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Continuation of Table 13.2<br />

Hydrogen 0.172 20<br />

Nitrogen 0.0234 20<br />

Oxygen 0.0238 20<br />

Nonmetals<br />

Water 0.565 0<br />

» 0.599 20<br />

» 0.627 40<br />

Concrete 2.43 20<br />

Wood 0.126 20<br />

Plastic 0.04 20<br />

Biological objects<br />

Fat 0.205 20<br />

Skin 0.502 20<br />

Muscles 0.4 20<br />

Fur 0.036 - 0.063 20<br />

Example. When a pig lies on concrete, the animal's belly and the<br />

concrete on which it lies are in contact. The temperature of the concrete's<br />

surface approximates that of the pig's belly surface. Assume that<br />

the 8-cm-thick concrete slab is on ground with a temperature of O°C,<br />

that belly-floor contact area is 3000 ern", the body temperature of pig is<br />

38'C, and the thermal conductivity of the concrete is 2.43 W·m-i.K-I.<br />

Estimate the conductive heat transfer under steady-state conditions.<br />

Solution. Conductive heat transfer flux from the belly to the concrete<br />

can be calculated as:<br />

2(0<br />

Qc =-«.s t1.T = -2.43~. 3000 .10- 4 m - 38) K K8 .10- 4 m =<br />

t1.x<br />

m·K<br />

=- 2.43 ·3 ·10 -I ( - 38) / 8·10 -2 = 346.27 J .s:'<br />

13.3.2. Convection<br />

Heat transferred by the movement of a heated substance is said<br />

to have been transferred by convection. When the movement results<br />

from differences in density, it is referred to as natural convection.<br />

When the heated substance is forced to move by a fan or<br />

pump, the process is called forced convection.<br />

Consider the convective heat exchange of objects with various<br />

shapes. The amount of heat conducted across the boundary layer<br />

102<br />

and convected away from the tJdL i-'~di.e (e.g., the surface of a leaf<br />

per unit time and area) by forced convection is:<br />

J = _ Zlc: (~eal - Talr )<br />

e air 8<br />

(13.2)<br />

where k air<br />

is the thermal conductivity coefficient of air, T'eal<br />

the leaf temperature, and T alr<br />

the temperature of the air outside<br />

a boundary layer of thickness 8. This can be expressed as:<br />

8 (mm) = 4.0 I L(m) (13.3)<br />

, Vtm/s)<br />

where L is the mean length of the leaf, V is the ambient wind<br />

speed, and the factor 4.0 has dimensions in m/s!".<br />

In the case of a cylinder (e.g., an animal), the heat flux<br />

density is:<br />

J = _ 2k . (Tsuif - Talr )<br />

e air .' + 8] (13.4)<br />

rln--,<br />

r )<br />

where r is the cylinder radius, T,urf surface temperature, and 8 is<br />

calculated as:<br />

D(m)<br />

8 (mm) =5.8,/V(m/s) (13.5)<br />

where D is the cylinder diameter.<br />

It is possible to use the .following relation for objects of<br />

irregular shape which is known as Newton's law of cooling. It describes<br />

the rate of heat loss (Jc) in W1m 2 per unit surface area of a<br />

body in a cool air stream as:<br />

J e = k/T,uif - To) (13.6)<br />

where k, is the convection coefficient with units W·m- 2·deg- J •<br />

Example. Calculate the heat flux density conducted across the<br />

boundary layer and convected away from the surface of a sheep if the<br />

body of the animal approximates a cylinder with a radius of 60 ern,<br />

103

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