克劳福德电池的电磁剂量测定:225至500兆赫。

A S Segal, R L Magin, C A Cain
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引用次数: 1

摘要

在225至500 MHz频率范围内,使用克劳福德细胞暴露室(主部分30平方厘米)进行电磁剂量测定。在细胞内测量电场模式。在500mhz以下的频率上没有观察到高阶模式,但在2450mhz处观察到明显的场扰动。测量了长球状仓鼠体和不同大小的含盐球体的能量吸收。在E极化下,仓鼠幻影的标准化全身比吸收率(SAR)从0.11 (225 MHz)增加到0.42 (450 MHz), K极化从0.06 (325 MHz)增加到0.20 (500 MHz), H极化从0.03 (325 MHz)增加到0.12 (500 MHz)。虽然这些值超出了对功率吸收的长波长远场近似的预测,但测量的sar直接使用量热法得到了证实。此外,使用含盐球体获得的量热数据表明,克劳福德电池中的吸收功率只有在从隔膜到外壁的垂直尺寸小于20%的物体上才会收敛到远场平面波理论值。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Electromagnetic dosimetry in a Crawford cell: 225 to 500 MHz.

A Crawford cell exposure chamber (main section 30 cm square) was used for electromagnetic dosimetry in the 225 to 500 MHz frequency range. Electric field patterns were measured within the cell. No higher-order modes were observed at any of the frequencies studied below 500 MHz, but significant field perturbations were seen at 2450 MHz. Energy absorption in a prolate spheroidal hamster phantom and in saline-filled spheres of various sizes was measured. The normalized whole-body specific absorption rate (SAR) in watts/kg per mW/cm2 increased from 0.11 (at 225 MHz) to 0.42 (at 450 MHz) for the hamster phantom in E polarization, from 0.06 (at 325 MHz) to 0.20 (at 500 MHz) for K polarization, and from 0.03 (at 325 MHz) to 0.12 (at 500 MHz) for H polarization. Although these values exceed predictions from the long-wavelength far-field approximation for power absorption, the measured SARs were corroborated directly using calorimetry. In addition, calorimetric data obtained using saline-filled spheres suggests that absorbed power in a Crawford cell converges to the far-field plane wave theoretical values only for objects occupying less than 20% of the vertical dimension from the septum to the outer wall.

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