Gandhi O P, Lazzi G, Tinniswood A, Yu Q S
Electrical Engineering Department, University of Utah, Salt Lake City 84112-9206, USA.
Bioelectromagnetics. 1999;Suppl 4:93-101. doi: 10.1002/(sici)1521-186x(1999)20:4+<93::aid-bem11>3.0.co;2-8.
Some recent developments in both the numerical and experimental methods for determination of SARs and radiation patterns of handheld wireless telephones are described, with emphasis on comparison of results using the two methods. For numerical calculations, it was possible to use the Pro-Engineer CAD Files of cellular telephones for a realistic description of the device. Also, we used the expanding grid formulation of the finite-difference time-domain (FDTD) method for finer-resolution representation of the coupled region, including the antenna, and an increasingly coarser representation of the more-distant, less-coupled region. Together with the truncation of the model of the head, this procedure led to a saving of computer memory needed for SAR calculations by a factor of over 20. Automated SAR and radiation pattern measurement systems were used to validate both the calculated 1-g SARs and radiation patterns for several telephones, including some research test samples, using a variety of antennas. Even though widely different peak 1-g SARs were obtained, ranging from 0.13 to 5.41 W/kg, agreement between the calculated and the measured data for these telephones, five each at 835 and 1900 MHz, was excellent and generally within +/-20% (+/-1 dB). An important observation was that for a maximum radiated power of 600 mW at 800/900 MHz, which may be used for telephones using AMPS technology, the peak 1-g SARs can be higher than 1.6 W/kg unless antennas are carefully designed and placed further away from the head.
本文描述了用于确定手持无线电话比吸收率(SAR)和辐射方向图的数值方法和实验方法的一些最新进展,重点是比较这两种方法的结果。对于数值计算,可以使用手机的Pro-Engineer CAD文件来逼真地描述设备。此外,我们使用了时域有限差分法(FDTD)的扩展网格公式,以便更精细地表示耦合区域(包括天线),而对距离更远、耦合较弱的区域则采用越来越粗糙的表示。连同头部模型的截断,这一过程使SAR计算所需的计算机内存节省了20倍以上。使用自动化的SAR和辐射方向图测量系统,对包括一些研究测试样品在内的几部手机,使用各种天线,验证了计算得到的1 g SAR和辐射方向图。尽管获得的峰值1 g SAR差异很大,范围从0.13到5.41 W/kg,但对于这些手机(835和1900 MHz各五部),计算数据与测量数据之间的一致性非常好,通常在±20%(±1 dB)以内。一个重要的观察结果是,对于800/900 MHz下600 mW的最大辐射功率(这可能用于采用AMPS技术的手机),除非天线经过精心设计并放置得离头部更远,否则峰值1 g SAR可能会高于1.6 W/kg。