Oil mist transport process in a long pipeline on turbulent flow transition region |
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Affiliation: | 1. Pipeline Technology Center, Tokyo Gas Co., Ltd., 1-7-7 Suehiro-cho, Tsurumi-ku, Yokohama, 230-0045, Japan;2. Division of Energy & Environmental Systems, Faculty of Engineering, Hokkaido University, N13W8, Sapporo 060-8628, Japan;3. Department of Mechanical, Aerospace, and Materials Engineering, Muroran Institute of Technology, 27-1 Mizumoto-cho, Muroran, Hokkaido, 050-8585, Japan;4. School of Science and Engineering, Meisei University, 2-1-1, Hodokubo, Hino, Tokyo, 191-8506, Japan;1. Czestochowa University of Technology, Al. Armii Krajowej 21, Czestochowa 42-201, Poland;2. University of Twente, P.O. Box 217, 7500 AE Enschede, the Netherlands |
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Abstract: | Internal gas velocity fluctuations and their effects on the mist diffusion process were examined in a long horizontal pipe to understand oil mist transportation, particularly in the laminar-to-turbulent flow transition region. Three hot-wire anemometers and aerosol concentration monitors were used to deduce these effects as the two-phase mist flow gradually developed in the stream-wise direction. We found significant axial mist diffusion at Reynolds numbers (Re) < 1000 because of passive scalar transport by Poiseuille flow. However, this diffusion was restricted by the non-zero inertia of the mist at a Stokes number, O(10−5), relying on the Brownian motion of the mist. At Re > 2400, a sharp mist waveform was maintained by a turbulent flow with active radial mixing. New data were obtained within the range of 1000 < Re < 2400, which cannot be explained by interpolation between the above-mentioned two states. The mist concentration displays multiple temporal peaks at Re < 2000 owing to perturbations of localized turbulence as well as radial anisotropy as being conveyed more than 2000-diameters in distance. This behavior is caused by intermittent disturbances induced by the pipe wall roughness, which sharply distorts the wall-aligned laminar mist layer left by parabolic axial stretching of local laminar flow. |
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