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Thermal Food Processing

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Modeling <strong>Thermal</strong> <strong>Processing</strong> Using Computational Fluid Dynamics (CFD) 145<br />

colder and the wall of the cylindrical section is heated (the top may also be<br />

heated), then the circulation should start from the hot side wall surface and<br />

move up to the top due to buoyancy effect, and then drop down to the lower<br />

region due to the gravity effect. As such, when all the sides are heated, including<br />

the bottom plate, there are at least two recirculation regions that compete<br />

against each other, forming the pattern shown in Figure 5.3c. For different<br />

physical properties of the fluid of concern, and the variation in the height-todiameter<br />

ratio, the ratio of the size of the side region circulation to that of the<br />

bottom region should vary.<br />

The above interpretation is schematically shown in Figure 5.3 and Figure 5.4.<br />

Figure 5.5 clearly shows how the velocity generated affects the location of the<br />

lowest temperature region (SHZ or CZ).<br />

As is evident in Figure 5.4, the main fluid flow pathway corresponds nicely<br />

to the whereabout of the coldest zone. Figure 5.5 shows more explicitly such a<br />

phenomenon, while the effect of natural convection may be grossly viewed in a<br />

one-dimensional manner, i.e., a one-dimensional heat transfer affected by an<br />

overall downward fluid (at a velocity generated due to natural convection effect)<br />

(see Figure 5.6). This velocity is determined by the Grashof (Gr) number and<br />

Prandtl (Pr) number. 27<br />

y=H<br />

y=0<br />

y<br />

Fluid in<br />

Fluid out<br />

FIGURE 5.6 An equivalent one-dimensional system simulating the effect of natural convection<br />

on the development of SHZ or CZ (X.D. Chen, unpublished results, 2004).<br />

V<br />

T CP<br />

T w<br />

T w

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