Ultrahigh CHF Prediction for Subcooled Flow Boiling Based on Homogenous Nucleation Mechanism

Homogeneous nucleation, although being discounted as a mechanism for vapor formation for water in most conditions, is found to possibly occur under some extreme conditions in subcooled flow boiling. Under the conditions, vapor bubbles of molecular dimensions generated in the superheated liquid adjacent to channel wall from homogeneous nucleation due to the local temperature exceeds homogeneous nucleation temperature. The condition is called in this paper as homogeneous nucleation governed condition. Under the condition, conventional flow pattern for subcooled flow boiling, which is characterized by the existence of Net Vapor Generation (NVG) point and the followed bubble detachment, movement and coalescence processes, cannot be established. Critical heat flux (CHF) triggering mechanism so far proposed, which employs a premise assumption that the conventional flow pattern has been established, such as liquid sublayer dryout model, is no more appropriate for the homogeneous nucleation governed condition. In this paper, first, the existence of the homogeneous nucleation governed condition is indicated

[1]  Charles Stanley Loosmore,et al.  Subcooled critical heat flux for water in round tubes , 1965 .

[2]  J. Weisman,et al.  A phenomenological model for prediction of critical heat flux under highly subcooled conditions , 1988 .

[3]  W. R. Gambill,et al.  HEAT TRANSFER, BURNOUT, AND PRESSURE DROP FOR WATER IN SWIRL FLOW THROUGH TUBES WITH INTERNAL TWISTED TAPES , 1960 .

[4]  A. Mariani,et al.  Experimental evaluation of the onset of subcooled flow boiling at high liquid velocity and subcooling , 1997 .

[5]  A. Mariani,et al.  Rationalization of existing mechanistic models for the prediction of water subcooled flow boiling critical heat flux , 1994 .

[6]  Ronald D. Boyd,et al.  Subcooled Water Flow Boiling Transition and the L/D Effect on CHF for a Horizontal Uniformly Heated Tube , 1990 .

[7]  K. Mishima,et al.  Critical Heat Flux for Flow-Boiling of Water in Small-Diameter Tubes under Low-Pressure Conditions. , 1995 .

[8]  J. W. Schaefer,et al.  INVESTIGATION OF FORCED-CONVECTION NUCLEATE BOILING OF WATER FOR NOZZLE COOLING AT VERY HIGH HEAT FLUXES , 1962 .

[9]  J. Mayersak,et al.  Confirmation of Gambill-Greene Straight-Flow Burnout Heat Flux Equation at Higher Flow Velocity , 1964 .

[10]  I. Mudawar,et al.  Ultra-high critical heat flux (CHF) for subcooled water flow boiling—I: CHF data and parametric effects for small diameter tubes , 1999 .

[11]  C. Lee,et al.  A mechanistic critical heat flux model for subcooled flow boiling based on local bulk flow conditions , 1988 .

[12]  J. Lienhard Corresponding States Correlations of the Spinodal and Homogeneous Nucleation Limits , 1982 .

[13]  Ronald D. Boyd,et al.  Subcooled Water Flow Boiling Experiments Under Uniform High Heat Flux Conditions , 1988 .

[14]  Ronald D. Boyd,et al.  Subcooled water flow boiling at 1. 66 MPa under uniform high heat flux conditions , 1989 .

[15]  J. Hopenfeld,et al.  Onset of stable film boiling and the foam limit , 1963 .

[16]  J. Weisman,et al.  Prediction of critical heat flux in flow boiling at low qualities , 1983 .

[17]  Y. Katto,et al.  A prediction model of subcooled water flow boiling CHF for pressure in the range 0.1–20 MPa , 1992 .

[18]  H. Nariai,et al.  Prediction of critical heat flux for subcooled flow boiling , 2000 .

[19]  R. Boyd Reply to “Comments on ‘Subcooled Water Flow Boiling Experiments Under Uniform High Heat Flux Conditions’” , 1989 .

[20]  S. Levy Forced convection subcooled boiling—prediction of vapor volumetric fraction , 1967 .

[21]  Gian Piero Celata,et al.  Assessment of correlations and models for the prediction of CHF in water subcooled flow boiling , 1994 .