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Next: Lower plenum flow path, Up: Primary coolant circulation loop Previous: Feedwater inlet flow path,   Contents   Index

Downcomer flow path, \fbox{5}

The mass flux in the downcomer, $\mbox{$<\!{G}\!>$}_{\framebox[1.5ex]{\raisebox{-2.2pt}[0pt][0ex]{\scriptsize 5}}}$ [ ${\mbox{kg}}/({\mbox{m}}^2\cdot{\mbox{s}})$], is given by

\begin{displaymath}
\mbox{$<\!{G}\!>$}_{\framebox[1.5ex]{\raisebox{-2.2pt}[0pt]...
...framebox[1.5ex]{\raisebox{-2.2pt}[0pt][0ex]{\scriptsize 5}}}}}
\end{displaymath} (5.21)

where $\mbox{$\dot{m}$}_i$ represents the total recirculation mass flow rate [kg/s].

The pressure change along the downcomer, $\Delta p_{\framebox[1.5ex]{\raisebox{-2.2pt}[0pt][0ex]{\scriptsize 5}}}$ [Pa], is taken as

\begin{displaymath}
\Delta p_{\framebox[1.5ex]{\raisebox{-2.2pt}[0pt][0ex]{\scr...
...5ex]{\raisebox{-2.2pt}[0pt][0ex]{\scriptsize 5}}}}^2}{2\rho_i}
\end{displaymath} (5.22)

The density of the water at the core inlet, $\rho_i$ [kg/${\mbox{m}}^3$], corresponds to the equilibrium enthalpy hi (see (5.20)), ie

\begin{displaymath}
\rho_i = \rho_\ell(p,T_i)
\end{displaymath} (5.23)

where

\begin{displaymath}
T_i = T_\ell(p,h_i)
\end{displaymath} (5.24)

and p is the pressure at the downcomer inlet [Pa]5.1. Note that wee have silently assumed that the feedwater is sufficiently subcooled such that all carry-under vapor is condensed and the combined fluid is subcooled. This assumption is in practice very sound since stability requirements5.2 demand a certain amount of core inlet subcooling.


next up previous contents index
Next: Lower plenum flow path, Up: Primary coolant circulation loop Previous: Feedwater inlet flow path,   Contents   Index  
 
 
 
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