Influence of the substrate permeability on Leidenfrost temperature

Author(s):  
Datta Prasad ◽  
Akshay Sharma ◽  
Susmita Dash
2013 ◽  
Vol 44 ◽  
pp. 170-180 ◽  
Author(s):  
P. Dunand ◽  
G. Castanet ◽  
M. Gradeck ◽  
D. Maillet ◽  
F. Lemoine

2021 ◽  
Vol 2119 (1) ◽  
pp. 012079
Author(s):  
I P Starodubtseva ◽  
A N Pavlenko

Abstract The results of computational experiments simulating the triggering of the quench front propagation on the superheated vertically oriented metal plates are presented. The plates are quenched by a gravitationally flowing down liquid nitrogen film. The temperature of the test samples at the beginning of the process was higher than the critical temperature and the Leidenfrost temperature, which means that direct long-term liquid-solid contact is impossible. For this reason, the front is initially motionless. As a result of numerical simulation, a dynamic pattern of the quench front propagation on a high-temperature surface was obtained. Analysis of the results allowed to find the realistic values of heat sink into the cooling medium, as well as the parameters of the local temperature disturbance, its spatial extent and amplitude, at which the conditions are created for triggering the process of quench front propagation on the high-temperature surface. Direct comparison of the numerical simulations results with experimental data on the velocity, geometry of the quench front and on the dynamical pattern of the process confirmed the reliability of the results obtained.


2000 ◽  
Author(s):  
John D. Bernardin ◽  
Issam Mudawar

Abstract This study presents a theoretically-based model of the Leidenfrost point (LFP); the minimum liquid/solid interface temperature required to support film boiling on a smooth surface. The model is structured around bubble nucleation, growth, and merging criteria, as well as surface cavity size characterization. It is postulated that for liquid/solid interface temperatures at and above the LFP, a sufficient number of cavities (about 20%) are activated and the bubble growth rates are sufficiently fast that a continuous vapor layer is established nearly instantaneously between the liquid and the solid. The model is applicable to both pools of liquid and sessile droplets. The effect of surface cavity distribution on the LFP predicted by the model is verified for boiling on aluminum, nickel and silver surfaces, as well as on a liquid gallium surface. The model exhibits good agreement with experimental sessile droplet data for water, FC-72, and acetone. While the model was developed for smooth surfaces on which the roughness asperities are of the same magnitude as the cavity radii (0.1–1.0 μm), it is capable of predicting the boundary or limiting Leidenfrost temperature for rougher surfaces with good accuracy.


2022 ◽  
Vol 168 ◽  
pp. 108910
Author(s):  
Rodolfo Ienny Martins ◽  
Maria de Lourdes Moreira ◽  
Jian Su

2005 ◽  
Vol 38 (6) ◽  
pp. 945-950 ◽  
Author(s):  
Lokesh Gakhar ◽  
John M. Wiencek

Traditional explanations for the efficacy of mineral oil in successful flash cooling of a protein crystal correctly point to the removal of excess liquid around the crystal to prevent external ice formation. Based on the physics of the well known Leidenfrost phenomenon, an additional role that mineral oil possibly plays in aiding vitrification is suggested: that of improving cooling rates for a protein crystal plunged into liquid nitrogen. The full potential of liquid heat transfer when using liquid nitrogen is not realized in conventional cooling techniques due to film boiling that occurs around larger protein crystals. However, a thin layer of an insulating material, such as a mineral oil, around the protein crystal can prevent this vapor film from forming by raising the Leidenfrost temperature. Surface cooling then occurs in the more efficient nucleate boiling regime where liquid nitrogen is in contact with the crystal throughout the quench. Using bare and coated thermocouples, the validity of a predictive Leidenfrost temperature equation for use in liquid-nitrogen plunge cooling of protein crystals is demonstrated.


Author(s):  
S. R. Darr ◽  
J. Dong ◽  
N. Glikin ◽  
J. W. Hartwig ◽  
J. N. Chung

In many convective liquid–vapor phase-change heat transfer engineering applications, cryogenic fluids are widely used in industrial processes, spacecraft and cryosurgery systems, and so on. For example, cryogens are usually used as liquid fuels such as liquid hydrogen, liquid methane, and liquid oxygen in the rocket industry, liquid nitrogen and helium are frequently used to cool superconducting magnetic device for medical applications. In these systems, proper transport, handling, and storage of cryogenic fluids are of extreme importance. Among all the cryogenic transport processes performed in room temperatures, quenching, also termed chilldown, is an unavoidable initial, transient phase-change heat transfer process that brings the system down to the cryogenic condition. The Leidenfrost temperature or rewet temperature that signals the end of film boiling is practically considered the completion point of a quenching process. Therefore, rewet temperature has been considered the most important parameter for the engineering design of cryogenic thermal management systems. As most of the previous correlations for predicting the Leidenfrost temperature and the rewet temperature have been developed for water, they are shown to disagree with recent liquid nitrogen pipe chilldown experiments in upward and downward flow directions over a wide range of flow rates, pressures, and degrees of inlet subcooling. In addition to a complete review of the literature, two modified correlations are presented, one based on bubble growth and another based on the theoretical maximum limit of superheat. Each correlation performs well over the entire dataset.


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