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Handbook of air conditioning and refrigeration / Shan K

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Steady-State Thermal Equilibrium<br />

Transient Energy Balance<br />

When the human body is maintained at a steady-state thermal equilibrium, i.e., the heat storage<br />

at the body core <strong>and</strong> skin surface is approximately equal to zero, then the heat exchange between<br />

the human body <strong>and</strong> the indoor environment can be expressed by the following heat balance<br />

equation:<br />

M � W � C � R � E sk � E res<br />

where M � metabolic rate, Btu/h�ft 2 (W/m 2 )<br />

W � mechanical work performed, Btu/h�ft 2 (W/m 2 )<br />

C � R � convective <strong>and</strong> radiative, or sensible heat loss from skin surface,<br />

Btu/h�ft 2 (W/m 2 )<br />

E sk � evaporative heat loss from skin surface, Btu/h�ft 2 (W/m 2 )<br />

E res � evaporative heat loss from respiration, Btu/h�ft 2 (W/m 2 )<br />

In Eq. (4.1), the ft 2 in the unit Btu/h�ft 2 applies to the skin surface area. The skin surface area <strong>of</strong> a<br />

naked human body can be approximated by an empirical formula proposed by Dubois in 1916<br />

where A D � Dubois surface area <strong>of</strong> naked body, ft 2 (m 2 )<br />

m b � mass <strong>of</strong> human body, lb (kg)<br />

H b � height <strong>of</strong> human body, ft (m)<br />

(4.1)<br />

A D � 0.657m b 0.425 Hb 0.725 (4.2)<br />

In an <strong>air</strong> conditioned space, a steady-state thermal equilibrium is usually maintained between the<br />

human body <strong>and</strong> the indoor environment.<br />

When there is a transient energy balance between the human body <strong>and</strong> the indoor environment, the<br />

thermal interaction <strong>of</strong> the body core, skin surface, <strong>and</strong> indoor environment forms a rate <strong>of</strong> positive<br />

or negative heat storage both in the body core <strong>and</strong> on the skin surface.<br />

The human body needs energy for physical <strong>and</strong> mental activity. This energy comes from the oxidation<br />

<strong>of</strong> the food taken into the human body. The heat released from this oxidation process is<br />

called metabolic heat. It dissipates from the skin surface <strong>of</strong> the human body into the surroundings.<br />

In a cold environment, the thermoregulatory mechanism reduces the rate <strong>of</strong> peripheral blood circulation,<br />

lowering the temperature <strong>of</strong> the skin <strong>and</strong> preventing any greater heat loss from the human<br />

body. However, if the heat loss <strong>and</strong> the mechanical work performed are greater than the rate <strong>of</strong><br />

metabolic heat produced, then the temperatures <strong>of</strong> both the body core <strong>and</strong> the skin surface fall, <strong>and</strong><br />

shivering or other spontaneous activities occur to increase the production <strong>of</strong> heat energy within the<br />

human body.<br />

On the other h<strong>and</strong>, in a hot environment, if a large amount <strong>of</strong> heat energy needs to be dissipated<br />

from the human body, the physiological control mechanism increases the blood flow to the skin<br />

surface. This raises the skin temperature. If the heat produced is still greater than the heat actually<br />

dissipated <strong>and</strong> the temperature <strong>of</strong> the body core increased from its normal temperature <strong>of</strong> about<br />

97.6 to about 98.6°F (36.4 to about 37.0°C), then liquid water is released from the sweat gl<strong>and</strong>s for<br />

evaporative cooling.<br />

For a transient state <strong>of</strong> energy balance between the human body <strong>and</strong> the indoor environment, the<br />

rate <strong>of</strong> heat storage in the body core S cr <strong>and</strong> the skin surface S sk, both in Btu/h�ft 2 (W/m 2 ), can be<br />

calculated as<br />

S cr � S sk � M � W � (C � R) � E sk � E res<br />

INDOOR AND OUTDOOR DESIGN CONDITIONS 4.3<br />

(4.3)

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