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An Improved Perturbation Pressure Closure for Eddy-Diffusivity Mass-Flux Schemes
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  • Jia He,
  • Yair Cohen,
  • Ignacio Lopez-Gomez,
  • Anna Jaruga,
  • Tapio Schneider
Jia He
California Institute of Technology, California Institute of Technology

Corresponding Author:[email protected]

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Yair Cohen
California Institute of Technology, California Institute of Technology
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Ignacio Lopez-Gomez
California Institute of Technology, California Institute of Technology
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Anna Jaruga
Caltech, Caltech
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Tapio Schneider
California Institute of Technology, California Institute of Technology
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Abstract

Convection parameterizations such as eddy-diffusivity mass-flux (EDMF) schemes require a consistent closure formulation for the perturbation pressure, which arises in the equations for vertical momentum and turbulence kinetic energy (TKE). Here we derive an expression for the perturbation pressure from approximate analytical solutions for 2D and 3D rising thermal bubbles. The new closure combines a modified pressure drag and virtual mass effects with a new momentum advection term. This momentum advection is an important source in the lower half of the thermal bubble and at cloud base levels in convective systems. It represents the essential physics of the perturbation pressure, that is, to ensure the 3D non-divergent properties of the flow. Moreover, the new formulation modifies the pressure drag to be inversely proportional to updraft depth. This is found to significantly improve simulations of the diurnal cycle of deep convection, without compromising simulations of shallow convection. It is thus a key step toward a unified scheme for a range of convective motions. By assuming that the pressure only redistributes TKE between plumes and the environment, rather than vertically, a closure for the velocity pressure-gradient correlation is obtained from the perturbation pressure closure. This novel pressure closure is implemented in an extended EDMF scheme and is shown to successfully simulate a rising bubble test case as well as shallow and deep convection cases in a single column model.