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KURENAI : Kyoto University Research Information Repository

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x<br />

o-= f2e(82)<br />

A similar pressure drop equation can be written for the other two-phase<br />

sections, i.e., the upper plenum and condensation section. From this formu-<br />

lation, it is clear that the density ratio, viscosity ratio, exit quality,<br />

and void-quality (or drift velocity) correlations are very important for the<br />

similarity of two-phase systems in addition to the similarity conditions for<br />

single phase flow. In essence, the exit quality corresponds to the tempera-<br />

ture rise AT in a single phase flow. Furthermore, the frictional, convective,<br />

and gravitational pressure drops depend strongly on the exit quality, property<br />

ratios and void-quality correlation. These dependencies make the similarity<br />

requirement for two-phase flow much more severe than that for single phase<br />

flow.<br />

as<br />

For a natural circulation system, the total driving force can be written<br />

Apdr ="PATZb.+QZc +E(ApgQ)i .(83)<br />

On the other hand, the resistance to.the flow is given by<br />

TP<br />

2<br />

AD =pu2ftKao2 fr2di (?)<br />

SP<br />

ft1 + ppx/Pg (aoy2<br />

TP(1 + Aux/11)0.25 i ai<br />

+ K.(1+epxl . 5/p )•()2} •(84)<br />

gi<br />

Here SP and TP denote the single phase and two-phase regions. The net convec-<br />

tiVe acceleration term has been neglected because the large part of it should<br />

cancel out between the boiling and condensation processes. The right hand<br />

side of Eq. (83) represents the single phase and two-phase driving force due<br />

351

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