Peters, J. M., and R. S. Schumacher, 2015

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Peters, J. M., and R. S. Schumacher, 2015 The Simulated Structure and Evolution of a Quasi-Idealized Warm-Season Convective System with a Training Convective Line Professor : Ming-Jen Yang Student : Jyong-En Miao Date : 2015/12/24 Peters, J. M., and R. S. Schumacher, 2015 J. Atmos. Sci., 72, 1987-2010.

Introduction primary mechanism for heavy rainfall generation in MCS involves the continuous motion of individual convective elements within the larger convective system over a fixed geographic region Two processes—training and backbuilding Training involves a convective line comprised of smaller convective-scale updrafts that move in a line-parallel direction, resulting in their repeated motion over a fixed geographic region Backbuilding involves the repeated upstream redevelopment of convective updrafts, resulting in a near-zero net motion of the larger convective system

Introduction small spatial scales (of order 10–100 km) meso-a-to-synoptic scale(>200km)phenomena low-level warm-air advection convergence along the nose of a low-level jet a supply of low-level CAPE low-level frontal circulations upper-level jet streaks

Introduction isolated convective systems within an horizontally homogeneous thermodynamic and kinematic environment Mahoney et al. (2009) artificially constructed a zonal jet and associated baroclinic zone by varying the meridional tropospheric temperature (and thus the meridional pressure and wind fields ), while retaining zonal homogeneity.

Introduction Coniglio and Stensrud (2001) constructing a large-scale environment from composite atmospheric fields => both zonal and meridional inhomogeneity!

Experiment degign rotated principal component analysis (RPCA) synoptic type events (24 cases) warm season type events (26 cases) Time, forcing, traing&backbuilding, ROD Rearward Off-boundary Development

composite atmospheric progressions spatially centered at the location of the maximum 1-h precipitation accumulation and temporally centered at the time of the maximum 1-h accumulation.

Control simulation No microphysics simulation

Control simulation (CNTL) No microphysics simulation (NOMP) to assess the similarity between the simulated environment and that of the composites and later to define convective perturbation fields.

merry christmas and happy new year 2016