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Hagen-Poiseuille law Hagen-Rubens relation, between electrical and optical constants, Hall Taylor, N S, Halogenated hydrocarbons: Handley and Heggs equation for fixed bed pressure drop, Hankinson and Thomson method, for liquid density: Hardening (precipative) of stainless steels, Hardwick, R, Harris, D, Hausen equation for developing laminar flow, Hays, G F Headers in shell-and-tube heat exchangers, Heads, in heat exchangers: Heat and mass transfer: Heat exchanger design, introduction, Heat exchangers: Heat of vaporisation (see Enthalpy of vaporisation), of pure substances Heat pipes: Heat pumping, relation to heat exchanger network design, Heat storage (see Regenerators and thermal energy storage) entropy generation in, Heat transfer: Heat transfer coefficient: Heat transfer media, Heat transfer salt, Heat transfer regimes: Heat of vaporization, Heated cavity reflectometer, Heating media, for reboilers, Heavy water, physical properties of, Heggs, P J, Helical coils of circular cross section: Helical coils of rectangular cross section, Helical inserts, for enhancement of heat transfer in boiling, Helium: Helmholtz reciprocity principle, in radiative heat transfer, Henry, J A R, Henry-Fauske model, for critical two-phase flow, Henry's law, for partial pressure, Heptadecane: Heptadecene: Heptane: 1-Heptanol: 1-Heptene: Herman, K W, Hermes, C L L, Heterogeneous conveyance in horizontal pipes, Heterogeneous nucleation in boiling, Hewitt, G F Hexachloroethane (Refrigerant 116): Hexacyclopentane, superheated vapor properties, Hexadecane: Hexadecene: 1,5-Hexadiene: Hexagonal cells, in free convection, Hexamethylbenzene: Hexane: Hexanoic acid: 1-Hexanol: 1-Hexene: Hexylbenzene: Hexylcyclohexane: Hexylcyclopentane, Hicks equation, for fixed-bed pressure drop, High pressure closures, ASME VIII code guidance for, High-chrome steels, thermal and mechanical properties, High-finned tubes, correlations for single-phase heat transfer in flow over, Hills, P D Hohlraum cavity, Holdup, in liquid-liquid flow, Holland, guide to national practice for mechanical design of heat exchangers, Homogeneous condensation (fog formation), Homogeneous model: Homogeneous nucleation: Honeycombs: Hopkins, D, Horizontal condensers: Horizontal cylinders: Horizontal layers, of fluid, free convection heat transfer in, Horizontal pipes: Horizontal shell-side evaporator, Horizontal surfaces: Horizontal thermosiphon reboilers: Horizontal tube-side evaporator, Horizontal tubes: Hottel's rule, in absorption of radiation by gases, Hsu criterion, for onset of nucleate boiling, Hybrid cooling towers, Hydraulic conveyance: Hydraulic expansion, of tubes into tube sheets in shell-and-tube heat exchangers, Hydraulic turbine, lost work in, Hydraulic resistance, in flow of supercritical fluids, Hydraulically smooth surface, Hydrazine: Hydrocarbons: Hydrodynamic entrance length, in single-phase flow in ducts, Hydrogen: Hydrogen bromide: Hydrogen chloride: Hydrogen cyanide: Hydrogen fluoride: Hydrogen iodide: Hydrogen peroxide: Hydrogen sulfide: Hydrostatic testing of shell-and-tube heat exchangers, Hysteresis:
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Boiling Outside Tubes and Tube Bundles

DOI 10.1615/hedhme.a.000195

2.7 BOILING AND EVAPORATION
2.7.5 Boiling outside tubes and tube bundles

A. Boiling outside single tubes in cross flow

(a) Flow patterns

This section deals with the case where the flow past the tube or cylinder is by forced rather than by natural convection. This latter situation is dealt with in Section 192. Photographs presented by Vliet and Leppert (1962a) show very clearly the flow patterns that occur when nearly saturated water flows upward across a uniformly heated cylindrical tube. At moderate heat fluxes, typically around 20% of the critical heat flux, a vapor cavity forms in the cylinder’s wake. Initially this cavity is not continuous along the length of the cylinder, but as the heat flux is increased, the increase in the length of the cavity in the direction of flow results in the formation of a very uniform vapor sheet. An increase of velocity from 0.4 to 1.5 m/s or of tube diameter from 0.254 mm to 4.8 mm also results in a large stable vapor cavity behind the cylinder. Under these circumstances the only liquid reaching the top half of the cylinder is that which is supplied between the vapor bubbles and the heater surface as the bubbles enter the cavity wake near the horizontal diameter. For low heat fluxes, more liquid is supplied than evaporated and the excess is removed by entrainment in the cavity. The critical heat flux is reached when the liquid supplied in this manner becomes insufficient to cool the upper half of the cylinder.

In a parallel study, Vliet and Leppert (1962b) extended their work to include the effect of subcooled water flowing across the heated rod. For low subcoolings (< 16 °C), the flow pattern observed was similar to that for water at the saturation temperature. For greater subcoolings there is insufficient vapor to form a cavity in the wake of the cylinder because of the rapid condensation.

(b) Boiling heat transfer at heat fluxes lower than the critical heat flux

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