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The liquid deposition fraction of sprays impinging vertical walls and flowing films
Affiliation:1. Department of Mathematics, Faculty of Science, Universiti Putra Malaysia, 43400 UPM Serdang, Selangor, Malaysia;2. Institute for Mathematical Research, Universiti Putra Malaysia, 43400 UPM Serdang, Selangor, Malaysia;3. School of Mathematical Sciences, Faculty of Science & Technology, Universiti Kebangsaan Malaysia, 43600 UKM Bangi, Selangor, Malaysia;4. Department of Mathematics, Babeş-Bolyai University, R-400084 Cluj-Napoca, Romania;1. Key Laboratory for Advanced Materials Processing of Ministry of Education, Institute of Advanced Materials and Technology, University of Science and Technology Beijing, Beijing 100083, PR China;2. Beijing Laboratory of Metallic Materials and Processing for Modern Transportation, University of Science and Technology Beijing, Beijing 100083, PR China;3. State Key Laboratory of Advanced Technologies for Comprehensive Utilization of Platinum Metals, Kunming Institute of Precious Metals, Kunming 650106, PR China;1. School of Materials Science and Engineering, Harbin Institute of Technology, Harbin 150001, China;2. National Key Laboratory Precision Hot Processing of Metals, Harbin Institute of Technology, Harbin 150001, China;1. South China Institute of Environmental Sciences, the Ministry of Environmental Protection of PRC, Guangzhou 510655, China;2. Department of Environmental Science, School of Environmental Science and Engineering, Sun Yat-sen University, Guangzhou 510275, China
Abstract:The impingement of coarse sprays with a mean diameter in the order of millimeters on vertical walls with and without an additionally supplied wall film was studied at conditions well below the Leidenfrost limit. The fraction of the sprayed liquid deposited on the wall was determined experimentally and theoretically for various impingement angles with the help of a flat fan spray directed against the wall. The deposition fraction shows a distinct minimum in the range of intermediate impingement angles. This fact cannot be described by single-droplet-based deposition-splash criteria when considering the droplet’s impact momentum alone. The investigation demonstrates that the measurement results can be explained by including the collision of splashed droplets with incoming ones. In principle, the entrainment of the primary spray’s fine fraction in the gas flow field may also be of relevance. For the coarse and relatively sparse sprays investigated, the importance of the collisions in determining the overall balance of deposited and splashed liquid was estimated by event statistics derived from Monte Carlo simulations. The main outcome of wall interaction for the coarse spray is splashing. The splashed droplets form a secondary spray. When the impingement angle is steep, the splashed liquid is redirected towards the wall as a result of the collision between the incoming primary spray and splashed droplets.
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