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Simulation of Dual-Band MWCNT Ink-Based Spiral Antenna: A Comparative Study

机译:MWCNT墨基双频螺旋天线的仿真研究

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In this paper, we compare a dual-band, square spiral microstrip patch antenna constructed from Multi-Walled Carbon Nanotubes (MWCNT) ink for wearable application simulated by Computer Simulation Technology Microwave Studio (CST MWS) by our work simulated by Advanced Design System (ADS) electromagnetic simulator using the same material characterization. The reflection coefficient is –12 dB at 1.2276 GHz for MWCNT and –13 dB at 1.25 GHz for the copper simulated by CST MWS and reflection coefficient is –12.235 dB at 1.234 GHz for MWCNT and –18.36 dB at 1.243 GHz for the copper simulated by ADS and the reflection coefficient is –27dB at 2.47 GHz for MWCNT and –13 dB at 2.53 GHz for the copper simulated by CST MWS and the reflection coefficient is –26.08 dB at 2.48 GHz for MWCNT and –17.031 dB at 2.47 GHz for the copper simulated by ADS. We show the meandering of the surface current on the radiating in spiral patch. The antenna gain is found to be –12.5 dBi at 1.22 GHz for MWCNT and is found –12.05 dBi at 1.25 GHz at CST MWS and the antenna gain is found to be –11.85 dBi at 1.235 GHz for MWCNT and is found –12.25 dBi at 1.243 GHz at ADS and the antenna gain is found to be –4.25 dBi at 2.47 GHz for MWCNT and is found –4.01 dBi at 2.53 GHz at CST MWS and the antenna gain is found to be –4.23 dBi at 2.47 GHz for MWCNT and is found –4.88 dBi at 2.45 GHz at ADS. We show a close agreement in the results obtained by the two simulation software's CST MWS and ADS. The results are given for both MWCNT and Copper characterizations.
机译:在本文中,我们通过计算机模拟技术Microwave Studio(CST MWS)对我们的工作进行了比较,并使用Advanced Design System(Advanced Design System)模拟了由多壁碳纳米管(MWCNT)墨水构造的可穿戴应用的双频段,方形螺旋微带贴片天线( ADS)电磁模拟器使用相同的材​​料表征。 CST MWS模拟的铜的反射系数在1.2276 GHz时为–12 dB,在1.25 GHz的铜反射率为–13 dB,在MWCNT的1.234 GHz处的反射系数为–12.235 dB,在1.243 GHz时,铜的反射系数为–18.36 dB。 ADS和MWCNT在2.47 GHz处的反射系数为–27dB,对于CST MWS模拟的铜,反射系数为–13 dB在2.53 GHz处,并且MWCNT在2.48 GHz处的反射系数为–26.08 dB(在2.47 GHz处),对于铜为2.37 GHz由ADS模拟。我们在螺旋形斑块中显示了辐射表面电流的曲折。 MWCNT的天线增益在1.22 GHz时为–12.5 dBi,CST MWS在1.25 GHz的情况下为–12.05 dBi,MWCNT在1.235 GHz时的天线增益为–11.85 dBi,在CNT时为–12.25 dBi。在ADS处为1.243 GHz,对于MWCNT,在2.47 GHz处,天线增益为–4.25 dBi;在CST MWS,为2.53 GHz,在2.47 GHz处,天线增益为–4.01 dBi;对于MWCNT,在2.47 GHz处,天线增益为–4.23 dBi。在ADS处发现2.45 GHz时为–4.88 dBi。我们在两个模拟软件的CST MWS和ADS获得的结果中显示出非常一致的结果。给出了MWCNT和铜表征的结果。

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