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A B C D E F G H I J K L M N O P Q R
Rabas and Taborek correlation, for heat transfer in banks of low fin tubes, Rackett equation (modified) for liquid density Radiation: Radiation shields, in radiation heat transfer, Radiation source analysis, Radiative heat transfer: Radiators, automotive, construction, Radiometers, application in gas radiation property measurement, Radiosity, Stephan's law for, Radiosity-irradiation formulations in radiative heat transfer, Rankine cycle in refrigeration, Rao, B K Raoult's law for partial pressure, Rating of heat exchangers, Rayleigh instability, in free convection, Rayleigh number Reay, D Reboilers: Reciprocal mode integrating sphere, for reflection and transmission measurements in radiation, Rectangles: Rectangular ducts: Rectangular enclosures, free convective heat transfer in: Rectangular fins, for plate fin exchangers Reduced pressure, correlations for pool boiling using, Reference temperature: Refinery processes, fouling in, Reflection, of thermal radiation, from solid surfaces: Reflectivity, of solid surfaces, Reflectometer, heated cavity, Reflux condensers, Refractories, density of, Refractory surfaces, Refrigerants: Refrigerant 11 (Trichlorofluoromethane): Refrigerant 12 (Dichlorodifluoromethane): Refrigerant 13 (Chlorotrifluoromethane): Refrigerant 21 (Dichlorofluoromethane): Refrigerant 22 (Chlorodifluoromethane): Refrigerant 116: Refrigerant plant, entropy generation in, Refrigeration, heat transfer in, Regenerators and thermal energy storage, Regimes of heat transfer, in ducts, single phase flow, Reidel method, for predicting enthalpy of vaporisation, Reinforcing rings, for expansion bellows, Relaminarization, of turbulent flow, Reichenberg method, for effect of pressure on gas viscosity, Relief system design for shell-and-tube heat exchangers with tube side failure, Removal of fouling deposits: Renewable fuels, properties of, Renotherm, heat transfer medium, Repair, of expansion bellows, Residence times, in dryers: Resistance network analysis, Resistance (thermal) due to fouling: Reversible (minimum) work, in Reynolds number, Reynolds stress models, for turbulence, Rheologically complex materials, properties of: Rheological properties of drag reducing agents Rheology, shear flow experiments used in, Rhine, J M, Ribatski, G, Riblets for drag reduction, Richardson number, Richie, J M, Ring cells, in free convection, RODbaffles, in tube bundles with longitudinal flow, Rod bundles: Rohsenow correlation, for nucleate boiling,
Pool Boiling appliation in forced convection boiling in vertical tubes,
Roll cells, in free convection, Roller expansion, of tubes into tube sheets, Rose, J W, Rossby number, Rotary dryer, Rotating drums, heat transfer to particle bed in, Rotating surface, in an annular duct Rotation, as device for heat transfer augmentation, Roughness, surface: Rough walled passages, radiative heat transfer down, Rubber (sponge) balls, in fouling mitigation, Ryznar index for water quality,
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R Rohsenow correlation, for nucleate boiling,
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Pool Boiling

DOI 10.1615/hedhme.a.000192

2.7 BOILING AND EVAPORATION
2.7.2 Pool boiling

J.G. Collier and V. Wadekar

Pool boiling is defined as boiling from a heated surface submerged in a large volume of stagnant liquid. This liquid may be at its boiling point, in which case the term saturated pool boiling is employed, or below its boiling point, when the term subcooled pool boilingis used. The results of investigations into heat transfer rates in pool boiling are usually plotted on a graph of surface heat flux (q̇) against heater wall surface temperature (Tw) — the boiling curve. Such a curve for water boiling at atmospheric pressure is shown diagrammatically in Figure 1. An alternative presentation might use the wall superheat (Tw – Tsat) rather than the wall temperature itself.

Figure 1 Pool boiling curve for water at atmospheric pressure

The component parts of the boiling curve are as follows:

  1. The natural convection region AB, where temperature gradients are set up in the pool and heat is removed by natural convection to the free surface and thence by evaporation to the vapor space.

  2. The onset of nucleate boiling (ONB), where the wall superheat becomes sufficient to cause vapor nucleation at the heating surface. This may occur close to the point where the curves AB and B'C meet, as is usually the case for water at atmospheric pressure and above. Alternatively, it may occur at much larger superheats than those required to support fully developed nucleate boiling, resulting in a sharp drop in surface temperature from B to B' for the case of a constant surface heat flux. This latter behavior is associated with fluids at very low reduced pressures, e.g., water below atmospheric pressure and liquid metals in particular.

  3. The nucleate boiling region (B'C), where vapor nucleation occurs at the heating surface. Starting with a few individual sites at low heat fluxes, more sites become active as the heat flux is increased. Bubble departure frequency also increases with increasing heat flux. Finally, at high heat fluxes, the vapor structure changes significantly with bubble coalescence leading to formation of vapor patches and columns close to the surface.

  4. The critical heat flux (CHF or point D) marks the upper limit of nucleate boiling where the interaction of the liquid and vapor streams causes a restriction of the liquid supply to the heating surface.

  5. The transition boiling region (DE) is characterized by the existence of an unstable vapor blanket over the heating surface that releases large patches of vapor at more or less regular intervals. Intermittent wetting of the surface is believed to occur. This region can be studied only under conditions approximating a constant surface temperature.

  6. The film boiling region (EF), where a stable vapor film covers the entire heating surface and vapor is released from the film periodically in the form of regularly spaced bubbles. Heat transfer is accomplished principally by conduction and convection through the vapor film, with radiation becoming significant as the surface temperature is increased.

In the natural convection region (1), the liquid may be at or below the saturation temperature. The temperature gradient away from the surface may be established from work on single-phase natural convection (see Section 174). The remaining regions of the boiling curve will now be considered in more detail.

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