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The blown sand flux over a sandy surface: a wind tunnel investigation on the fetch effect
Institution:1. Department of Health and Environmental Sciences, Xi''an Jiaotong-Liverpool University, Suzhou, Jiangsu 215123, China;2. School of Environmental Sciences, University of Liverpool, Liverpool L69 7ZT, UK;3. Department of Geography, University of South Carolina, Columbia, SC 29208, USA;1. Department of Soil Science, Faculty of Agriculture, University of Shahrekord, Shahrekord, Iran;2. Department of Soil Science, Faculty of Agriculture, Vali–e–Asr University of Rafsanjan, Rafsanjan, Iran;1. Department of Health and Environmental Sciences, Xi’an Jiaotong-Liverpool University, Suzhou, China;2. School of Environmental Sciences, University of Liverpool, Liverpool, UK;3. Third Institute of Oceanography, Ministry of Natural Resources, Xiamen, China;4. College of Marine Geosciences, Ocean University of China, Qingdao, China;1. Key Laboratory of Water Cycle and Related Land Surface Processes, Institute of Geographic Sciences and Natural Resources Research, Chinese Academy of Sciences, Beijing 100101, China;2. University of Chinese Academy of Sciences, Beijing 100049, China
Abstract:Detailed wind tunnel tests were conducted to examine the fetch effect of a sandy surface on a sand cloud blowing over it. The results suggest that the fetch length of a sandy surface has a significant effect on both the vertical flux profile and total horizontal flux. The sand flux over a sandy surface increases with height in the very near surface layer, but then decays exponentially. In agreement with the widely accepted conclusion, the decay function can be expressed by q=aexp(−h/b), where q is the sand flux at height h. Coefficient a that tends to increase with wind speed implies the influence of wind, while coefficient b that defines the relative decay rate shows the influence of both the fetch and wind. The relative decay rate increases with fetch when the fetch length is short, then becomes constant when the fetch reaches a certain length. The threshold fetch length over which the relative decay rate keeps constant increases with wind speed. The average saltation height generally increases with fetch. Both the relative decay rate and average saltation height show that the fetch effect on the flux profile becomes more significant when the wind speed increases. The total sand transport equation for the total fetch can be expressed by Q=C(1−Ut/U)2U3(ρ/g), where Q is the total sand transport rate, U and Ut are the wind velocity and threshold wind velocity at the centerline height of the wind tunnel, respectively, g is gravitational acceleration, ρ is the density of air, and C is a proportionality coefficient that increases with the fetch length, implying that the total sand flux increases with the fetch length.
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