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Cork insulation; a complete illustrated textbook on cork insulation ...

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96<br />

CORK INSULATION<br />

and the temperature difference,—may be expressed in symbols,<br />

thus:<br />

H=K A (ti—t.)<br />

in which H is the total heat transfer in B.t.u. per hour, K is<br />

the total heat transfer coefficient in B.t.u. per hour per degree<br />

temperature difference F., A is the area of the heat trans-<br />

mitting surface in square feet, and (t^—U) is the temperature<br />

difference in degrees Fahrenheit between the regi<strong>on</strong>s of high-<br />

est and lowest levels.<br />

It is evident, therefore, that if the heat transmitting area<br />

and the temperature levels are held c<strong>on</strong>stant, the heat transfer<br />

depends entirely up<strong>on</strong> c<strong>on</strong>ducti<strong>on</strong>, c<strong>on</strong>vecti<strong>on</strong> and radiati<strong>on</strong>.<br />

FIG 34.—TRANSFER OF HEAT BY CONDUCTION.<br />

65.—C<strong>on</strong>ducti<strong>on</strong>.—Heat transfer by c<strong>on</strong>ducti<strong>on</strong> is accom-<br />

plished in a body of material by the vibrati<strong>on</strong> or impact of<br />

the molecules or particles of matter that compose the body<br />

itself, such molecular disturbance being produced by an unbal-<br />

anced thermal c<strong>on</strong>diti<strong>on</strong> within the mass. Thus heat may be<br />

interchanged between different parts of the same body, or<br />

between two separate bodies in actual c<strong>on</strong>tact, by c<strong>on</strong>ducti<strong>on</strong><br />

but due to fricti<strong>on</strong> and adhesi<strong>on</strong> between the molecules of a<br />

body, the vibrati<strong>on</strong> or impact of the particles of matter will<br />

become slower as the heat energy passes from <strong>on</strong>e molecule to<br />

the other, and c<strong>on</strong>sequently the amount of heat that will be<br />

transmitted through the body will be something less than<br />

that applied to it. The amount of heat that will be transmitted<br />

through a given material, due to a given temperature<br />

difference, depends <strong>on</strong> the characteristic internal thermal c<strong>on</strong>-<br />

; ;<br />

J

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