Analysis, Geometry and Stochastics for Planet Earth Date: September 29, 2015 Location: Room Lyle G74 CDT-Suite, University of Reading Supported by: London Mathematical Society Institute and EPSRC-CDT Mathematics of Planet Earth Speaker: Prof Darryl Holm (Imperial College London) Title: “Stochastic Variational Principles for Geophysical Fluid Dynamics (GFD)” Abstract: Abstract: Suppose your data for a GFD system had some noisy-looking, complicated, small-scale motions (variability); but it also had some large-scale spatial correlations, as seen, for example, in the Figure below (courtesy of E Van Sebille, Grantham Institute, Imperial College) showing thirty years worth of satellite measurements of the paths of drifters in the Pacific Ocean in the region between Australia and New Zealand. How could you modify your deterministic basic GFD equations to incorporate into them the randomness and statistics you have seen in your data; so that numerical simulations of your modified GFD equations would reproduce the same sort of randomness and statistics as seen in your data? Hint: you would want to do it in an optimal way, so that some kind of variational principle would be needed, and you would need to constrain your variations to be consistent with the statistics of your data. This talk will discuss a mathematical approach via stochastic variational principles for solving such problems, in examples ranging from wobbling rotating bodies in classical mechanics, to realistic GFD models. Speaker: Dr Glenn Shutts (MetOffice) Title: "Physical parametrization of unresolved and partially-resolved phenomena in weather forecast models." Abstract: Current Numerical Weather Prediction (NWP) models have sufficiently fine grid meshes to be able to resolve the rotationally- and hydrostatically-balanced atmospheric flow that achieves the required energy and moisture transport from the tropics to the Polar Regions (i.e. planetary Rossby waves, cyclone waves and fronts). The success of NWP (mainly outside of the tropics) comes from the strong constraint placed upon large-scale airflows of the Earth's rotation and manifest in the geostrophic wind approximation and balanced forms of the potential vorticity (which determine the flow through elliptic equations). Theories of geostrophic turbulence explain the tendency for steep energy spectra (k^(-3) ) and for energy to be locked into the largest permissible scales on the planet for which solar forcing dominates. The transport of moisture takes place in narrow 'atmospheric rivers' ahead of cold fronts and it appears that gridlengths finer than 30 km are required to capture these. Unfortunately, this mathematically-elegant view leaves out a very important meteorological phenomenon that atmospheric physicists call 'convection' which takes the form of cumulus clouds of varying scale and intensity. They transport heat, moisture and momentum vertically through the buoyancy forces that accompany water phase changes (dominated by latent heat release in updraughts). These unbalanced motions are most unstable at horizontal scales of the order of 100 metres and limited by turbulence at smaller scales. Small cumulus clouds are composed of ensembles of these narrow convective plumes thereby giving them their cauliflower appearance. Severe convective storms have tilted airflows (in the vertical plane) that are organized so that hydrometeors (rain, snow, hail etc) fall into dry air and the resultant cooling due to evaporation and melting drives strong downdraughts. Some of the most intense convective storms occur in mid-latitudes and the associated upward transport of mass and subsequent horizontal spreading in the upper troposphere disturbs the position of jetstreams and creates pools of zero absolute vorticity. These Mesoscale Convective Systems (MCSs) are responsible for forecast errors since their updraughts are sub-grid-scale and so rely on a parametrized representation of their effect. The balanced flow picture of global atmospheric flows is also upset by the presence of mountain ranges. For the highest mountains, much of the airflow is around rather than over the mountain but the air that does flow over generates internal gravity waves that typically radiate their energy vertically upwards into the stratosphere. This wave motion is accompanied by a wave stress on the mountain and an opposite stress is transmitted upwards with the wave. The air that flows around the mountain may generate wakes and eddies which in turn cause a drag force on the mountain. These stresses/drag forces exert a powerful influence on the balanced flow and also require parametrization. Along with the representation of boundary layer turbulence and cloud microphysical processes, these parametrizations for convection and mountain waves are semi-empirical and assume a unique relationship between the statistical mean of the relevant process and the instantaneous state of a model grid column. My talk will reflect on the challenges of parametrization and forecast model improvement. Speaker: Caroline Muller (Ecole Polytechnique) Title: Spatial organization of clouds in the tropical atmosphere Abstract: Clouds have been recognized as a key source of uncertainty for climate predictions. In particular, cloud feedbacks are responsible for a large fraction of the intermodel scatter in climate sensitivity. One source of uncertainty is the spatial distribution of deep convection, and its response to warming. We will analyze the properties of deep convection in idealized high-resolution simulations of homogeneous radiative-convective equilibrium. The numerical results will be linked to theoretical expectations based on the physics of clouds. We will also compare the numerical and theoretical results to observations of deep clouds over the tropical oceans. Under certain conditions, the homogeneous radiative-convective equilibrium has been shown to be unstable to large-scale overturning circulations. The resulting new equilibrium is a spatially organized atmosphere composed of two distinct areas: a moist area with intense convection, and a dry area with strong radiative cooling. In nature, the organized state can take the form of cloud clusters or tropical cyclones. We will investigate the physical processes responsible for the spontaneous organization of deep clouds.
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