Abstract
This article presents a study on heat transfer in condensation of pure and mixtures of hydrocarbons in a compact welded plate heat exchanger. Three pure fluids (pentane, butane, and propane) and two mixtures (butane + propane) have been used. The operating pressure ranges from 1.5 to 18 bar. For pure fluids, two heat transfer mechanisms have been identified. For low Reynolds numbers, the condensation occurs almost filmwise and the heat transfer coefficient decreases with increasing Reynolds number. For higher values of the Reynolds number, the heat transfer coefficient increases gently. The transition between the two regimes is between Re = 100 and 1,000 and depends on the operating conditions. For mixtures, the behavior is different. For low Reynolds numbers, mass transfer affects heat transfer and reduces the heat transfer coefficient by a factor of up to 4. Correlations for filmwise and in-tube condensation do not predict the results accurately, and a specific correlation is proposed for pure fluid condensation. For mixtures, the condensation curve method does not allow mass transfer effects to be taken into account, and more work is required to establish an accurate predictive model.
Highlights
To cite this version: Bernard Thonon, André Bontemps
For low Reynolds numbers, the condensation occurs almost lmwise and the heat transfer coef cient decreases with increasing Reynolds number
The results indicate that the condensation is gravity-controlle d for low Reynolds numbers, and shear-controlled for higher Reynolds number
Summary
The Nusselt theory is valid only if the liquid lm is smooth, but for lm Reynolds numbers over 30, waves appear at the interface and increase the heat transfer coef cient. The average heat transfer coef cient is given by [1]. For Reynolds numbers above 1,600, the liquid lm becomes turbulent and the Labuntsov correlation can be applied. The most common ones are the Akers correlation modi ed by Cavallini and Zecchin (as presented by Cavallini et al [2]), the Boyko-Kruzhilin [3], and the Shah [4] correlations. Where the heat transfer coef cient of the liquid phase (a LO) is deduced from speci c correlations for forced convection and F is the enhancement factor
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