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Dataset . 2023
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MetUM Simulations of 2nd February Case Study

Authors: Saffin, Leo; Lock, Adrian;

MetUM Simulations of 2nd February Case Study

Abstract

This repository contains data to support the publication "Kilometre-scale simulations of trade-wind cumulus capture processes of mesoscale organization" submitted to JAMES. The data is from Met Office Unified Model simulations of the 2nd February 2020 EUREC4A case study. There are 3 kilometre-scale resolutions (1.1km, 2.2km, 4.4km) nested in ERA5 boundary conditions, and two 100m-scale resolutions (300m, 500m) nested in the 1.1km simulation. The simulations are initialised at 1st February 00:00. Also included are two sensitivity tests with the kilometre-scale simulations run with 1) evaporation of rain switched off and 2) a later start time (2nd February 00:00). The code used to analyse this data is at https://github.com/leosaffin/moisture_tracers. The data is across four folders (full directory structure at the bottom) regridded - Contains model data regridded to the lowest resolution (4.4km) either fixed on the 100m-scale domain (coarse_grid) or following a Lagrangian trajectory for the kilometre-scale resolutions and sensitivity tests (lagrangian_grid). There are also files with model data following a different trajectory and smaller domain, to be consistent with Narenpitak et al. (2021), for the default kilometre-scale simulations (lagrangian_grid_Ron_Brown). trajectories - Contains all the trajectories used to extract the domains in "regridded" simulated_satellite - Contains model simulated brightness temperatures from 11Z-21Z for each resolution simulation. These simulations were run with the same setup but on a different machine and also include a 150m-resolution simulation. full_grid - Contains 2d model output a T+36 from the 500m and 1.1km simulations which were used to make figure 1 in the paper. Full directory structure: full_grid D100m_500m model-diagnostics_20200201T0000_T+35.nc km1p1 model-diagnostics_20200201T0000_T+35.nc regridded D100m_300m coarse_grid 20200201T0000_D100m_300m_T+{24..48}_coarse_grid.nc D100m_500m coarse_grid 20200201T0000_D100m_500m_T+{24..48}_coarse_grid.nc km1p1 coarse_grid 20200201T0000_km1p1_T+{24..48}_coarse_grid.nc lagrangian_grid 20200201T0000_km1p1_T+{01..48}_lagrangian_grid.nc 20200202T0000_km1p1_T+{01..24}_lagrangian_grid.nc lagrangian_grid_no_evap 20200201T0000_km1p1_T+{24..48}_lagrangian_grid_no_evap.nc lagrangian_grid_Ron_Brown 20200201T0000_km1p1_T+{24..48}_lagrangian_grid_Ron_Brown.nc km2p2 coarse_grid 20200201T0000_km2p2_T+{24..48}_coarse_grid.nc lagrangian_grid 20200201T0000_km2p2_T+{24..48}_lagrangian_grid.nc 20200202T0000_km2p2_T+{01..24}_lagrangian_grid.nc lagrangian_grid_no_evap 20200201T0000_km2p2_T+{24..48}_lagrangian_grid_no_evap.nc lagrangian_grid_Ron_Brown 20200201T0000_km2p2_T+{24..48}_lagrangian_grid_Ron_Brown.nc km4p4 coarse_grid 20200201T0000_km4p4_T+{24..48}_coarse_grid.nc lagrangian_grid 20200201T0000_km4p4_T+{24..48}_lagrangian_grid.nc 20200202T0000_km4p4_T+{01..24}_lagrangian_grid.nc lagrangian_grid_no_evap 20200201T0000_km4p4_T+{24..48}_lagrangian_grid_no_evap.nc lagrangian_grid_Ron_Brown 20200201T0000_km4p4_T+{24..48}_lagrangian_grid_Ron_Brown.nc regridded_large_scale km1p1 lagrangian_grid 20200201T0000_km1p1_T+{24..48}_lagrangian_grid_large_scale.nc 20200202T0000_km1p1_T+{01..24}_lagrangian_grid_large_scale.nc lagrangian_grid_no_evap 20200201T0000_km1p1_T+{24..48}_lagrangian_grid_no_evap_large_scale.nc lagrangian_grid_Ron_Brown 20200201T0000_km1p1_T+{24..48}_lagrangian_grid_Ron_Brown_large_scale.nc km2p2 lagrangian_grid 20200201T0000_km2p2_T+{24..48}_lagrangian_grid_large_scale.nc 20200202T0000_km2p2_T+{01..24}_lagrangian_grid_large_scale.nc lagrangian_grid_no_evap 20200201T0000_km2p2_T+{24..48}_lagrangian_grid_no_evap_large_scale.nc lagrangian_grid_Ron_Brown 20200201T0000_km2p2_T+{24..48}_lagrangian_grid_Ron_Brown_large_scale.nc km4p4 lagrangian_grid 20200201T0000_km4p4_T+{24..48}_lagrangian_grid_large_scale.nc 20200202T0000_km4p4_T+{01..24}_lagrangian_grid_large_scale.nc lagrangian_grid_no_evap 20200201T0000_km4p4_T+{24..48}_lagrangian_grid_no_evap_large_scale.nc lagrangian_grid_Ron_Brown 20200201T0000_km4p4_T+{24..48}_lagrangian_grid_Ron_Brown_large_scale.nc simulated_satellite UMRA3p3_MOapp_20200201T0000Z_HMscale_2D_Hourly_150m_Baseline_goes16_brt.nc UMRA3p3_MOapp_20200201T0000Z_HMscale_2D_Hourly_300m_Baseline_goes16_brt.nc UMRA3p3_MOapp_20200201T0000Z_HMscale_2D_Hourly_500m_Baseline_goes16_brt.nc UMRA3p3_MOapp_20200201T0000Z_KMscale_2D_Hourly_1p1km_Baseline_goes16_brt.nc UMRA3p3_MOapp_20200201T0000Z_KMscale_2D_Hourly_2p2km_Baseline_goes16_brt.nc UMRA3p3_MOapp_20200201T0000Z_KMscale_2D_Hourly_4p4km_Baseline_goes16_brt.nc trajectories trajectories_20200201_km1p1_500m.pkl trajectories_20200201_km2p2_500m.pkl trajectories_20200201_km4p4_500m.pkl trajectories_20200201_km1p1_500m_no_evap.pkl trajectories_20200201_km2p2_500m_no_evap.pkl trajectories_20200201_km4p4_500m_no_evap.pkl trajectories_20200201_km1p1_500m_Ron_Brown.pkl trajectories_20200201_km2p2_500m_Ron_Brown.pkl trajectories_20200201_km4p4_500m_Ron_Brown.pkl trajectories_20200202_km1p1_500m.pkl trajectories_20200202_km2p2_500m.pkl trajectories_20200202_km4p4_500m.pkl

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This indicator reflects the "current" impact/attention (the "hype") of an article in the research community at large, based on the underlying citation network.
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This indicator reflects the overall/total impact of an article in the research community at large, based on the underlying citation network (diachronically).
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