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Understanding Neutron Radiography Reading V-Kodak Part 2 of 3

Understanding Neutron Radiography Reading V-Kodak Part 2 of 3

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These show the necessary emitter-film distances and thicknesses <strong>of</strong> lead that<br />

should surround the various gamma-ray emitters to provide protection <strong>of</strong><br />

stored film. These recommendations allow for a slight but harmless degree <strong>of</strong><br />

fog on films when stored for the recommended periods. The lead thicknesses<br />

and distances in tables above are considered the minimum tolerable. To<br />

apply the cobalt 60 table to radium, values for source strength should be<br />

multiplied by 1.6 to give the grams <strong>of</strong> radium in a source that will have the<br />

same gamma-ray output and hence will require the same lead protection.<br />

This table can be extended to larger or smaller source sizes very easily. The<br />

half-value layer, in lead, for the gamma rays <strong>of</strong> radium or cobalt 60 is about ½<br />

inch. Therefore, if the source strength is doubled or halved, the lead<br />

protection should be increased or decreased by 1/2 inch. The table can also<br />

be adapted to storage times longer than those given in the tabulation. If, for<br />

example, film is to be stored in the vicinity <strong>of</strong> cobalt 60 for twice the<br />

recommended time, the protection recommendations for a source twice as<br />

large as the actual source should be followed. Iridium 192 has a high<br />

absorption for its own gamma radiation. This means that the external<br />

radiation from a large source is lower, per curie <strong>of</strong> activity, than that from a<br />

small source.<br />

Charlie Chong/ Fion Zhang<br />

<strong>Radiography</strong> in Modern Industry. Rochester, NY: Eastman <strong>Kodak</strong> Co. 1980

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