Wong T Z, Trembly B S
Department of Radiology, New England Deaconess Hospital, Boston, MA 02215.
Int J Radiat Oncol Biol Phys. 1994 Feb 1;28(3):673-82. doi: 10.1016/0360-3016(94)90193-7.
Two important characteristics for interstitial microwave antennas used in clinical hyperthermia are: (1) a good impedance match to minimize reflected power; and (2) a good power deposition pattern which is independent of insertion depth. A major problem of the miniature coaxial dipole antennas used for interstitial hyperthermia is the fact that the impedance and power deposition patterns of these antennas change with insertion depth. One possible solution is the addition of a coaxial choke. A theoretical model for calculating the input impedance of interstitial microwave antennas having a coaxial choke is presented, which may serve as the first step in the design of such antennas.
A theoretical model for calculating the input impedance of coaxial microwave antennas with and without a choke is presented using insulated antenna theory. The theoretical model was used to calculate the input impedance of several prototype antennas having various choke and feedline dimensions, and comparison was made with experimentally measured impedance measurements in tissue-equivalent phantom.
The choke section of the antenna is not ideal if conventional plastic insulation is used as the choke dielectric, because the desired radiating length of the antenna is significantly shorter than the quarter-wavelength in the choke dielectric. Impedance calculations based on the theoretical model correlate reasonably well with experimentally measured impedance. Based on these calculations, the effect of parameters such as choke layer thickness and choke dielectric constant are discussed for a 915 MHz antenna with choke.
The theoretical model can serve as a design aid for optimizing choked microwave antenna designs, as well as predicting the impedance match of a given antenna design at a given insertion depth. The model allows the effect of some variables not accessible experimentally such as termination impedance to be studied, which may also be useful in the understanding of these antennas. Calculations are easily performed on a desktop computer.
用于临床热疗的间质微波天线有两个重要特性:(1)良好的阻抗匹配以最小化反射功率;(2)良好的功率沉积模式,且该模式与插入深度无关。用于间质热疗的微型同轴偶极天线的一个主要问题是,这些天线的阻抗和功率沉积模式会随插入深度而变化。一种可能的解决方案是添加同轴扼流圈。本文提出了一种用于计算具有同轴扼流圈的间质微波天线输入阻抗的理论模型,这可作为此类天线设计的第一步。
利用绝缘天线理论,提出了一种用于计算有无扼流圈的同轴微波天线输入阻抗的理论模型。该理论模型用于计算具有各种扼流圈和馈线尺寸的几个原型天线的输入阻抗,并与在组织等效体模中实验测量的阻抗进行比较。
如果使用传统塑料绝缘作为扼流圈电介质,天线的扼流圈部分并不理想,因为天线所需的辐射长度明显短于扼流圈电介质中的四分之一波长。基于理论模型的阻抗计算与实验测量的阻抗相当吻合。基于这些计算,讨论了诸如扼流层厚度和扼流圈介电常数等参数对带有扼流圈的915 MHz天线的影响。
该理论模型可作为优化带扼流圈微波天线设计的辅助工具,以及预测给定天线设计在给定插入深度下的阻抗匹配。该模型允许研究一些实验上无法获取的变量(如终端阻抗)的影响,这对于理解这些天线也可能是有用的。计算可在台式计算机上轻松完成。