A compact microstrip antenna for GPS and DCS application
Compact Microstrip Defected Ground Structured Antenna for Reduction of Harmonics and Cross Polarized
Compact Microstrip Defected Ground Structured Antenna for Reduction of Harmonics and Cross Polarized RadiationsSarat K Kotamraju1,2, B.T.P.Madhav1, T.V.Rama Krishna1, Habibulla Khan1 1Department of Electronics & Communication Engineering, K L University, Vaddeswaram, AP, India2Visiting Professor, Department of Electrical & Electronics Engineering, Shaqra University, Shaqra, Kingdom ofSaudi ArabiaAbstract: A novel Inset fed microstrip patch antenna is designed on defected ground structure (DGS) to reduce the higher order harmonics and cross polarized radiations. Square rings, and square shaped slots are placed on the ground plane of the microstrip patch antenna to get the desired operation. These annular ring and arc DGS appears to be highly efficient in terms of suppressing the cross polarization. Relative suppression of radiated field is observed by placing and without placing the defected ground structures. The stop band property exhibited by the DGS is used to filter out the harmonics. The current model successfully reduced the DGS size and by comparing with the well known design, size reduction of 20% is achieved. Instead of normal square patch, a slotted aperture patch model is considered in the current design to reduce the overall size of the antenna.Keywords: Defected Ground Structure (DGS), Cross Polarized Radiations, Reduction of Harmonics, Microstrip Patch Antenna.I.INTRODUCTION:Photonic band gap structures (PBG) is one of the promising technique to reduce the harmonic radiations from the microstrip patch antennas. An array of different types of slots will be etched on the ground plane beneath the antenna and the feed line. The stop band property exhibited by the PBG was used to filter out the harmonics. It was one of the simple technique which involved no additional circuitry and complexity [1].In recent years defected ground structures became popular to suppress higher harmonics, which are constructed f rom PBG’s etched on grounded substrates. As per the design is concerned physical part of the defect appears to be an important aspect, especially in the microwave integrated circuits. Square-headed dumbbell shaped DGS will suppress up to the second harmonic and a pair of dumbbell shaped DGS will suppress up to the third harmonic [2-7]. Harmonics in a microstrip patch indicate the multiples of the fundamental frequency and they belong to the category of higher order modes, excited in the radiating patch depending on its geometry. In between the harmonics and the fundamental resonance, few other higher order modes may exist [8].In this paper harmonic control of antennas in terms of quantitative suppression of radiated fields has been presented. This investigation is also successful to reduce the DGS size significantly and by compared to the known compact design, 20% reduction in size is attained.II.ANTENNA DESIGN ANDSPECIFICATIONS:Fig 1 Slotted Square patch antennaA square patch fed by conventional microstrip line is shown in fig 1. Instead of normal square patch, aslotted aperture square patch is taken in this design to reduce the overall size of the antenna. The modes have been identified primarily by resonating frequencies. To control the harmonics, a compact DGS on the ground plane with square rings and beneath the feed line with annular square ring has been examined to achieve the aim. Fig 2 shows thisarrangement.Fig 2a. Square Slotted DGS on ground plane, Fig 2b.Annular Square ring DGS beneath feed lineIII.RESULTS AND DISCUSSION:Fig 3. Return loss Vs Frequency Schematic view of antenna is shown in fig 1 and DGS models are shown in fig 2. RT-Duroid substrate with permittivity 2.2 and height of 1.6 mm is taken in this work. Fig 3 shows the S11 characteristics of the conventional ground plane and DGS ground plane based antenna. Results showing the excellent agreement with the computed parameters of the antenna. The radiation characteristics are examined at resonant frequencies 2.6 GHz and 4.8 GHz. Fig 3 indicating the mismatch in the input impedance over the target frequency range covering the 2-6 GHz. This ensures suppression of all higher order modes up to the second harmonic of the fundamental. This will significantly reduce radiations at those frequencies. This has been addressed extensively.Fig 4. Gain curve for three modelsThe three dimensional radiation patterns caused by the higher order modes can be visualized by observing the model fields as shown in fig 7 and 8. Figure 5 and 6 shows the radiation pattern of cross polarization and co-polarization with and without DGS.Fig 5. E-Plane and H-Plane Radiation patterns with and without DGS. Frequency 2.6 GHzPresence of DGS shows no significant effect on the radiation, considering both co-polarized and cross polarized fields. Gain is obtained up to 4.9 dB for all the configurations.Fig 6. E-Plane and H-Plane Radiation patterns with and without DGS. Frequency 4.8 GHzWe compared our present designs with the earlier ones in terms of area required to implement the defected ground plane. However the size of the present design is reduced almost by 20% compared to nearest early design.Fig 7. E-Field Distribution of Three models at 2.6and 4.8 GHzFig 8 Current distribution at 2.6 and 4.8 GHzIV.CONCLUSION:In this paper Control of higher modes up to second harmonic has been successfully achieved by placing square rings on ground plane and square annular ring beneath the feed line. The DGS used in the design is compact in size, easy to implement and no compromise in the performance compared to earlier ones. The performance of the DGSs has been verified in two different frequency bands and hence they are expected to be equally effective for all rectangular patches. The DGS will find different applications where polarization purity of antenna is an important aspect.ACKNOWLEDGEMENTSAuthors like to express their deep gratitude towards department of ECE and management of K L University for their support and encouragement during this work. This work is supported by Ministry of Science and Technology (F.No: SR/FST/EIT-316/2012) through FIST program and other projects (F.No: SR/FTP/ETA-079/2009) and AICTE (F.NO: 8023/RID/RPS-32/Pvt (II Policy)/2011-12.REFERENCES[1] Y. Horri and M. Ts utsumi, “Harmonic control by photonic bandgap on microstrip patch antenna,” IEEE Microwave Guided Lett., vol. 9, pp.13–15, Jan. 1999.[2] I. Chang and B. Lee, “Design of defected ground structures for harmonic control of active microstrip antenna,” in Proc. IEEE Antennas and Propagation Soc. Int. Symp., 2002, vol. 2, pp. 852–855.[3] H. Liu, Z. Li, X. Sun, and J. Mao, “Harmonic suppression with photonic bandgap and defected ground structure for a microstrip patch antenna,” IEEE Microw. Compon. Lett., vol. 15, no. 2, pp.55–56, Feb. 2005.[4] Y. J. Sung and Y. S. Kim, “An improved design of microstrip patch antennas using photonic bandgap structure,” IEEE Trans. Antennas Propag., vol. 53, no. 5, pp. 1799–1803, May 2005.[5] Y. J. Sung, M.Kim, and Y.-S. Kim, “Harmonic reductionwith defected ground structure of a microstrip patch antenna,” IEEE Antennas Wireless Propag. Lett., vol. 2, pp. 111–113, 2003.[6] M. K. Mandal, P. Mondal, S. Sanyal, and A. Chakrabarty, “An improved design of harmonic suppression for microstrip patch antennas,” Microwave and Opt. Tech. Lett., vol. 49, no. 1, pp. 103–105, Jan. 2007.[7] Chandrakanta Kumar, Debatosh Guha, “Nature of Cross-Polarized Radiations from Probe-Fed Circular Microstrip Antennas and their Suppression Using Different Geometries of Defected Ground Structure (DGS)”, IEEE TRANSACTIONS ON ANTENNAS AND PROPAGATION, VOL. 60, NO. 1, JANUARY 2012.[8] Sujoy Biswas, Debatosh Guha, Chandrakanta Kumar, “Control of Higher Harmonics and Their Radiations in Microstrip Antennas Using Compact Defected Ground Structures”, IEEE TRANSACTIONS ON ANTENNAS AND PROPAGATION, 2013.。
2.4g板载天线工作原理
2.4g板载天线工作原理2.4GHz板载天线工作原理随着无线通信技术的发展,2.4GHz频段的应用越来越广泛,而板载天线作为一种常见的天线形式,被广泛应用于无线设备中。
本文将介绍2.4GHz板载天线的工作原理。
一、背景介绍随着物联网、无线通信等技术的迅猛发展,无线设备的需求也越来越大。
尤其是在2.4GHz频段,无线网络、蓝牙、无线传感器等应用广泛。
而板载天线作为一种集成度高、适用于小型设备的天线形式,成为了2.4GHz频段应用中常见的选择。
二、板载天线的结构组成板载天线是指将天线直接集成在电路板上的天线形式。
通常由天线元件、馈线以及与电路板相连的匹配电路等组成。
其中,天线元件一般采用PCB打印工艺制作,可以是线性天线、贴片天线等形式。
三、天线元件的特性与选择天线元件的特性直接影响着天线的性能。
在2.4GHz频段中,一般选择具有较好性能的天线元件,如PCB打印的贴片天线。
这种天线元件体积较小,频段适应性好,并且具有较高的辐射效率和天线增益。
四、馈线与匹配电路在设计板载天线时,合适的馈线和匹配电路能够提高天线的性能。
馈线的长度和宽度应根据设计需求和电路板的尺寸来确定,以确保天线能够正常工作,并且有良好的阻抗匹配。
匹配电路一般采用电感和电容来实现,以进一步提高天线的阻抗匹配。
通过合理设计匹配电路的参数,可以改善天线的反射损耗和传输效率。
五、板载天线的辐射原理板载天线的工作原理基于安培环路定理和法拉第电磁感应定律。
当电流通过天线元件时,会在周围产生一个电磁场。
通过馈线和匹配电路的设计,将电磁能量转化为电磁波,并向空间辐射。
六、优化设计与性能提升在设计2.4GHz板载天线时,需要考虑到天线的辐射效率、工作带宽、方向性等因素。
通过优化天线元件的几何结构、馈线的设计以及匹配电路的参数选择,可以提高天线的性能。
七、应用领域及发展趋势2.4GHz板载天线广泛应用于各种无线设备中,如智能穿戴设备、智能家居、车联网等。
一种接地板开槽的小型化蝶形天线设计
一种接地板开槽的小型化蝶形天线设计张壹;左建宏;陈新伟;张文梅【摘要】本文设计了一个新型小型化蝶形微带天线,该天线采用微带馈线,通过优化辐射贴片和在接地板开槽的方法,减小了天线尺寸,最终所实现的天线尺寸为32 mm×32 mm,与传统蝶形天线相比尺寸减小23%.测量结果表明:天线S11<-10 dB的阻抗带宽能达到120 MHz(2.49 GHz~2.61 GHz).同时,天线最大增益为2.5 dBi,可以应用于无线传输领域.【期刊名称】《测试技术学报》【年(卷),期】2016(030)003【总页数】4页(P227-230)【关键词】蝶形微带天线;阻抗带宽;天线增益【作者】张壹;左建宏;陈新伟;张文梅【作者单位】山西大学物理电子工程学院,山西太原030006;山西大学物理电子工程学院,山西太原030006;山西大学物理电子工程学院,山西太原030006;山西大学物理电子工程学院,山西太原030006【正文语种】中文【中图分类】TN821+.3随着个人通信装备的不断增加,小型化紧凑的微带天线得到很大程度的发展. 同时为了减少天线尺寸,不少学者提出了各种方法,比如电阻负载技术,曲流技术和加槽技术等[1-3]; 在辐射贴片中刻蚀一个合适形状的缝隙,或者在接地板开槽的方法来减小天线尺寸[4]. 此外,蝶形微带天线可以减小尺寸并且增加带宽[5]. 矩形微带天线和蝶形微带天线的辐射特性有相似之处,而蝶形天线的面积却有很大程度的减小[6]. 蝶形天线的带宽调节是通过共面波导馈电的外延角来实现的,也可以通过减少金属化实现新颖的蝶形天线[7-9].本文中,通过优化贴片结构和在接地板开槽的方法设计了一个小型化的蝶形天线,并且给出设计公式. 和文献[6]中的天线相比,天线尺寸减小23%. 仿真和测量的结果表明:该天线工作在2.49~2.61 GHz, 带宽S11≤-10 dB是4.7%,同时得到了天线最大增益为2.5 dBi.本文设计的天线如图 1 所示,该天线采用FR4介质基板,相对介电常数4.4,厚度1.6 mm,整个尺寸为32 mm×36 mm,天线的辐射单元是一个带有微带馈线的对称蝶型贴片,其中馈线长为h1宽为l2,微带线的另一端与SMA接头同轴探针相连. 接地板上有一个长为a宽为b的长方形槽. 不同的开槽尺寸所对应的阻抗曲线如图 2 所示. 结果表明当接地板槽的面积变大时,输入阻抗的虚部变化很大,而实部变化很小. 天线的谐振频率随着开槽面积的增大而降低. 在文献[6]中,作者提出一种修正公式,用来修正对于TM10模结构的谐振频率. 在本文中,通过用下述公式来修正所设计的天线结构.式中: h是介质厚度,ε是相对介电常数, wc是连间两个蝶形天线间距, c 是自用空间光速. 其他参数l1=32 mm, l=24 mm, l2=3.1 mm, w1=36 mm, w=28 mm, h1=12.5 mm, εr=4.4, α=45°.通过上述公式计算了不同槽对应的谐振频率,并与仿真软件HFSS的仿真结果做比较,结果如表 1 所示,两个结果最大和最小的相对误差分别为4.46%和0.40%. 仿真和计算结果表明长度b对天线的谐振频率影响很大,而长度a则几乎没有影响.通过式(1)~式(7),设计了一个工作频率在2.55 GHz天线,最终优化尺寸为l1=32 mm, l=24 mm, l2=3.1 mm, w1=36 mm, w=28 mm, h1=12.5mm,ε=4.4, α=45°, a=16 mm, b=24 mm. 测量和仿真的S11结果在图 3 中,测量的阻抗带宽为4.7%(2.49~2.61 GHz).在图 4 中,描述了2.55 GHz时仿真和测量的辐射模式. 从图 4 中可以看出,仿真和测量的结果基本一致. 在E面主极化是8字形,交叉极化水平比较低. 同时,在H面得到较好的全向辐射特性和低的交叉极化.最后,测量的天线在2.49~2.61 GHz的增益如图 5 所示,可以得出设计的天线增益工作频率优于0.25 dBi,最高增益是2.5 dBi.本文设计了一个小型化蝶形微带天线,通过优化天线的辐射贴片和接地板开槽的方法来减少天线的尺寸. 与文献6的天线尺寸相比,减少了23%. 仿真和测量的结果也表明,天线工作在2.49~2.61 GHz,相对带宽4.7%. 同时,设计的天线在相对稳定性和全向辐射特性方面有所改进,天线最大增益为2.5 dBi.【相关文献】[1] Boccia L, Amendola G, Massa G D. A dual frequency microstrip patch antenna for high-precision GPS applications[J]. IEEE Antennas and Wireless Propagation Letters, 2004(3): 157-160.[2] Chiu C Y, Chan C H, Luk K M. Small dual-band antenna with folded-patch technique[J]. IEEE Antennas and Wireless Propagation Letters, 2004(3): 108-110.[3] Dey S, Mittra R. Compact microstrip patch antenna[J]. Microwave Opt. Technol. Lett, 1996(13): 12-14.[4] Chen Y J, Long Y L. The development of the small wideband microstrip antenna[J]. Systems Engineering and Electronics, 2000(22): 20-24.[5] Karacolak T, Topsakal E. A double-sided rounded bow-tie antenna (DSRBA) for UWB communication[J]. IEEE Antennas and Wireless Propagation Letters, 2006(5): 446-449. [6] George J, Deepukumar M, Aanandan C K. New compact microstrip antenna[J]. Electronics Letters, 1996(32): 509.[7] Jen-Fen Huang, Chih-Wen Kuo. Cpw-fed bow-tie slot antenna[J]. Microwave AndOptical Technology Letters, 1998(19): 358-360.[8] Ahmet Cemal Durgun, Constantine A. Balanis, Craig R. Birtcher, and David R. Allee, design, simulation, fabrication and testing of flexible bow-tie antennas[J]. IEEE Transactions on Antenas and Propagation, 2011(59): 4425-4435.[9] Ming-Tien Wu, Ming-Lin Chuang. Multibroadband slotted bow-tie monopole antenna[J]. IEEE Antennas and Wireless Propagation Letters, 2015(14): 887-890.。
Antenna for GPS
专利名称:Antenna for GPS发明人:Ching-Chia Mai,Cheng-Han Lee,Chi-YuehWang,Boon-Tiong Chua申请号:US11849393申请日:20070904公开号:US07652633B2公开日:20100126专利内容由知识产权出版社提供专利附图:摘要:This invention relates to an antenna for GPS. The antenna of the invention comprises a ground metal plate, a parasitic metal plate, a radiation metal plate and at least one supporting element. The parasitic metal plate is disposed above the groundmetal plate and connects to the ground metal plate. The radiation metal plate is an independent metal plate and is disposed above the ground metal plate. The parasitic metal plate cooperates with the radiation metal plate to induce a resonance mode. The supporting element is disposed on the ground metal plate and is used to support the radiation metal plate. Whereby, the problems of large size and limited receiving angle of signal according to a conventional circular polarization antenna for GPS could be improved.申请人:Ching-Chia Mai,Cheng-Han Lee,Chi-Yueh Wang,Boon-Tiong Chua地址:Kaohsiung TW,Kaohsiung TW,Kaohsiung TW,Kaohsiung TW国籍:TW,TW,TW,TW代理机构:Volentine & Whitt, PLLC更多信息请下载全文后查看。
天津大学信息与通信工程考研复习辅导资料及导师分数线信息
天津大学信息与通信工程考研复习辅导资料及导师分数线信息天津大学信息与通信工程考研科目包括政治、外语、数学一以及通信原理、信号与系统。
主要研究方向分为两个,方向一考试科目为通信原理,方向二考试科目为信号与系统,此专业是报考人数较多的专业,考生需进一步把握备考方向。
考试科目备注专业代码、名称及研究方向081000信息与通信工程①101思想政治理论②201英语一③301数学一④814通信原理①101思想政治理论②201英语一③301数学一④815信号与系统天津大学信息与通信工程考研录取情况院(系、所) 专业 报考人数 录取人数信息与通信工程506 95 电子信息工程学院(2012年)信息与通信工程463 92 电子信息工程学院(2013年)天津大学信息与通信工程2012年的报考人数为506人,录取人数为95人,2013年的报考人数为463人,录取人数为92人。
由真题可以发现,现在考点涉及的广度和深度不断扩宽和加深。
由天津考研网签约的天津大学在读本硕博团队搜集整理了天津大学电子信息工程学院信息与通信工程考研全套复习资料,帮助考生梳理知识点并构建知识框架。
真题解析部分将真题按照知识点划分,条理清晰的呈现在同学们眼前。
然后根据各个考点的近几年真题解析,让同学对热点、难点了然于胸。
只有做到了对真题规律和趋势的把握,8—10月底的提高复习才能有的放矢、事半功倍!天津大学电子信息工程学院信息与通信工程考研导师信息刘开华纵向课题经费课题名称情境感知服务位置信息获取机理与算法2009-01-01--2011-12-31负责人:刘开华科技计划:国家基金委拨款单位:国家基金委合同经费:32 课题名称智能航空铅封技术研究2010-01-01--2012-12-31 负责人:刘开华科技计划:天津市科技支撑计划重点项目拨款单位:天津市科学技术委员会合同经费:50 横向课题经费课题名称基于相位法的RFID定位技术2013-01-01--2013-12-31 负责人:刘开华科技计划: 拨款单位:中兴通信有限公司合同经费:16课题名称基于ADoc芯片组的产品开发2008-09-01--2009-08-31 负责人:刘开华科技计划: 拨款单位:THOMSON宽带研发(北京)有限公司合同经费:6.3 期刊、会议论文Tan, Lingling; Bai, Yu; Teng, Jianfu; Liu, Kaihua; Meng, WenqingTrans-Impedance Filter Synthesis Based on Nodal Admittance Matrix Expansion CIRCUITS SYSTEMS AND SIGNAL PROCESSINGnullTan, Lingling; Liu, Kaihua; Bai, Yu; Teng, Jianfu Construction of CDBA and CDTA behavioral models and the applications in symbolic circuits analysis ANALOG INTEGRATED CIRCUITS AND SIGNAL PROCESSINGnullMa Yongtao,Zhou Liuji,Liu Kaihua A Subcarrier-Pair Based Resource AllocationScheme Using SensorsnullMa Yongtao,Zhou Liuji,Liu Kaihua, Wang Jinlong Iterative Phase Reconstruction and Weighted IEEE sensorsnull罗蓬,刘开华,闫格基于FrFT能量重心谱校正的LFM信号参数估计信号处理null 潘勇, 刘开华,等 A novel printed microstrip antenna with frequency reconfigurable characteristics for Bluetooth/WLAN/WiMAX applications Microwave and Optical Technology Lettersnull阎格,刘开华,吕西午基于分数阶Fourier变换的新型时频滤波器设计哈尔滨工业大学学报nullLin Zhu, Kaihua Liu, Zhang Qijun, Yongtao Ma and Bo Peng An enhanced analytical Neuro-Space Mapping method for large-signal microwave device modeling null罗蓬,刘开华,于洁潇,马永涛一种相干宽带线性调频信号的波达方向估计新方法通信学报nullLin Zhu, Yongtao Ma, Qijun Zhang and Kaihua Liu An enhanced Neuro-Space Mapping method for nonlinear device modeling nullYue Cui, Kaihua Liu, Junfeng Wang Direction-of-arrival estimation for coherent GPS signals based on oblique projection Signal ProcessingnullLV Xi-wu, LIU Kai-hua, et al. Efficient solution of additional base stations in time-of-arrival positioning systems Electronics Lettersnull省部级以上获奖刘开华;等数字电视接收系统、软件技术的研发与应用”天津市科技进步奖三等奖2011-04-29李华;刘开华;等数字视频压缩与码流测试技术的研发及应用天津市科技进步奖二等奖2009-04-29知识产权刘开华, 于洁潇高速公路上车辆的车速和相对位置实时测量系统及方法刘开华;潘勇;于洁潇;陈征一种基于无联网的车载自动实时监控远程终端刘开华,黄翔东,于洁潇,王兆华,闫格基于相位差测距的RFID无线定位方法王安国纵向课题经费课题名称基带处理与天线协同2007-07-16--2011-11-16 负责人:王安国科技计划:国家科技部拨款单位:财政部合同经费:157.41课题名称无线网络多源稀疏协作编码研究2011-01-01--2013-12-31 负责人:韩昌彩科技计划:国家基金委拨款单位:国家基金委合同经费:20横向课题经费课题名称具有波束多选择性的多频段可重构天线研究2013-01-01--2014-12-31 负责人:王安国科技计划: 拨款单位:东南大学毫米波国家重点实验室合同经费:5课题名称双方向图算法在室内定位中的应用2012-01-01--2012-12-31 负责人:冷文科技计划: 拨款单位:中兴通讯股份有限公司合同经费:14.5期刊、会议论文马宁王安国姬雨初石和平Cooperative Space Shift Keying for Multiple-Relay Network IEEE Communications Lettersnull裴静王安国高顺,冷文Miniaturized Triple-Band Antenna With a Defected Ground Plane for WLAN/WiMAX Applications IEEE Antennas and Wireless Propagation Lettersnull赵国煌王安国冷文陈彬陈华Wideband internal antenna with coupled feeding for 4G mobile phone Microwave and Optical Technology Lettersnull陈彬王安国赵国煌Design of a novel ultrawideband antenna with dualband-notched characteristics Microwave and Optical technology lettersnull 蔡晓涛王安国马宁冷文 A Novel Planar Parasitic Array Antenna with Reconfigurable Azimuth pattern IEEE Antennas and Wireless Propagation Lettersnull 马宁王安国聂仲尔曲倩倩姬雨初Adaptive Mapping Generalized Space Shift Keying Modulation China Communicationsnull王安国蔡晓涛冷文带寄生贴片的圆盘形方向图可重构天线设计电波科学学报null 王安国陈彬冷文赵国煌一种小型化五频段可重构蝶形天线的设计电波科学学报null蔡晓涛王安国马宁冷文Novel radiation pattern reconfigurable antenna with six beam choices The Journal of China Universities of Posts and Telecommunicationsnull 曲倩倩王安国聂仲尔郑剑锋Block Mapping Spatial Modulation Scheme forMIMO Systems The Journal of China Universities of Posts and Telecommunicationsnull王安国刘楠兰航方向图可重构宽带准八木天线的设计天津大学学报null李锵纵向课题经费课题名称基于稀疏核支持向量机的音乐自动分类系统关键技术研究2009-06-01--2010-06-01 负责人:李锵科技计划: 拨款单位:天津大学建筑设计研究院合同经费:3课题名称jg预研项目2010-03-01--2010-12-01 负责人:李锵科技计划:拨款单位:渤海石油运输有限责任公司合同经费:3课题名称超声波热治疗中非侵入式温度成像与弹性成像关键技术研究2015-01-01--2018-12-31 负责人:李锵科技计划:国家自然科学基金项目拨款单位: 国家自然科学基金委员会合同经费:85课题名称高等学校学科创新引智计划综合管理平台的设计与开发2010-04-01--2012-04-01 负责人:李锵科技计划: 拨款单位:苏州国芯科技有限公司合同经费:3横向课题经费课题名称微粒捕集器数据采集系统开发2008-01-01--2008-06-01 负责人:李锵科技计划: 拨款单位:润英联新加坡私人有限公司合同经费:22.5课题名称电子系统可靠性增长建模与仿真2006-12-01--2008-01-01 负责人:李锵科技计划: 拨款单位:中国人民解放军海军航空工程学院合同经费:5期刊、会议论文李锵,滕建辅,赵全明,李士心Wavelet domain Wiener filter and its application in signal denoising null张立毅,李锵,刘婷,滕建辅The research of the adaptive blind equalizer's steady residual error null徐星,李锵,关欣Chinese folk instruments classification via statistical features and sparse-based representation null张立毅,李锵,刘婷,滕建辅Study of improved constant modulus blind equalization algorithm null张立毅,孙云山,李锵,滕建辅Study on the fuzzy neural network classifier blind equalization algorithm null郭继昌,滕建辅,李锵Research of the gyro signal de-noising method based on stationary wavelets transform null肖志涛,于明,李锵,国澄明Symmetry phase congruency: Feature detector consistent with human visual system characteristics nullCai wei,李锵,关欣Automatic singer identification based on auditory features. null李锵,滕建辅,王昕,张雅绮,郭继昌Research of gyro signal de-noising with stationary wavelets transform null郭继昌,滕建辅,李锵,张雅绮The de-noising of gyro signals by bi-orthogonalwavelet transform nullLiu Tianlong,李锵,关欣Double boundary periodic extension DNA coding sequence detection algorithm combining base content null关欣,滕建辅,李锵,苏育挺Blind acoustic source separation combiningtime-delayed autocorrelation and 4TH-order cumulants null张立毅,李锵,滕建辅Kurtosis-driven variable step size blind equalization algorithm with constant module nullQin Lu,李锵,关欣Pitch Extraction for Musical Signals with Modified AMDF null Zhang Xueying,李锵,关欣The Improved AMDF Gene Exon Prediction null 李锵,Jian Dong,Ming-Guo Wang,滕建辅Analysis and simulation of antenna protocol optimization for ad hoc networks nullFeng Yanyan,李锵,关欣Entropy of Teager Energy in Wavelet-domain Algorithm Applied in Note Onset Detection nullBao Hu, Li ShangSheng, 李锵,滕建辅Research on the technology of RFSS in large-scale universal missile ATE null张立毅,Haiqing Cheng,李锵,滕建辅 A research of forward neural network blind equalization algorithm based on momentum term null张立毅,李锵,滕建辅 A New Adaptive Variable Step-size Blind Equalization Algorithm Based on Forward Neural Network nullYutao Ma,李锵,Chao Li,Kun Li,滕建辅Design of active transimpedanceband-pass filters with different Q values International Journal of Electronicsnull 夏静静,李锵,刘浩澧,Wen-shiang Chen,Po-Hsiang Tsui An Approach for the Visualization of Temperature Distribution in Tissues According to Changes in Ultrasonic Backscattered Computational and Mathematical Methods in Medicinenull 耿晓楠,李锵,崔博翔,王荞茵,刘浩澧超声温度影像与弹性成像监控组织射频消融南方医科大学学报null谭玲玲, 李锵, 李瑞杰, 滕建辅Design of transimpedance low-pass filters International Journal of Electronicsnull李锵,李秋颖,关欣基于听觉图像的音乐流派自动分类天津大学学报(自然科学与工程技术版)nullChong Zhou, Wei Pang, 李锵, Hongyu Yu, Xiaotang Hu, HaoZhang, Extracting the Electromechanical Coupling Constant of Piezoelectric Thin Film by the High-Tone Bulk Acoustic Resonator IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency Controlnull朱琳, 李锵, 刘开华基于ADS的声表面波单端对谐振器建模压电与声光null董丽梦, 李锵, 关欣基于稀疏表示分类器的音乐和弦识别系统研究计算机工程与应用null关欣,李锵,田洪伟基于差分全相位MFCC的音符起点自动检测计算机工程null 关欣,李锵,郭继昌,滕建辅二、四阶组合时延统计量多乐器盲分离计算机工程与应用null杨甲沛, 李锵, 刘郑, 袁晓琳基于自适应学习速率的改进型BP算法研究计算机工程与应用null李锵, 张法朝, 张瑞峰System design of DPF data recorder and data analysisnull李锵, 袁晓琳, 杨甲沛Application of ant colony algorithm in the optimization of the time environmental conversion factor of the reliability models null 张立毅,白煜,李锵,滕建辅复数系统中五二阶归一化积累盲均衡算法的研究通信学报null郭继昌,关欣,李锵,刘志杨红外图像预处理系统中模拟视频输出时序设计电子技术应用null关欣,滕建辅,李锵,苏育挺,Wang Shu-Yan Blind source separation combining time-delayed second and fourth order statistics 天津大学学报(自然科学与工程技术版)null张立毅,李锵,滕建辅复数系统中三、二阶归一化累积量盲均衡算法的研究计算机工程与应用null张立毅,李锵,滕建辅经典盲均衡算法中稳态剩余误差的分析天津大学学报null 滕建辅,董健,李锵,关欣Design of maximally flat FIR filters based on explicit formulas combined with optimization 天津大学学报(英文版)null郭继昌,陈敏俊,李锵,关欣红外焦平面失效元处理方法及软硬件实现光电工程null 马杰,王昕,李锵,滕建辅基于特征值和奇异值分解方法的盲分离天津大学学报(自然科学与工程技术版)null李锵,郭继昌,关欣,滕建辅基于通用DSP的红外焦平面视频图像数字预处理系统天津大学学报(自然科学与工程技术版)null李锵,郭继昌,关欣,刘航,童央群基于DSP的红外焦平面视频图像数字处理系统的设计测控技术null马杰,滕建辅,李锵具有参考噪声源的多路传感器信号盲分离方法测控技术null 周郭飞,李锵,滕建辅微带扇形分支线在低通滤波器设计中应用电子测量技术null 李锵,滕建辅,李士心,肖志涛小波域Wiener滤波器信号的去噪方法天津大学学报(自然科学与工程技术版)null肖志涛,于明,李锵,唐红梅,国澄明Log Gabor小波性能分析及其在相位一致性中应用天津大学学报(自然科学与工程技术版)null罗批,李锵,郭继昌,滕建辅Improved genetic algorithm and its performance analysis 天津大学学报(英文版)null罗批,郭继昌,李锵,滕建辅一种实用的电子线路参数优化算法电路与系统学报null 罗批,李锵,郭继昌,滕建辅基于偏最小二乘回归建模的探讨天津大学学报null 知识产权李锵,闫志勇,关欣一种结合SVM和增强型PCP特征的和弦识别方法中国2014100089231李锵, 冯亚楠, 关欣基于Teager能量熵的音符切分方法学术专著(关欣, 杨爱萍, 白煜, 李锵), 信号检测与估计:理论与应用(译著), 电子工业出版社2012-01-31(白煜, 李锵), 模拟集成电路设计的艺术(译著), 人民邮电出版社2010-11-04(李锵,周进等), 无线通信基础(译著), 人民邮电出版社2007-06-30(李锵,董健,关欣,鲍虎), 数字通信(原书第2版)(译著), 机械工业出版社2006-02-28(张为,关欣,刘艳艳,李锵), 电子电路设计基础(译著), 电子工业出版社2005-10-01(张雅绮,李锵等), Verilog HDL高级数字设计(译著), 电子工业出版社2005-01-31(李锵,侯春萍,赵宇), 网络(原书第2版)(译著), 机械工业出版社2004-11-30(李锵,郭继昌), 无线通信与网络, 电子工业出版社2004-06-30本文内容摘自《天津大学814通信原理考研红宝书》,更多考研资料可登陆网站下载!。
单馈双频GPS微带天线
小型化双频段GPS微带天线*彭祥飞1,钟顺时1,许赛卿2,1,武强1(1.上海大学通信及信息工程学院,上海 200072;2. 浙江正原电气股份有限公司浙江嘉兴 314003)摘要:最近为了满足GPS定位准确性和可靠性的需要,要求天线在GPS两个频率上实现圆极化。
本文介绍一种通过单个探针馈电的双层正方形切角的微带贴片天线,采用不同介电常数的微波陶瓷基片。
及常规的双频圆极化天线相比,天线尺寸减小了且没有在两层贴片间引入空气层,结构紧凑,便于加工。
文中给出天线的详细设计及实验结果,并进行了讨论,实测结果证明了本设计的有效性。
关键词:微带天线;全球定位系统;双频段;圆极化;A COMPACT DUAL-BAND GPS MICROSTRIP ANTENNAPENG xiang-fei, ZHONG Shun-shi, XU Sai-qing , WU Qiang(1.School of Communication and Information Engineering,Shanghai University,Shanghai 200072;2.Zhejiang Zhengyuan electric limited Company , Jiaxing Zhejiang 314003)Abstract: Recently in order to satisfy the demanded precision and reliability for the globe positioning system(GPS) , the dual-band circularly polarized(CP) is required. This paper describes thedesign of a probe-fed stacking two corner-truncated square microstrip patch antennas, which are using two different relative permittivity microwave ceramic substrates. Comparing with the conventional dual-band CP antenna with a same low relative permittivity and an air-gap layer between two patches, the size of this antenna is reduced and its fabrication is easier. Details of the proposed antenna design and experimental results are presented and discussed .The measured results confirm the validity of this design.Key words:microstrip antenna;GPS;dual-band ; circular polarization1 引言近年来微带天线由于它的尺寸小,成本低,易实现圆极化等优点在全球定位系统(GPS)应用中独占鳌头。
平面小型化三频微带天线
平面小型化三频微带天线王公晗;冯全源【摘要】针对多频天线结构复杂,天线尺寸较大,设计了一款紧凑型结构的三频单极性微带贴片天线。
该天线的辐射单元由双C型结构和加载倒L型结构构成,利用低频段的高次模,从而产生天线的高频段。
该方法可以有效实现多频特性,并能够有效地减小天线尺寸。
天线尺寸仅为20×31×1.6 mm3。
实测频段为2.40~2.50 GHz,3.17~3.90 GHz,4.67~5.83 GHz。
该天线具有体积小,结构简单,辐射特性良好的优点,实现了对3.5/5.5 GHz WIMAX频段和2.4/5.2/5.8 GHz WLAN频段的全覆盖,能够很好的适用于无线通信系统的应用。
%This paper proposed a compact structure of tri-band microstrip antenna in order to solve the problems complex structure and the larger size of multi-frequency antenna.The antenna was composed by the two C-ring structures with a pair of inverted L-shaped stubs.Besides,this design utilized high-order mode to generate high frequency.This method could effectively achieve multi-frequency characteristics and reduced the antenna size. The experimental results showed that the antenna had the impedance bandwidths of 100MHz (2.40-2.50 GHz), 730MHz (3.17-3.90 GHz)and 1160 MHz (4.67-5.83 GHz),which could cover both WLAN in the 2.4/5.2/5.8 GHz bands and WIMAX in the 3.5/5.5 GHz bands.【期刊名称】《探测与控制学报》【年(卷),期】2014(000)005【总页数】4页(P64-67)【关键词】天线;三频;高次模;小型化【作者】王公晗;冯全源【作者单位】西南交通大学信息科学与技术学院,四川成都 610031;西南交通大学信息科学与技术学院,四川成都 610031【正文语种】中文【中图分类】TN8210 引言近年来,随着无线通信的迅速发展,各类天线的发展也受到越来越多的关注。
A Compact, High Isolation and Wide Bandwidth Antenna Array for Long Term Evolution Wireless Devices
A Compact,High Isolation and Wide Bandwidth AntennaArray for Long Term Evolution Wireless Devices Mina Ayatollahi,Qinjiang Rao,and Dong WangAbstract—A compact dual-port,multiple input-multiple output(MIMO) antenna array for handheld devices is introduced.The antenna structure consists of two quarter wavelength monopole slots etched on the ground plane of a printed circuit board(PCB)and a meandered slot cut between them.The meandered slot not only reduces the coupling between the two slot antennas,but also improves the bandwidth and efficiency of the array by acting as a radiating parasitic element.Simulated and measured results show that the meandered isolating slot allows the antennas to achieve wider bandwidth,higher efficiency,higher isolation and better diversity perfor-mance,compared to other types of isolating slots.Index Terms—Antenna mutual coupling,MIMO antennas,mobile de-vice,slot antennas.I.I NTRODUCTIONWith the emergence of new wireless standards such as long-term evolution(LTE),multiple-input-multiple output(MIMO)technology which uses multiple antennas,has become a very promising technique for enhancing the performance of wireless communication systems [1]–[3].Optimal MIMO performance requires low correlation between signals received by each of the antennas.This requires low mutual coupling between the antenna ports which is not normally possible in a compact device,because the antennas are closely spaced.The high mutual coupling,which is due to the surface waves induced in the ground plane,increases the received signal correlation and decreases diversity gain and channel capacity[4].To reduce the mutual coupling between the antenna elements,var-ious approaches have been used,including neutralization technique[5], simultaneous matching[6],etching slits in the middle of the ground plane[7]and using EBG substrates[8].These techniques either occupy a considerable space on the PCB or need special fabrication techniques. Another approach is etching an isolating slot between the antenna el-ements.For example a vertical slot[9],a T-shaped slot[10],or two L-shaped slots[11]have been used.Although these isolating slots re-duce the mutual coupling between the antennas,they do not improve their bandwidth.In this communication,a compact multiband MIMO antenna array for handheld devices is presented.The structure consists of two monopole radiating slots and a new meandered isolating slot, all etched along an edge of the ground plane of the PCB[12].As a design example,the proposed antenna system has been designed to operate in the2.6GHz LTE band(2.5–2.7GHz),as well as the2.5 GHz(2.4–2.5GHz)WLAN band.Simulated and experimental results, including S-parameters,radiation patterns,radiation efficiency and signal correlations,are presented and discussed.The results show that the meandered isolating slot reduces the mutual coupling between the two slot antennas and also acts as a radiating parasitic element, Manuscript received October25,2010;revised May30,2011;accepted May 04,2012.Date of publication July05,2012;date of current version October02, 2012.The authors are with the Research in Motion Limited(RIM),Waterloo,ON N2V2P1,Canada(e-mail:mayatollahi@).Color versions of one or more of thefigures in this communication are avail-able online at .Digital Object Identifier10.1109/TAP.2012.2207312Fig.1.MIMO slot antenna array.which introduces an additional resonance frequency and increases thebandwidth of the antennas.The performance of the proposed antennasystem has also been compared to the one with other isolating slotshapes such as T-shaped,vertical,a pair of L-shaped and also withoutan isolating slot.The comparisons show that the bandwidth of theproposed antenna system is4times the one when no isolation slot isused,and more than three times the bandwidth using other slot types.This communication is organized as follows.Section II presents thedesign and layout of the proposed antenna array.In Section III,the sim-ulated and measured results of the array are presented and compared tothe system without the isolating slot.The diversity parameters and per-formance of the proposed MIMO system are discussed in Section IV.Section V compares the performance of the proposed array to a similararray with other isolating slot shapes.Finally,Section VI provides theconcluding remarks.II.A NTENNA A RRAY S TRUCTUREAs shown in Fig.1,the proposed antenna structure consists of twoquarter wavelength radiating slots cut close to an edge of a groundplane,on one side of a FR4substrate with a thickness of1.5mm anda relative permittivity of4.4.The length and width of the substrate andthe ground plane are95mm and55mm,respectively.The antennasystem is designed to operate at2.6GHz LTE application band.Basedon the required impedance bandwidth and resonance frequency,the di-mensions of the radiating slots and their distance to the edge of theground plane,which are denoted by l,w,and d in Fig.1,has been op-timized using a Finite Difference Time Domain commercial software.These parameters have been obtained as20mm,1mm and3mm,re-spectively.Each antenna is fed with a50 impedance feed at a distanceof3mm from its closed end.A meandered isolating slot is cut between the two antennas,as shownin Fig.1.The width of the meandered slot is1mm and its total length isoptimized at about quarter of the wavelength at the center frequency of2.6GHz,which is around30mm.The lengths of the three arms of themeandered slot parallel to the top edge of the PCB are6mm,11mmand5mm,respectively.Other dimensions are shown in Fig.1.Basedon the optimized dimensions,the antenna array is prototyped and theantennas are fed by coaxial cables,as shown in Fig.2.0018-926X/$31.00©2012IEEEFig.2.Prototype of the antenna array with the meandered isolatingslot.Fig.3.Simulated and measured S parameters (dB)for antenna P1of Fig.1with and without (w/o)the meandered isolating slot.III.S IMULATED AND M EASURED R ESULTSTo investigate the effect of the meandered slot on the performance of the antenna array,antenna P1in Fig.1is excited at the frequency of 2.6GHz while the other antenna is terminated to a 50 load.The simulated S parameters of the array with and without (w/o)the meandered slot,and the measured S parameters of the prototype of Fig.2,are shown in Fig.3.The results obtained for port 2are similar and not presented here.A very good agreement between the simulated and measured S parameters is observed.As shown,the meandered slot has increased the isolation between the two ports from 8dB to 15dB at 2.6GHz,and the isolation is more than 15dB across the entire bandwidth.It is also observed that the meandered slot has increased the bandwidth of the antennas at 10dB return loss more than 4times,from 100MHz to more than 400MHz The bandwidth which is from 2.4–2.84,covers two application bands,LTE 2.6GHz and W ALN 2.5GHz.The S11plots show that in the structure with the meandered slot,there are two resonance frequencies close to each other,resulting in a wider band-width.Since the meandered slot has branches close to the excited an-tenna,there is a strong coupling between the two slots.The meandered slot is then parasitically fed through the excited antenna and acts as a parasitic radiator,contributing to the total radiation and improving the bandwidth.To demonstrate the effect of the meandered slot on the performance of the antennas,the current distribution on the ground plane with and without the meandered slot are obtained at the frequency of 2.6GHz and shown in Fig.4.As shown in Fig.4(a),a high concentration of current is observed on the ground plane close to the second antenna,and on the top edge of the ground plane,which demonstrates the high mutual coupling between the two slot antennas when the isolatingslotFig.4.Current distribution for the antenna array of Fig.1,when P1is excited.(a)Without the isolating slot.(b)With the meandered isolatingslot.Fig.5.Measured impedance curves for Port 1in the 2.4–2.7GHz frequency range.(a)Without the meandered slot.(b)With the meandered slot.is not used.As seen in Fig.4(b),adding the meandered slot reduces the current around the second antenna considerably.This is because the surface waves are suppressed from reaching the second antenna,which improves the isolation between the two antennas.Also,a strong current distribution around the meandered slot is ob-served,especially around the portion which is adjacent the excited an-tenna.This shows a strong coupling between the meandered slot and the excited antenna.The meandered slot acts as a parasitic radiating element coupled to the excited antenna and contributes to the total ra-diation.In addition,this coupling creates an additional resonance fre-quency for the excited antenna and improves the impedance bandwidth of the excited antenna considerably.This is shown in the measured input impedance of antenna P1,with and without the meandered slot,in Fig.5for the 2.4-2.7GHz frequency range.The simulated radiation patterns at the frequency of 2.6GHz are shown in Fig.6for antenna P1with and without (W/O)the isolating slot.As seen,the radiation pattern with the isolating slot is more omni-directional in the horizontal XY plane in the direction of the secondFig.6.Simulated gain patterns at 2.6GHz for radiating slot P1of Fig.1.(a)X -Y plane.(b)Y -Z plane.(c)X -Zplane.Fig.7.Measured radiation efficiency for antenna P1.antenna,compared to when the slot is not used.The simulated radiation efficiency of the antenna is also obtained at the frequency of 2.6GHz for both cases.The radiation efficiency without the meandered slot is obtained as 81.7%.The isolating slot increases the efficiency to 86.4%,which is due to the reduced mutual coupling between the slot antennas and also radiation from the meandered slot which acts as a parasitic radiating element.The measured radiation efficiency of antenna P1is shown in Fig.7.The measured radiation efficiency is around 78%at the frequency of 2.6GHz and more than 70%over the entire bandwidth.The measured radiation patterns of antenna P1is shown in Fig.8for the frequency of 2.6GHz.It should be noted that the simulated gain patterns and effi-ciency are obtained by considering the conductor and dielectric losses of the structure,but with the assumption of an ideal feeding arrange-ment.The measured results include the insertion loss of the actual feed network and connector and cable loss.Therefore there are some dis-crepancies between the measured and simulated radiation patterns and efficiency as a result of the physical feeding arrangement.IV .D IVERSITY P ERFORMANCE OF THE A NTENNA A RRAYThe envelope correlation coefficient (ECC)is used to evaluate the diversity performance of multi antenna systems.The envelope correlation coefficient can be calculated using the far-field pattern data [13].Diversity gain is obtained when the envelope correlation coefficient is less than 0.5,and in uniform environment,when the radiation efficiencies of the two antennas are close toeachFig.8.Measured radiation patterns at the frequency of 2.6GHz for antenna P1.(a)X -Y plane.(b)Y -Z plane.(c)X -Z plane.TABLE ID IVERSITY P ARAMETERS OF THE MIMO A RRAY OF F IG .1.TABLE IIP ERFORMANCE C OMPARISON OF THE S TRUCTURE OF F IG .1W ITH V ARIOUSI SOLATING S LOT SHAPESother.The envelope correlation coefficient of the antenna array of Fig.1has been computed and shown in Table I for various frequencies in the operating bandwidth.The uniform angular power spectrum and isotropic environment is considered for this calculation.It is observed that the envelope correlation is close to zero over the bandwidth,which means that the patterns of the two antennas are de-correlated and demonstrates excellent diversity condition.V .C OMPARISON W ITH O THER I SOLATING S LOT S HAPESThe radiation and diversity performance of the antenna array of Fig.1is simulated and compared to the performance of the array when other isolating slot shapes are used in place of the meandered slot.The slot shapes that are considered are T-shaped,dual L and a quarter wavelength vertical slot.The isolating slot in each case is also designed for a center frequency of 2.6GHz using the commercial FDTD software,and the antenna parameters have been obtained using the same software.Table II shows the simulated results for each case.As seen above,the meandered isolating slot provides a significantly broader bandwidth,higher gain and higher efficiency compared to other slot shapes and when no isolating slot is used.The variation of the gainof the antenna structure with meandered isolating slot is from3.3dB at 2.4GHz to2.87dB at2.8GHz with a maximum of3.6dB at2.6GHz.VI.C ONCLUSIONSA compact low mutual coupling MIMO antenna array for mobile handsets has been presented.The radiating elements are quarter wave-length slot antennas and a meander shaped slot has been used between the two antennas to isolate them.The measured and simulated S param-eters and the impedance Smith chart show that the meandered slot not only improves the isolation of the radiating elements,but also improves the bandwidth of the antennas significantly by coupling to the excited antenna and introducing additional resonance frequency for it.The an-tenna structure covers a broad bandwidth between2.4–2.84GHz,suit-able for LTE2.6GHz and WLAN2.5GHz.The diversity parameters of the array have been evaluated,which show a very good diversity performance.The measured and simulated radiation performance of the proposed array has been evaluated.The simulated performance has been compared with the ones of a similar two element slot array,but with other shapes of isolating slot.The results show that the proposed design has obvious advantages over other isolating slot shapes in terms of bandwidth,efficiency,isolation and diversity performance.R EFERENCES[1]W.C.Y.Lee,Mobile Communications Engineering.New York:Wiley,1982.[2]R.G.Vaughan and J.B.Andersen,“Antenna diversity in mobile com-munications,”IEEE Trans.Veh.Technol.,vol.36,pp.149–172,Nov.1987.[3]J.S.Colburn,Y.Rahmat-Samii,M.A.Jensen,and G.J.Pottie,“Eval-uation of personal communications dual antenna handset diversityperformance,”IEEE Trans.Veh.Technol.,vol.47,pp.737–746,Aug.1998.[4]S.Lu,T.Hui,and M.Bialkowski,“Optimizing MIMO channel capac-ities under the influence of antenna mutual coupling,”IEEE AntennasWireless Propag.Lett.,vol.7,pp.287–290,2008.[5]A.Diallo,C.Luxey,P.Le Thuc,R.Staraj,and G.Kossiavas,“En-hanced two-antenna structures for universal mobile telecommunica-tions system diversity terminals,”IET Microw.,Antennas Propag.,vol.2,pp.93–101,Feb.2008.[6]J.Rahola and J.Ollikainen,“Analysis of isolation of two-port antennasystems using simultaneous matching,”in Proc.Eur.Conf.on An-tennas and Propagation:EuCAP,Edinburgh,U.K.,Nov.2007,pp.11–16.[7]C.-Y.Chiu,C.-H.Cheng,R.D.Murch,and C.R.Rowell,“Reductionof mutual coupling between closely packed antenna elements,”IEEETrans.Antennas Propag.,vol.55,pp.1732–1738,Jun.2007.[8]F.Yang and Y.Rahmat-Samii,“Microstrip antennas integrated withelectromagnetic band-gap(EBG)structures:A low mutual couplingdesign for array applications,”IEEE Trans.Antennas Propag.,vol.51,pp.2936–2946,Oct.2003.[9]M.Karaboikis,C.Soras,G.Tsachtsiris,and V.Makios,“Compactdual-printed inverted F antenna diversity systems for portable wire-less devices,”IEEE Antennas Wireless Propag.Lett.,vol.3,pp.9–14,2004.[10]H.-T.Chou,H.-C.Cheng,H.-T.Hsu,and L.-R.Kuo,“Investigationsof isolation improvement techniques for multiple input multiple output(MIMO)WLAN portable terminal applications,”Progr.Electromagn.Res.,vol.PIER85,pp.349–366,2008.[11]K.Kim,W.Lim,and J.Yu,“High isolation internal dual band planarinverted-F antenna diversity system with band-notched slots for MIMOterminals,”in Proc.36th Eur.Microwave Conf.,2006,pp.1414–1417.[12]M.Ayatollahi,Q.Rao,and D.Wang,“Wideband High Isolation TwoPort Antenna Array for Multiple Input Multiple Output Handheld De-vices,”U.S.patent8085202.[13]T.Taga,“Analysis for mean effective gain of mobile antennas in landmobile radio environments,”IEEE Trans.Veh.Technol.,vol.39,pp.117–131,May1990.Experimental Characterization of a BroadbandTransmission-Line Cloak in Free SpacePekka Alitalo,Ali E.Culhaoglu,Andrey V.Osipov,Stefan Thurner,Erich Kemptner,and Sergei A.Tretyakov Abstract—The cloaking efficiency of afinite-size cylindrical transmis-sion-line cloak operating in the X-band is verified with bistatic free space measurements.The cloak is designed and optimized with numerical full-wave simulations.The reduction of the total scattering width of a metal ob-ject,enabled by the cloak,is clearly observed from the bistatic free space measurements.The numerical and experimental results are compared re-sulting in good agreement with each other.Index Terms—Scattering,scattering cross section.I.I NTRODUCTIONThe transmission-line cloak concept has been recently introduced [1],[2]as an alternative to the transformation-optics[3]–[7]and scat-tering cancellation approaches[8]–[10].In addition to these,there exist several other cloaking techniques and variations of these concepts.A detailed overview can be found,e.g.,in recent review papers[2],[6], [7],[9].Instead of utilizing anisotropic(and often resonant)metamaterials [6],[7]or plasmonic materials[9],the transmission-line cloak enables the electromagnetic wave to smoothly travel through the cloaked ob-ject inside a volumetric network of transmission lines,resulting in a simple and cheap way to obtain broadband cloaking of objects with se-lected geometries.It should be emphasized that the transmission-line cloak can only“hide”objects thatfit inside the volumetric network of transmission lines[2],i.e.,these objects cannot be bulky and electri-cally large objects.The technique allows cloaking of arrays of electri-cally small objects or mesh-like objects that let transmission lines go through them.A clear distinction should be made between cloaks that can hide an object in free space and the so-called ground-plane cloaks that can be used to hide an object above a boundary[11].In ground-plane cloaks the complexity of the material parameters is not as demanding as in cloaks operating in free space.Recent developments in ground-plane cloaks show that it is possible to realize such devices even for large objects operating within the visible frequency spectrum[12]–[15].In this work we study afinite-size,three-dimensional transmission-line cloak that can hide a three-dimensional metallic object from elec-tromagnetic waves in free space.The basic cloak geometry is known from previous results[2]and the dimensions of the cloak are here op-timized for operation in the X-band(8GHz–12GHz).The previous realizations of the cylindrical transmission-line cloak utilized a cou-pling layer made of widening metal strips to couple the electromagnetic Manuscript received October07,2011;revised January18,2012;accepted May11,2012.Date of publication July10,2012;date of current version October 02,2012.This work was supported in part by the Academy of Finland and Nokia through the centre-of-excellence program.The work of P.Alitalo was supported by the Academy of Finland via post-doctoral project funding.P.Alitalo and S.A.Tretyakov are with the Department of Radio Science and Engineering/SMARAD Centre of Excellence,Aalto University School of Elec-trical Engineering,FI-00076Aalto,Finland(e-mail:pekka.alitalo@aalto.fi).A.E.Culhaoglu,A.V.Osipov,S.Thurner and E.Kemptner are with the Microwaves and Radar Institute,German Aerospace Center(DLR),82234 Wessling,Germany.Color versions of one or more of thefigures in this communication are avail-able online at .Digital Object Identifier10.1109/TAP.2012.22073390018-926X/$31.00©2012IEEE。
基于缝隙耦合的微带天线设计
Lu SiweiꎬShan ZhiyongꎬCheng YunpengꎬOu Yang
( School of Information Science and TechnologyꎬDonghua UniversityꎬShanghai 201600ꎬChina)
Abstract:Broadband antennaꎬwhich can be applied to radio frequency identificationꎬglobal microwave wireless Internet and wireless lo ̄ cal area network ( WLAN) ꎬis becoming more and more demandingꎬsuch as small size and low cost. Microstrip antenna is small in sizeꎬ low in profile and high in integration. It is suitable for mass productionꎬbut its bandwidth is narrow and its application range is limited. In this paperꎬa compact broadband microstrip patch antenna is proposed. The antenna introduces L ̄slots and triangular slots. The simu ̄ lation results show that the impedance bandwidth of the antenna - 10 dB can reach 100% ꎬand its working frequency bandwidth is 1. 5 GHz ~ 4. 3 GHzꎻ the axial ratio bandwidth is 3. 4 GHz ~ 3. 8 GHzꎬand the circular polarization bandwidth is 11% . The gain in this range is all over 3 dBꎻthe wide bandwidth and high gain characteristics are realized in the whole working frequency band rangeꎬwhich are suitable for radio frequency identificationꎬBluetoothꎬand circular polarization WLAN frequency band. Key words: WLANꎻ broadbandꎻ microstrip patch antennaꎻ gainꎻ circular polarization
资深人士关于PIFA天线的理解与讨论
1。
PIFA天线是微带天线演变而来。
很多的英文资料介绍Patch Antenna,建议看看基本原理。
最简单的patch天线是一个金属片平行放置于地平面上,用同轴线或者微带线馈电即可。
其辐射主要靠边缘场。
假设该天线平行于大地放置,其形状为矩形,长边左右摆放,长边的长度为1/4波长。
如果左边缘的场是从patch到地,那么右边缘刚好反向从地到将左右两个边缘的电场分解成水平和垂直分量,你会发现垂直分量抵消,水平分量加强。
这样将会产生平行于地平面的线极化远场。
就手机而言,pifa天线的主极化一般是平行于手机主地平面。
此时,可以得到两个基本结论,1)这种天线的谐振波长为贴片长边的4倍(实际中请考虑介质的波长缩短效应,正比于1/sqrt(epsilon);2)这种天线的辐射主要靠边缘。
而边缘的场越往外倾斜,辐射越好(开放场)。
这就是为什么PIFA天线的高度如此重要的原因。
2。
加一个接地片(很多加在馈电附近)后,从微观角度来看贴片上的电流将改变流向,部分电流从右侧会流回来再回到地。
这样天线的谐振频率就会降低,一般波长会在4倍于贴片长边和短边之和左右(同样要考虑波长缩短效应)。
从另一个角度来说,馈电柱与短路柱是一段双线传输线。
它将变换天线的阻抗。
是一种变压器效应,它将部分容抗变换成感抗,从而使整个天线形成谐振。
这段线越长(极限是长到1/4波长)其变化效果越明显(越敏感,实际中就是天线的高度增加)。
传输变换原理大家应该清楚。
当改变馈电柱和短路柱的横向尺寸或者他们之间的距离时,实际上你是在改变该段传输线的特征阻抗。
也就相应地改变变换公式中平方的那部分。
这就是为什么我们常说馈电电和短路的改变将比较大的改变天线的阻抗。
同时也是为什么说PIFA天线一般可以不要匹配电路可以优化的(事实上,加匹配有时候会反而降低天线的传输性指标)。
3。
这个问题的解释是要配上图可能会更清楚。
的确有些问题是要有坚实的理论基础以及现实经验才会有比较深的理解的。
实验10:微带天线(MicrostripAntenna)
实验十: 微带天线(Microstrip Antenna ) **一、实验目的:1.了解天线之基原理与微带天线的设计方法。
2.利用实验模组的实际测量得以了解微带天线的特性。
二、预习内容:1.熟悉天线的理论知识。
2.熟悉天线设计的理论知识。
三、实验设备:四、理论分析:天线基本原理:天线的主要功能是将电磁波发射至空气中或从空气中接收电磁波。
所以天线亦可视为射频发收电路与空气的信号耦合器。
在射频应用上,天线的类型与结构有许多种类。
就波长特性分有八分之一波长、四分之一波长、半波天线;就结构分,常见有单极型(Monopole )、双极型(Dipole )、喇叭型(Horn )、抛物型(Parabolic Disc )、角型(Corrner )、螺旋型(Helix )、介电质平面型(Dielectric Patch )及阵列型(Array )天线,如图9-1所示。
就使用频宽来分别有窄频带型(Narrow-band,10%以下)及宽频带型(Broad-band,10%以上)。
(a)单极型(b)偶极型 (c)喇叭型λ/ 2图9-1 常见天线(一)天线特性参数1. 天线增益(Antenna Gain ’G ):isotropicP P G =其中 G ——天线增益P ——与测量天线距离R 处所接收到的功率密度,Watt / m 2Pisotropic —— 与全向性天线距离R 处所接收到的功率密度,Watt / m 2由此可推导出,与增益为G 的天线距离R 处的功率密度应为接收功率密度:24R P G P tx rec ⋅⋅=π其中 G ——天线增益P tx ——发射功率,Watt / m 2 R ——与天线的距离,m2. 天线输入阻抗(Antenna Input Impedance ’Zin ):IV Z in =其中 Z in ——天线输入阻抗V ——在馈入点上的射频电压 I ——在馈入点上的射频电流以偶极天线为例,其阻抗由中心处73Ω变化到末端为2500Ω。
超宽频微带天线设计
Ultra-Wideband Microstripe Antenna Design陳建宏Chien-Hung Chen摘要近十年來由於微帶天線具有體積小、重量輕、製作容易、價格低廉、可信度高,同時可附著於任何物體之表面上的特性,在無線通訊的應用上扮演著重要的角色。
本文將利用全平面正方形單極微帶天線當作設計天線的原型,藉由調整金屬貼片的上緣、下緣部份與接地面的上緣部份來研製適用於超寬頻通訊系統的微帶天線。
由模擬與實驗結果比較得知,可以發現其響應非常吻合,是一個適用於超寬頻通訊產品的天線。
關鍵詞:微帶天線、單極、超寬頻、簡介美國聯邦通信委員會(Federal Communication Commission,FCC)在西元2002年2月14日允許超寬頻技術使用於消費性電子產品上,並公佈了初步規格,FCC開放3.1GHz~10.6GHz提供超寬頻通信及測試使用。
為了研究開發適用於此頻段的天線技術。
將利用微帶天線的優點:體積小、重量輕、低成本、容易製作等特性,來研製適用於超寬頻通訊系統的微帶天線。
傳統的寬頻天線[2]中有行進波線天線(Traveling-Wave Wire Antenna)、螺旋形天線(Helical Antenna)、偶極圓錐形天線(Biconical Antenna)、單極圓錐形天線(Monoconical Antenna)、盤錐形天線(Discone Antenna)、袖子形天線(Sleeve Antenna)、渦狀天線(Spiral Antenna)和對數週期天線(Log-Periodic Antenna),不過其中適用於超寬頻系統的只有偶極圓錐形天線、單極圓錐形天線和盤錐形天線[3]。
因為其不僅有大的輸入阻抗頻寬(Large Input Impedance Bandwidth)、其輻射場形(Radiation Pattern)也能控制在一定的頻寬中。
利用虛像法(Method of Image)[4]及接地面(Ground Plane)來使偶極天線變成單極天線,從早期的線型單極天線-窄頻(Narrowband),演化成單極圓錐形天線-中頻寬(Intermediate),到最後的火山煙狀天線(V olcano Smoke Antenna)-寬頻(Broadband)[5]。
基于GPS卫星导航系统的天线设计
本科毕业设计(论文)基于GPS卫星导航系统的天线设计学院自动化学院专业电子信息科学与技术级(11)班年级班别2007级(学号**********学生姓名黄龙华指导教师李学识2011年6月基于G P S 卫星导航系统的天线设计黄龙华自动化学院摘要随着卫星定位系统在军事、通信、农业、防灾等方面得到了广泛的应用,特别是在军事上发挥着不可或缺的重要地位,更多的国家大力发展属于自己的卫星导航系统。
全球定位系统(GPS)在生活中的使用更为广泛,天线作为全球定位系统的重要部分,为GPS的精确度、灵敏度以及可靠性提供了保障。
GPS天线正沿着多频段、圆极化以及宽频带的方向发展。
本文首先介绍全球定位系统(GPS)的组成,然后介绍常用的微带天线的理论分析方法,其中包括传输线模型理论、空腔模型理论以及全波理论,然后介绍了单馈电和双馈点这两种微带天线圆极化实现方法。
根据微带天线的传输线模型理论,设计了GPS单频段圆极化微带天线以及基于双层结构的GPS双频段微带天线,其中单频段以及双频段圆极化微带天线都使用了单馈电方式实现其圆极化。
本次设计使用采用有限元法的Ansoft HFSS全波三维电磁场仿真软件,对天线的设计进行了大量的数据仿真。
设计出分别工作在全球卫星定位系统的L1频段(1575.42MHz)以及L2频段(1227.60MHz)的单频段圆极化微带天线,同时设计出能够同时工作在L1频段和L2频段的双频段圆极化微带天线,并满足全球卫星导航系统的天线要求。
关键词:圆极化,单馈电,双频天线,微带天线,全球定位系统注:本设计(论文)题目来源于教师的校级科研项目,项目编号为:405115008。
AbstractAlong with the satellite positioning system has been widely applied in military,communications,agriculture,disaster prevention,etc.Especially in the military is playing a very important position.So the more countries develop belongs to own satellite navigation system.Global positioning system(GPS)is used more widely in the live.Antenna is an important part of the global positioning system,maintained precision,sensitivity and reliability of GPS.The antenna of GPS is walking along much frequency band,circular polarization and wideband direction.This essay first introduces global positioning system(GPS),then introduces the used theoretical analysis method of microstrip antennas,including transmission line model theory,cavity model theory and the wave theory.At the same time,introduces the microstrip antenna circular polarization method of the sheet feeder and doubly-fed point.According to transmission line model theory,designs the signal-frequency interference and double frequency band circular polarization microstrip antennas of GPS,the signal-frequency interference and double frequency band circular polarization microstrip antennas of GPS used single feeder realize its circular polarization.This design using the finite element method Ansoft HFSS,a full-wave three-dimensional electromagnetic simulation software.Through to large amounts of data simulation for antenna performance,designed the optimization of antenna.Finished the circular polarization microstrip antennas of GPS working in the L1band(1575.42 MHz)and L2band(1227.60MHz),but also finishen the double frequency band circular polarization microstrip antennas of GPS,and corresponded the antenna's requirements of global satellite navigation system.Key words:Circular polarization,Single feeder,Double-frequency antenna,Microstrip antenna,Global positioning system目录1绪论 (1)1.1引言 (1)1.2GPS终端天线研究现状 (2)1.2.1微带天线 (2)1.2.2GPS天线的研究进展 (3)1.3GPS卫星导航系统天线的要求 (4)1.4本文主要工作 (5)2微带天线理论分析 (6)2.1微带天线辐射原理 (6)2.1.1传输线模型理论 (7)2.1.2空腔模型理论 (9)2.1.3全波理论 (10)2.2微带天线的馈电方法 (11)2.2.1微带线馈电 (11)2.2.2同轴线馈电 (12)2.2.3电磁耦合馈电 (12)2.3微带天线圆极化技术 (13)2.3.1圆极化波 (13)2.3.2微带天线圆极化实现方法 (13)2.4本章小结 (15)3GPS圆极化微带贴片天线的设计与优化 (16)3.1使用HFSS建立微带天线模型 (16)3.2GPS单频段微带天线的设计与优化 (17)3.2.1GPS单频段天线的设计指标 (17)3.2.2L2频段的微带天线设计与优化 (18)3.2.2L1频段的微带天线设计与优化 (21)3.3GPS双频段微带天线的设计与优化 (24)3.4介质对微带天线频率带宽以及增益的影响 (29)3.5介质层高度对微带天线阻抗带宽以及增益的影响 (30)3.6本章小结 (31)结论 (32)参考文献 (34)致谢 (36)1绪论1.1引言随着科学技术的不断发展,当今社会已进入电子信息时代。
Lassen iQ GPS模块说明书
Key Featuresand Benefits• Ultra-low power: 86 mW• Trimble quality at low cost• Aided GPS through TSIP for faster acquisition• Dual sensitivity modes with automatic switching• 12-channel simultaneous operation • Supports NMEA 0183, TSIP, TAIP and DGPS Lassen iQ GPS ModuleLow-power, high-quality GPS solution for your mobile productsT rimble’s Lassen® iQ module isone smart buy. It adds powerful,12-channel GPS functionalityto your mobile product in apostage-stamp-sized footprintwith ultra-low power consump-tion and extreme reliability—allat a very economical price.Designed for portable handheld,battery-powered applicationssuch as cell phones, pagers,PDAs, digital cameras, and manyothers, the module is also idealfor standard GPS applicationssuch as tracking.The 12-channel Lassen iQmodule is fully compatible withT rimble’s popular Lassen SQmodule. Using T rimble’s break-through, patented FirstGPS®architecture, the module deliverscomplete position, velocity andtime (PVT) solutions for use inthe host application.Powerful PerformanceThe Lassen iQ module fea-tures two GPS signal sensitivitymodes: Standard and Enhanced.With Enhanced mode enabled,the module automaticallyswitches to higher sensitivitywhen satellite signals are weak.The module also supports TSIPdownload of critical startupinformation for fast acquisition.This aided GPS (A-GPS) startupprovides hot start performancefor each power-up.The Lassen iQ module is the onlystamp-sized GPS product thatsupports the four most popu-lar protocols: DGPS (RTCM),TSIP(T rimble Standard InterfaceProtocol), TAIP (T rimble ASCIIInterface Protocol) and NMEA 0183.The Lassen iQ module combinesT rimble performance and qual-ity with low cost. With an MTBF(mean time between failures) fi gureof 60 years, it is one of the most reli-able GPS receivers on the market.HardwareA metal shield encloses themodule for protection and easeof handling. The package hasa small form factor, (approxi-mately 26 mm x 26 mm,including the shield). It typi-cally requires less than 90 mWof power at 3.3 VDC.The highly integrated moduleis a miniature board containingT rimble GPS hardware corebased on our Colossus® RFASIC and IO-TS digital signalprocessor (DSP), a 32-bit RISCCPU and fl ash memory.AntennasThe Lassen iQ module is com-patible with active, 3.3-VDCantennas. Three such antennasare available from T rimble andare recommended for use accord-ing to your application; see thereverse side for antenna details.The module provides both anten-na open and short detection plusantenna short protection.Starter KitThe Lassen iQ Starter Kit pro-vides everything you need toget started integrating state-of-the-art GPS capability into yourapplication.Lassen iQ GPS receiver with metal shieldLassen iQ GPS ModuleLow-power, high-quality GPS solution for your mobile productsVibration0.008 g 2/Hz 5 Hz to 20 Hz 0.05 g 2/Hz 20 Hz to 100 Hz–3 dB/octave 100 Hz to 900 HzOperating Humidity5% to 95% R.H. non-condensing, at +60° CEnclosureMetal enclosure with solder mounting tabs Dimensions26 mm W x 26 mm L x 6 mm H(1.02” W x 1.02” L x 0.24” H)Weight6.5 grams (0.2 ounce) including shieldnGothDEMI 7ptModuleLassen iQ module, in metal enclosure with soldermounting tabs Starter Kit Includes Lassen iQ module mounted on interface motherboard in a durable metal enclosure, AC/DC power converter, compact magnetic-mount GPS antenna, ultra-compact embedded antenna, serial interface cable, cigarette lighter adapter, TSIP , NMEA, and TAIP protocols, software toolkit and manual on CD-ROMAntenna Transition Cable, MCXRF cable for connecting antennas with MCX connector to on-module H.FL-RF connector. Cable length: 10 cmAntenna Transition Cable, SMARF cable for connecting antennas with SMA connector to on-module H.FL-RF connector.Cable length: 12.9 cm.Ultra-Compact Embedded Antenna3.3V active miniature unpackaged antennaCable length: 8 cmDim: 22 mm W x 21 mm L x 8 mm H (0.866” x 0.827” x 0.315”)Connector: HFL; mates directly to on-module RF connectorCompact Unpackaged Antenna3V active micropatch unpackaged antenna Cable length: 11 cmDim: 34.6 mm W x 29 mm L x 9 mm H (1.362” x 1.141” x 0.354”)Connector: MCX; mates through the optional RF transition cable to on-module RF connectorCompact Magnetic-Mount Antenna, MCX or SMA3V active micropatch antenna with magnetic mount Cable length: 5 mDim: 42 mm W x 50.5 mm L x 13.8 mm H (1.65” x 1.99” x 0.55”)Connectors: MCX or SMA, mates through the optional RF trasition cable to the module RF connectorSpecifi cations subject to change without notice.© C o p y r i g h t 2004, T r i m b l e N a v i g a t i o n L i m i t e d . A l l r i g h t s r e s e r v e d . T h e G l o b e a n d T r i a n g l e , T r i m b l e , C o l o s s u s , F i r s t G P S , a n d L a s s e n a r e t r a d e m a r k s o f T r i m b l e N a v i g a t i o n L i m i t e d r e g i s t e r e d i n t h e U n i t e d S t a t e s P a t e n t a n d T r a d e m a r k O f fi c e . A l l o t h e r t r a d e m a r k s a r e t h e p r o p e r t y o f t h e i r r e s p e c t i v e o w n e r s . T I D 13442 (9/04)• 12-channel simultaneous operation• Ultra-low power consumption: less than 90 mW (27 mA) @ 3.3 V • Dual sensitivity modes with automatic switching • Aided GPS through TSIP• Antenna open and short circuit detection and protection • Compact size: 26 mm W x 26 mm L x 6 mm H• Supports NMEA 0183, TSIP , TAIP , DGPS protocols • Trimble quality at low costGeneralL1 (1575.42 MHz) frequency, C/A code, 12-channel,continuous tracking receiverUpdate Rate TSIP @ 1 Hz; NMEA @ 1 HZ; TAIP @ 1 Hz Accuracy Horizontal: <5 meters (50%), <8 meters (90%) Altitude: <10 meters (50%), <16 meters (90%) Velocity: 0.06 m/sec PPS (static): ±50 nanosecondsAcquisition (Autonomous Operation in Standard Sensitivity Mode) Reacquisition: <2 sec. (90%) Hot Start: <10 sec (50%), <13 sec (90%) Warm Start: <38 sec (50%), <42 sec (90%) Cold Start: <50 sec (50%), <84 sec (90%)Cold start requires no initialization. Warm start implies last position, time and almanac are saved by backup power. Hot start implies ephemeris also saved.Operational (COCOM) LimitsAltitude: 18,000 mVelocity: 515 m/sEither limit may be exceeded, but not bothConnectorsI/O:8-pin (2x4) 2 mm male header, micro terminal strip ASP 69533-01 RF: Low-profi le coaxial connectorH.FL-R-SMT (10), 50 Ohm Serial Port 2 serial ports (transmit/receive)PPS3.3 V CMOS-compatible TTL-level pulse, once per secondProtocolsTSIP , TAIP , NMEA 0183 v3.0, RTCM SC-104 NMEA MessagesGGA, VTG, GLL, ZDA, GSA, GSV and RMC Messages selectable by TSIP commandSelection stored in fl ash memory- BFranGothDEMI 7ptPrime Power+3.0 VDC to 3.6 VDC (3.3 V typ.) Power ConsumptionLess than 90 mW (27 mA) @ 3.3 VBackup Power +2.5 VDC to +3.6 VDC (3.0V typ.)Ripple Noise Max 60 mV, peak to peak from 1 Hz to 1 MHz Antenna Fault Protection Open and short circuit detection and protectionOperating Temperature –40° C to +85° C Storage Temperature–55° C to +105° CT rimble Navigation Limited is not responsible for the operation or failure of operation ofGPS satellites or the availability of GPS satellite signals.Trimble Navigation Limited Corporate Headquarters 645 North Mary Avenue Sunnyvale, CA Trimble Navigation Europe Ltd, UKPhone: 44 1256-760-150Trimble Export Ltd, Korea Phone: 82-2-5555-361***********************Trimble Navigation Ltd, ChinaPhone: 86-21-6391-7814/iQ。
Microstrip Antenna
1An Introduction to Microstrip Antennas1.1IntroductionDeschamps first proposed the concept of the MSA in1953[1].However, practical antennas were developed by Munson[2,3]and Howell[4]in the 1970s.The numerous advantages of MSA,such as its low weight,small volume,and ease of fabrication using printed-circuit technology,led to the design of several configurations for various applications[5–9].With increas-ing requirements for personal and mobile communications,the demand for smaller and low-profile antennas has brought the MSA to the forefront.An MSA in its simplest form consists of a radiating patch on one side of a dielectric substrate and a ground plane on the other side.The top and side views of a rectangular MSA(RMSA)are shown in Figure1.1.However, other shapes,such as the square,circular,triangular,semicircular,sectoral, and annular ring shapes shown in Figure1.2,are also used.Radiation from the MSA can occur from the fringing fields between the periphery of the patch and the ground plane.The length L of the rectangular patch for the fundamental TM10mode excitation is slightly smaller than/2,whereis the wavelength in the dielectric medium,which in terms of free-space wavelengtho is given aso/√⑀e,where⑀e is the effective dielectric constant of a microstrip line of width W.The value of ⑀e is slightly less than the dielectric constant⑀r of the substrate because thefringing fields from the patch to the ground plane are not confined in the12Broadband Microstrip AntennasFigure1.1MSA configuration.Figure1.2Different shapes of microstrip patches.dielectric only,but are also spread in the air.To enhance the fringing fields from the patch,which account for the radiation,the width W of the patch is increased.The fringing fields are also enhanced by decreasing the⑀r or by increasing the substrate thickness h.Therefore,unlike the microwave integrated circuit(MIC)applications,MSA uses microstrip patches with larger width and substrates with lower⑀r and thicker h.The details of various substrates used for MSA are given in Appendix A.For MSA applications in the microwave frequency band,generally h is taken greater than or equal to 1/16th of an inch(0.159cm).A typical comparison of MSA with MIC in the microwave frequency range is given in Table1.1.An Introduction to Microstrip Antennas3Table1.1A Comparison of MIC and MSAMIC MSAh≤0.159cm≥0.159cm⑀r≥9.8≤9.8W Small LargeRadiation Minimized Maximized1.2Characteristics of MSAsThe MSA has proved to be an excellent radiator for many applications because of its several advantages,but it also has some disadvantages.The advantages and disadvantages of the MSA are given in Sections1.2.1and 1.2.2.1.2.1AdvantagesMSAs have several advantages compared to the conventional microwave antennas.The main advantages of MSAs are listed as follows:•They are lightweight and have a small volume and a low-profileplanar configuration.•They can be made conformal to the host surface.•Their ease of mass production using printed-circuit technology leadsto a low fabrication cost.•They are easier to integrate with other MICs on the same substrate.•They allow both linear polarization and CP.•They can be made compact for use in personal mobile communica-tion.•They allow for dual-and triple-frequency operations.1.2.2DisadvantagesMSAs suffer from some disadvantages as compared to conventional micro-wave antennas.They are the following:•Narrow BW;•Lower gain;•Low power-handling capability.4Broadband Microstrip AntennasMSAs have narrow BW,typically1–5%,which is the major limiting factor for the widespread application of these antennas.Increasing the BW of MSAs has been the major thrust of research in this field,and broad BW up to70%has been achieved[9,10].Various broadband MSA configurations are summarized in this chapter,and they are detailed in the following chapters.1.2.3Applications of MSAsThe advantages of MSAs make them suitable for numerous applications [6–11].The telemetry and communications antennas on missiles need to be thin and conformal and are often MSAs.Radar altimeters use small arrays of microstrip radiators.Other aircraft-related applications include antennas for telephone and satellite communications.Microstrip arrays have been used for satellite imaging systems.Patch antennas have been used on commu-nication links between ships or buoys and satellites.Smart weapon systems use MSAs because of their thin profile.Pagers,the global system for mobile communication(GSM),and the global positioning system(GPS)are major users of MSAs.Some of the applications of MSAs are listed in Table1.2.1.3Feeding TechniquesThe MSA can be excited directly either by a coaxial probe or by a microstrip line.It can also be excited indirectly using electromagnetic coupling or aperture coupling and a coplanar waveguide feed,in which case there is noTable1.2Typical Applications of MSAsSystem ApplicationAircraft and ship antennas Communication and navigation,altimeters,blindlanding systemsMissiles Radar,proximity fuses,and telemetrySatellite communications Domestic direct broadcast TV,vehicle-basedantennas,communicationMobile radio Pagers and hand telephones,man pack systems,mobile vehicleRemote sensing Large lightweight aperturesBiomedical Applicators in microwave hyperthermiaOthers Intruder alarms,personal communication,and soforthAn Introduction to Microstrip Antennas5direct metallic contact between the feed line and the patch[9–12].Feeding technique influences the input impedance and characteristics of the antenna, and is an important design parameter.The coaxial or probe feed arrangement is shown in Figure1.1.The center conductor of the coaxial connector is soldered to the patch.The main advantage of this feed is that it can be placed at any desired location inside the patch to match with its input impedance.The disadvantages are that the hole has to be drilled in the substrate and that the connector protrudes outside the bottom ground plane,so that it is not completely planar.Also, this feeding arrangement makes the configuration asymmetrical.A patch excited by microstrip line feed is shown in Figure1.3(a).This feed arrangement has the advantage that it can be etched on the same substrate,so the total structure remains planar.The drawback is the radiation from the feed line,which leads to an increase in the cross-polar level.Also, in the millimeter-wave range,the size of the feed line is comparable to the patch size,leading to increased undesired radiation.For thick substrates,which are generally employed to achieve broad BW,both the above methods of direct feeding the MSA have problems.In the case of a coaxial feed,increased probe length makes the input impedance more inductive,leading to the matching problem.For the microstrip feed, an increase in the substrate thickness increases its width,which in turn increases the undesired feed radiation.The indirect feed,discussed below, solves these problems.An electromagnetically coupled RMSA is shown in Figure1.3(b).The electromagnetic coupling is also known as proximity coupling[9,12,13].The feed line is placed between the patch and the ground plane,which is separated by two dielectric media.The advantages of this feed configuration include the elimination of spurious feed-network radiation;the choice between two different dielectric media,one for the patch and the other for the feed line to optimize the individual performances; and an increase in the BW due to the increase in the overall substrate thickness of the MSA.The disadvantages are that the two layers need to be aligned properly and that the overall thickness of the antenna increases.Another method for indirectly exciting a patch employs aperture cou-pling[14].In the aperture-coupled MSA configuration,the field is coupled from the microstrip line feed to the radiating patch through an electrically small aperture or slot cut in the ground plane,as shown in Figure1.3(c). The coupling aperture is usually centered under the patch,leading to lower cross-polarization due to symmetry of the configuration.The shape,size, and location of the aperture decide the amount of coupling from the feed line to the patch[15–17].The slot aperture can be either resonant or6Broadband Microstrip AntennasFigure1.3Rectangular MSA fed by(a)microstrip line,(b)electromagnetic coupling,(c)aperture coupling,and(d)coplanar waveguide(CPW).An Introduction to Microstrip Antennas7nonresonant[10,11].The resonant slot provides another resonance in addition to the patch resonance thereby increasing the BW at the expense of an increase in back radiation.As a result,a nonresonant aperture is normally used.The performance is relatively insensitive to small errors in the alignment of the different layers.Similar to the electromagnetic coupling method,the substrate parameters of the two layers can be chosen separately for optimum antenna performance.This feeding method gives increased BW as described in Chapter4.The coplanar waveguide feed,shown in Figure1.3(d),has also been used to excite the MSA[18].In this method,the coplanar waveguide is etched on the ground plane of the MSA.The line is excited by a coaxial feed and is terminated by a slot,whose length is chosen to be between0.25 and0.29of the slot wavelength.The main disadvantage of this method is the high radiation from the rather longer slot,leading to the poor front-to-back ratio.The front-to-back ratio is improved by reducing the slot dimension and modifying its shape in the form of a loop[19].1.4Methods of AnalysisThe MSA generally has a two-dimensional radiating patch on a thin dielectric substrate and therefore may be categorized as a two-dimensional planar component for analysis purposes.The analysis methods for MSAs can be broadly divided into two groups.In the first group,the methods are based on equivalent magnetic current distribution around the patch edges(similar to slot antennas).There are three popular analytical techniques:•The transmission line model;•The cavity model;•The MNM.In the second group,the methods are based on the electric current distribution on the patch conductor and the ground plane(similar to dipole antennas,used in conjunction with full-wave simulation/numerical analysis methods).Some of the numerical methods for analyzing MSAs are listed as follows:8Broadband Microstrip Antennas•The method of moments(MoM);•The finite-element method(FEM);•The spectral domain technique(SDT);•The finite-difference time domain(FDTD)method.This section briefly describes these methods.1.4.1Transmission Line ModelThe transmission line model is very simple and helpful in understanding the basic performance of a MSA.The microstrip radiator element is viewed as a transmission line resonator with no transverse field variations(the field only varies along the length),and the radiation occurs mainly from the fringing fields at the open circuited ends.The patch is represented by two slots that are spaced by the length of the resonator.This model was originally developed for rectangular patches but has been extended for generalized patch shapes.Many variations of this method have been used to analyze the MSA[9,20–22].Although the transmission line model is easy to use,all types of configu-rations can not be analyzed using this model since it does not take care of variation of field in the orthogonal direction to the direction of propagation.1.4.2Cavity ModelIn the cavity model,the region between the patch and the ground plane is treated as a cavity that is surrounded by magnetic walls around the periphery and by electric walls from the top and bottom sides.Since thin substrates are used,the field inside the cavity is uniform along the thickness of the substrate[23–25].The fields underneath the patch for regular shapes such as rectangular,circular,triangular,and sectoral shapes can be expressed as a summation of the various resonant modes of the two-dimensional resonator.The fringing fields around the periphery are taken care of by extending the patch boundary outward so that the effective dimensions are larger than the physical dimensions of the patch.The effect of the radiation from the antenna and the conductor loss are accounted for by adding these losses to the loss tangent of the dielectric substrate.The far field and radiated power are computed from the equivalent magnetic current around the periphery.An alternate way of incorporating the radiation effect in the cavity model is by introducing an impedance boundary condition at the walls of the cavity.The fringing fields and the radiated power are not included insideAn Introduction to Microstrip Antennas9the cavity but are localized at the edges of the cavity.However,the solution for the far field,with admittance walls is difficult to evaluate[9].1.4.3MNMThe MNM for analyzing the MSA is an extension of the cavity model[9, 26,27].In this method,the electromagnetic fields underneath the patch and outside the patch are modeled separately.The patch is analyzed as a two-dimensional planar network,with a multiple number of ports located around the periphery.The multiport impedance matrix of the patch is obtained from its two-dimensional Green’s function.The fringing fields along the periphery and the radiated fields are incorporated by adding an equivalent edge admittance network.The segmentation method is then used to find the overall impedance matrix.The radiated fields are obtained from the voltage distribution around the periphery.Appendix C details this method.The above three analytical methods offer both simplicity and physical insight.In the latter two methods,the radiation from the MSA is calculated from the equivalent magnetic current distribution around the periphery of the radiating patch,which is obtained from the corresponding voltage distribution.Thus,the MSA analysis problem reduces to that of finding the edge voltage distribution for a given excitation and for a specified mode. These methods are accurate for regular patch geometries,but—except for MNM with contour integration techniques—they are not suited for arbitrary shaped patch configurations.For complex geometries,the numerical tech-niques described below are employed[9].1.4.4MoMIn the MoM,the surface currents are used to model the microstrip patch, and volume polarization currents in the dielectric slab are used to model the fields in the dielectric slab.An integral equation is formulated for the unknown currents on the microstrip patches and the feed lines and their images in the ground plane[28].The integral equations are transformed into algebraic equations that can be easily solved using a computer.This method takes into account the fringing fields outside the physical boundary of the two-dimensional patch,thus providing a more exact solution.This book makes extensive use of a commercially available software IE3D[29] based on MoM to analyze various MSA configurations.10Broadband Microstrip Antennas1.4.5FEMThe FEM,unlike the MoM,is suitable for volumetric configurations.In this method,the region of interest is divided into any number of finite surfaces or volume elements depending upon the planar or volumetric structures to be analyzed[30].These discretized units,generally referred to as finite elements,can be any well-defined geometrical shapes such as triangular elements for planar configurations and tetrahedral and prismatic elements for three-dimensional configurations,which are suitable even for curved geometry.It involves the integration of certain basis functions over the entire conducting patch,which is divided into a number of subsections.The problem of solving wave equations with inhomogeneous boundary conditions is tackled by decomposing it into two boundary value problems,one with Laplace’s equation with an inhomogeneous boundary and the other corre-sponding to an inhomogeneous wave equation with a homogeneous boundary condition[10].1.4.6SDTIn the SDT,a two-dimensional Fourier transform along the two orthogonal directions of the patch in the plane of substrate is employed.Boundary conditions are applied in Fourier transform plane.The current distribution on the conducting patch is expanded in terms of chosen basis functions, and the resulting matrix equation is solved to evaluate the electric current distribution on the conducting patch and the equivalent magnetic current distribution on the surrounding substrate surface.The various parameters of the antennas are then evaluated[31].1.4.7FDTD MethodThe FDTD method is well-suited for MSAs,as it can conveniently model numerous structural inhomogenities encountered in these configurations[10].It can also predict the response of the MSA over the wide BW witha single simulation.In this technique,spatial as well as time grid for the electric and magnetic fields are generated over which the solution is required. The spatial discretizations along three Cartesian coordinates are taken to be same.The E cell edges are aligned with the boundary of the configuration and H-fields are assumed to be located at the center of each E cell.Each cell contains information about material characteristics.The cells containing the sources are excited with a suitable excitation function,which propagates along the structure.The discretized time variations of the fields are deter-mined at desired ing a line integral of the electric field,the voltage across the two locations can be obtained.The current is computed by a loop integral of the magnetic field surrounding the conductor,where the Fourier transform yields a frequency response.The above numerical techniques,which are based on the electric current distribution on the patch conductor and the ground plane,give results for any arbitrarily shaped antenna with good accuracy,but they are time-consuming.These methods can be used to plot current distributions on patches but otherwise provide little of the physical insight required for antenna design.1.5Review of Various Broadband Techniques for MSAsAs mentioned earlier,the most serious limitation of the MSA is its narrow BW.The BW could be defined in terms of its VSWR or input impedance variation with frequency or in terms of radiation parameters.For the circularly polarized antenna,BW is defined in terms of the axial ratio(AR)[9]. Therefore,before describing the various methods for increasing the BW,the various definitions of the BW are described.1.5.1Definition of BWThe VSWR or impedance BW of the MSA is defined as the frequency range over which it is matched with that of the feed line within specified limits. The BW of the MSA is inversely proportional to its quality factor Q and is given by[32]BW=VSWR−1Q√VSWR(1.1)where VSWR is defined in terms of the input reflection coefficient⌫as:VSWR=1+|⌫|1−|⌫|(1.2)The⌫is a measure of reflected signal at the feed-point of the antenna. It is defined in terms of input impedance Z in of the antenna and the characteristic impedance Z0of the feed line as given below:⌫=Z in −Z 0Z in +Z 0(1.3)The BW is usually specified as frequency range over which VSWR is less than 2(which corresponds to a return loss of 9.5dB or 11%reflected power).Sometimes for stringent applications,the VSWR requirement is specified to be less than 1.5(which corresponds to a return loss of 14dB or 4%reflected power).Conversion of BW from one VSWR level to another can be accomplished byBW 1BW 2=(VSWR 1−1)√VSWR 1√VSWR 2(VSWR 2−1)(1.4)where BW 1and BW 2correspond to VSWR 1and VSWR 2,respectively.The variation of percentage BW for VSWR ≤2and efficiency of a square MSA with normalized substrate thickness h /0for two different values of ⑀r (2.2and 10)are given in Figure 1.4(a).Also,the variation of percentage BW with frequency for three commonly used values of h and ⑀r =2.32is given in Figure 1.4(b).The BW of a single-patch antenna increases with an increase in the substrate thickness and a decrease in the ⑀r of the substrate [9,33,34].The BW is approximately 15%for ⑀r =2.2and h =0.10.The ⑀r can be chosen close to 1to obtain a broader BW.The larger thickness of the substrate givesrise to an increase in probe reactance Figure 1.4(a)Variation of percentage BW and efficiency of a square MSA versus h /0.(——)⑀r =2.2,(---)⑀r =10and (b)variation of percentage BW with frequency for three values of h and ⑀r =2.32:(——)0.318,(---)0.159,(–-–)0.079cm.for the coaxial feed and the excitation of surface waves,which reduces the efficiencyof the antenna as can be seen from Figure1.4(a).The efficiency of the MSA is defined in Appendix C.The BW enhancement of the single regularly shaped MSA is discussed in Chapter2.The expressions for approximately calculating the percentage BW of the RMSA in terms of patch dimensions and substrate parameters is given by%BW=Ah0√⑀r√W L(1.5)whereA=180forh0√⑀r≤0.045A=200for0.045≤h0√⑀r≤0.075A=220forh0√⑀r≥0.075where W and L are the width and length of the RMSA.With an increase in W,BW increases.However,W should be taken less thanto avoid excitation of higher order modes.For other regularly shaped patches,values of equivalent W can be obtained by equating the area with that of the RMSA as described in Chapter2[35,36].Another simplified relation for quick calculation of BW(in megahertz) for VSWR=2of the MSA operating at frequency f in gigahertz,with h expressed in centimeters,is given by[37]BW≅50hf2(1.6) The BW can also be defined in terms of the antenna’s radiation parame-ters.It is defined as the frequency range over which radiation parameters such as the gain,half-power beamwidth(HPBW),and sidelobe levels are within the specified minimum and maximum limits.This definition is more complete as it also takes care of the input impedance mismatch,which also contributes to change in the gain.The expression for approximately calculating the directivity D of the RMSA is given byD≅0.2W+6.6+10log1.6/√⑀rdB(1.7) For other geometries,the values of equivalent W can be obtained by equating its area with that of the RMSA as described in Chapter2[35,36].The above definitions for BW are mainly for a linearly polarized MSA. For a circularly polarized MSA,the BW is generally limited by its AR.This BW is the frequency range over which AR is less than a maximum limit (e.g.,3or6dB).There are various techniques for increasing the BW of the MSAs.The main techniques used to increase the BW are presented briefly in the following sections.1.5.2Modified Shape PatchesThe regular MSA configurations,such as rectangular and circular patches have been modified to rectangular ring[38]and circular ring[39],respectively,to enhance the BW.The larger BW is because of a reduction in the quality factor Q of the patch resonator,which is due to less energy stored beneath the patch and higher radiation.When a U-shaped slot is cut inside the rectangular patch,it gives a BW of approximately40%for VSWR≤2[40]. Similar results are obtained when a U-slot is cut inside a circular or a triangular MSA[41,42].These configurations are discussed in detail in Chapter6.1.5.3Planar Multiresonator ConfigurationsThe planar stagger–tuned coupled multiple resonators yield wide BW in the same way as in the case of multistage tuned circuits.Several configurations are available yielding BW of5–25%[43–49].Various parasitic patches like narrow strips,shorted quarter-wavelength rectangular patches,and rectangu-lar resonator patches have been gap-coupled to the central-fed rectangular patch.Three combinations of gap-coupled rectangular patches are shown in Figure1.5.To reduce the criticality of the gap coupling,direct coupling as depicted in Figure1.6has been used to obtain broad BW.Both gap and direct(hybrid)coupling have been used with circular MSAs(CMSAs)and equilateral triangular MSAs(ETMSAs)to yield broad BW.Figure1.5Various gap-coupled multiresonator RMSA configurations:(a)three RMSAs gap-coupled along radiating edges,(b)three RMSAs gap-coupled along non-radiating edges,and(c)five gap-coupled RMSAs.These planar multiresonator configurations yield broad BW but have the following disadvantages:•The large size,which makes them unsuitable as an array element;•The variation in the radiation pattern over the impedance BW.A modification of the multiresonator patches—to avoid the above-mentioned problems—entails using five or six narrow strips that are gap-coupled along the width[49].This yielded wide BW with a relatively small variation in pattern over the BW.Various broadband planar multiresonator configurations are covered in Chapter3.1.5.4Multilayer ConfigurationsIn the multilayer configuration,two or more patches on different layers of the dielectric substrate are stacked on each other.Based on the coupling mechanism,these configurations are categorized as electromagnetically cou-pled or aperture-coupled MSAs.Figure1.6Various direct-coupled multiresonators:(a)three RMSAs direct-coupled along radiating edges,(b)three RMSAs direct-coupled along nonradiating edges,and(c)five direct-coupled RMSAs.1.5.4.1Electromagnetically Coupled MSAsIn the electromagnetically coupled MSA,one or more patches at the different dielectric layers are electromagnetically coupled to the feed line located at the bottom dielectric layer as shown in Figure1.3(b).Alternatively,one of the patches is fed by a coaxial probe and the other patch is electromagnetically coupled.Either the bottom or top patch is fed with a coaxial probe as shown in Figure1.7.The patches can be fabricated on different substrates,and accordingly the patch dimensions are to be optimized so that the resonance frequencies of the patches are close to each other to yield broad BW.TheseFigure1.7An electromagnetically coupled MSA,in which(a)the bottom patch is fed and(b)the top patch is fed.two layers may be separated by either air-gap or foam yielding BW of15–30% [50–56].1.5.4.2Aperture-Coupled MSAsIn the aperture-coupled MSA,the field is coupled from the microstrip feed line placed on the other side of the ground plane to the radiating patch through an electrically small aperture/slot in the ground plane,as shown in Figure1.3(c).Two different dielectric substrates could be chosen,one for the patch and the other for the feed line to optimize the individual perfor-mances.The coupling to the patch from the feed line can be maximized by choosing the optimum shape of the aperture[14–16].Two patches of rectangular or circular shapes,which are stacked on each other in different dielectric layers yield around30%BW[57–60].A BW of nearly70%has been obtained by stacking patches with resonant apertures[61].The multilayer broadband MSAs,unlike single-layer multiresonator configurations,show a very small degradation in radiation pattern over the complete VSWR BW.The drawback of these structures is the increased height,which is not desirable for conformal applications and increased back radiation for aperture-coupled MSAs.Multilayered configurations using both electromagnetic as well as aperture coupling are described in Chapter4.1.5.5Stacked Multiresonator MSAsThe planar and stacked multiresonator techniques are combined to further increase the BW and gain.A probe-fed single rectangular or circular patch located on the bottom layer has been used to excite multiple rectangular or circular patches on the top layer,respectively[62,63].Besides increasing the BW,these configurations also provide an increase in gain as described in Chapter5.1.5.6Impedance-Matching Networks for Broadband MSAsThe impedance-matching networks are used to increase the BW of the MSA. Some examples that provide about10%BW are the rectangular MSA with a coplanar microstrip impedance-matching network and an electromagnetically coupled MSA with single-stub matching as shown in Figure1.8[12,64–66].1.5.7Log-Periodic MSA ConfigurationsThe concept of log-periodic antenna has been applied to MSA to obtain a multi-octave BW.In this configuration,the patch dimensions are increased。
一种紧凑型多频段手机内置环形天线的设计
一种紧凑型多频段手机内置环形天线的设计代传堤;吴多龙;吴艳杰;黎宇彪;林青【摘要】The design of a compact internal multiband folded loop antenna for GSM850/900/GPS/DCS1800/PCS1900/UMTS2100 multiple mobile operation has been proposed.The whole antenna struc-ture consists of a single folded meander loop track and a T-shape back-coupling element, whereas the loop pattern is activated through the electromagnetic coupling mechanism by the T-shape element which is connected to the microstrip feeding line.The size of the total structure is 114 mm ×61.6 mm ×6 mm, meanwhile the area left for the loop track is only 61.6 mm ×15 mm ×6 mm.The compact structure makes the design very suitable for the mobile phone requirements for slim space.The design and optimi-zing of the performance of the proposed antenna were performed by using the simulator software HFSS. An actual model has been prototyped for testing.Measured and electromagnetic simulated results are in good agreement, thus indicating that the proposed antenna can meet the actual demands.%设计了一种应用于GSM850/900/GPS/DCS1800/PCS1900/UMTS2100多频段移动通信制式的紧凑型手机内置环形天线.整个天线结构包括一个弯折线形的折叠环形辐射体和T型背面耦合单元,其中环形辐射体由连接至微带馈线的T型单元通过电磁耦合机制激励.整个结构尺寸为114 mm ×61.6 mm ×6 mm,其中环形辐射体仅占空间61.6 mm ×15 mm ×6 mm,结构紧凑,适合满足移动手机狭小的空间要求.使用HFSS仿真软件设计和优化天线,并构建一个实际的测试模型.测量结果和仿真结果吻合良好,表明此天线能够满足实际需求.【期刊名称】《广东工业大学学报》【年(卷),期】2014(000)004【总页数】4页(P100-103)【关键词】手机天线;折叠环形天线;多频段天线;阻抗带宽【作者】代传堤;吴多龙;吴艳杰;黎宇彪;林青【作者单位】广东工业大学物理与光电工程学院,广东广州510006;广东工业大学物理与光电工程学院,广东广州510006;广东工业大学物理与光电工程学院,广东广州510006;广东工业大学物理与光电工程学院,广东广州510006;广州思泰信息技术有限公司,广东广州510663【正文语种】中文【中图分类】TN828.61 问题的提出随着无线通信技术的飞速发展,特别是近几年来智能手机的日新月异,手机越来越趋向小型化、多功能、高性能发展,在小体积的手机中集成更多的无线服务的需求不断增大,这对手机天线的设计提出了更高的要求.为满足实际需要,多频段多功能的手机天线越来越多地被研究与应用.宽频段、多带宽、结构紧凑是手机内置多频段天线设计的重要因素,如mon-opole[1-3]、PIFA[4-7]和许多其他类型的天线设计[8-15].近来,许多文献提到环形天线由于自身独特的多模特征,可为多频段手机天线的应用提供可行的解决方案.环形天线可以看作是工作在0.5λ和1.5 λ两个非平衡模式下的折叠型单极子天线(folded monopole)[5],也可以看作是工作在1λ平衡模式下的折叠型偶极子天线(folded dipole)[8-10],因此单个环形天线就可以产生多达3个谐振模式,从而适合于移动手机多通信制式的频段需求.但由于环天线具有高谐振阻抗的特征[11],在手机狭小的空间内配置环形天线良好的阻抗匹配对天线工程师来说是项挑战,各种调谐技术也被相继研究和应用.文献[8,13]提到通过增加调谐贴片能够改善天线谐振阻抗,文献[11-12]则采用了可重构技术,利用在电流密集处增加匹配桥或P-I-N二极管来控制电流流向,从而控制环形天线的谐振特性.文献[14-15]则采用辐射体耦合馈电方式,利用馈电单极子天线(feeding monopole)通过电磁耦合激励辐射环形天线.本文提出了一种紧凑型手机内置环形天线系统,由环形辐射体和T形耦合单元组成.其中环形辐射体采用弯折线折叠型结构,通过PCB板下平面的T形单元进行电磁耦合馈电,从而克服了环形天线自身高阻抗的缺点,充分利用其多模多谐振的优点.以VSWR=3∶1计算,所制天线系统能够产生777~1 620 MHz和1 390~2 155 MHz两个频段的谐振带宽,从而能够覆盖GSM-850/GSM900/GPS/DCS1800/PCS1900/UMTS2100通信制式(Low Band:824-960 MHz,High Band:1575-2170 MHz).设计中的环形天线辐射体仅占61.6×15×6 mm3的空间,结构紧凑,高度较低,非常容易满足移动终端狭小的空间限制.实验中对天线进行了软件仿真、样品构造和测试,其仿真结果和测试结果吻合良好,证明此天线能够满足实际需求.2 天线设计图1给出了所述天线的结构示意图.其中图1(a)为系统的三维视图,整个天线系统由PCB板、上层地面、介质衬底和天线金属部分组成.其中PCB板采用厚度为1mm的FR-4介质基板,其相对介电常数为4.4,损耗正切为0.02,并设定其长宽为114 mm×61.6 mm.介质衬底则由介电常数为1.07,体积尺寸为15 mm×61.6 mm×6 mm的泡沫构成.天线的金属部分由折叠环形带(folded loop strip)和电容耦合馈线(capacitivly coupling feeding line)组成,其中环形带由一单连续的弯折形环形单元组成,采用左右对称、等线宽等间隔的分布方式,并沿图1(b)所示的弯折线(bending line)折叠成3个区域,以增加其电长度的同时减少其所占的空间,最后通过短路点1和短路点2连接到PCB板的上层地面.为了增加与下层馈线间的耦合程度,环形带在①区域增加了3 mm宽度的调谐片(tuning pad).通过仿真验证,调节调谐片的长度可以达到调节天线阻抗匹配的效果.耦合馈线则由两个线宽相等的T型耦合单元组成,并连接至线宽为1.9 mm,阻抗为50 Ω的微带馈线,如图1(c)所示.图1 天线的几何形状(单位:mm)Fig.1 Geometry of the proposedantenna:(a)3D view,(b)Plan view of the loop radiating track,and(c)Bottom view3 结果与分析图2为采用耦合馈电(Coupling feeding)与在环形天线短路点1处采用同轴线直接馈电(Direct feeding)所得到的反射系数曲线.图2 不同馈电机制仿真的反射系数Fig.2 Simulated results of the reflection coefficient with different feeding mechanisms由图2可知,采用耦合馈电方式,能够使得环形天线在低频段处产生的两个谐振合为一个谐振,并扩大-6 dB的谐振带宽,同时降低高频段的谐振频率,使其能够覆盖GPS通信制式.为实验测试需要,实验中构建了天线的实际测试模型,如图3所示.其中图3(b)中PCB顶端的两个白色过孔为印刷电路板安装孔,经仿真验证,其对天线反射系数的影响基本可以略去.馈电末端连接至50 Ω阻抗的SMA测试线,并使用Agilent E5515C型射频矢量网络分析仪进行测试,测试结果如图4所示.由图4可知,天线在低频段产生一个谐振,在高频段产生两个谐振,以反射系数return coefficient=-6 dB(VSWR=3∶1)计算,谐振低频带宽为777~1 620 MHz,高频带宽为1 390~2 155 MHz,基本能够满足Low GSM850/GSM900 Band(LB:824~960 MHz)和High GPS/DCS1800/PCS1900/UMTS2100Band(HB:1 575~2 170 MHz)的频段要求.图5所示为仿真所得的环形天线分别在3个谐振频点0.911 GHz,1.655 GHz和2.107 GHz,在X-Z和Y-Z截面上的增益方向图(Gain(dB)).图3 天线的实际测试模型与测试线连接图Fig.3 Manufactured antenna prototypes and testing line:(a)Top View,and(b)Bottom view图4 天线模型的仿真和实测反射系数曲线Fig.4 Measured and simulated reflection coefficient for the proposed antenna prototypes图5 仿真所得天线在不同频点上的辐射增益方向图Fig.5 Simulated radiation patterns at(a)0.911 GHz,(b)1.655 GHz,and(c)2.107 GHz for the proposed antenna4 结论设计了一种手机内置多谐振多频段环形天线,通过采用PCB背面的馈线进行耦合馈电方式,克服了环形天线高阻抗的缺点,实现了天线的宽频特性.天线结构简单,设计紧凑,具有易共形、易美化和制作方便的优点.通过加工制作实物测试,证实了该环形天线可满足824~960MHz和1575~2170 MHz的频段带宽要求,适用于当前采用GSM850/900/GPS/GSM1800/GSM1900/UMTS2100制式的移动终端.参考文献:[1]Wong Kin-Lu,Chen Shu-Chuan.Printed single-strip monopole using a chip inductor for penta-band WWAN operation in the mobile phone [J].IEEE Transactions on Antennas and Propagation,2010,58(3):1011-1014.[2]Chu Fang-Hsien,Wong Kin-Lu.Simple folded monopole slot antenna for penta-band clamshell mobile phone application[J].IEEE Transactions on Antennas and Propagation,2009,57(11):3680-3684.[3]Xu Jing,Du Zheng-wei,Gong pact planar monopole antenna for multi-band mobile phones[C]∥2005 Asia-Pacific Microwave Conference Proceedings(APMC’2005),Suzhou,Jiangsu,China,2005:2703-2706.[4]Jiao Sheng-cai,Niu Jian-min,Jiang Ming.A compact multi-band PIFA antenna for mobile devices[C]∥2012 International Conference on Computer Science and Electronics Engineering(ICCSEE’2012),Hangzhou,Zhejiang,China,2012:278-281.[5]Chen Jin-Hua,Ban Yang-Ling,Ying pact PIFA using capacitive coupled-fed for LTE/GSM/UMTS WWAN operation in the mobile application[C]∥2011 Cross Strait Quad-Regional Radio Science and wireless techn-ology conference(CSQRWC’2011),Harbin,Heilongjiang,China,2011:414-417.[6]Kang Do-Gu,Sung pact hexaband PIFA antenna for mobile handset applications[J].IEEE Antennas and Wireless Propagation Letters,2010,9:1127-1130.[7]Chiu Chien-Wen,Chi Yu-Jen.Planar hexa-band inverted-F antennafor mobile device applications[J].IEEE Antennas and Wireless Propagation Letters,2009,8:1099-1102.[8]Zheng Ming,Wang Han-yang.Internal hexa-band folded Monopole/Dipole/Loop antenna with four resonances for mobile device [J].IEEE Transactions on Antennas and Propagation,2012,60(6):2880-2885.[9]Chi Yun-Wen,Wong pact multiband folded loop chip antenna for small-size mobile phone[J].IEEE Transactions on Antennas and Propagation,2007,56(12):3797-3803.[10]Hayashida S,Morishita H,Fujimoto K.Self-balanced wideband folded loop antenna[J].IEEE Proceedings Microwaves,Antennas and Propagation,2006,153(1):7-12.[11]Li Yue,Zhang Zhi-jun,Zheng Jian-feng,et al.A compact hepta-band Loop-Inverted F reconfigurable antenna for mobile phone[J].IEEE Transactions on Antennas and Propagation,2012,60(1):389-392. [12]Li Yue,Zhang Zhi-jun,Zheng Jian-feng,et pact Hepta-band reconfigurable loop antenna for mobile handset[J].IEEE Antennas and Wireless Propagation Letters,2011,10:1162-1165.[13]Wong Kin-Lu,Huang Chih-Hong.Printed loop antenna with a perpendicular feed for penta-band mobile phone application[J].IEEE Transactions on Antennas and Propagation,2008,56(7):2138-2141. [14]Sang Heun Lee,Ki Joon Kim,Jong Ho Jung,et al.Meander line loop antenna with coupled feed for multiband mobile phone[C]∥2011 International Workshop on Antenna Technology(iWA T’2011),HongKong,China,2011:194-197.[15]Sang Heun Lee,Ki Joon Kim,Byoung-nam Kim,et al.Multi-band coupled feed loop antenna for mobile handset[C]∥2009 Asia-Pacific Microwave Conference Proceedings(APMC’2009),Suntec City,Singapore,2009:2703-2706.。
A Compact Dual-Band Microstrip-Fed Monopole Antenna
Antenna Configuration and Results
The configuration of the microstrip-fed uniplanar monopole antenna is shown in Fig. 1, which is printed on a microwave substrate of thickness
Introduction
The rapid developments in the wireless communications industry demand novel antenna designs that can be used in more than one frequency band. Recently, dual-band cellular phones capable of operating in two different cellular systems are increasing. A cellular phone operating at both frequencies (900 MHz and 1800 MHz) requires the antenna to operate equally well at both frequency bands. Dual-band antenna are not used in cellular networks alone, in fact, they are widely used for dual-band ISM applications. As an example, many laptop computers use 900 MHz or 1800 MHz band for wireless printer and modem connections. The 2400 MHz band is used by laptops in wireless local area network (LAN) applications and the Bluetooth is being considered as a cable replacement between portable and fixed electronic devices. Dual-band antennas with one feed have some advantages over multi-feed antennas and were proposed in [1]-[4] for cellular applications. The antenna in [ I ] consists of a straight radiating element and a helically wound element, while the antenna in [2] uses a non-uniform helix radiating element. An internal dual-band mobile phone antenna [3 J is derived from a quarter-wave planar inverted F-type antenna (PIFA), which has compact size and good performance. All the above antennas are designed to operate at 900 MHz (GSM) and 1800 MHz (DCS). In reference [4], a dual-band strip-sleeve antenna is described for use on a laptop computer, which is designed to resonate at 0.85 and 1.9 GHz. In this paper we will extend the antenna design to be used for dual-band ISM applications. In this application there is a particular interest to obtain an increased operational bandwidth of the antenna. The effects of design parameters of the microstrip-fed uniplanar monopole antenna on its operational frequency and impedance bandwidth are presented and discussed.
正交缝隙耦合馈电宽带圆极化微带天线设计
正交缝隙耦合馈电宽带圆极化微带天线设计张昭;曹祥玉;李思佳;郭蓉【摘要】为了实现圆极化微带天线的频带拓宽和增益提高,在缝隙耦合天线的基础上,设计了一种Ku频段正交缝隙耦合馈电的宽带圆极化微带天线.该天线以双层方形贴片为辐射单元,在拓展天线阻抗带宽的同时提高了增益;采用微带线结合正交左旋缝隙结构实现耦合馈电,通过优化缝隙结构改善了天线轴比特性.测量结果表明:阻抗带宽(VSWR<2)和轴比带宽(AR<3 dB)分别达到22.5%和16.2%,轴比带宽内天线增益均大于9 dBi.该结构天线以其简单的馈电设计为宽带圆极化微带天线设计提供了一定的参考价值.【期刊名称】《空军工程大学学报(自然科学版)》【年(卷),期】2014(015)002【总页数】5页(P57-61)【关键词】微带天线;宽频带;圆极化;正交左旋缝隙【作者】张昭;曹祥玉;李思佳;郭蓉【作者单位】空军工程大学信息与导航学院,陕西西安,710077;空军工程大学信息与导航学院,陕西西安,710077;空军工程大学信息与导航学院,陕西西安,710077;空军工程大学信息与导航学院,陕西西安,710077【正文语种】中文【中图分类】TN82现阶段圆极化微带天线具有体积小、剖面低、易共形、能接收任意线极化来波等优点在卫星通信领域中拥有广阔的应用前景,因此对其研究具有重要意义[1-2]。
但是由于圆极化微带天线阻抗带宽和轴比带宽通常较窄、增益较低需要进一步的研究。
针对拓展圆极化轴比带宽、提高天线增益的问题,文献[3]提出一种双层贴片结构,利用威尔金森功分器通过H形口径耦合馈电,轴比带宽虽达到30%,但增益仅大于6 dBi;文献[4~5]深入介绍了通过微带巴伦为4个L型探针馈电的单贴片圆极化微带天线,3 dB轴比带宽均达到了80%,但带内增益仅在3 dBi以上;文献[6~7]应用三馈电方式实现圆极化辐射,3 dB轴比带宽分别达到19.8%和33%,带内增益大于3 dBi;以上设计虽然轴比带宽得到很大扩展,但是馈电网络的设计都很复杂,且带内增益较低。
微带天线综述
微带天线综述摘要:微带天线具有结构紧凑、外观优美、体积小重量轻等优点,得到广泛的应用。
但是,近年来,随着个人通讯和移动通讯技术的迅速发展,在天线的设计上提出了小型化的要求。
本文除了对微带天线做了基本介绍外,还对微带天线最基本的小型化技术进行了探讨、分析和归纳。
关键词:微带天线小型化宽频带一、引言随着全球通信业务的迅速发展,作为未来个人通信主要手段的无线移动通信技术己引起了人们的极大关注,在整个无线通讯系统中,天线是将射频信号转化为无线信号的关键器件,其性能的优良对无线通信工程的成败起到重要作用。
快速发展的移动通信系统需要的是小型化、宽频带、多功能(多频段、多极化)、高性能的天线。
微带天线作为天线家祖的重要一员,经过近几十年的发展,已经取得了可喜的进步,在移动终端中采用内置微带天线,不但可以减小天线对于人体的辐射,还可使手机的外形设计多样化,因此内置微带天线将是未来手机天线技术的发展方向之一,设计出具有小型化的微带天线不但具有一定的理论价值而且具有重要的应用价值,这也成为当前国际天线界研究的热点之一。
二、微带天线2.1微带天线[1]的发展史及种类早在1953年G. A. DcDhamps教授就提出利用微带线的辐射来制成微带微波天线的概念。
但是,在接下来的近20年里,对此只有一些零星的研究。
直到1972年,由于微波集成技术的发展和空间技术对低剖面天线的迫切需求,芒森(R.E.Munson)和豪威尔(J.Q.Howell)等研究者制成了第一批实用的微带天线[1]。
随之,国际上展开了对微带天线的广泛研究和应用。
1979年在美国新墨西哥州大学举行了微带天线的专题目际会议,1981年IEEE天线与传播会刊在1月号上刊载了微带天线专辑。
至此,微带天线已形成为天线领域中的一个专门分支,两本微带天线专辑也相继问世。
80年代中,微带天线无论在理论与应用的深度上和广度上都获得了进一步的发展;今天,这一新型天线已趋于成熟,其应用正在与日俱增。
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Communications______________________________________________________________________A Compact Microstrip Antenna for GPS and DCSApplicationShun-Yun Lin and Kuang-Chih Huang Abstract—This communication presents a novel design of a compact mi-crostrip antenna practical for both the global positioning system(GPS)and dig ital communication system(DCS).The proposed antenna consists of two parts:a fundamental mode truncated square patch antenna and a higher-order mode annular ring patch antenna.The truncated square patch oper-ated in right-hand circular polarization at1575MHz with8-MHz CP band-width,making the desig n suitable for the GPS.Further,four slots were em-bedded into a ground plane to meander the current path of the annular ring patch at the TM mode,which considerably lowered the resonant fre-quency and effectively increased the impedance bandwidth.These features reduce the antenna size and make the desig n appropriate for DCS.Both radiators are placed in a common space but operate independently.The experimental results show that this design is ideally suited for GPS/DCS dual-band mobile communications.Index Terms—Conical radiation pattern,high-order mode antenna,mo-bile communication,satellite communication,slotted ground plane.I.I NTRODUCTIONMobile communications have been indispensable in modern life. There are various communication systems,such as the global posi-tioning system(GPS)and digital communication system(DCS),im-plemented to meet various needs.The GPS offers global positioning function via satellites[1],[2],and the DCS provides personal mobile communication services[3],[4].Because of different radiation perfor-mances of the GPS and DCS,conventional dual-band antennas with single radiation characteristics are not practical for the GPS/DCS ap-plications.The TM21mode annular ring patch antenna could be a promising so-lution with its omnidirectional radiation pattern on the azimuthal plane [4],[5].However,it is impractical for the DCS with its large patch size and narrow impedance bandwidth.Some methods have been devel-oped to reduce the antenna size[6].These techniques mainly centered around two issues:meandering current path and increasing substrate’s permittivity.However,these methods achieved compact design at the expenses of impedance bandwidth and antenna gain.This communication presents a compact dual-band antenna for the GPS and DCS.The design consisted of an annular ring patch and a trun-cated square patch.The truncated square patch was equipped within the annular ring patch,and excited two degenerated modes to obtain cir-cular polarization.A substrate with high permittivity was adopted to make the square patch more compact tofit in with the inner radius of the annular ring.To improve performance,the design integrated an in-novation[5],in which four radial slots were embeded into the square ground plane at diagonal direction to meander the current path of the annular ring patch antenna at the TM21mode.The experimental re-sults show that the resonant frequency is significantly lowered,which brings more compact size;and the impedance bandwidth is enhanced, which yields high performance.Manuscriptreceived February16,2003;revised February23,2004.The authors are with the Department of Electronics Engineering,Cheng Shiu University,Kaohsiung,Taiwan833,R.O.C.(e-mail:yun@.tw). Digital Object Identifier10.1109/TAP.2004.842597Fig.1.Configuration of the compact antenna for GPS and DCS application.II.A NTENNA D ESIGNThe proposed antenna mainly consisted of two radiators:a truncatedsquare patch,which offered a right-hand circular polarization radiationfor communication via the GPS;and a TM21mode annular ring patch,which featured an omnidirectional radiation pattern for the DCS.Bothpatches were centered above a slotted ground plane.The dimension ofthe internal radius of the annular-ring patch was set to be large enoughto contain the concentric configuration.The annular ring radiation patch with outer radius R1and inner ra-dius R2operated at the TM21mode and its resonant frequency can becalculated according to the following[7]:wR=0:4(1)k2R=2(2) where k is2 = 0,w is(R10R2)=2;and R is(R1+R2)=2.To achieve compact size of the annular ring patch,four radial slotswere embedded on the square ground plane.The embedded slots wereoriented at45 to the x-or y-axis(see Fig.1)such that the narrow slotswere in perpendicular to the excited surface currents on the groundplane for the antenna operated at the TM21mode[5].To avoid af-fecting the performance of the GPS antenna,the slots had a distance ofR2(identical to the patch’s inner radius)from the ground-plane center.The width of the slots was set to be2mm for adequate current me-andering,but without sacrificing the antenna gain and F=B ratio.The 0018-926X/$20.00©2005IEEETABLE IP ERFORMANCES OF THE TM M ODE A NNULAR -R ING P ATCH A NTENNA W ITH S LOTTED G ROUND P LANE .T HE O UTER R ADIUS ,I NNER R ADIUS ,H EIGHT OF A IR S UBSTRATE AND W IDTH OF THE S LOTS ARE S ET TO BE 47,19.5,3,AND 2MM ,R ESPECTIVELY .T HEfIS C ALCULATED BY (3),ANDfIS M EASURED BY N ETWORK ANALYZER Fig.2.(a)Measured input impedance on a Smith chart for the GPS antenna.(b)Measured input impedance on a Smith chart for DCS antenna.The geometric dimensions are L =21:4,1L =2:2,R =52:5,R =22,h =6,S =12,L =60,d =38,and d =3:38mm ;and ground plane =1802180mm .resonantfrequency of TM 21mode is about linearly decreased with the increasing slot length,and the following derived linear function can be used to estimate the resonant frequency:f c =f 0019:42L s :(3)where f c is the resonant frequency of the annular ring patch with a slotted ground plane and f 0is the resonant frequency of a regular ground plane.Table I lists the performances of the annular ring patch antenna with embeded slots on the ground plane,indicating that(3)Fig.3.Measured isolation between the feeding points of GPS and DCSantennas studied in Fig.2.Fig.4.Measured radiation pattern of the proposed antenna studied in Fig.2.(a)1575MHz for GPS.(b)1800MHz for DCS.can well describe the resonant frequency of an actual antenna.Different from conventional dual-band designs,this antenna has considerably re-duced size and increased impedance bandwidth.Furthermore,the measured results show that the antenna gain and F =B ratio were lowered with the increasing slot length.The detrimental effects of the proposed are mainly caused by the power leakage through the embedded slots of the ground plane.For applications that a large F =B ratio is preferred,a conducting plate can be added behind the antenna’s ground plane to reflect or block the backward radiation [5].Also,due to the reflection of the backward radiation,the antenna gain can be enhanced simultaneously by the adding of the conducting plate.III.E XPERIMENTAL R ESULTS AND D ISCUSSIONThe prototype of the proposed antenna for the GPS/DCS applica-tions is shown in Fig.1.The geometric parameters were chosen to make the antenna performance meet the requirements of the GPS and DCS.Fig.2(a)shows that the impendance bandwidth for VSWR 2.0was 24MHz (1568–1592MHz)for the GPS antenna.Next,the measured radiation performance indicates that the CP bandwidth was about 8MHz.In addition,Fig.2(b)indicates that the impedance bandwidth was 175MHz for DCS (1705–1880MHz,9.8%).The large enhancement may be caused by the embedded radial slots,which lowered the quality factor of the proposed DCS antenna.Fig.3demonstrates the measuredisolation between the two feeding ports.There is a peak around the res-onant frequency of the truncated square patch.It possibly caused by the inherent drawback of poor radiation efficiency for the substrate with high permittivity,and therefore the resonance of the GPS antenna is easily interfered with other intensed radiation.The isolation was about 020dB in the GPS band,and less than040dB for another band, showing that each antenna operated correctly without significant per-turbation from another band.The radiation patterns were also investigated.Fig.4(a)depicts the patterns of the GPS antenna,indicating that the truncated square patch antenna with high permittivity operated with RHCP pattern at1575 MHz,which meets the requirement of the GPS.Fig.4(b)illustrates the radiation pattern of the DCS antenna.The conical patterns on the x-z and y-z planes indicate that an omnidirectional radiation occured on the azimuthal plane.This monopolarized feature makes the high-order patch antenna suitable for mobile communication.IV.C ONCLUSIONThis communication presents a compact antenna design with high performances for the applications of the GPS and DCS,by using high permittivity substrates and a slotted ground plane.Here,a truncated square patch was adopted for circular polarization,which operated at 1575MHz and with8MHz bandwidth,suitable for the GPS.On the other hand,the antenna is also practical for the DCS with the high performance of the TM21mode and9.8%impedance bandwidth.The experimental results show that this design is ideally practical for dual-band GPS/DCS applications.R EFERENCES[1]H.Ohmine,Y.Sunara,and M.Matsunaga,“An annular-ring microstripantenna fed by a co-planar feed circuit for mobile satellite communica-tion use,”IEEE Trans.Antennas Propag.,vol.45,no.6,pp.1001–1008, Jun.1997.[2]N.Padros,J.I.Ortigosa,J.Baker,M.F.Iskander,and B.Thornberg,“Comparative study of high-performance GPS receiving antenna de-sign,”IEEE Trans.Antennas Propag.,vol.45,no.4,pp.698–706,Apr.1997.[3]J.Ollikainen,M.Fischer,and P.Vainikainen,“Thin dual-resonantstacked short patch antenna for mobile communication,”Electron.Lett., vol.35,pp.437–438,Mar.1999.[4]J.C.Batchelor and ngley,“Microstrip annular ring slot antennasfor mobile applications,”Electron.Lett.,vol.32,pp.1635–1636,1996.[5]S.Y.Lin and K.L.Wong,“Enhanced performances of a compactcon-ical-pattern annular-ring patch antenna using a slotted ground plane,”in Proc.2001Asia-Pacific Microwave Conf.,pp.1036–1039.[6]K.Fujimoto,A.Henderson,K.Hirasawa,and J.R.James,Small An-tennas.New York:Wiley,1987.[7]Y.S.Wu and F..Rosenbaum,“Mode chartfor microwave ring res-onators,”IEEE Trans.Microw.Theory Tech.,vol.21,pp.487–489,1973.Frequency Tuning of the Dielectric Resonator AntennaUsing a Loading CapH.K.Ng and K.W.LeungAbstract—A rigorous analysis of the slot-coupled hemispherical dielec-tric resonator top-loaded by a conducting cap is presented.The resonant frequency of the antenna can be tuned by changing the size of the loading cap.Measurements were carried out to verify the calculations,and reason-able agreement between theory and experiment is obtained.Index Terms—Dielectric resonator antenna(DRA),frequency tuning, parasitic patch.I.I NTRODUCTIONIn the last two decades,the dielectric resonator antenna(DRA)[1] has been studied extensively for a number of advantages,such as its small size,low loss,low cost and ease of excitation.The resonant fre-quency of a DRA depends on its operating mode,dielectric constant and physical shape.Although the source-free resonant frequencies of bare DRAs can be calculated by solving secular equations[2],[3],the method does not take any excitation effects into account and,conse-quently,the results normally deviate from the actual values.Even if a rigorous theory that considers the excitation source is used,the mea-sured and calculated resonant frequencies are usually different from each other because of fabrication tolerances.In recent years,attention has been paid on developing postmanufacturing frequency-tuning tech-niques for DRAs[4]–[6].However,all of them are purely experimental. Lately,an approach for frequency tunable designs using a parasitic slot has been studied theoretically and experimentally[7],but it is used for the design stage rather than for postmanufacturing tuning.In this com-munication,a rigorous theory for postmanufacturing frequency tuning of the hemispherical DRA is presented,with the DRA excited in its fundamental broadside TE111mode by a coupling aperture.The aper-ture-coupled source is commonly used for DRAs because it has sev-eral merits such as the feasibility of integration with monolithic mi-crowave integrated circuits(MMICs)and the avoidance of large probe reactance.In the analysis,use is made of the spectral-domain method to for-mulate the microstrip feedline part[8],whereas exact modal Green’s functions are employed for the DRA part.Integral equations for the cap currentand slotcurrentare formulat ed,which are solved using the method of moments(MoM).By changing the radius of the loading cap,the resonant frequency of the antenna can be tuned easily.Mea-surements were done to verify the calculations and good agreement between them is obtained.II.T HEORYFig.1(a)and(b)shows the side and top views of the DRA config-uration,respectively.The coupling slot of length L s and width W s couples the energy from the microstrip feedline to the hemispherical DRA of radius a=12:5mm and dielectric constant"ra=9:5. The grounded dielectric slab has dielectric constant"rs=2:33andheight d=1:57mm,and the50- microstrip feedline of width W f=Manuscript received July16,2004.This work was supported by the Research Grant Council of the Hong Kong SAR under Project CityU1284/03E.The authors are with the Wireless Communications Research Centre and De-partment of Electronic Engineering,City University of Hong Kong,Kowloon, Hong Kong.Digital Object Identifier10.1109/TAP.2004.8425830018-926X/$20.00©2005IEEE。