Proceeding of International Heat Transfer Conference 6 1978
DOI: 10.1615/ihtc6.1550
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On Turbulent Pipe Flow With Heat Transfer and Chemical Reaction

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Cited by 3 publications
(2 citation statements)
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“…The mean velocity and mean shear stress averaged over one period agree very well with experimental data for a particular choice of the period, which turns out to be quite close to the interval between two successive events of intense turbulent activity in the wall region, the so-called 'bursts' (Laufer & Badri Narayanan 1971). The model, because of its simplicity and modest predictive capability, has proved very popular in diverse applications (see for example Thomas, Chung & Mahaldar 1971;Ooms et al 1978). The model is, however, far too crude to serve the purposes of providing an explanation for the complex processes that take place in the wall region of a turbulent boundary layer, as will be shown later.…”
Section: A C M Begaars I ? Lirishna Prasad and D A De Vriessupporting
confidence: 64%
“…The mean velocity and mean shear stress averaged over one period agree very well with experimental data for a particular choice of the period, which turns out to be quite close to the interval between two successive events of intense turbulent activity in the wall region, the so-called 'bursts' (Laufer & Badri Narayanan 1971). The model, because of its simplicity and modest predictive capability, has proved very popular in diverse applications (see for example Thomas, Chung & Mahaldar 1971;Ooms et al 1978). The model is, however, far too crude to serve the purposes of providing an explanation for the complex processes that take place in the wall region of a turbulent boundary layer, as will be shown later.…”
Section: A C M Begaars I ? Lirishna Prasad and D A De Vriessupporting
confidence: 64%
“…They found reductions of up to 27%. Ooms et al carried out finite-difference solutions for first-order, irreversible, endothermic reactions in general, using penetration theory, which is of questionable accuracy as a model of the turbulent transport, and thereby determined the enhancement factor for the heat-transfer coefficient as a function of the Reynolds number Re = 2au m ρ / μ , the Prandtl number Pr = c μ/ λ , and the Schmidt number Sc = μ/ ρ D f as well as of three parameters representing the imposed heat flux density at the wall, the rate of reaction, and the heat of reaction.…”
Section: Energetic Effectsmentioning
confidence: 99%