In nuclear reactor design and safety analysis, post-dryout heat transfer has been received great impetus on the thermal hydraulic concerns. The post-dryout heat transfer, which is characterized by a two-phase flow mixture of superheated vapor and disp...
In nuclear reactor design and safety analysis, post-dryout heat transfer has been received great impetus on the thermal hydraulic concerns. The post-dryout heat transfer, which is characterized by a two-phase flow mixture of superheated vapor and dispersed droplets, exists in most of the sequence events during a hypothetical large-break loss-of-coolant accident (LB LOCA). In the present study, an improved heat transfer correlation has been developed from an extensive experimental dataset obtained from vertical tubes for the rediction of local wall temperature in the post-dryout region. The improved correlation modified the ellknown film-boiling look-up table to be applied to the developing post-dryout region. The newly-developed correlation has been validated using various postdryout datasets covering not only LB LOCA but also other pressurized conditions for different purposes. The wall temperature prediction results showed very good agreement to the experimental data except for some cases of low mass flux and heat flux inlet conditions.
At the early stage of reflood in an LB LOCA, the dispersed droplets would be mostly evaporated due to the verheating process, and the cooling water from the emergency core cooling systems has not levelled up yet. Hence, the prevailing wall-to-vapor convective heat transfer plays the most important role on the heat removal process. Under the harsh conditions in the reactor core, the fuel cladding could become ballooned due to the increase in surface temperature and the difference between the inner and outer pressures of the fuel rod. The deformation of the fuel cladding would restrict the subchannel flow area resulting in severe
flow blockage. In this work, a series of steam cooling experiments has been conducted to study the effect of flow blockage on the local wall-to-vapor convective heat transfer with consideration of fuel relocation phenomenon. The experimental results have been used to derive a new flow blockage model which is able to complement the conventional flow blockage model implemented in the COBRA-TF code. The new flow blockage model has been generalized to universally apply to different flow blockage configurations.
The upward flow inside a partially blocked core would be redistributed leading to remarkable changes in local flow pattern. The local mass flux in the intact subchannels are remarkably larger than those in the blocked subchannels due to the flow bypass effect. Additionally, the turbulence intensity and vorticity downstream of the blockage in the blocked subchannel are greatly enhanced owing to the flow separation effect. As a result, the local heat transfer in the vicinity of flow blockage may significantly altered. In order to investigate the local flow pattern in the partially blocked core, a new experimental facility has been designed by the author and constructed in Korea Atomic Energy Research Institute. The Particle Image Velocimetry measurement technique was adopted to capture the fluid motion inside a rod bundle containing partial flow blockage through a transparent test housing. The pressure drop caused by different flow blockage configurations as well as the information of local subchannel velocity have been recorded and analyzed. A new flow blockage pressure loss factor has been derived using Buckingham Pi theorem and regression technique, expressed as a function of flow blockage ratio, maximum flow blockage length, and divergence angle. The newly-developed flow blockage pressure loss factor has been used to improve the flow diversion model in the literature*.