. The data indi-<br />

cate a minimum ductility for a rupture life of 1 to<br />

10 hr, with ductility increasing with increasing<br />

rupture life. A lower ductility of heat 5085 after<br />

irradiation in <strong>the</strong> MSRE is also indicated, although<br />

<strong>the</strong> data scatter will not permit this as an un-<br />

equivocal conclusion. The superior ductility of<br />

heat 5081 and <strong>the</strong> least ductility of heat 5085 (heat<br />

used for <strong>the</strong> top and bottom heads of <strong>the</strong> MSRE) are<br />

clearly illustrated.<br />

4W. H. Cook and H. E. McCoy, MSR Program Semiann.<br />

Progr. Rept. Feb. 28, 1967, <strong>ORNL</strong>-4119, pp. 95-103.

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