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PhD Thesis - staffweb - University of Greenwich

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<strong>PhD</strong> <strong>Thesis</strong> by John Ewer.using a 90 MHz Pentium PC with 64MB RAM. The first example involves a single compartmentwith two doors. Both doors open to the outside and hence involve two extended flow regions.The second example involves a similar compartment in which one door opens to the outsidewhile the other door opens to a second closed compartment. For simplicity, all confiningboundaries are assumed to be adiabatic. In both cases a small volumetric fire source <strong>of</strong> 50 kWis situated in the centre <strong>of</strong> the fire compartment.In the first example, one <strong>of</strong> the doors is open throughout the simulation while the second dooris opened 40 seconds into the fire simulation. The solution domain is thus made up <strong>of</strong> threedistinct regions, the first external region outside <strong>of</strong> the open door, the fire compartment itselfand the second external region beyond the closed door. The computational mesh in each regioncomprises <strong>of</strong> 8 x 21 cells, 22 x 21 cells and 8 x 21 cells respectively i.e. a total <strong>of</strong> 798 cells.Using standard CFD solution techniques the solvers operate equally in all <strong>of</strong> the cells throughoutthe solution domain, even the cells in the initially dormant external region beyond the closeddoor. This is clearly a waste <strong>of</strong> CPU time as nothing <strong>of</strong> significance occurs in the external regionbeyond the closed door.FIGURE 7.2.3-1 : Solution prior to opening <strong>of</strong> second doorobtained using conventional and groups solvers.7-107

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