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Prediction of batch heat transfer coefficients for pseudoplastic fluids ...

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29<br />

In both Newtonian and non-Newtoni~D<br />

<strong>fluids</strong> the shear<br />

rates flere found to be directly proportional to the agitator<br />

speed.<br />

There seemed to be an impeller diameter effect 'tv-hich<br />

was greater <strong>for</strong> Newtonian than <strong>for</strong> non-Newtonian <strong>fluids</strong>.<br />

The shear rate at a given distance from the impeller is<br />

slightly greater as the impeller diameter is increased.<br />

For dilatant <strong>fluids</strong> the effect might be even greater.<br />

In the laminar region (NR~ - 7.0) the al110Ullt <strong>of</strong> fluid<br />

movement is much greater <strong>for</strong> Ne1-vtonian <strong>fluids</strong> than <strong>for</strong> the<br />

<strong>pseudoplastic</strong>s at the same rotational speed, a.nd flO1~<br />

extends<br />

almost to the periphery <strong>of</strong> the tank <strong>for</strong> the NevJtonians<br />

vJhile flow is circular and is confined to the region <strong>of</strong><br />

the impeller <strong>for</strong> the non-Newtonian <strong>fluids</strong>.<br />

In the first half <strong>of</strong> the transition region (NR~<br />

about<br />

10.3) fluid turnover begins <strong>for</strong> the Ne,-vtonian <strong>fluids</strong> and<br />

mixing is carried out by the transport and blending.<br />

The<br />

radial veloci ty increases 14i th rotational speed quite<br />

rapidly. However, <strong>for</strong> the <strong>pseudoplastic</strong>s the movement is<br />

still confined to the center and does not extend to the<br />

edges <strong>of</strong> the baffles until the Reynolds number reaches 28.<br />

At a Reynolds number <strong>of</strong> 78 the floH is 1>Jell into the<br />

transition region and the radial velocity component <strong>of</strong> the<br />

<strong>pseudoplastic</strong> <strong>fluids</strong> is high and there l.s an infloVling<br />

vertical component..<br />

Tll.e flo"V>J patterns <strong>for</strong> the NevJtonian<br />

<strong>fluids</strong> are similar but the vertical inflm-.r is s lightly less

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