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Next: Two-phase flow modeling Up: Core flow modeling Previous: Introduction   Contents   Index

Flow boiling in a channel with subcooled inlet

The flow scenario of a fluid which enters a heated channel as subcooled liquid and undergoes boiling is investigated in this section. As pointed out earlier the heat in a BWR is added mainly through a wall heat flux but also by direct energy decomposition in terms of volumetric heat sources. In Figure 6.1 we depict a schematic illustration of the different flow regimes likely to occur in a BWR core.

The fluid enters as subcooled liquid and a thermal boundary layer starts to build up. At point zn a narrow bubble layer starts to form and we have entered the wall voidage subcooled boiling region. The liquid outside the bubble layer is highly subcooled, ie $\mbox{$<\!{h_\ell}\!>$}_\ell \ll h_f$ which keeps the voids from reaching into the liquid. The void fraction in this region is normally very small and can in many cases be neglected. At point zd the void departure point we move into the detached voidage region. Since the liquid core is only slightly subcooled, $\mbox{$<\!{h_\ell}\!>$}_\ell < h_f$, the voids travel further into the liquid core. In the detached region the subcooled void fraction increases considerable and in an accurate BWR analysis6.1 it is therefore necessary to include a calculation of this subcooled void fraction.

When we reach the point zbulk the mixture enthalpy corresponds to the saturation enthalpy, ie $\mbox{$<\!{h}\!>$}= h_f$. If we had neglected subcooled boiling (ie the presence of non-equilibrium) the void profile which we will call the equilibrium void profile would have started here. The zbulk point divides the channel into a subcooled boiling and a saturated boiling part. Note that due to the non-equilibrium we still have $\mbox{$<\!{h_\ell}\!>$}_\ell < h_f$!

At the equilibrium point, zeq, all the liquid has been brought up to saturation, ie $\mbox{$<\!{h_\ell}\!>$}_\ell = h_f$ and we have obtained equilibrium. This point can be characterized by the point at which the actual void profile and the equilibrium void profile merge.

\begin{figure}
% latex2html id marker 24221\rule{\textwidth}{0.2mm}
\rule{0cm}...
...\hspace{1em}Flow regimes in
a boiling channel with subcooled inlet.}\end{figure}


next up previous contents index
Next: Two-phase flow modeling Up: Core flow modeling Previous: Introduction   Contents   Index  
 
 
 
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