%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% W. G. Pritchard Lab Seminar: 4:30-5:30 PM, 320 Whitmore Laboratory **Monday May 2, 2005** High Rayleigh number convection in a fluid saturated porous layer Charles Doering Dept of Mathematics University of Michigan Abstract: Thermal convection and fluid mechanics in a porous medium are relevant to a variety of phenomena ranging from groundwater flow and geothermal energy transport to the effectiveness of fiberglass insulation. In the research described here, the most basic model (the Darcy-Boussinesq equations at infinite Darcy-Prandtl number) is used to study convection and heat transport over a broad range of heating levels as measured by the nondimensional Rayleigh number Ra. High resolution direct numerical simulations are performed to explore the modes of convection and measure the heat transport as quantified by the Nusselt number Nu, the enhancement factor of total (conductive plus convective) heat flux over pure conduction alone. We present simulation results from onset at Ra=4 pi^2 up to Ra=10^4. Over an intermediate range of increasing Ra, the simulations display the `classical' (jargon to be explained) heat transport scaling. As the Rayleigh number is increased beyond Ra = 1255 we observe a sharp crossover to a form fit by Nu = .0174 Ra^{.9} over nearly a decade, up to the highest Ra accessible. Rigorous upper bounds on the high Rayleigh number heat transport have also been derived: they are of the classical scaling form with an explicit prefactor: Nu <= .0297 Ra. The bounds are compared directly to the results of the simulations as well as to real laboratory experiments. This is joint work with J. Otero, L. Dontcheva, H. Johnston, R. Worthing, A. Kurganov and G. Petrova; it is the content of a paper published in Journal of Fluid Mechanics (2004). %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%