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Wall 2 and 3 inner surface temperature subsystem<br />

VIII.3.1 Water surface heat transfer subsystem<br />

This subsystem is exactly the same as the one in section VIII.2.2 with the same name.<br />

However, the subsystem here is for calculating the heat the chamber air acquired from<br />

water through surface convection while the subsystem in section VIII.2.2 is for<br />

calculating the convectional heat loss from water to the chamber air through the same<br />

surface.<br />

VIII.3.2 Water surface mass transfer (evaporation) subsystem<br />

This subsystem is also exactly the same as the one in section VIII.2.3 with the same<br />

name. However, the subsystem here is for calculating amount of vapour gained from<br />

water while the subsystem used in section VIII.2.3 is for calculating the amount of<br />

water lost to chamber air through the same surface.<br />

VIII.3.3 Sharable energy from vapour calculation subsystem<br />

This simple subsystem provides the amount of energy stored in the evaporated water<br />

molecules which is sharable when the water vapour is mixing with air. Input to this<br />

subsystem is water temperature which is also the temperature of vapour molecules when<br />

escaping from the water.<br />

Figure VIII. 15 Sharable thermal energy from vapour calculation subsystem<br />

VIII.3.4 In-chamber air specific thermal capacity subsystem<br />

This subsystem is created based on Eq. (3.2). Input is specific humidity of air in the<br />

chamber. Output is specific thermal capacity of air in the chamber.<br />

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