Finally, Fig. 6 displays the variation of the removed energy parameter
with nanofluid concentration for different concentrations of
nanofluid. As seen, at each mass flow rate, there is an optimal concentration
in which the removed energy parameter is minimized. It is also
clearly observed that the removed energy parameter has an inverse
relationship with the mass flow rate. When the liquid passes with a
smaller velocity in the collector the thermal dissipation in the collector
rises, and, hence, the corresponding parameter i.e. removed energy
parameter, increases.
Finally, Fig. 6 displays the variation of the removed energy parameterwith nanofluid concentration for different concentrations ofnanofluid. As seen, at each mass flow rate, there is an optimal concentrationin which the removed energy parameter is minimized. It is alsoclearly observed that the removed energy parameter has an inverserelationship with the mass flow rate. When the liquid passes with asmaller velocity in the collector the thermal dissipation in the collectorrises, and, hence, the corresponding parameter i.e. removed energyparameter, increases.
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