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

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42<br />

disadvantage is the installation <strong>of</strong> the thermocouples so<br />

that the junction measures the <strong>heat</strong> <strong>transfer</strong> surface and<br />

does not disturb the <strong>heat</strong> flow through the wall.<br />

By proper<br />

installation techniques, hov-rever, this can be closely<br />

approximated.<br />

In some cases the thermocouple junction has<br />

been embedded in the 't\fall rather than at the surface..<br />

However,<br />

if the exact position <strong>of</strong> the junction and the thermal<br />

conductivity <strong>of</strong> the wall is knovrn the results can be<br />

corrected to give the surface temperature.<br />

The Correlation <strong>of</strong> Results<br />

- ,<br />

The correlation <strong>of</strong> the data is difficult because <strong>of</strong><br />

the large number <strong>of</strong> variables.. A fe'ltJ authors used a<br />

method <strong>of</strong> plotting the Nusselt n~mber versus a dimensionless<br />

group on logarithmic coordinates, keeping all the variables<br />

constant (39, 58, 137,1;D)"<br />

Once the effect <strong>of</strong><br />

Ylgroup 1" has been determined the Nusselt number, divided<br />

by the IIgroup ll! effect, is plotted versus "group 2".<br />

The effect <strong>of</strong> "group 3 11<br />

is found by plotting the Nusselt<br />

number, divided by 'che product <strong>of</strong> the "group 111<br />

and flgroup<br />

211 effect, versus ltgroup 3". There are disadvantages to<br />

this method since it is very difficult, experimentally, to<br />

change the value <strong>of</strong> only one dimensionless group at a time.<br />

Some authors seem to have assltmed that the Chilton (39<br />

equation and exponents are accurate and thus use his exponents<br />

<strong>for</strong> some <strong>of</strong> the dimensionless groups and by plotting

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