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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):
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Thermal Contact Resistance (TCR)/Thermal Contact Conductance (TCC)

DOI 10.1615/hedhme.a.000164

2.4.6 Thermal contact resistance (TCR) / thermal contact conductance (TCC)

A. Introduction

When two similar or dissimilar solid materials at different temperatures are brought into contact, energy is transferred across the interface of contact. If the two surfaces could be obtained free of contamination and brought into perfect contact without any gaps at the interface, the resistance to the flow of heat would be negligible. However, this condition is not one obtainable in practice. Hard surfaces, including metals, even when highly polished and apparently flat, show appreciable contact resistance to heat flow. This resistance is caused by a lack of complete contact between the mating surfaces: i.e., when two surfaces are pressed together, contact is actually made only at a few discrete points due to the individual surface roughness and microscopic asperities, as illustrated in Figure 1. As the interface is approached, heat flux lines tend to converge to the direct solid-to-solid contact points since this path offers less resistance than the gaps which may be filled with air or evacuated. The result is the formation of a temperature discontinuity at the interface.

Figure 1 Imperfect mating of contacting solid surfaces

For metal surfaces, the solid-to-solid contact area between the surfaces is generally a small fraction of the apparent area over which they meet. The direct contact area may be less than 1 percent of the total and generally exceeds 10 percent only when bonding agents or surface enhancements are used. When the pressure on the contact is increased, the peaks in contact will deform and the contact points will increase in both size and number. For dissimilar metals, the irregularities of the softer surface may undergo full plastic deformation while the peaks of the harder metal embed in the softer.

Thermal contact resistance (TCR) is defined as

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