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Next: Lower plenum flow path,
Up: Primary coolant circulation loop
Previous: Feedwater inlet flow path,
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The mass flux in the downcomer,
[
], 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}](img966.gif) |
(5.21) |
where
represents the total recirculation mass flow rate [kg/s].
The pressure change along the downcomer,
[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}](img969.gif) |
(5.22) |
The density of the water at the core inlet,
[kg/ ], corresponds
to the equilibrium enthalpy hi (see (5.20)), ie
 |
(5.23) |
where
 |
(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: Lower plenum flow path,
Up: Primary coolant circulation loop
Previous: Feedwater inlet flow path,
  Contents
  Index
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