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52 E. Moryń-Kucharczyk and R. Gnatowska<br />

Fig. 9.4. Computational distributions of a) stream function b) amplitude of transverse<br />

velocity oscillations<br />

simulation mentioned above provided the mean velocity distributions as<br />

well as characteristics of turbulence structure around tandem arrangement.<br />

The special emphasize has been put on intensity of velocity oscillation in<br />

space around bluff-bodies. The sample results, shown in Fig. 9.4a present the<br />

instantaneous computational distributions of stream function corresponding<br />

to different dynamic states of the flow in body system environment. The centreline<br />

distributions of amplitude of transverse velocity oscillations are also<br />

juxtaposed in Fig. 9.4b. One may suppose that transport of pollutants is intensified<br />

by periodical velocity component, generated in flow around bluff-bodies<br />

arrangement, especially for the critical body spacing. In this case the maximum<br />

of concentration, move forwards in the centreline of the wake.<br />

9.3 Conclusions<br />

In an experimental study of bluff-bodies tandem arrangement the significant<br />

changes have been observed in the concentration field of the tracer gas for different<br />

spacing ratio. Depending on body spacing the maximum concentration<br />

of CO2 is localized outside of the gap (double peak) or migrates towards the<br />

centreline. The interbody gap is filled up by the emitted gas more intensively<br />

as the level of energy of oscillating velocity component increases (critical body<br />

spacing). The problem needs further studies.<br />

References<br />

1. Jar˙za J, Gnatowska R (2004) Lock-on effect on unsteady loading of rigid bluff -<br />

body in tandem arrangement. Proceedings of International Conference Urban<br />

<strong>Wind</strong> Engineering and Buildings Aerodynamics Cost C14. Rhode-St-Genese<br />

Belgium

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