Figure Return loss of gap-coupled circular patch antenna derived by using three methods 4.0 and 1.6 mm, respectively. The cell size along the thickness of the substrate is 0.4 mm, while it is 0.6965 mm along the other two directions. Figure compares the result for the return loss of the antenna de
Reflection and penetration depth of millimeter waves in murine skin
β Scribed by S.I. Alekseev; O.V. Gordiienko; M.C. Ziskin
- Book ID
- 101704658
- Publisher
- John Wiley and Sons
- Year
- 2008
- Tongue
- English
- Weight
- 89 KB
- Volume
- 29
- Category
- Article
- ISSN
- 0197-8462
No coin nor oath required. For personal study only.
β¦ Synopsis
Abstract
Millimeter (mm) wave reflectivity was used to determine murine skin permittivity. Reflection was measured in anesthetized Swiss Webster and SKH1βhairless mice in the 37β74 GHz frequency range. Two skin models were tested. Model 1 was a single homogeneous skin layer. Model 2 included four skin layers: (1) the stratum corneum, (2) the viable epidermis plus dermis, (3) fat layer, and (4) muscle which had infinite thickness. We accepted that the permittivity of skin in the mm wave frequency range results from the permittivity of cutaneous free water which is described by the Debye equation. Using Fresnel equations for reflection we determined the skin parameters best fitting to the reflection data and derived the permittivity of skin layers. The permittivity data were further used to calculate the power density and specific absorption rate profiles, and the penetration depth of mm waves in the skin. In both murine models, mm waves penetrate deep enough into tissue to reach muscle. In human skin, mm waves are mostly absorbed within the skin. Therefore, when extrapolating the effects of mm waves found in animals to humans, it is important to take into account the possible involvement of muscle in animal effects. Bioelectromagnetics 29:340β344, 2008. Β© 2008 WileyβLiss, Inc.
π SIMILAR VOLUMES
The surface impedance of several c-axis oriented YBa2Cu3O7 thin-film samples was measured in a copper host cavity at 87 GHz between 4.2 K and 300 K. High aualitv films between 0.17 urn and 0.8 um In thickness have been grown epitaxially on SrTiO3 by pulsed excimer laser~ablation. The partial penetra
## Abstract Recently we showed that the Pennes bioheat transfer equation was not adequate to quantify mm wave heating of the skin at high blood flow rates. To do so, it is necessary to incorporate an βeffectiveβ thermal conductivity to obtain a hybrid bioheat equation (HBHE). The main aim of this s