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Code Manual for CONTAIN 2.0 - Federation of American Scientists

Code Manual for CONTAIN 2.0 - Federation of American Scientists

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13.3.2.2.2 Standard Prescription Input and Model Choices. Thepresent discussion will delimited<br />

tothefinal version thatwas recommended <strong>for</strong> NPPanalysis. Itisimportant tounderstand thatthis ~<br />

version is still considered applicable to experimental analysis; in fact, the modifications introduced<br />

would make very little difference in the analysis <strong>of</strong> any <strong>of</strong> the experiments considered in the<br />

<strong>CONTAIN</strong> validation ef<strong>for</strong>t. The experimental validation presented in Reference Wi195 and<br />

summarized in Figure 13-3 is there<strong>for</strong>e considered equally applicable to the present prescription.<br />

The principal reason <strong>for</strong> the modifications was the recognition that NPP analyses may encounter a<br />

wider range <strong>of</strong> conditions than any studied experimentally, and that the prescription used in the<br />

experimental analysis could encounter pitfalls under some conditions even though problems did not<br />

arise <strong>for</strong> the conditions <strong>of</strong> the experiments. In addition, the NPP prescription includes a few<br />

simplifications; e.g., elimination <strong>of</strong> some nondefault parameter specifications now considered to be<br />

unnecessary.<br />

The current standard input prescription <strong>for</strong> DCH analysis is summarized in Table 13-1. All<br />

parameters and model options not given in the table are left at the <strong>CONTAIN</strong> default values.<br />

In the analyses <strong>of</strong> the experiments, parameters describing vessel blowdown, the fraction <strong>of</strong> the debris<br />

dispersed from the cavity (f&,P),and the time-dependence <strong>of</strong> the debris source rate [S~(t)]were based<br />

upon experimental results. This approach is obviously inapplicable <strong>for</strong> scenarios not studied<br />

experimentally, including NPP analysis. Hence semi-empirical means <strong>of</strong> providing this in<strong>for</strong>mation<br />

are adopted. These will be described next.<br />

Melt Characteristics and Vessel Failure Size. In any <strong>CONTAIN</strong> DCH analysis, definition <strong>of</strong> the melt<br />

characteristics (total mass ~, composition, initial temperature T$ must be obtained from an invessel<br />

analysis or some other in<strong>for</strong>mation source; <strong>CONTAIN</strong> has no models <strong>for</strong> calculating these<br />

quantities. The diameter <strong>of</strong> the hole in the vessel head, d~,likewise must be determined by the user,<br />

except that the effect <strong>of</strong> ablation on the hole size can be calculated by the RPV models if these are<br />

used.<br />

Blo wdown. In the standard prescription, the blowdown <strong>of</strong> steam from the primary system can be<br />

modeled by defining one or more cells to represent the primary system. The initial conditions <strong>for</strong><br />

these cells should be specified to correspond to the gas composition (steam plus any hydrogen<br />

present), temperature, and pressure <strong>of</strong> the primary system immediately prior to vessel breach. If the<br />

ideal gas equation <strong>of</strong> state <strong>for</strong> steam is being used, the volume specified <strong>for</strong> the primary system<br />

should be increased so that the code will calculate the correct mass <strong>of</strong> steam <strong>for</strong> the specified<br />

conditions; if the real equation <strong>of</strong> state is used, the volume specified should correspond to the actual<br />

free volume <strong>of</strong> the primary system.<br />

The blowdown is calculated by opening a flow path from the primary system cell(s) to the cell<br />

representing the cavity. Let t: represent the time the blowdown begins; it corresponds to the time<br />

<strong>of</strong> gas blowthrough in the melt ejection process, not the actual moment <strong>of</strong> vessel breach. Rather than<br />

opening the flow path area abruptly to its final size, & = nd~4, it is more realistic to specify a flow<br />

path area that increases linearly with time over an interval <strong>of</strong> duration z~given by the semi-empirical<br />

relation ~i195]<br />

Rev. O 13-28 6/30/97

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