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Handbook of air conditioning and refrigeration / Shan K

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duced ambient <strong>air</strong> at a comparatively higher pressure presses the <strong>air</strong> jet against the surface, even<br />

when it is a curved surface. Such a phenomenon is called the surface effect or the Conda effect.<br />

Friction between the <strong>air</strong> jet <strong>and</strong> the boundary decreases the centerline velocity <strong>of</strong> confined <strong>air</strong><br />

jets, as shown in Fig. 18.4. However, because <strong>of</strong> the surface effect, the throw <strong>of</strong> a confined <strong>air</strong> jet is<br />

longer, <strong>and</strong> the drop from the horizontal axis smaller, than that <strong>of</strong> a free <strong>air</strong> jet.<br />

Airflow Pattern. The flow pattern <strong>and</strong> characteristics <strong>of</strong> a confined <strong>air</strong> jet using a sidewall outlet<br />

were introduced by Russian scientists during the 1950s. In an <strong>air</strong> conditioned room whose supply<br />

outlet is located above the occupied zone <strong>and</strong> whose exhaust opening is on the same side <strong>of</strong> the supply<br />

outlet, the supply <strong>air</strong> jet clings to the surface <strong>of</strong> the ceiling <strong>and</strong> mixes with the room <strong>air</strong>. An induced<br />

reverse <strong>air</strong>stream, with more even velocity <strong>and</strong> temperature distribution than that <strong>of</strong> the <strong>air</strong><br />

jet, covers the occupied zone.<br />

Figure. 18.5 shows the <strong>air</strong>flow pattern <strong>of</strong> a typical confined isothermal jet. When supply <strong>air</strong> is discharged<br />

from the circular outlet <strong>and</strong> moves along the surface <strong>of</strong> the ceiling, the fluctuating velocity<br />

components continue to transport momentum across the boundary <strong>of</strong> the <strong>air</strong> jet. Therefore, ambient <strong>air</strong><br />

is induced into the <strong>air</strong> jet, <strong>and</strong> the induced circulating <strong>air</strong>flow occupies most <strong>of</strong> the enclosed space.<br />

As the <strong>air</strong> jet moves forward, its mass flow rate increases <strong>and</strong> mean <strong>air</strong> velocity decreases until it<br />

arrives at a cross-sectional plane where dimensionless distance s � 0.22. Term s is defined as<br />

s � (18.12)<br />

ax<br />

√0.5A r<br />

AIR SYSTEMS: SPACE AIR DIFFUSION 18.9<br />

where a � turbulence factor; for a circular nozzle a � 0.076, <strong>and</strong> for a rectangular outlet without<br />

guide vanes a � 0.15.<br />

FIGURE 18.5 Airflow pattern <strong>of</strong> a typical confined <strong>air</strong> jet.

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