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Experimental and Numerical Analysis of a PCM-Supported ...

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It could be interpreted that this particular behavior <strong>of</strong> <strong>PCM</strong> based system represents<br />

some first signs on the potentially important role <strong>of</strong> establishing multiple effects <strong>of</strong><br />

heating <strong>and</strong> humidification due to existence <strong>of</strong> thermally conductive elements in the<br />

system. It is worth to mention that this behavior can also be realized using other<br />

kinds <strong>of</strong> sensible heat storage or conductive media since it is not associated with the<br />

solid-liquid phase change phenomenon inside the packing medium but rather related<br />

to its thermal conductivity.<br />

The phenomena <strong>of</strong> multiple effects <strong>of</strong> heating/humidification <strong>and</strong><br />

cooling/dehumidification have been elaborated in chapters 3 <strong>and</strong> 4. For the <strong>PCM</strong><br />

packing there is complex interaction between various boundary conditions <strong>and</strong> the<br />

geometrical parameters. For instance, increasing the water mass flow rate increases<br />

the wetted area, enhances axial thermal stratification in all phases in the bed, <strong>and</strong><br />

increases the solid-gas temperature difference while decreasing the dry interfacial<br />

area between solid <strong>and</strong> gas phases.<br />

On the other h<strong>and</strong>, for a specific inlet hot water temperature <strong>and</strong> mass flow rate, the<br />

heat transfer between air <strong>and</strong> both water <strong>and</strong> solid phases depend on the air mass<br />

flow rate, which in turn has effects on the heat flow between water <strong>and</strong> solid. As<br />

mentioned earlier, there is a trade-<strong>of</strong>f between direct contact heat <strong>and</strong> mass transfer<br />

at the liquid-gas interface <strong>and</strong> indirect heat <strong>and</strong> mass transfer resulting from the<br />

MEHH phenomena. When the water vapor diffusion at the liquid-gas interface<br />

dominates, for instance due to large interfacial area or high mass transfer coefficient<br />

or both, this will come at the expense <strong>of</strong> the MEHH <strong>and</strong> vice versa.<br />

The energy flow between all <strong>and</strong> each pair <strong>of</strong> phases plays the major role in plotting<br />

the system behavior under each specific boundary <strong>and</strong> geometrical conditions. For<br />

instance, the energy flows in the evaporator are mainly dependent on:<br />

<br />

<br />

<br />

<br />

<br />

The heat capacity flow <strong>of</strong> inlet hot water,<br />

Air to water mass flow ratio,<br />

Interfacial areas,<br />

Packing height, <strong>and</strong><br />

The thermal conductivity <strong>of</strong> the packing (i.e. Biot numbers).<br />

The maximum sensible heat transfer rates between solid <strong>and</strong> gas occur if the <strong>PCM</strong><br />

is infinitely conductive <strong>and</strong> fluid-solid heat transfer coefficients are infinite. In this<br />

case the temperature <strong>of</strong> the <strong>PCM</strong> will be always at the heat source temperature (i.e.<br />

water in the evaporator or gas in the condenser), which may give rise to the MEHH<br />

to dominate. These particular characteristics have to be seen as the basic<br />

background for describing <strong>and</strong> reading the comparative results between <strong>PCM</strong> (as a<br />

conductive medium) <strong>and</strong> Non-<strong>PCM</strong> packing types.<br />

115

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