2017
DOI: 10.1134/s0001433817050103
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The influence of the spatial heterogeneity of vegetation cover and surface topography on vertical CO2 fluxes within the atmospheric surface layer

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Cited by 7 publications
(3 citation statements)
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“…To describe the spatial distribution of GHG concentrations within the atmospheric boundary layer over a non-uniform surface, a 3D hydrodynamic model of turbulent GHG transfer in the atmospheric boundary layer has been implemented [15]. It is based on the E-ω closure scheme [16][17][18] of the averaged Navier-Stokes equation, the continuity equation and the 'diffusion-advection' equation for the transfer of GHGs [19][20][21][22]. In this study we use a modified version of a previously developed 3D hydrodynamic model [15,23] to describe the airflow distribution over the area with complex topography and vegetation.…”
Section: Formulation Of the Full Forward Problem For Ghg Concentratio...mentioning
confidence: 99%
“…To describe the spatial distribution of GHG concentrations within the atmospheric boundary layer over a non-uniform surface, a 3D hydrodynamic model of turbulent GHG transfer in the atmospheric boundary layer has been implemented [15]. It is based on the E-ω closure scheme [16][17][18] of the averaged Navier-Stokes equation, the continuity equation and the 'diffusion-advection' equation for the transfer of GHGs [19][20][21][22]. In this study we use a modified version of a previously developed 3D hydrodynamic model [15,23] to describe the airflow distribution over the area with complex topography and vegetation.…”
Section: Formulation Of the Full Forward Problem For Ghg Concentratio...mentioning
confidence: 99%
“…where C µ is a dimensionless numerical parameter and the functions E and ω = ε/E satisfy the following equations of the "diffusion-reaction-advection" type [15,32,33]:…”
Section: Airflow Modelmentioning
confidence: 99%
“…The values of E and ε are found from the system of differential equations (Sogachev and Panferov 2006;Mukhartova et al 2017;Olchev et al 2017): where φ (φ=ε•E -1 ) is the supplemented function characterizing the scale of turbulence. The dimensionless constants σ E =σ φ =2 introduce the Prandtl number for turbulent…”
Section: Data Post-processingmentioning
confidence: 99%