Abstract
The critical heat flux (CHF) in forced
convective up flow has been investigated in a
uniformly heated vertical steel tube of 18 mm
internal diameter and 3.66 m length, with water as
the working fluid. The CHF was determined by the
sudden rise in the wall temperature of the
electrically heated tube. Experiments were
performed at nominal pressure 50 bar over three
mass flux values 0.11kg/s, 0.055kg/s and 0.027
kg/s, and heat flux with up to 400 kW maximum
power. The CHF results in the present experimental
ranges rise linearly as the mass flux increases.
Finally, a comparison of the experimental data with
available fluid correlations has been performed. The
present results of CHF are found to be an acceptable
agreement with those predicted by using (Bowring
Correlation) and are slightly higher when compared
with those predicted by Katto and Ohne Correlation
convective up flow has been investigated in a
uniformly heated vertical steel tube of 18 mm
internal diameter and 3.66 m length, with water as
the working fluid. The CHF was determined by the
sudden rise in the wall temperature of the
electrically heated tube. Experiments were
performed at nominal pressure 50 bar over three
mass flux values 0.11kg/s, 0.055kg/s and 0.027
kg/s, and heat flux with up to 400 kW maximum
power. The CHF results in the present experimental
ranges rise linearly as the mass flux increases.
Finally, a comparison of the experimental data with
available fluid correlations has been performed. The
present results of CHF are found to be an acceptable
agreement with those predicted by using (Bowring
Correlation) and are slightly higher when compared
with those predicted by Katto and Ohne Correlation