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首页> 外文期刊>Journal of Geophysical Research. Biogeosciences >Supply-limited horizontal sand drift at an ephemerally crusted, unvegetated saline playa
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Supply-limited horizontal sand drift at an ephemerally crusted, unvegetated saline playa

机译:在有表壳,无植被的盐碱滩上的供应有限的水平沙流

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A site at Owens Dry Lake was observed for more than 4 years. The site was a vegetation-free saline playa where the surface formed "ephemeral crusts," crusts that form after rainfall. Sometimes these crusts were destroyed arid often a layer of particles on the crust would engage in vigorous aeolian activity. Three "phases" of active sand drifting are defined as almost no movement (extreme supply limitation), loose particles on crust with some degree of sand drift (moderate supply limitation), and unlimited source movement corresponding to a destroyed surface crust (unlimited supply). These "phases" occurred 45, 49, and 6% of the time, respectively. The accumulation of loose particles on the crust was mostly the result of in situ formation. Crusted sediments with loose particles on top can exhibit mass flux rates about the same as for noncrusted sediments. Crusted sediments limit or eliminate sand drift in two conditions: for rough crusts that effect a sufficiently high threshold friction velocity (above the wind friction velocity) and for limited amounts of loose particles on the crust where particle supply is less than would be transported in normal saltation for a thick sandy surface. These "supply-limited" cases are similar to wind erosion of limited spilled material on a hard concrete surface. We quantified "Supply limitation" by defining a "potential" or "supply unlimited" sand drift function Q = AG where A represents supply limitation that decreases as the particle source is depleted. Here Q is the mass of sand transported through a surface perpendicular to the ground and to the wind and having unit width during time period t, and G = integral u(*)(u(*)(2) - u(*t)(2)) dt for u(*) > u(*t). G is integrated for the same time period t as for Q, u(*) is the friction velocity of the wind, and u(*t) is the threshold friction velocity of the wind. Hard crusts (usually formed in the summer) tended to show almost no change of threshold friction velocity with time and often gave total protection from wind erosion. Rough crusts provided sufficient protection expressed as high threshold friction velocities. For these high threshold friction velocities, aeolian activity was greatly reduced or practically prevented. The softest crusts, usually formed in the winter, provided much less protection and sometimes were destroyed by the wind. Following this destruction the "potential" or "supply unlimited" sand drift would be observed. [References: 23]
机译:观察到欧文斯干旱湖的一个地点已有4年以上。该地点是一个无植被的盐滩,其表面形成了“短暂结皮”,结皮是在降雨后形成的。有时这些地壳会被破坏,并且经常会在地壳上形成一层颗粒,从而引起剧烈的风沙活动。活跃的砂流的三个“阶段”定义为几乎没有运动(极端的供应限制),地壳上的松散颗粒具有一定程度的砂漂移(中等的供应限制)以及与被破坏的地壳相对应的无限的源运动(无限的供应) 。这些“阶段”分别出现在45、49和6%的时间上。松散的颗粒在地壳上的堆积主要是原位形成的结果。顶部有疏松颗粒的结壳沉积物的质量通量率与未结壳沉积物的质量通量率大致相同。结垢的沉积物可在两种情况下限制或消除砂粒的漂移:对于产生足够高的阈值摩擦速度(高于风摩擦速度)的粗糙结壳,以及在结壳上有限数量的松散颗粒(颗粒供应少于正常输送)的情况盐渍可形成厚厚的沙质表面。这些“供应受限”的情况类似于硬质混凝土表面上有限的溢出物料的风蚀。我们通过定义“潜在”或“无限供应”的沙粒漂移函数Q = AG来量化“供应限制”,其中A表示随着颗粒源耗尽而减少的供应限制。此处Q是在时间段t内通过垂直于地面并垂直于风且表面具有单位宽度的表面传输的沙的质量,G =积分u(*)(u(*)(2)-u(* t) (2))dt表示u(*)> u(* t)。 G在与Q相同的时间段t内积分,u(*)是风的摩擦速度,而u(* t)是风的阈值摩擦速度。硬皮(通常在夏季形成)往往没有显示出阈值摩擦速度随时间变化几乎没有变化,并且经常提供全面的保护以防风蚀。粗糙的外壳提供了足够的保护,表现为高阈值摩擦速度。对于这些高阈值摩擦速度,极大地降低了或实际上阻止了风活动。通常在冬天形成的最软的硬皮提供的保护作用少得多,有时被风破坏。破坏之后,将观察到“潜在的”或“供应无限的”沙子漂移。 [参考:23]

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