CN110707421A - Dual-polarization tightly-coupled phased array antenna based on end overlapping - Google Patents
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Abstract
本发明公开一种基于末端重叠的双极化紧耦合相控阵天线,包括多个周期排布的阵列单元,所述阵列单元包括正方形介质基板(1),偶极子天线(2),介质宽角匹配层(3),馈电结构(4),金属地板(5);所述介质宽角匹配层(3)叠置于介质基板(1)上表面,偶极子天线(2)紧贴于介质基板(1)下表面,所述金属地板(5)平行置于介质基板(1)之下,所述馈电结构(4)置于介质基板(1)与金属地板(5)之间,上端与偶极子天线(2)相连,下端与金属地板(5)相连;所述偶极子天线(2)为末端重叠的双极化紧耦合天线。本发明的双极化紧耦合相控阵天线,阻抗匹配好、宽带宽角、便于加工生产。
The invention discloses a dual-polarization tightly coupled phased array antenna based on overlapping ends, comprising a plurality of periodically arranged array units, the array units comprising a square dielectric substrate (1), a dipole antenna (2), a dielectric A wide-angle matching layer (3), a feeding structure (4), and a metal floor (5); the dielectric wide-angle matching layer (3) is stacked on the upper surface of the dielectric substrate (1), and the dipole antenna (2) is tightly Affixed to the lower surface of the dielectric substrate (1), the metal floor (5) is placed under the dielectric substrate (1) in parallel, and the feeding structure (4) is placed between the dielectric substrate (1) and the metal floor (5). In between, the upper end is connected to the dipole antenna (2), and the lower end is connected to the metal floor (5); the dipole antenna (2) is a dual-polarized tightly coupled antenna with overlapping ends. The dual-polarization tightly coupled phased array antenna of the invention has good impedance matching, wide bandwidth angle, and is convenient for processing and production.
Description
技术领域technical field
本发明属于宽带相控阵天线技术领域,特别是一种基于末端重叠的双极化紧耦合相控阵天线。The invention belongs to the technical field of broadband phased array antennas, in particular to a dual-polarization tightly coupled phased array antenna based on overlapping ends.
背景技术Background technique
相控阵天线是在阵列天线的基础上发展起来的一种现代天线形式。利用宽带天线单元,按照一定规律,将其排列成一维,二维或者其他阵列形式,避免可能产生的方向图畸变和扫描盲点,就构成了宽带相控阵的基本结构。相控阵是根据口径场相位做线性渐变时波束产生偏移的原理,用电子控制的方法改变阵列天线中各个单元的辐射场相位,利用主瓣波束进行扫描的。当宽带特性和宽角扫描特性结合起来的时候,就构成了宽带相控阵天线。Phased array antenna is a modern antenna form developed on the basis of array antenna. Using broadband antenna units, according to certain rules, they are arranged in one-dimensional, two-dimensional or other array forms to avoid possible pattern distortion and scanning blind spots, which constitute the basic structure of broadband phased array. The phased array is based on the principle that the beam shifts when the phase of the aperture field is linearly changed, and the phase of the radiation field of each element in the array antenna is changed by electronic control, and the main lobe beam is used for scanning. When the broadband characteristics and the wide-angle scanning characteristics are combined, a broadband phased array antenna is formed.
随着电子对抗与雷达领域迅猛发展,特别是宽频带干扰与反干扰、高分辨率和多维成像、目标识别等方面的发展,对阵列天线的工作频带有了更高的要求。另一方面,对于电子对抗与雷达系统平台,所用天线数目的降低能减少电子设备的复杂度和各个天线之间的互耦,所以该类系统平台对超宽带阵列天线有着迫切的需求。With the rapid development of electronic countermeasures and radar fields, especially the development of broadband interference and anti-jamming, high-resolution and multi-dimensional imaging, target recognition, etc., there are higher requirements for the working frequency band of array antennas. On the other hand, for electronic countermeasures and radar system platforms, the reduction of the number of antennas used can reduce the complexity of electronic equipment and the mutual coupling between each antenna, so this type of system platform has an urgent need for ultra-wideband array antennas.
传统的超宽带阵列天线多采用Vivaldi天线作为阵元形式,由于这种设计方法有其局限性,带宽拓宽的余地很小。譬如说,天线单元带宽会限制阵列带宽,空间扫描角度会受到单元间互耦的影响。为了保持阵列的辐射性能,传统的超宽带天线阵往往采用一些方法抑制单元间的耦合,例如在单元间加入金属隔板,或者加入吸波材料等等。除了物理上的隔离外,也有选择补偿的方式来抑制耦合,即在馈电前将信号乘以一个逆耦合因子,以消除互耦的影响。但是这些方法往往会带来一定负面影响,例如增益下降,方向图畸变,增加设计难度等等。同时传统宽带相控阵需要通过划分子阵、应用光调制和解调技术以及光纤延迟线来实现,设备量大,技术复杂,成本高,且不便于调试和维护。在相控阵天线的设计中,除了要解决一般阵列天线的宽带匹配问题外,还需要解决宽角扫描的匹配问题。Traditional ultra-wideband array antennas mostly use Vivaldi antennas as array elements. Due to the limitations of this design method, there is little room for bandwidth expansion. For example, the antenna element bandwidth will limit the array bandwidth, and the spatial scan angle will be affected by the mutual coupling between elements. In order to maintain the radiation performance of the array, traditional ultra-wideband antenna arrays often use some methods to suppress the coupling between units, such as adding metal partitions between units, or adding absorbing materials and so on. In addition to physical isolation, there is also a way to select compensation to suppress coupling, that is, multiply the signal by an inverse coupling factor before feeding to eliminate the influence of mutual coupling. However, these methods often bring certain negative effects, such as gain reduction, pattern distortion, increased design difficulty, and so on. At the same time, the traditional broadband phased array needs to be realized by dividing sub-arrays, applying optical modulation and demodulation technology, and optical fiber delay lines, which requires a large amount of equipment, complex technology, high cost, and inconvenient debugging and maintenance. In the design of phased array antenna, in addition to solving the broadband matching problem of general array antennas, it is also necessary to solve the matching problem of wide-angle scanning.
除了耦合问题外,超宽带天线阵存在体积较大的缺陷,传统Vivaldi天线阵、脊型渐变开槽天线阵为了实现阻抗的渐变,往往需要较长的长度;而传统的平面螺旋天线,为了实现超宽带特性,需要较大的半径。可见传统的超宽带天线阵由于体积问题,难以实现小型化、易共形等要求。In addition to the coupling problem, the ultra-wideband antenna array has the disadvantage of being large in size. The traditional Vivaldi antenna array and the ridge-shaped gradient slotted antenna array often need a long length in order to realize the gradient of the impedance; while the traditional flat helical antenna, in order to achieve Ultra-broadband characteristics require larger radii. It can be seen that the traditional ultra-wideband antenna array is difficult to achieve the requirements of miniaturization and easy conformality due to the volume problem.
例如,2018年张辉、汪俊等人在其发表的一篇名为《一种可重构的紧耦合宽带阵列天线》的专利(申请号为CN201810126029.2)中,提出了一个可实现紧耦合模式与常规模式切换且能实现S/C/X/Ku频段全覆盖的天线,该天线包括偶极子天线板、介质宽角匹配板以及金属地板。虽然其得到了三个倍频的天线带宽且实现了在S/C/X/Ku频段全覆盖,但并未采用馈电巴伦结构,不易于实现不平衡到平衡馈电的转换,且天线结构较为复杂,尤其是为了实现可重构特性设置的四个开关结构,不易加工。For example, in a patent (application number CN201810126029.2) published by Zhang Hui, Wang Jun and others in their patent titled "A Reconfigurable Tightly Coupled Broadband Array Antenna" (application number CN201810126029.2), they proposed a An antenna that can switch between the coupling mode and the conventional mode and can achieve full coverage of the S/C/X/Ku frequency bands. The antenna includes a dipole antenna plate, a dielectric wide-angle matching plate and a metal floor. Although it obtains three times the antenna bandwidth and achieves full coverage in the S/C/X/Ku frequency band, it does not use the feed balun structure, which is not easy to realize the conversion from unbalanced to balanced feed, and the antenna The structure is relatively complex, especially the four switch structures for realizing reconfigurable characteristic settings, which are not easy to process.
例如,2017年张帅,刘爽等人发表了一篇名为《超宽带阵列天线》的专利(申请号:CN201710483872.1),该专利包括偶极子天线阵列板、电阻型频率选择表面板、接地板和馈电巴伦,天线阵列板由多个偶极子辐射周期单元组成,并利用单元间的紧耦合,在0.63GHz~4.6GHz频段满足反射系数小于等于6dB。但是该阵列天线带宽不是很宽,并且结构比较复杂。For example, in 2017, Zhang Shuai, Liu Shuang and others published a patent called "Ultra Wideband Array Antenna" (application number: CN201710483872.1), which includes a dipole antenna array plate, a resistive frequency selective surface plate, The grounding plate and the feeding balun, the antenna array plate is composed of multiple dipole radiation periodic elements, and the tight coupling between the elements is used to satisfy the reflection coefficient of less than or equal to 6dB in the frequency band of 0.63GHz to 4.6GHz. However, the bandwidth of the array antenna is not very wide, and the structure is relatively complex.
发明内容SUMMARY OF THE INVENTION
本发明的目的在于提供一种基于末端重叠的双极化紧耦合相控阵天线,阻抗匹配好、宽带宽角、便于加工生产。The purpose of the present invention is to provide a dual-polarized tightly coupled phased array antenna based on overlapping ends, which has good impedance matching, wide bandwidth angle, and is easy to process and produce.
实现本发明目的的技术解决方案为:The technical solution that realizes the purpose of the present invention is:
一种基于末端重叠的双极化紧耦合相控阵天线,包括多个周期排布的阵列单元,A dual-polarized tightly coupled phased array antenna based on overlapping ends, comprising a plurality of periodically arranged array elements,
所述阵列单元包括正方形介质基板1,偶极子天线2,介质宽角匹配层3,馈电结构4,金属地板5;The array unit includes a square
所述介质宽角匹配层3叠置于介质基板1上表面,偶极子天线2紧贴于介质基板1下表面,所述金属地板5平行置于介质基板1之下,所述馈电结构4置于介质基板1与金属地板5之间,上端与偶极子天线2相连,下端与金属地板5相连;The dielectric wide-angle matching
所述偶极子天线2为末端重叠的双极化紧耦合天线。The
本发明与现有技术相比,其显著优点为:Compared with the prior art, the present invention has the following significant advantages:
1、阻抗匹配好:本发明通过加强阵元间的耦合拓宽天线带宽,能够在很宽的频带内保证阻抗的匹配,实现宽频带内的低电压驻波比,容易共形;1. Good impedance matching: the present invention widens the antenna bandwidth by strengthening the coupling between the array elements, can ensure impedance matching in a wide frequency band, realize a low voltage standing wave ratio in a wide frequency band, and is easy to conform;
2、宽带宽角:本发明采用微带结构的Marchand巴伦实现阻抗转换和场匹配,实现了相控阵天线的宽带宽角性能,同时便于天线的集成。2. Wide bandwidth angle: The present invention adopts the Marchand balun of the microstrip structure to realize impedance conversion and field matching, realizes the wide bandwidth angle performance of the phased array antenna, and facilitates the integration of the antenna.
3、便于加工生产:本发明采用超表面代替传统介质匹配板,降低了天线剖面;微带功分器采用微带结构,进一步简化加工的难度,便于将天线整体加工在一块PCB板材上。3. It is easy to process and produce: the present invention uses a metasurface to replace the traditional dielectric matching plate, which reduces the antenna profile; the microstrip power divider adopts a microstrip structure, which further simplifies the difficulty of processing and facilitates the overall processing of the antenna on a PCB board.
4、体积小:通过减小天线单元间的互耦,从而减小天线单元间的距离,使得天线单元之间更加紧凑,缩小天线整体体积。4. Small size: By reducing the mutual coupling between the antenna units, the distance between the antenna units is reduced, making the antenna units more compact and reducing the overall volume of the antenna.
此外,下面结合附图和具体实施方式对本发明作进一步的详细描述。In addition, the present invention will be further described in detail below with reference to the accompanying drawings and specific embodiments.
附图说明Description of drawings
图1是本发明实施例的单元结构示意图。FIG. 1 is a schematic diagram of a unit structure according to an embodiment of the present invention.
图2是本发明实施例的偶极子单元结构示意图。FIG. 2 is a schematic structural diagram of a dipole unit according to an embodiment of the present invention.
图3是本发明实施例的超表面结构示意图。FIG. 3 is a schematic diagram of a metasurface structure according to an embodiment of the present invention.
图4是本发明实施例的馈电巴伦结构示意图。FIG. 4 is a schematic structural diagram of a feeding balun according to an embodiment of the present invention.
图5是本发明实施例的金属地板结构示意图。FIG. 5 is a schematic structural diagram of a metal floor according to an embodiment of the present invention.
图6是本发明实施例的2×2阵列结构示意图。FIG. 6 is a schematic structural diagram of a 2×2 array according to an embodiment of the present invention.
图7是本发明实施例的天线单元工作带宽图。FIG. 7 is a diagram of a working bandwidth of an antenna unit according to an embodiment of the present invention.
图8是本发明实施例的天线单元回波损耗图。FIG. 8 is a return loss diagram of an antenna unit according to an embodiment of the present invention.
图9是本发明实施例的天线单元方向图。FIG. 9 is a directional diagram of an antenna unit according to an embodiment of the present invention.
图中,介质基板1,偶极子天线2,介质宽角匹配层3,馈电结构4,金属地板5,超表面6,In the figure, the
第一偶极子单元21,第二偶极子单元22,第一偶极子臂211,第二偶极子臂212,第三偶极子臂221,第四偶极子臂222,
第一介质板41,第二介质板42,印刷板411、412。The first
具体实施方式Detailed ways
本发明基于末端重叠的双极化紧耦合相控阵天线,包括多个周期排布的阵列单元。The present invention is based on a dual-polarized tightly coupled phased array antenna with overlapping ends, which includes a plurality of periodically arranged array elements.
如图1所示,所述阵列单元包括正方形介质基板1,偶极子天线2,介质宽角匹配层3,馈电结构4,金属地板5;As shown in FIG. 1 , the array unit includes a square
所述介质宽角匹配层3叠置于介质基板1上表面,偶极子天线2紧贴于介质基板1下表面,所述金属地板5平行置于介质基板1之下,所述馈电结构4置于介质基板1与金属地板5之间,上端与偶极子天线2相连,下端与金属地板5相连;The dielectric wide-angle matching
所述偶极子天线2为末端重叠的双极化紧耦合天线。The
如图2所示,as shown in
所述偶极子天线2包括形状相同的第一偶极子单元21和第二偶极子单元22,The
所述第一偶极子单元21呈领结形状,包括对称设置的第一偶极子臂211和第二偶极子臂212,所述第一偶极子臂211和第二偶极子臂212均由一矩形与一梯形底边连接面成,第一偶极子臂211的梯形顶边与第二偶极子臂212的梯形的边相对,两梯形顶边之间设有缝隙;The
所述第二偶极子单元22呈领结形状,包括对称设置的第三偶极子臂221和第四偶极子臂222,所述第三偶极子臂221和第四偶极子臂222均由一矩形与一梯形底边连接面成,第三偶极子臂221的梯形顶边与第四偶极子臂222的梯形的边相对,两梯形顶边之间设有缝隙;The
所述第一偶极子单元21的轴线平行于正方形介质基板1的一边,且第一偶极子单元21靠近该边,所述第二偶极子单元22的轴线与第一偶极子单元21的轴线垂直,且靠近正方形介质基板1的另一边,所述第二偶极子单元22的第四偶极子臂222的矩形与第一偶极子单元21的第二偶极子臂212的矩形垂直叠置。The axis of the
如图3所示,As shown in Figure 3,
所述馈电结构4包括竖向放置且相互垂直交叉的第一介质板41、第二介质板42,The feeding
所述第一介质板41的上端与第一偶极子单元21中轴线相连,所述第二介质板42的上端与第二偶极子单元22中轴线相连。The upper end of the
所述第二介质板42与第一介质板41的形状、结构相同;The
所述第一介质板41外观呈矩形,包括两层印刷板411、412和置于所述两层印刷板411、412间的微带结构馈电巴伦。The first
如图5所示,As shown in Figure 5,
所述金属地板5与第一介质板41下端相连处开有第一矩形缝隙51,所述第一矩形缝隙51位于第一偶极子臂211中轴线正下方;A first rectangular slot 51 is opened at the connection between the
所述金属地板5与第二介质板42下端相连处开有第二矩形缝隙52,所述第二矩形缝隙52位于第三偶极子臂221中轴线正下方。A second
如图4所示,As shown in Figure 4,
所述介质宽角匹配层3的上表面涂覆一层开口谐振环结构的超表面6。The upper surface of the dielectric wide-
优选地,所述超表面6在天线工作频率为0到15GHz时,其等效的介质宽角匹配层的介电常数为3.66。Preferably, the dielectric constant of the equivalent dielectric wide-angle matching layer of the
所述介质宽角匹配层3的厚度为6mm,相对介电常数为1.7。The thickness of the dielectric wide-
实施例中,所述介质基板1为方形板状结构,边长17.25mm,厚度0.508mm。In the embodiment, the
所述偶极子天线2包括偶极子单元21和22,所述偶极子单元21呈领结型,包括偶极子臂211和212,臂长d1=6.65mm,臂宽d2=2.75mm,两天线臂中间设置一个矩形缝隙,缝隙长w1=0.5mm,宽w0=0.45mm,天线臂与缝隙相接部分呈梯形,梯形高L=2.75mm,偶极子单元21水平放置于介质基板1的下表面,其中线与介质基板1的边长相互平行,且距离介质基板一边4.2226mm。The
偶极子单元22交叉垂直于偶极子单元21,且其中线距离介质基板1的一边4.2226mm。在组成阵列天线时,偶极子21的一臂212的末端和相邻天线单元的偶极子臂的末端重叠,重叠部分长2.6mm,偶极子22的一臂222的末端同样与另一相邻天线单元的偶极子臂的末端重叠,“十”字形每一端重叠部分长2mm。The
重叠部分实现了阵列天线的紧耦合,因此可以拓宽天线带宽,能够在很宽的频带内保证阻抗的匹配,实现宽频带内的低电压驻波比,容易共形。另外,由于减小了天线单元间的互耦,从而减小天线单元间的距离,使得天线单元之间更加紧凑,缩小天线整体体积。The overlapping part realizes the tight coupling of the array antenna, so the bandwidth of the antenna can be widened, the impedance matching can be ensured in a wide frequency band, and the low voltage standing wave ratio in the wide frequency band can be achieved, which is easy to conform. In addition, since the mutual coupling between the antenna units is reduced, the distance between the antenna units is reduced, so that the antenna units are more compact and the overall volume of the antenna is reduced.
介质宽角匹配层3是矩形块状结构,紧贴介质基板1放置,所述介质宽角匹配层3的长和宽均为17.25mm,厚度为6mm,介质宽角匹配层的上层可涂覆一层开口谐振环结构的超表面,谐振环缺口部分长0.435mm,半径为1.35mm,The dielectric wide-
加载超表面可降低介质宽角匹配层厚度,实现低剖面、小型化天线的设计。Loading the metasurface can reduce the thickness of the dielectric wide-angle matching layer and realize the design of low-profile and miniaturized antennas.
馈电结构4,包括两块介质板41、42,厚度均为0.3048mm,高16.992mm,长17.25mm,垂直放置于介质基板1和金属地板之间,金属地板与介质基板平行,且介质板41和42互相交叉垂直,其上端分别与偶极子单元21和22的中线对应相接,其下端分别与金属地板5上所开矩形缝隙51、52连接。介质板41(或42)包括两层印刷板412(或421)和412(或422),两层印刷板上中间夹层内印有馈电巴伦。The feeding
所述馈电巴伦可以采用微带结构实现阻抗转换和场匹配,进而实现相控阵天线的宽带宽角性能,同时便于天线的集成。The feeding balun can adopt a microstrip structure to realize impedance conversion and field matching, thereby realizing the wide bandwidth angle performance of the phased array antenna, and at the same time facilitating the integration of the antenna.
馈电巴伦由微带线和短接线构成,宽6mm,高16.992mm,厚0.3084mm,巴伦与介质基板下表面相接部分开有两缺口,宽2.25mm、高0.5mm,两缺口中间开有一条型槽,宽w1=0.05mm、高1.65mm,条型槽下接矩形空心槽。矩形空心槽中线与巴伦中线重合,宽3.7mm,高12.5mm。微带线宽Wfeed=0.015mm,下接金属地板,垂直于金属地板向上延伸1.0825mm,然后平行于介质基板延伸2.16mm,进而连接到短接线的尖端,短接线由尖端渐变为矩形,矩形宽度doc=0.5mm,所述矩形短接线的水平部分的上边距介质基板1为0.825mm、下边距介质基板1为1.325mm,竖直部分的长边长8mm,短边长7.5mm,短接线垂直于金属地板部分的中线与巴伦中线相距2.425mm。The feeding balun is composed of microstrip lines and short wires, with a width of 6mm, a height of 16.992mm, and a thickness of 0.3084mm. There are two gaps between the balun and the lower surface of the dielectric substrate, with a width of 2.25mm and a height of 0.5mm. There is a slot, width w1=0.05mm, height 1.65mm, the slot is connected to a rectangular hollow slot. The centerline of the rectangular hollow groove coincides with the centerline of the balun, with a width of 3.7mm and a height of 12.5mm. The width of the microstrip line is Wfeed=0.015mm, the bottom is connected to the metal floor, it extends upwards by 1.0825mm perpendicular to the metal floor, and then extends 2.16mm parallel to the dielectric substrate, and then connects to the tip of the short wire. The short wire gradually changes from the tip to a rectangle with a width of the rectangle. doc=0.5mm, the upper edge of the horizontal part of the rectangular short wire is 0.825mm away from the
由于短接线的阻抗转换,可以将馈电得到的能量通过短接线辐射向空间。Due to the impedance conversion of the short wire, the energy obtained by the feeding can be radiated to the space through the short wire.
所述金属地板5上开有两个矩形缝隙51和52,并且分别位于偶极子臂211和221中线的正下方,缝隙的宽度均为0.3048mm,其中矩形缝隙51的深度s1=3.125mm,矩形缝隙52的深度s2=3.18065mm,矩形缝隙内设有激励单元511和521,激励单元511的长为1.15mm,激励单元521的长为0.6096mm,且激励单元511和521的外端靠近金属地板5边缘的长度均为ss=1.5702mm。There are two
所述金属地板5下方可以连接微带功分器,组成天线阵列之后,可以通过相位补偿,使相位做线性渐变从而实现波束方向偏移。所述微带功分器采用微带结构,进一步简化加工的难度,便于将天线整体加工在一块PCB板材上。A microstrip power divider can be connected under the
在金属地板5的激励单元511和521处设置激励后,电流沿着微带线传播到短接线的尖端部位,能量汇集于此处,也就是偶极子单元21和22的两天线臂中间的矩形缝隙处,再沿着短接线传播并最终辐射出去。After the excitation is set at the
图6是本发明实施例的2×2阵列结构示意图。FIG. 6 is a schematic structural diagram of a 2×2 array according to an embodiment of the present invention.
根据上述实施例,利用电磁仿真软件HFSS可以得到如图7以及图8所示的端口驻波比曲线,从该曲线可以看出,在端口驻波比小于2.5的前提下,本实施例所示的超宽带宽角紧耦合天线阵,可以在2GHz到7GHz的超宽带内实现E面以及H面最高到45°的宽角扫描性能。According to the above embodiment, the electromagnetic simulation software HFSS can be used to obtain the port VSWR curves as shown in FIG. 7 and FIG. 8 . It can be seen from the curves that, on the premise that the port VSWR is less than 2.5, as shown in this embodiment The ultra-wide bandwidth angle tightly coupled antenna array can achieve wide-angle scanning performance of E-plane and H-plane up to 45° in the ultra-wideband of 2GHz to 7GHz.
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