zastosowania elektromagnetyzmu w nowoczesnych ... - PTZE
zastosowania elektromagnetyzmu w nowoczesnych ... - PTZE
zastosowania elektromagnetyzmu w nowoczesnych ... - PTZE
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30<br />
XVIII Sympozjum <strong>PTZE</strong>, Zamość 2008<br />
l is shown in Fig.1. The spheroid is an isotropic lossy dielectric. Time-harmonic fields with<br />
the time-dependence e jωt as a uniform plane wave are suppressed. The external medium is<br />
assumed to be free space. The relative permittivity ε’-jε” and the conductivity of tissue<br />
depend on frequency. European Standard EN-50361 establishes values of ε, γ for fantom<br />
liquid at mobile frequency band 300 – 3000 MHz to be used in SAR calculations. The<br />
simulations were done for GSM frequencies used in mobile telephony: 900 MHz and 1800<br />
MHz. The rms value of the electric field strength incident was 61,4 V/m. The values of the<br />
SAR were calculated using semi-analytical method. The method of calculations was described<br />
in [3]. The SAR for different configuration have been calculated. The spheroidal body<br />
dimensions taken into account are corresponding to dimensions of human body.<br />
Results<br />
Regarding statistical data avaible on human height and body mass 18 models were<br />
considered. The conductivity and permeability of tissues of young organism are higer<br />
comparing to the adult organism. In Figure 2 values of SAR at polarization H and two<br />
frequencies have been presented in relation of longer axis l of the body. The variation of the<br />
SAR at 900MHz is observed to be rather small. The SAR has larger value at larger frequency<br />
and the values of SAR in the body depend on dimensions of the body. The values of the<br />
SAR are higer for young person and they correspond to higer values of conductivity and<br />
permeability of tissues of young organism comparing to the adult organism .<br />
References<br />
SAR [W/kg]<br />
0.26<br />
0.24<br />
0.22<br />
0.2<br />
0.18<br />
0.16<br />
0.14<br />
0.12<br />
0.1<br />
0.08<br />
1800 MHz<br />
900 MHz<br />
0.06<br />
60 80 100 120<br />
l [cm]<br />
140 160 180<br />
Fig. 2. Calculated values of SAR at polarization H.<br />
[1] Ciosk K., Krawczyk A., Kubacki R.: The influence of the electromagnetic wave parameters on SAR<br />
coefficient, in: Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering (eds.<br />
A.Krawczyk, S.Wiak, X.M.Lopez-Fernandez), IOS Press, Amsterdam 2006<br />
[2] Ciosk K., Krawczyk A: The influence of the electromagnetic wave frequency on SAR in biological object.,<br />
EHE’06, Madeira, pp.2.97-2.100<br />
[3] Ciosk, A. Krawczyk, R. Kubacki, The comparison of phantom model and simulation results in SAR<br />
analysis , in: Computer Engineering in Applied Electromagnetism (eds. S. Wiak, A. Krawczyk, M. Trlep),<br />
Springer, 2005