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Code Manual for CONTAIN 2.0 - Federation of American Scientists

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Stage 2 accounts <strong>for</strong> the flashing because <strong>of</strong> the source if the BOIL option has been specified.<br />

Otherwise, the amount flashed is set to zero. The amount <strong>of</strong> pool mass flashing A% is given by<br />

Am . Qp + AQP - (mp+Amp)ht<br />

f<br />

h - hl<br />

V,s<br />

if positive, and the energy carried by the flashed water is<br />

(1 1-34)<br />

AQf = hv,,Amf (11-35)<br />

where QPand ~ are the initial pool energy and mass, respectively, and ~ and ~,, are the saturated<br />

liquid and saturated vapor enthalpy, respectively.<br />

Stage 3 accounts <strong>for</strong> the vapor taken up by the noncondensable gas bubbles <strong>of</strong> the vent flow. The<br />

bubble vapor pressure is assumed to be 0.95 times that <strong>of</strong> the pool vapor pressure at a self-consistent<br />

pool temperature T’ to avoid numerical problems. The pressure in bubbles containing the<br />

noncondensable gases at the pool surface is assumed to be the same as the atmosphere pressure Pi<br />

in the cell i in question. Thus,<br />

0.95 PS(T’) +P~C(T’) = Pi<br />

where P,(T’) the saturation pressure at the new self-consistent<br />

pool, correctly adjusted <strong>for</strong> the vapor energy removed by<br />

noncondensable gas pressure in the bubble.<br />

(11-36)<br />

equilibrium temperature T’ <strong>of</strong> the<br />

the bubbles; and P~C(T’)is the<br />

If the BOIL option has been specified, Equation (11-33) combined with the ideal gas assumption<br />

provides the vapor mass in the outflow ~,Ou,<br />

mv,o”t=<br />

MV0.95P$T’)N~C<br />

Pi - 0.95PS(T’)<br />

(11-37)<br />

where M, is the molecular weight <strong>of</strong> water vapor, and N~C is the moles <strong>of</strong> noncondensable gas.<br />

Otherwise nqOU~is set to zero.<br />

The linearized energy balance <strong>for</strong> the suppression pool, taking into account the fact that vaporization<br />

into the bubbles cools the pool and the gas passing through, is given by<br />

mv,out%v@’J = AQ; - (Cp+ cg)ALq<br />

(11-38)<br />

where hCv(T’)is the latent heat <strong>of</strong> evaporation (~,, - h~,,)evaluated at T‘; AQ~equals AQP- AQ~-<br />

(~ - AI%)L(TP) ~d represents the ch~ges in the POO1energy because OfPrOCeSSeSCOnSidered<br />

in Stage 1 and Stage 2; CPis the specific heat <strong>of</strong> the pool multiplied by the sum <strong>of</strong> the pool mass and<br />

any additional mass <strong>of</strong> vapor condensed in the pool minus any flashed; C~is the specific heat <strong>of</strong><br />

O 11 21 6/30/97

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