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Regional Basic Professional Training Course in Korea

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<strong>Regional</strong> <strong>Basic</strong> <strong>Professional</strong> <strong>Tra<strong>in</strong><strong>in</strong>g</strong> <strong>Course</strong> (BPTC) on Nuclear Safety<br />

the beg<strong>in</strong>n<strong>in</strong>g of the corium‐concrete <strong>in</strong>teraction ‐ ow<strong>in</strong>g to the very large amount of<br />

turbulence of the corium‐concrete mixture – fission products can still be released, by<br />

boil<strong>in</strong>g or vaporization effect.<br />

16.5.2.2. Fission product behaviour <strong>in</strong> the primary system and conta<strong>in</strong>ment<br />

After a core or corium release, fission products (<strong>in</strong> gas or liquid form) travel through the<br />

reactor coolant system and the reactor conta<strong>in</strong>ment or escape paths, such as the nuclear<br />

auxiliary build<strong>in</strong>g, where they can either rema<strong>in</strong> for some time before escap<strong>in</strong>g to the<br />

environment, or can become temporarily or permanently deposited. The fission products<br />

behaviour along their path to the environment is governed by important physical<br />

phenomena that are specifically related to the thermal hydraulics conditions <strong>in</strong> the<br />

primary system and the thermodynamics of the conta<strong>in</strong>ment.<br />

Release from fuel:<br />

The first important macroscopic phenomenon is obviously the release of core or corium<br />

fission products. The important factors are the k<strong>in</strong>etic release rates and the physical and<br />

chemical species formed. The latter depend on the atmosphere prevail<strong>in</strong>g <strong>in</strong> the vic<strong>in</strong>ity<br />

of the core (temperature, hydrogen formed by the zirconium‐water reaction and reactions<br />

with products result<strong>in</strong>g from structure vaporization, especially silver).<br />

Modern severe accident fission products release models <strong>in</strong>clude empirically based fission<br />

product <strong>in</strong>ventory escape rate and fractional release models. These models <strong>in</strong>troduced <strong>in</strong><br />

computer codes are validated aga<strong>in</strong>st available experimental programs. Generally, at high<br />

temperatures (above 2000°C), the release from the fuel for the volatile elements depends<br />

almost entirely on the temperature and the time spent at those temperatures. The<br />

surround<strong>in</strong>g atmosphere, oxidiz<strong>in</strong>g or reduc<strong>in</strong>g, are of some importance for the chemical<br />

form but not so much for the released fraction. The volatile elements, that are mostly rare<br />

gases, iod<strong>in</strong>e, caesium, tellurium and strontium, are completely released from the fuel,<br />

❙ 938 ❙

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