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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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VTOPEN<br />

= vtopen<br />

TYPE<br />

= {GAS or<br />

POOL}<br />

RESOLVHD<br />

VEQLENB<br />

= veqlnb<br />

VEQLENF<br />

= veqlnf<br />

VELEVB<br />

= velevb<br />

the time at which the vent should open or begin to open. The vent by default<br />

is initially open. Specification <strong>of</strong> this option will result in the vent being<br />

initially closed unless “vtclos” is also specified and “vtclos” < “vtopen.”<br />

Default = -1030. (s)<br />

keyword to specify whether the path is to carry gas and its associated<br />

constituents or liquid coolant and its constituents from the pool. A given path<br />

may carry only one <strong>of</strong> these groups.<br />

the keyword to resolve the gravitational head <strong>of</strong> an engineered vent <strong>of</strong> type<br />

GAS into three segments: the elevation change between the gas center <strong>of</strong><br />

elevation in one cell and the elevation at which the vent is attached to the cell,<br />

the elevation change between the ends <strong>of</strong> the flow path, and the elevation<br />

change within the second cell. As discussed in Section 4.4.5.1, if<br />

RESOLVHD is specified, the appropriate cell density is always used <strong>for</strong> f~st<br />

and third segments. Normally, the gas gravitational head is calculated on the<br />

basis <strong>of</strong> the net elevation change between cell gas centers <strong>of</strong> elevation and<br />

either a VDI or average density. The latter is used if MSTABLE is specified<br />

in the FLOWS input block. As discussed in Section 4.4.5.1, use <strong>of</strong><br />

RESOLVHD is not recommended unless the user has demonstrated that the<br />

resulting gravitational head is acceptable. The user invoking RESOLVHD<br />

should be aware that the default flow path elevations have changed horn prior<br />

versions--gas paths are by default connected to the top <strong>of</strong> the cell to avoid<br />

flooding by the pool.<br />

the characteristic height over which the gas exiting from a submerged back<br />

(FROM) end <strong>of</strong> a vent is equilibrated with the downstream pool as it rises.<br />

This height, designated as Iji in the discussion following Equation (4-16), is<br />

assumed to control the equilibration <strong>of</strong> both the coolant vapor in the bubbles<br />

and the gas temperatures, as discussed in that section. In contrast to the<br />

treatment in the dedicated suppression vent model, <strong>for</strong> regular flow paths and<br />

engineered vents, aerosols and fission products in the flow are removed<br />

completely from the flow and placed in the pool. As in the dedicated<br />

suppression vent model, core debris (in debris droplet fields) is completely<br />

removed and placed in the intermediate layer, if present, in the lower cell.<br />

Default = 0.01. (m)<br />

the characteristic height over which the gas exiting from a submerged Iiont<br />

(TO) end <strong>of</strong> a vent, in the case <strong>of</strong> reverse flow, is equilibrated with the<br />

downstream pool as it rises. This height is defined in a manner similar to<br />

“veqlnb.” (m)<br />

the absolute elevation <strong>of</strong> the back (FROM) end <strong>of</strong> an engineered vent. The<br />

default value <strong>of</strong> “velevb” is the top <strong>of</strong> the cell to which the end is attached<br />

(Htias shown in Figure 44) <strong>for</strong> a gas path and the bottom <strong>of</strong> the cell (~i) <strong>for</strong><br />

Rev O 14 28 6/30/97

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