2018
DOI: 10.1007/s13351-018-7185-8
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Effect of Mesoscale Land Use Change on Characteristics of Convective Boundary Layer: Semi-Idealized Large Eddy Simulations over Northwest China

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Cited by 3 publications
(4 citation statements)
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“…First, τ S at the oasis site is longer than that at the Gobi site (Figure 4, Table 4). This is because the SBL at the oasis site is influenced by the “oasis effect” (Chu et al ., 2005; Cao et al ., 2018). The evaporation of water will consume large amounts of solar radiation over the oasis site, while only a small fraction of energy will be used in the same way at the Gobi site.…”
Section: Resultsmentioning
confidence: 99%
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“…First, τ S at the oasis site is longer than that at the Gobi site (Figure 4, Table 4). This is because the SBL at the oasis site is influenced by the “oasis effect” (Chu et al ., 2005; Cao et al ., 2018). The evaporation of water will consume large amounts of solar radiation over the oasis site, while only a small fraction of energy will be used in the same way at the Gobi site.…”
Section: Resultsmentioning
confidence: 99%
“…However, in the arid and semi‐arid areas of China, there are many complex heterogeneous surfaces (Cao et al ., 2018; 2020; Liu et al ., 2011; Li et al ., 2013; Zhang et al ., 2016), including Gobi, desert, rural, and oasis areas, among others. The DTR should differ significantly over these surfaces, which may have different relationship with LW net24 .…”
Section: Introductionmentioning
confidence: 99%
“…Ref. [12] found that when soil moisture in oases approaches saturation, the secondary circulation (SC)/turbulent organized structure (TOS) is strongest/weakest. As the soil moisture content in the oasis decreases, SC (TOS) will become weaker (stronger).…”
Section: Introductionmentioning
confidence: 99%
“…In recent years, large-eddy simulation (LES) models have been developed to explicitly simulate heterogeneous land surface processes to provide the basis for the parameterization of land surface heterogeneity in large-scale models. In LES models (e.g., Deardorff, 1978;Moeng, 1984;Cao et al, 2018), turbulence is divided into grid-resolved large eddies and sub-grid eddies in the inertial subrange. The effects of sub-grid eddies are commonly quantified using a sub-grid closure scheme, such as the Smagorinsky closure (Smagorinsky, 1963) or the k-l closure (Deardorff, 1980).…”
mentioning
confidence: 99%