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ORNL-4191 - the Molten Salt Energy Technologies Web Site

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c<br />

41<br />

Table 2.1. Radiation Levels Following Steps in Decontamination of an MSRE Sampler-Enricher Manipulator Hand<br />

_____I____<br />

Cleaning Radiation Level<br />

Cleaning Treatment Time Ntri Treatment<br />

None (as received)<br />

Detergent (Duz) jet Spray<br />

Rinse (water)<br />

Detergent (Duz) jet spray<br />

Formula 50<br />

Dilute HNO,<br />

Bolt freeing solvent with acetone tinse<br />

Concentrated HNO,<br />

Scrub with scouring powder (&IB-O)~<br />

Scrub with scouring powder (BaB-0)<br />

Formula 50<br />

Concentrated HNO,<br />

Scrub with scouring powder (Ran-0)<br />

Clean with concentrated HNO,<br />

Acetone rinse<br />

smears '<br />

aRemoved to laboratory hood.<br />

bZirconium and rutlienium.<br />

CIn disintegrations per minute.<br />

system and in planning for maintenance of <strong>the</strong><br />

components. On <strong>the</strong> basis of <strong>the</strong>se needs, a study<br />

of possibly useful devices was started.<br />

The concept of <strong>the</strong> pinhole camera using radiation<br />

shielding and gamma-ray-sensitive film was<br />

evaluated dong with a system using a portable<br />

collimator and a small gamma-sensitive dosimeter.<br />

It was determined that while <strong>the</strong> camera method<br />

was feasible, <strong>the</strong> results to date did not provide<br />

very good resolution of position, intensity, and<br />

size. The problem of calibration of <strong>the</strong> film for<br />

use in radiation fields of unknown energy appeared<br />

difficult. However, <strong>the</strong> time required to survey an<br />

area would be short, approximately Equal to <strong>the</strong><br />

required exposure time for <strong>the</strong> film. The use of<br />

<strong>the</strong> collimator method would take longer to complete<br />

a survey, but possibly could yield better<br />

resolution. This method also offered <strong>the</strong> potential<br />

of giving information on <strong>the</strong> gamma-ray energy<br />

spectrum of <strong>the</strong> source. A series of experiments<br />

with <strong>the</strong> collimator was conducted to evaluate <strong>the</strong><br />

method, with <strong>the</strong> results described below.<br />

(min) (r/hr)<br />

5<br />

5<br />

10<br />

10<br />

5<br />

10<br />

5<br />

5<br />

5<br />

5<br />

5<br />

5<br />

5<br />

300<br />

100<br />

75<br />

25<br />

7.5<br />

5.0<br />

3.0<br />

0..5--1.0<br />

0.2-1 .o<br />

No reduction<br />

No reduction<br />

No reduction<br />

0.2-0.3<br />

No reduction<br />

800-13, O0OC<br />

Experiment with a 5-curie 137@s Gamma Source<br />

A collimator was constructed by casting lead in<br />

a 4-im-diam steel pipe 48 in. long and providing a<br />

1-in.-diam hole <strong>the</strong> length of thc tube. The collimator<br />

tube was placed in a suitable hole in <strong>the</strong><br />

portable shield which was positioned over a pit<br />

containing a S-curie I3'cs source.<br />

Radiation measurements were made with <strong>the</strong><br />

equipment and source arranged as shown in Fig.<br />

2.3. The radiation source could be raised and<br />

lowered, and <strong>the</strong> collimator tube could be moved<br />

horizontally over <strong>the</strong> source. Weasurcments were<br />

made with <strong>the</strong> source 13 ft and 15 ft 6 in. below<br />

<strong>the</strong> top of <strong>the</strong> portable shield. The source was<br />

about f/4 in. in diameter and 2 in. long and was<br />

enclosed in a 1-in.-diam tube 5 in. deep in <strong>the</strong><br />

carrier.<br />

The results of <strong>the</strong> radiation measurements are<br />

shown in Fig. 2.4. It will be noted that as <strong>the</strong><br />

collimated ion chamber was moved horizontally<br />

over <strong>the</strong> source, <strong>the</strong> radiation readings changed

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