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Next: Overview of the primary Up: Singular pressure changes Previous: Two-phase flows   Contents   Index

Sudden expansion

For a sudden contraction the expression

\begin{displaymath}
\Delta p_{\mbox{\protect\scriptsize cont}} \;\hbox{$=$\kern...
...( \frac{\rho_\ell}{\rho_g}
-1\right)\mbox{$<\!{x}\!>$}\right]
\end{displaymath} (5.30)

correlates both single and two-phase flow reasonably well [18]. As seen in (5.31) we use a homogeneous two-phase friction multiplier in order to account for the increased pressure change in two-phase flow.

The contraction loss coefficient $K_{\mbox{\protect\scriptsize cont}}$ [--] is given in Table 5.2. When compared to the figure in Weismann [11] we conclude that the values in the table correspond to a very high Reynolds number. We should note that the values of $K_{\mbox{\protect\scriptsize cont}}$ as a function of $\sigma$ given by different authors show considerable scatter probably because some authors fail to recognize a dependence of Reynolds number on the contraction loss coefficient. For reference we have compared values of $K_{\mbox{\protect\scriptsize cont}}$ from different sources in Figure 5.3.


\begin{table}
% latex2html id marker 20349\rule{\textwidth}{0.8mm} \refstepcou...
...\
0.8 & 0.053 \\
1.0 & 0.00\\ \hline
\end{tabular*}\end{minipage}\end{table}

\begin{figure}
% latex2html id marker 20412\rule{\textwidth}{0.2mm}
\rule{0cm}...
...d ($\cdot$): Collier \& Thome
\protect\cite[p. 111]{Collier1}.}
\par\end{figure}

 
 

 
 
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