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

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NONIONIZING RADIATION SAFETY 773<br />

The effectiveness of an absorber for radiation of any given wavelength is measured<br />

by the penetration depth in the absorber. At an absorber thickness t = 1/α, the power<br />

density is reduced by absorption <strong>to</strong><br />

E 2<br />

E 1<br />

= e −2 = 0.135<br />

of its original value. Since the power density is reduced <strong>to</strong> 13.5%, this means that<br />

86.5% of the energy is absorbed in a thickness equal <strong>to</strong> 1/α. This thickness is called<br />

the penetration depth, δ, and its exact value depends on the frequency of the radiation<br />

and on the electrical and magnetic properties (μ, σ , and ɛ) of the absorber.<br />

In the case of the 2450-MHz radiation of Example 14.24, the penetration depth in<br />

muscle tissue is<br />

δ = 1<br />

α<br />

δ =<br />

1<br />

= 1.67 cm.<br />

0.6 cm−1 (14.39)<br />

The rate of heat generation in any absorber, such as biological tissue, is inversely<br />

proportional <strong>to</strong> the square of the penetration depth. Thus, a tissue with a relatively<br />

small penetration depth because of high water content, such as muscle, will heat<br />

much faster under microwave radiation than will a tissue such as fat, whose penetration<br />

depth is relatively large because of its very low water content. At 2450 MHz, for<br />

example, the penetration depths in muscle and fat are 1.7 and 11.2 cm, respectively.<br />

The rate of heating in the muscle, therefore, from a given power density, will be<br />

about (11.2/1.7) 2 = 43.4 times greater than in the fat. Table 14-17 lists the dielectric<br />

parameters and penetration depth for muscle tissue for several frequencies and<br />

Table 14-18 lists these parameters for several other frequencies for muscle and for<br />

fat. Note that the penetration depth decreases with increasing frequency, and that<br />

at a frequency of 100,000 MHz (100 GHz), only a very thin layer of tissue, 0.03 cm,<br />

absorbs 86.5% of the incident energy.<br />

TABLE 14-17. Penetration Depth and Dielectric Parameters for Muscle Tissue vs. Frequency<br />

RELATIVE PENETRATION<br />

FREQUENCY DIELECTRIC CONDUCTIVITY, DEPTH,<br />

(MHz) CONSTANT ɛ T σ (S/m) δ (cm)<br />

0.1 1850 0.56 213<br />

1.0 411 0.59 70<br />

10 131 0.68 13.2<br />

100 79 0.81 7.7<br />

1000 60 1.33 3.4<br />

10000 42 13.3 0.27<br />

100000 8 60 0.03<br />

Reproduced with permission from Adair ER, Peterson RC. Biological effects of radiofrequency/microwave radiation. IEEE<br />

Trans Microw Theory Tech. 2002; 50(3):953–962.

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