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Heat transfer from laminar flow in ducts with elliptic cross-section
Authors:J. Schenk and Bong Swy Han
Affiliation:(1) Laboratorium voor Technische Natuurkunde der Technische Hogeschool, Delft, Nederland
Abstract:Summary The cooling of a hot fluid in laminar Newtonian flow through cooled elliptic tubes has been calculated theoretically. Numerical data have been computed for the two values 1.25 and 4 of the axial ratio of the elliptic cross-section epsi. For epsi=1.25 the influence of non-zero thermal resistance between outmost fluid layer and isothermal surroundings has also been investigated. Special attention has been given to the distribution of heat flux around the perimeter; when epsi increases the flux varies more with the position at the circumference. This positional dependence becomes less pronounced, however, as the (position-independent) thermal resistance of the wall increases.Flattening of the conduit, while maintaining its cross-sectional area constant, improves the cooling. Comparison with rectangular pipes shows that this improvement is not as marked with elliptic as with rectangular pipes.Nomenclature Ak=Am, n coefficients of expansion (6) - a, b half-axes of ellipse, b - ap=ar, s coefficients of representation (V) - D hydraulic diameter, = 4S/P; S = cross-sectional area, P = perimeter - De equivalent diameter, according to (13) - n coordinate (outward) normal to the tube wall - T temperature of fluid - Ti temperature of fluid at the inlet - Ts temperature of surroundings - v0 mean velocity of fluid - vz longitudinal velocity of fluid - x, y carthesian coordinates coinciding with axes of ellipse - z coordinate in flow direction - agr, beta dimensionless half-axes of ellipse, agr=a/D and beta=b/D - agrt heat transfer coefficient from fluid at bulk temperature to surroundings; equation (11) - agrw heat transfer coefficient at the wall; equation (3) - epsi axial ratio of ellipse, = a/b = agr/beta - xgr, eegr, zeta, ngr dimensionless coordinates; xgr=x/D, eegr=y/D, zeta=z/D, ngr=n/D - thetav dimensionless temperature, = (T–Ts)/(TiTs) - thetav0 cup-mixing mean value of thetav; equation (10) - lambda thermal conductivity of fluid - mgrm,n=mgrk eigenvalue - rgrc volumetric heat capacity of fluid - phgrm, n=phgrk=thetak eigenfunction; equations (6) and (I) - Nu total Nusselt number, = agrtD/lambda - 
$$Nu_infty  $$
Nusselt number at large distance from the inlet - Nuw wall Nusselt number, = agrwD/lambda, based on agrw - Pé Péclet number, = ngr0Drgrc/lambda
Keywords:
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