Modeling and simulation of dense cloud dispersion in urban areas by means of computational fluid dynamics.

The formation of toxic heavy clouds as a result of sudden accidental releases from mobile containers, such as road tankers or railway tank cars, may occur inside urban areas so the problem arises of their consequences evaluation. Due to the semi-confined nature of the dispersion site simplified models may often be inappropriate. As an alternative, computational fluid dynamics (CFD) has the potential to provide realistic simulations even for geometrically complex scenarios since the heavy gas dispersion process is described by basic conservation equations with a reduced number of approximations. In the present work a commercial general purpose CFD code (CFX 4.4 by Ansys(®)) is employed for the simulation of dense cloud dispersion in urban areas. The simulation strategy proposed involves a stationary pre-release flow field simulation followed by a dynamic after-release flow and concentration field simulations. In order to try a generalization of results, the computational domain is modeled as a simple network of straight roads with regularly distributed blocks mimicking the buildings. Results show that the presence of buildings lower concentration maxima and enlarge the side spread of the cloud. Dispersion dynamics is also found to be strongly affected by the quantity of heavy-gas released.

Growth patterns and gravitropic curvature of radish hypocotyls.

The rapid growth rate of radish cells makes the hypocotyl particularly valuable in research on growth phenomena and gravitropism. An examination of mean data regarding the growth of aetiolated radish seedlings not subjected to gravitropic stimulation showed that there was an increase in the growth rate from day 3 to day 5. When the hypocotyl was placed horizontally all zones showed an increase in growth of the lower surface of the hypocotyl and generally a decrease in the growth rate in the upper surface. The upper apical part of the gravistimulated hypocotyl grew almost the same as controls. In some cases, in both 4- and 5-day-old seedlings, in the upper median part there was a lower growth rate than in controls. The zones of growth during the development of the hypocotyl were different. Analysis of curvature showed that the growth rate of the different zones was a function of their location in the hypocotyl and that the rate of curvature was different in various parts of the hypocotyl.