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Next: Singular pressure changes Up: Primary coolant circulation loop Previous: Downcomer flow path, Contents Index

Lower plenum flow path, $\fbox{6}$

Analogously with the other flow paths we can write the mass flux in the lower plenum, $\mbox{$<\!{G}\!>$}_{\framebox[1.5ex]{\raisebox{-2.2pt}[0pt][0ex]{\scriptsize 6}}}$ [ ${\mbox{kg}}/({\mbox{m}}^2\cdot{\mbox{s}})$ ], as

$\begin{displaymath} \mbox{$<\!{G}\!>$}_{\framebox[1.5ex]{\raisebox{-2.2pt}[0pt]... ...framebox[1.5ex]{\raisebox{-2.2pt}[0pt][0ex]{\scriptsize 6}}}}} \end{displaymath}$

(5.25)

and the pressure change, $\Delta p_{\framebox[1.5ex]{\raisebox{-2.2pt}[0pt][0ex]{\scriptsize 6}}}$ [Pa], as

$\begin{displaymath} \Delta p_{\framebox[1.5ex]{\raisebox{-2.2pt}[0pt][0ex]{\scr... ...5ex]{\raisebox{-2.2pt}[0pt][0ex]{\scriptsize 6}}}}^2}{2\rho_i} \end{displaymath}$

(5.26)

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