An adaptive discontinuous Galerkin method for modeling cumulus clouds

Theoretical understanding and numerical modeling of atmospheric moist convection still pose great challenges to meteorological research. The present work addresses the following question: How important is mixing between cloudy and environmental air for the development of a cumulus cloud? A Direct Numerical Simulation of a single cloud is way beyond the capacity of today’s computing power. The use of a Large Eddy Simulation in combination with semi-implicit time-integration and adaptive techniques offers a significant reduction of complexity. So far this work is restricted to dry flow in two-dimensional geometry. The compressible Navier-Stokes equations are discretized using a discontinuous Galerkin method introduced by Giraldo and Warburton in 2008. Time integration is done by a semi-implicit backward difference. For the first time we combine these numerical methods with an h-adaptive grid refinement. This refinement of our triangular grid is implemented with the function library AMATOS and uses a space filling curve approach. Validation through different test cases shows very good agreement between the current results and those from the literature. For comparing different adaptivity setups we developed a new qualitative error measure for the simulation of warm air bubbles. With the help of this criterion we show that the simulation of a rising warm air bubble on a locally refined grid can be more than six times faster than a similar computation on a uniform mesh with the same accuracy.

[1]  Francis X. Giraldo,et al.  A Conservative Discontinuous Galerkin Semi-Implicit Formulation for the Navier-Stokes Equations in Nonhydrostatic Mesoscale Modeling , 2009, SIAM J. Sci. Comput..

[2]  Francis X. Giraldo,et al.  A high‐order triangular discontinuous Galerkin oceanic shallow water model , 2008 .

[3]  J. Wyngaard,et al.  Resolution Requirements for the Simulation of Deep Moist Convection , 2003 .

[4]  Francis X. Giraldo,et al.  A study of spectral element and discontinuous Galerkin methods for the Navier-Stokes equations in nonhydrostatic mesoscale atmospheric modeling: Equation sets and test cases , 2008, J. Comput. Phys..

[5]  H. Jonker,et al.  Subsiding Shells Around Shallow Cumulus Clouds , 2008 .

[6]  Natalja Rakowsky,et al.  amatos: Parallel adaptive mesh generator for atmospheric and oceanic simulation , 2005 .

[7]  Chi-Wang Shu,et al.  Runge–Kutta Discontinuous Galerkin Methods for Convection-Dominated Problems , 2001, J. Sci. Comput..

[8]  Louis J. Wicker,et al.  Numerical solutions of a non‐linear density current: A benchmark solution and comparisons , 1993 .

[9]  B. Stevens,et al.  Buoyancy reversal in cloud‐top mixing layers , 2009 .

[10]  Rick Damiani,et al.  The Structure of Thermals in Cumulus from Airborne Dual-Doppler Radar Observations , 2006 .

[11]  Wojciech W. Grabowski,et al.  Cumulus entrainment, fine‐scale mixing, and buoyancy reversal , 1993 .

[12]  A. Robert Bubble Convection Experiments with a Semi-implicit Formulation of the Euler Equations , 1993 .

[13]  T. N. Stevenson,et al.  Fluid Mechanics , 2021, Nature.

[14]  D. Randall,et al.  Conditional instability of the first kind upside-down. [in stratocumulus clouds] , 1980 .

[15]  Wojciech W. Grabowski,et al.  Entrainment and mixing in buoyancy‐reversing convection with applications to cloud‐top entrainment instability , 1995 .

[16]  Hamid Johari,et al.  Mixing in Thermals with and without Buoyancy Reversal , 1992 .

[17]  Francis X. Giraldo,et al.  High‐order semi‐implicit time‐integrators for a triangular discontinuous Galerkin oceanic shallow water model , 2009 .

[18]  Stephen J. Lord,et al.  Maturity of Operational Numerical Weather Prediction: Medium Range , 1998 .