The threat of chemical and biological terrorism: preparing a response

When a deadly contaminant is released in a city, the window of time for meaningful response is brief. High-performance computing can play a major role in preparing an effective response. This article describes one such effort, which exploits detailed 3D computational fluid dynamics simulations of the airflow in buildings and cities.

[1]  Bohdan Z. Cybyk Coupling of external winds and recirculations with interior contaminant release modeling , 2000 .

[2]  Alexandra Landsberg,et al.  Analysis of the nonlinear coupling effects of a helicopter downwash with an unsteady ship airwake , 1995 .

[3]  Jay P. Boris,et al.  Simulation of Fluid Dynamics Around Complex Urban Geometries , 2001 .

[4]  M. J. Dwyer,et al.  Turbulent kinetic energy budgets from a large-eddy simulation of airflow above and within a forest canopy , 1997 .

[5]  J. Hunt,et al.  Kinematical studies of the flows around free or surface-mounted obstacles; applying topology to flow visualization , 1978, Journal of Fluid Mechanics.

[6]  A. Robins,et al.  The flow around a surface-mounted cube in uniform and turbulent streams , 1977, Journal of Fluid Mechanics.

[7]  Jay P. Boris,et al.  Flux-corrected transport. I. SHASTA, a fluid transport algorithm that works , 1973 .

[8]  S. T. Chan,et al.  A Model for Flow and Dispersion Around Buildings and Its Validation Using Laboratory Measurements , 2000 .

[9]  F. Grinstein,et al.  Large Eddy simulation of high-Reynolds-number free and wall-bounded flows , 2002 .

[10]  Charles A. Lind,et al.  A detailed contaminant transport model for facility hazard assessment in urban areas , 1999 .

[11]  J. P. Boris,et al.  New insights into large eddy simulation , 1992 .

[12]  Joel H. Ferziger,et al.  Status of Large Eddy Simulation: Results of a Workshop , 1997 .

[13]  F. Grinstein,et al.  Monotonically integrated large eddy simulation of free shear flows , 1999 .

[14]  Tomoyasu Nakagawa,et al.  On the SHASTA FCT Algorithm for the Equation ∂ρ ∂t + ∂ ∂x (υ(ρ)ρ) = 0 , 1979 .

[15]  William H. Snyder,et al.  A Comparison of Numerical and Physical Modeling of Stable Atmospheric Flow and Dispersion around a Cubical Building , 1996 .

[16]  W. Rodi,et al.  Calculation of the flow past a surface-mounted cube with two-layer turbulence models , 1997 .

[17]  Tomoyasu Nakagawa,et al.  On the SHASTA FCT algorithm for the equation ∂/∂+(∂/∂)(())=0 , 1979 .

[18]  C. Tropea,et al.  The Flow Around Surface-Mounted, Prismatic Obstacles Placed in a Fully Developed Channel Flow (Data Bank Contribution) , 1993 .

[19]  Elaine S. Oran,et al.  Numerical Simulation of Reactive Flow , 1987 .

[20]  William C. Sandberg,et al.  DDG-51 FLT-IIA Airwake Study Part 3: Temperature Field Analysis for Baseline and Upgrade Configurations , 2000 .

[21]  C. J. Apelt,et al.  Simulation of flow past a cube in a turbulent boundary layer , 1990 .

[22]  Elaine S. Oran,et al.  LCPFCT-A Flux-Corrected Transport Algorithm for Solving Generalized Continuity Equations , 1993 .

[23]  J. Boris,et al.  Solution of continuity equations by the method of flux-corrected transport , 1976 .