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Question 13.16: Heating and Humidification Outdoor winter air enters a heati......

Heating and Humidification

Outdoor winter air enters a heating and humidification system at a rate of 900 cfm (425 L/s) and at 41°F (5°C) dry-bulb and 35°F (1.7°C) wet-bulb temperatures. The air is to be heated to 88°F (31°C) and humidified to a humidity ratio of 0.008  lb_{w}/lb_{a}. Determine the amount of sensible heating that needs to be provided by the heating coil and the amount of saturated steam at 212°F (100°C) that needs to be provided for humidification.

Given: T_{db1} = 41°F, T_{wb1} = 35°F, T_{db3} = 88°F, W_{3} = 0.008  lb_{w}/lb_{a}, and \dot{V}_{a} = 900  ft^{3}/min .
Figure: See Figure 13.18.
Find: \dot{Q}_{h} and \dot{m}_{w}.
Lookup values: Saturated steam enthalpy at 212°F from Table A3 is h_{vap} = 1150.5  Btu/lb_{w} (which is equal to h_{liq,2}). From psychrometric chart, h_{1} = 13  Btu/lb_{a}, v_{1} = 12.67  ft^{3}/lb_{a}, W_{1} = 0.003  lb_{w}/lb_{a}, and h_{3} = 30  Btu/lb_{a}.

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The mass flow rate of dry air is

\dot{m}_{a} = \frac{\dot{V}_{a}}{v_{1}} = \frac{900  ft^{3}/min}{12.67  ft^{3}/lb_{a}} = 71.03  lb_{a}/min = 4262  lb_{a}/h

The mass flow rate of steam is

\dot{m}_{w} = \dot{m}_{a} (W_{3}  –  W_{1}) = 4262  lb_{a}/h \times  (0.008  –  0.003)  lb_{w}/lb_{a}

 

= 21.31  lb_{w}/h (9.6  kg/h)

An energy balance on the humidifier only is used to determine the air enthalpy at state 2:

h_{2} = h_{3}  –  \left\lgroup \frac{\dot{m}_{w}}{\dot{m}_{a}} \right\rgroup \times h_{vap}

 

= 30  Btu/lb_{a}  –  \left\lgroup \frac{21.31}{4262} \right\rgroup \times 1150.5  Btu/lb_{a}

 

= 24.25  Btu/lb_{a}

From the psychrometric chart, this corresponds approximately to an exit condition of T_{db2} = 87°F, i.e., the humidication occurred essentially at constant T_{db}.
Finally, the heating coil energy is easily found as

\dot{Q}_{h} = \dot{m}_{a} (h_{2}  –  h_{1}) = 4,262  lb_{a}/h \times (24.25  –  13)  Btu/lb_{a}

= 47,936.8  Btu/h (14.05  kW)

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