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Reply to 'Comments on 'Application of Double Negative Materials to Increase the Power Radiated by Electrically Small Antennas''

机译:回复“关于“应用双负材料增加电小天线辐射功率的评论””

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I would like to thank Prof. Kildal for his interest in our work. However, I respectfully disagree with his comments on our reported results on several levels. I explain these below. In [1], we were considering the performance of an infinitesimal electric dipole antenna (i.e., a given infinitesimal current source) surrounded by a double negative (DNG) metamaterial shell. To describe the performance of this system, and in particular the effect of the DNG shell, we needed to compare the radiation property of this system with that of the same infinitesimal dipole without the DNG shell. As a quantitative measure for such comparison we took the ratio of the total power radiated by our DNG-shell-surrounded source to the power radiated by the same infinitesimal radiating current source in free space. In other words, the sources in both cases were ideal infinitesimal current dipoles driven with the same time-varying current value. We denoted this ratio by the term "radiated power gain." We emphasized the adjective "radiated" because we were discussing both the reactive and radiated powers throughout the paper and wanted to make a clear distinction on what quantity was being reported. Since the term was defined explicitly in the paper to avoid any confusion, I do not believe the term could be considered misleading.
机译:我要感谢基达尔教授对我们的工作感兴趣。但是,我谨不同意他对我们在几个层面上报告的结果的评论。我在下面解释这些。在[1]中,我们考虑了由双负(DNG)超材料外壳包围的极小电偶极天线(即给定的极小电流源)的性能。为了描述该系统的性能,特别是DNG壳的效果,我们需要比较该系统的辐射特性与不带DNG壳的相同无限小偶极子的辐射特性。作为这种比较的定量方法,我们采用了DNG外壳环绕的源辐射的总功率与自由空间中同一无限小辐射电流源辐射的功率之比。换句话说,两种情况下的源极都是以相同的时变电流值驱动的理想无限小电流偶极子。我们用术语“辐射功率增益”表示该比率。我们强调形容词“辐射”是因为我们在整篇论文中都讨论了无功功率和辐射功率,并希望对所报告的数量进行明确区分。由于该术语在本文中已明确定义以避免任何混淆,因此我认为该术语不会被误导。

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