2011
DOI: 10.1007/s10546-011-9654-9
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A Study of the Stable Boundary Layer Based on a Single-Column K-Theory Model

Abstract: We document numerical experiments with a single-column, high-resolution model of the stable boundary layer. The model resolves the logarithmic layer, and does not require inverting the Monin-Obukhov similarity functions in order to calculate the surface fluxes. The turbulence closure is based on the K-theory approach, with a new form of stability functions of the Richardson number, evaluated by using the Surface Heat Budget of the Arctic Ocean (SHEBA) and the Cooperative Atmosphere-Surface Exchange Study (CASE… Show more

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Cited by 15 publications
(6 citation statements)
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“…Figure 5 shows the vertical profiles of wind speed and direction, as well as of u and the potential temperature. The structure of the stable boundary layer over sea ice has already been considered in a number of idealized studies, which used the GABLS I scenario as a reference (e.g., [30,[38][39][40]). The profiles shown in Figure 5 were in a good agreement with results obtained in the earlier studies, e.g., with respect to the ABL height and the surface cross-isobar angle, and will not be discussed here in much detail.…”
Section: Single-column Modelingmentioning
confidence: 99%
“…Figure 5 shows the vertical profiles of wind speed and direction, as well as of u and the potential temperature. The structure of the stable boundary layer over sea ice has already been considered in a number of idealized studies, which used the GABLS I scenario as a reference (e.g., [30,[38][39][40]). The profiles shown in Figure 5 were in a good agreement with results obtained in the earlier studies, e.g., with respect to the ABL height and the surface cross-isobar angle, and will not be discussed here in much detail.…”
Section: Single-column Modelingmentioning
confidence: 99%
“…where H is the domain height. The initial profile of the potential temperature is constant Θ 0 = 300 K up to a certain height H c = 200 m and then increases according to the dry adiabatic lapse rate Γ = 0.01 K m 1 as used by Sorbjan (2012):…”
Section: Initial and Boundary Conditionsmentioning
confidence: 99%
“…Profiles of the Richardson Ri are depicted in Fig 3, and typically, Ri is small near the surface and increases with height (Sorbjan 2012). According to Sorbjan (2010), thermal stability in the stable boundary layer differs for individual layers, and can be classified based on the local values of the Richardson number.…”
Section: Potential Temperature and Wind Profilesmentioning
confidence: 99%