Liquid Heat Flux Research Articles

An investigation of the gravity effects on pool boiling heat transfer via high-fidelity simulations

Nucleate pool boiling simulations are carried out to study the effects of gravity on the dynamics of bubble formation, bubble departure, and the mutual bubble interactions. We focus on identifying the dominant trends associated with the flow and thermal behavior at different gravity levels using fixed values of wall superheat and liquid subcooling. This is accomplished by measuring the contributions to heat flux associated with turbulent flow resulting from the dynamics of bubble interaction. The time averaged fluctuations of velocity and temperature indicate that the wall heat flux conditioned by the wetted surface area - the liquid heat flux - provides a useful indication of high heat flux hot spots. Furthermore, despite substantial differences in the dynamics of large scale bubbles at different gravity levels, the average heat flux in the liquid region is found to be dominated by the sliding and merger type events associated with small scale bubbles over a wide range of gravity levels. This significance of near-wall, small scale bubble dynamics is reflected in the transition of vorticity structures from hairpin type vortices in the near-wall region to vortex ring patterns away from the wall. While the maximum value of average turbulent fluctuations occurs away from the wall for earth normal gravity, the near-wall peak is only slightly lower and is similar in magnitude to that in the case of low gravity. These observations reveal the significance of small scale dynamics in affecting the heat transfer which was previously thought to be dominated by large scale bubbles, particularly at low gravity levels.

Quality influence in post-burnout heat transfer

The analysis of many experimental results on post burnout heat transfer, obtained with a steam-water mixture flowing upward through a tubular duct at a pressure of 70 kg/cm 2 and at a specific mass flowrate of 220 g/cm 2s, has led the authors to the following main conclusions: In the post-burnout regime the heat flux ϑ goes partly to the liquid phase (ϑ gi) and partly to the vapor phase (ϑ gu): ϑ = ϑ gi + ϑ gu . The vapor heat flux is related to the wall-to-bulk temperature difference by a heat-transfer coefficient which is a linear function of the quality. The liquid heat flux is directly proportional to the liquid quality of the mixture.