{"title":"放置在地面上的领结天线输入阻抗共振","authors":"F. Kong","doi":"10.1117/12.462194","DOIUrl":null,"url":null,"abstract":"In the paper we have derived the following equation 4 f 0 L equi = c/ sqrt(e equi ) where f 0 is the resonant frequency of the antenna input impedance, c is the speed of light, L equi and e equi are respectively the equivalent length of antenna and the equivalent dielectric constant of the medium formed by half-space ground and half-space air. When measuring in air, the dielectric constant is known. One can obtain the antenna equivalent length from the measured f 0, by using the above equation. When L equi is obtained, one then can calculate e equi from a measured f 0 for the case when placing antenna on material interface. One can further estimate the ground dielectric constant by using the equation: e equi = (e iar + e ground )/2. Bow-tie antennas with different flange angles are constructed for experiments, in order to discuss the application of the above equation. The lengths of those antennas are all 30cm (length of the antenna conductor: 15cm). But the flange angles of the antenna conductors are respectively: 15, 40, 60, 75, 90 degrees. The antenna input reflections are measured over the frequency band up to 500 MHz, for cases when the antennas are placed in air and on sand, stone and water surfaces.","PeriodicalId":256772,"journal":{"name":"International Conference on Ground Penetrating Radar","volume":"19 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2002-04-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Resonance of input impedance of bow-tie antenna placed on ground surface\",\"authors\":\"F. Kong\",\"doi\":\"10.1117/12.462194\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"In the paper we have derived the following equation 4 f 0 L equi = c/ sqrt(e equi ) where f 0 is the resonant frequency of the antenna input impedance, c is the speed of light, L equi and e equi are respectively the equivalent length of antenna and the equivalent dielectric constant of the medium formed by half-space ground and half-space air. When measuring in air, the dielectric constant is known. One can obtain the antenna equivalent length from the measured f 0, by using the above equation. When L equi is obtained, one then can calculate e equi from a measured f 0 for the case when placing antenna on material interface. One can further estimate the ground dielectric constant by using the equation: e equi = (e iar + e ground )/2. Bow-tie antennas with different flange angles are constructed for experiments, in order to discuss the application of the above equation. The lengths of those antennas are all 30cm (length of the antenna conductor: 15cm). But the flange angles of the antenna conductors are respectively: 15, 40, 60, 75, 90 degrees. The antenna input reflections are measured over the frequency band up to 500 MHz, for cases when the antennas are placed in air and on sand, stone and water surfaces.\",\"PeriodicalId\":256772,\"journal\":{\"name\":\"International Conference on Ground Penetrating Radar\",\"volume\":\"19 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2002-04-15\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"International Conference on Ground Penetrating Radar\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1117/12.462194\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"International Conference on Ground Penetrating Radar","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1117/12.462194","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
摘要
在本文中,我们推导出如下公式:4f0lequi = c/ sqrt(e equi),其中f0为天线输入阻抗的谐振频率,c为光速,lequi和eequi分别为天线的等效长度和由半空间地面和半空间空气构成的介质的等效介电常数。在空气中测量时,介电常数是已知的。利用上述公式,可以从测量的f0得到天线等效长度。当得到lequi后,就可以根据测量到的f0计算出天线放置在材料界面上的情况下的eequi。我们可以用公式eequi = (ear + e ground)/2进一步估计地介电常数。构造不同翼缘角度的领结天线进行实验,探讨上述方程的应用。天线长度均为30cm(天线导体长度为15cm)。但天线导线的法兰角分别为:15度、40度、60度、75度、90度。当天线放置在空气中、沙子、石头和水面上时,天线的输入反射在500兆赫的频带内进行测量。
Resonance of input impedance of bow-tie antenna placed on ground surface
In the paper we have derived the following equation 4 f 0 L equi = c/ sqrt(e equi ) where f 0 is the resonant frequency of the antenna input impedance, c is the speed of light, L equi and e equi are respectively the equivalent length of antenna and the equivalent dielectric constant of the medium formed by half-space ground and half-space air. When measuring in air, the dielectric constant is known. One can obtain the antenna equivalent length from the measured f 0, by using the above equation. When L equi is obtained, one then can calculate e equi from a measured f 0 for the case when placing antenna on material interface. One can further estimate the ground dielectric constant by using the equation: e equi = (e iar + e ground )/2. Bow-tie antennas with different flange angles are constructed for experiments, in order to discuss the application of the above equation. The lengths of those antennas are all 30cm (length of the antenna conductor: 15cm). But the flange angles of the antenna conductors are respectively: 15, 40, 60, 75, 90 degrees. The antenna input reflections are measured over the frequency band up to 500 MHz, for cases when the antennas are placed in air and on sand, stone and water surfaces.