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Introduction to Health Physics: Fourth Edition - Ruang Baca FMIPA UB

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776 CHAPTER 14<br />

that we have a nonthermal effect. Thermal effects are associated with exposures greater<br />

than 10 mW per cm, while nonthermal effects generally are associated with exposures<br />

less than 10 mW per cm.<br />

Animal studies show that microwave radiation, in frequencies ranging from 200–<br />

24,000 MHz, is lethal if the product of exposure intensity and time is sufficiently<br />

great <strong>to</strong> increase the body temperature beyond the body’s homeostatic capabilities<br />

(≥5 ◦ C) for a sustained period. For example, rats exposed <strong>to</strong> 3000-MHz radiation at a<br />

power density of 300 mW cm −2 suffered a temperature increase of 8–10 ◦ C and died<br />

after 15 minutes of exposure; at a power density of 100 mW cm −2 , rats died after 25<br />

minutes of exposure, when their body temperature had risen by 6–7 ◦ C.<br />

The temperature rise in any absorbing medium is related <strong>to</strong> the absorbed power<br />

density Pa, by<br />

Pa =<br />

ρ kg J/kg<br />

× c × T<br />

m3 ◦C ◦ C<br />

t seconds<br />

where<br />

ρ = density of the absorbing medium,<br />

c = specific heat of the absorbing medium,<br />

T = temperature increase, and<br />

t = exposure time.<br />

W<br />

, (14.40)<br />

m3 If the absorbing medium is a living tissue, the temperature increase will differ from<br />

that predicted by Eq. (14.40) because of heat loss due <strong>to</strong> evaporative cooling, and<br />

convective and conductive heat loss or gain. The net amount of heat s<strong>to</strong>red in the<br />

body is given by the heat balance equation<br />

S = M ± R ± C − E , (14.41)<br />

where<br />

M = metabolic heat rate,<br />

R = radiative heat gain or loss,<br />

C = conductive and convective heat gain or loss,<br />

E = heat loss due <strong>to</strong> evaporative cooling, and<br />

S = rate of heat s<strong>to</strong>rage.<br />

While resting, a person generates metabolic heat at a rate of about 75 W; while<br />

engaged in moderate work or exercise, the metabolic heat output increases <strong>to</strong> about<br />

300 W. This metabolic heat is dissipated in the environment when the temperature<br />

and humidity do not exceed the comfort range. If the temperature and humidity are<br />

<strong>to</strong>o high <strong>to</strong> dissipate the metabolic heat, the person’s body temperature increases.<br />

The additional heat load due <strong>to</strong> absorption of microwave energy must be dissipated<br />

in exactly the same manner as any other heat load. An unacceptable heat stress<br />

results when the combination of heat load and environmental conditions lead <strong>to</strong> an<br />

increased body temperature of 1 ◦ C or more. The “comfort range” is measured by<br />

the temperature–humidity index (THI), which is defined by<br />

THI = 0.72(Td + Tw ) + 40.6, (14.42)

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