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The flow distribution through the perforated tiles is shown in the following figure. The horizontal air velocity decreases and
the pressure increases as one moves away from the CRAC units towards the center. The resistance to flow through a perforated tile is inversely proportional to its open area. Thus, by using tiles of decreasing
percentage open area, the resistance to flow through them increases with distance from the CRAC units. This counterbalances the increase in the pressure below the raised floor. Therefore, the resulting tile
flow distribution exhibits less nonuniformity than that in Case Study 1.
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