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Baffle leakage in shell-and-tube heat exchangers: Baffles in shell-and-tube heat exchangers: Baker flow regime map for horizontal gas-liquid flow, Balance equation (applied to complete equipment), Band dryer: Bandel and Schlunder correlations, for boiling in horizontal tubes, Basket-type evaporator, Barbosa, J R Jr, Bateman, G, Bayonet tube heat exchangers, constructional features of, Bayonet tube evaporators, Beaton, C F, Beer-Lambert law, Bejan, A, Bell-Delaware method for shell-side heat transfer and pressure drop in shell-and-tube heat exchangers, Bell and Ghaly method for calculation of multicomponent condensation, Benard cells in free convection in horizontal fluid layers, Bends: Benzaldehyde: Benzene: Benzoic acid: Benzonitrile: Benzophenone: Benzyl alcohol: Benzyl chloride: Berenson equation for pool film boiling from a horizontal surface, Bergles, Arthur E, Bernoulli equation, application to flow across cylinders, Bimetallic tubes: Binary mixtures: Bingham fluid (non-Newtonian), Biofouling, Biot number: Biphenyl: Bismarck A, Black liquor, in pulp and paper industry, fouling of heat exchangers by, Black surface: Blackbody radiation, Blades, in scraped surface heat exchangers, Blake-Carmen-Kozeny equation, Blasius equation for friction factor, Blenkin, R, Blunt bodies, drag coefficients for, Boilers: Boiling: Boiling curve: Boiling length: Boiling number, definition, Boiling point, normal, Boiling range (in multicomponent mixtures): Boiling surface in boiling in vertical tubes, Boiling Water Reactor (BWR), fouling problems in, Bolted channel head in shell-and-tube exchanger, Bolted cone head in shell-and-tube heat exchanger, Bolted joints, thermal contact resistance in, Bolting, Bolting of flanges in shell-and-tube heat exchangers, Boltzmann's constant, Bonnet head, in shell-and-tube heat exchanger, Borishanski, V M, Borishanski correlation for nucleate pool boiling, Bott, T R, Boundary layer: Boussinesq approximations: Boussinesq number, definition, Bowring correlations for critical heat flux, Bracket supports for heat exchangers: Brauner, N, Brazed plate exchanger, Brazing in plate fin heat exchanger construction, Bricks, drying of, Brine recirculation, in multistage flash-evaporation, Brinkman number, Brittle fracture, Bromine: Bromley equation for film boiling from horizontal cylinders, Bromobenzene: Bromoethane: Bromomethane: Bromotrifluoromethane (Refrigerant 13B1): Brush and cage system, for fouling mitigation, BS 5500 code for mechanical design of shell-and-tube heat exchangers (see also PD 5500), Bubble crowding as mechanism of critical heat flux, Bubble flow: Bubbles: Bulk viscosity, Bundle-induced convection in kettle reboilers, Bundle layout, in condensers Buoyancy effects: Buoyancy-induced flow in channels, free convective heat transfer with, Busemann-Crocco integral, application in boundary layer equations, 1,2-Butadiene: 1,3-Butadiene: Butane: 1-Butanol: 2-Butanol: Butene-1: cis-2-Butene: trans-2-Butene: Butterworth, D, Butyl acetate: t-Butyl alcohol: Butylamine: Butylbenzene: n-Butylbenzene: n-Butylcyclohexane: Butylcyclopentane: Butylene oxide: Butyr-aldehyde: Butyric acid: Butyronitrile: Bypass (shell-and-tube bundle):
C D E F G H I J K L M N O P Q R S T U V W X Y Z

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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