4.4 Article

Effects of Horizontal and Vertical Grid Spacing on Mixing in Simulated Squall Lines and Implications for Convective Strength and Structure

Journal

MONTHLY WEATHER REVIEW
Volume 143, Issue 11, Pages 4355-4375

Publisher

AMER METEOROLOGICAL SOC
DOI: 10.1175/MWR-D-15-0154.1

Keywords

Circulation; Dynamics; Deep convection; Turbulence; Mathematical and statistical techniques; Numerical analysis; modeling; Models and modeling; Mesoscale models

Funding

  1. Advanced Study Program at the National Center for Atmospheric Research (NCAR)
  2. National Oceanic and Atmospheric Administration's Climate Goal funding
  3. U. S. DOE ASR [DE-SC0008648]
  4. NASA [NNX14AO85G]
  5. NSF Science and Technology Center for Multiscale Modeling of Atmospheric Processes (CMMAP) [ATM-0425247]
  6. National Science Foundation
  7. NASA [675166, NNX14AO85G] Funding Source: Federal RePORTER
  8. U.S. Department of Energy (DOE) [DE-SC0008648] Funding Source: U.S. Department of Energy (DOE)

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The sensitivity of an idealized squall line to horizontal Delta(h) and vertical Delta(v) grid spacing is investigated using a new approach. Simulations are first performed at a horizontal grid spacing of 1 km until the storm reaches its mature stage. The model output is then interpolated to smaller (and larger) grid spacings, and the model is restarted using the interpolated state plus small thermodynamic perturbations to spin up small-scale motions. This framework allows an investigation of the sensitivity of the storm to changes in Delta(h) without complications from differences in storm initiation and early evolution. The restarted simulations reach a quasi steady state within approximately 1 h. Results demonstrate that there are two Delta(h)-dependent regimes with the transition between regimes occurring for Delta(h) between 250 and 500 m. Some storm characteristics, such as the mean convective core area, change substantially for Delta(h) >250 m but show limited sensitivity as Dh is decreased below 250 m, despite better resolving smaller-scale turbulent motions. This transition is found to be independent of the chosen Dy. Mixing in the context of varying Delta(h) and Delta(v) is also investigated via passive tracers that are initialized 1 h after restarting the simulations (i. e., after the spin up of small-scale motions). The tracer field at the end of the simulations reveals that entrainment and detrainment are suppressed in the simulations with Delta(h) >= 500 m. For decreasing Delta(h), entrainment and detrainment are substantially more important, limiting the flux of low-level tracer to the upper troposphere, which has important implications for modeling studies of convective transport from the boundary layer through the troposphere.

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