CN103078185B - High-gain low-radar cross section panel antenna based on artificial electromagnetic structural material - Google Patents
High-gain low-radar cross section panel antenna based on artificial electromagnetic structural material Download PDFInfo
- Publication number
- CN103078185B CN103078185B CN201310030029.XA CN201310030029A CN103078185B CN 103078185 B CN103078185 B CN 103078185B CN 201310030029 A CN201310030029 A CN 201310030029A CN 103078185 B CN103078185 B CN 103078185B
- Authority
- CN
- China
- Prior art keywords
- antenna
- span
- metal
- artificial
- gain
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Active
Links
- 239000000463 material Substances 0.000 title claims abstract description 57
- 229910052751 metal Inorganic materials 0.000 claims abstract description 53
- 239000002184 metal Substances 0.000 claims abstract description 53
- 230000000737 periodic effect Effects 0.000 claims abstract description 16
- 239000000758 substrate Substances 0.000 claims abstract description 13
- 238000010521 absorption reaction Methods 0.000 claims description 4
- 230000010287 polarization Effects 0.000 claims description 2
- 239000002594 sorbent Substances 0.000 claims 4
- 230000005855 radiation Effects 0.000 abstract description 4
- 239000011248 coating agent Substances 0.000 abstract 1
- 238000000576 coating method Methods 0.000 abstract 1
- 238000002310 reflectometry Methods 0.000 description 7
- 238000000034 method Methods 0.000 description 6
- 238000001035 drying Methods 0.000 description 4
- 238000005516 engineering process Methods 0.000 description 4
- 238000004088 simulation Methods 0.000 description 4
- 238000002834 transmittance Methods 0.000 description 4
- 238000013461 design Methods 0.000 description 3
- 238000000206 photolithography Methods 0.000 description 3
- 239000011358 absorbing material Substances 0.000 description 2
- 238000011161 development Methods 0.000 description 2
- 238000010586 diagram Methods 0.000 description 2
- 230000005684 electric field Effects 0.000 description 2
- 238000004519 manufacturing process Methods 0.000 description 2
- 238000012545 processing Methods 0.000 description 2
- 238000001039 wet etching Methods 0.000 description 2
- 238000004026 adhesive bonding Methods 0.000 description 1
- 229910052782 aluminium Inorganic materials 0.000 description 1
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 1
- 230000009286 beneficial effect Effects 0.000 description 1
- 230000005540 biological transmission Effects 0.000 description 1
- 238000001723 curing Methods 0.000 description 1
- 229920002120 photoresistant polymer Polymers 0.000 description 1
- 238000011160 research Methods 0.000 description 1
Landscapes
- Aerials With Secondary Devices (AREA)
Abstract
本发明提供一种基于人工电磁结构材料的高增益低雷达散射截面平板天线,该天线由微带贴片和正反两面具有不同反射特性的周期性人工结构材料构成。该人工结构材料由介质基板,以及在基板正面制作的周期性金属方环结构和反面制作的周期性开口缝隙金属平面结构构成。正面金属方环结构的四边中心处加载了集中电阻元件。当电磁波从人工结构材料正面入射时,电磁波能量主要被吸收;当电磁波从人工结构材料反面入射时,电磁波能量主要被反射。将人工结构材料放置在微带贴片上方作为覆层,其反面作为部分反射表面和微带贴片的金属接地板构成F-P谐振腔,提高天线的辐射增益;其正面可以吸收外来入射波,降低天线的雷达散射截面。
The invention provides a high-gain and low-radar-scattering cross-section planar antenna based on an artificial electromagnetic structure material. The antenna is composed of a microstrip patch and a periodic artificial structure material with different reflection characteristics on both sides. The artificial structure material is composed of a dielectric substrate, a periodic metal square ring structure fabricated on the front side of the substrate, and a periodic metal planar structure with open gaps fabricated on the reverse side. The center of the four sides of the metal square ring structure on the front is loaded with concentrated resistance elements. When the electromagnetic wave is incident from the front of the artificial structure material, the energy of the electromagnetic wave is mainly absorbed; when the electromagnetic wave is incident from the back of the artificial structure material, the energy of the electromagnetic wave is mainly reflected. The artificial structure material is placed on the top of the microstrip patch as a coating, and its reverse side is used as a part of the reflective surface and the metal ground plate of the microstrip patch to form a FP resonant cavity, which improves the radiation gain of the antenna; its front can absorb external incident waves and reduce The radar cross section of the antenna.
Description
技术领域technical field
本发明涉及一种高增益、低RCS平板天线,特别涉及一种基于人工电磁结构材料的高增益低RCS平板天线。The invention relates to a high-gain, low-RCS panel antenna, in particular to a high-gain, low-RCS panel antenna based on artificial electromagnetic structure materials.
背景技术Background technique
随着飞行器雷达截面的不断减小,机载天线系统对飞行系统的雷达散射截面的贡献就变得日益突出起来,因此降低天线系统的RCS已经成为目标隐身系统中一个重要的因素。平板天线(例如微带和F-P腔天线)具有质量轻、造价低、易于共型等优点,被广泛应用与飞行器件中。因此,降低平板天线的RCS和提高平板天线的增益引起了越来越科研人员的关注和研究。然而,传统的雷达吸波材料和雷达吸波结构在降低RCS的同时也降低了天线的增益和指向性。近几年,很多基于人工电磁结构材料降低天线的RCS技术被报道。Hong-Kyu Jang等科研人员利用新型电磁带隙结构作为雷达吸波材料实现了天线RCS的缩减(H.-K.Jang,et al.Design and fabrication of a microstrip patch antenna with a low radar crosssection in the X-band[J],Smart Mater.Struct.015007(2011)),加载电磁带隙结构材料后,微带贴片的RCS在8.5GHz到12GHz的频带内得到了很好的缩减,在11GHz附近,天线的RCS缩减近20分贝。因为材料在3.2GHz附近表现出很好的反射性能,所以对天线的指向性和增益影响很小,但是没有实现RCS带内缩减。Simone Genovesi等研究人员基于人工结构材料的频率选择表面实现了大角度RCS的缩减(S.Genovesi,et al.Low-Profile Array WithReduced Radar Cross Section by Using Hybrid Frequency Selective Surfaces[J],IEEETRANSACTIONS ON ANTENNAS AND PROPAGATION,VOL.60,NO.5,MAY2012),但是使用人工结构材料后,天线的指向性相对原天线降低了两个分贝左右。在本专利中,使用人工电磁结构材料加载在微带贴片上;即可提高天线辐射增益,同时又可以降低天线的RCS。As the radar cross section of the aircraft continues to decrease, the contribution of the airborne antenna system to the radar cross section of the flight system becomes increasingly prominent. Therefore, reducing the RCS of the antenna system has become an important factor in the target stealth system. Flat panel antennas (such as microstrip and F-P cavity antennas) have the advantages of light weight, low cost, and easy conformation, and are widely used in flight devices. Therefore, reducing the RCS of the panel antenna and increasing the gain of the panel antenna have attracted more and more attention and research of researchers. However, traditional radar absorbing materials and radar absorbing structures reduce the gain and directivity of the antenna while reducing the RCS. In recent years, many RCS technologies based on artificial electromagnetic structural materials to reduce antennas have been reported. Hong-Kyu Jang and other researchers used the new electromagnetic bandgap structure as the radar absorbing material to realize the reduction of the antenna RCS (H.-K.Jang, et al.Design and fabrication of a microstrip patch antenna with a low radar crosssection in the X-band[J], Smart Mater.Struct.015007(2011)), after loading the electromagnetic bandgap structure material, the RCS of the microstrip patch has been well reduced in the frequency band from 8.5GHz to 12GHz, and it is around 11GHz , the RCS of the antenna is reduced by nearly 20 decibels. Because the material exhibits good reflection performance near 3.2GHz, it has little influence on the directivity and gain of the antenna, but the RCS in-band reduction is not realized. Simone Genovesi and other researchers realized the reduction of large-angle RCS based on the frequency selective surface of artificial structural materials (S.Genovesi, et al. Low-Profile Array With Reduced Radar Cross Section by Using Hybrid Frequency Selective Surfaces[J], IEEETRANSACTIONS ON ANTENNAS AND PROPAGATION, VOL.60, NO.5, MAY2012), but after using artificial structural materials, the directivity of the antenna is reduced by about two decibels compared with the original antenna. In this patent, the artificial electromagnetic structure material is used to load on the microstrip patch; the radiation gain of the antenna can be improved, and the RCS of the antenna can be reduced at the same time.
综上所述,现有的降低天线RCS的设计方案中,在缩减RCS的同时对天线辐射性能也会有影响;而且很难实现带内和带外宽频带的RCS缩减。To sum up, in the existing design schemes for reducing the RCS of the antenna, the radiation performance of the antenna will be affected while the RCS is reduced; and it is difficult to realize the RCS reduction of the in-band and out-of-band broadband.
发明内容Contents of the invention
本发明要解决的技术问题是:克服现有天线RCS缩减技术中难以实现带内缩减、缩减带宽窄和对原天线增益的影响等困难;提出了一种基于人工电磁结构材料的高增益、低RCS平板天线,该设计方案不但可以提高原天线的增益,而且大幅度缩减的原天线带内和带外的RCS。The technical problem to be solved by the present invention is: to overcome the difficulty in realizing in-band reduction, narrow bandwidth reduction and the influence on the original antenna gain in the existing antenna RCS reduction technology; RCS panel antenna, this design scheme can not only improve the gain of the original antenna, but also greatly reduce the RCS in-band and out-of-band of the original antenna.
本发明解决其技术问题所采用的技术方案为:一种基于人工电磁结构材料的高增益低雷达散射截面平板天线,包括正反两面具有不同反射特性的周期性人工结构材料,以及微带贴片、金属接地板和微带贴片的介质板;正反两面具有不同反射特性的周期性人工结构材料由介质基板,以及介质基板上方的吸收表面和介质板下方的部分反射表面构成;其中吸收表面由周期性的金属方环结构,以及加载在方环四边中心的集中电阻元件构成;部分反射表面是由周期性的开口缝隙金属平面结构组成;一方面,当外来电磁波照射在吸收表面时,该材料可以将外来电磁波转换成热量损耗,从而降低了天线的RCS;另一方面,微带贴片辐射波的电场极化方向平行x轴,部分反射面和微带贴片的金属接地板构成一个F-P谐振腔,能够大幅度提高天线的增益。The technical solution adopted by the present invention to solve the technical problem is: a high-gain low radar cross-section planar antenna based on artificial electromagnetic structural materials, including periodic artificial structural materials with different reflection characteristics on the front and back sides, and microstrip patches , a metal ground plate and a dielectric plate with a microstrip patch; the periodic artificial structure material with different reflection characteristics on the front and back sides is composed of a dielectric substrate, an absorbing surface above the dielectric substrate, and a part of the reflective surface below the dielectric plate; the absorbing surface It is composed of a periodic metal square ring structure and a concentrated resistance element loaded in the center of the four sides of the square ring; part of the reflective surface is composed of a periodic open gap metal planar structure; on the one hand, when external electromagnetic waves irradiate on the absorbing surface, the The material can convert the external electromagnetic wave into heat loss, thereby reducing the RCS of the antenna; on the other hand, the electric field polarization direction of the microstrip patch radiation wave is parallel to the x-axis, and the partial reflective surface and the metal ground plate of the microstrip patch form a The F-P resonant cavity can greatly increase the gain of the antenna.
其中,所述介质基板的介电常数为εr1,介质基板的厚度h1的取值范围是λm1/20~λm1/5,金属方环结构的周期p的取值范围是λm1/5~3*λm1/5,金属方环结构的宽带w1的取值范围是λm1/30~λm1/10,金属方环结构的边长b的取值范围是λm1/6~λm1/2,金属方环结构的四边中心开口宽度g的取值范围是λm1/60~λm1/10;其中λm1为所述材料的吸波表面的吸收频段中心频率处对应的等效波长,λ01为中心频率处对应的真空中的波长。Wherein, the dielectric constant of the dielectric substrate is ε r1 , the value range of the thickness h 1 of the dielectric substrate is λ m1 /20~λ m1 /5, and the value range of the period p of the metal square ring structure is λ m1 / 5~3*λ m1 /5, the value range of the broadband w 1 of the metal square ring structure is λ m1 /30~λ m1 /10, the value range of the side length b of the metal square ring structure is λ m1 /6~ λ m1 /2, the value range of the central opening width g of the four sides of the metal square ring structure is λ m1 /60~λ m1 /10; where λ m1 is the corresponding value at the center frequency of the absorption frequency band of the wave-absorbing surface of the material effective wavelength, λ 01 is the wavelength in vacuum corresponding to the center frequency.
其中,开口缝隙金属平面结构的缝隙宽带为w2,w2的取值范围为λm2/300~λm2/50;开口缝隙金属平面结构的长度l取值范围为λm2/6~3*λm2/5;开口缝隙金属平面结构缝隙之间的间距d的取值范围为λm2/15~2*λm2/5;微带贴片的长和宽的取值范围为λm2/4~λm2;微带贴片的介质板的介电常数为εr2,微带贴片的介质板的厚度h2的取值范围为λm2/30~λm2/5;金属接地的厚度h3的取值范围为λm2/30~λm2/4;其中λm2为所述天线的工作频率处所对应的等效波长,λ02为工作频率处对应的真空中的波长。Among them, the gap broadband of the open gap metal planar structure is w 2 , and the value range of w 2 is λ m2 /300~λ m2 /50; the length l of the open gap metal planar structure ranges from λ m2 /6~3* λ m2 /5; the value range of the distance d between the gaps in the open gap metal planar structure is λ m2 /15~2*λ m2 /5; the value range of the length and width of the microstrip patch is λ m2 /4 ~λ m2 ; the dielectric constant of the dielectric plate of the microstrip patch is ε r2 , the thickness h 2 of the dielectric plate of the microstrip patch is in the range of λ m2 /30~λ m2 /5; the thickness of the metal grounding h3 The range of values is λ m2 /30~λ m2 /4; where λ m2 is the equivalent wavelength corresponding to the operating frequency of the antenna, λ 02 is the wavelength in vacuum corresponding to the operating frequency.
本发明具有的有益效果在于:The beneficial effects that the present invention has are:
(1)、本发明结构简单,正反两面具有不同反射特性的周期性人工结构材料1为平面结构,易于制作,利用PCB板加工工艺就可以制作,而这种加工工艺现在已经非常成熟。(1) The structure of the present invention is simple, and the periodic artificial structural material 1 with different reflection characteristics on the front and back sides is a planar structure, which is easy to manufacture and can be manufactured by using PCB board processing technology, and this processing technology is now very mature.
(2)、本发明在外来电磁波照射在吸收面5时,该材料可以束缚外来电磁波并将其转换成热量损耗,从而实现了在带内和带外降低了天线的RCS。另一方面,因为部分反射面7具有高反射和一定的透射,部分反射面7和金属接地3板可以构成一个F-P谐振腔,能够大幅度提高天线的增益。(2) In the present invention, when an external electromagnetic wave is irradiated on the absorbing surface 5, the material can bind the external electromagnetic wave and convert it into heat loss, thereby reducing the RCS of the antenna both in-band and out-of-band. On the other hand, because the partial reflection surface 7 has high reflection and certain transmission, the partial reflection surface 7 and the metal ground 3 can form an F-P resonant cavity, which can greatly improve the gain of the antenna.
附图说明Description of drawings
图1为本发明基于人工电磁结构材料的高增益、低RCS平板天线和正反两面具有不同反射特性的周期性人工结构材料1的单元结构图;Fig. 1 is a unit structure diagram of a high-gain, low RCS planar antenna based on artificial electromagnetic structural materials and a periodic artificial structural material 1 with different reflection characteristics on both sides of the present invention;
图2为本发明人工电磁结构材料的单元结构仿真得到透过率和吸波表面5和反射表面7的反射率;Fig. 2 obtains the transmittance and the reflectivity of the wave-absorbing surface 5 and the reflective surface 7 for the unit structure simulation of the artificial electromagnetic structure material of the present invention;
图3为本发明基于人工电磁结构材料的高增益、低RCS平板天线的回波损耗;Fig. 3 is the return loss of the high-gain, low RCS planar antenna based on the artificial electromagnetic structure material of the present invention;
图4为本发明基于人工电磁结构材料的高增益、低RCS平板天线和没有覆盖正反两面具有不同反射特性的周期性人工结构材料1时天线在11.5GHz时的E面的远场方向图。Fig. 4 is the far-field pattern of the E plane of the antenna at 11.5 GHz when the high-gain, low RCS panel antenna based on the artificial electromagnetic structure material and the periodic artificial structure material 1 with different reflection characteristics on the front and back sides are not covered in the present invention.
图5为本发明基于人工电磁结构材料的高增益、低RCS平板天线和没有覆盖正反两面具有不同反射特性的周期性人工结构材料1时天线在11.5GHz时的H面的远场方向图。Fig. 5 is the far-field pattern of the H surface of the antenna at 11.5 GHz when the high-gain, low-RCS panel antenna based on the artificial electromagnetic structure material and the periodic artificial structure material 1 with different reflection characteristics on the front and back sides of the present invention are not covered.
图6为本发明基于人工电磁结构材料的高增益、低RCS平板天线和没有覆盖正反两面具有不同反射特性的周期性人工结构材料1时天线的RCS与频率的关系图。Fig. 6 is a graph showing the relationship between RCS and frequency of the high-gain, low-RCS panel antenna based on the artificial electromagnetic structural material of the present invention and the periodical artificial structural material 1 with different reflection characteristics on the front and back without covering.
具体实施方式Detailed ways
下面结合附图及具体实施方式对本发明进行详细说明,但本发明的保护范围并不仅限于下面实施例,应包括权利要求书中的全部内容。而且本领域技术人员从以下的一个实施例即可实现权利要求中的全部内容。The present invention will be described in detail below in conjunction with the accompanying drawings and specific embodiments, but the scope of protection of the present invention is not limited to the following examples, but should include all content in the claims. Moreover, those skilled in the art can realize all the content in the claims from the following embodiment.
图1为基于人工电磁结构材料的高增益、低RCS平板天线和人工结构材料的单元结构材料图,图中1代表正反两面不同反射特性的周期性人工结构材料,2代表微带贴片,3代表金属接地板,4代表微带贴片的介质板,5代表反射表面,6代表介质基板,7代表吸收表面,8金属方环结构,9代表集中电阻元件,10代表开口缝隙金属平面结构,11代表外来入射波,12代表出射波。具体实现过程如下:Figure 1 is a high-gain, low-RCS panel antenna based on artificial electromagnetic structural materials and a unit structural material diagram of artificial structural materials. In the figure, 1 represents a periodic artificial structural material with different reflection characteristics on both sides, and 2 represents a microstrip patch. 3 represents the metal ground plane, 4 represents the dielectric plate of the microstrip patch, 5 represents the reflective surface, 6 represents the dielectric substrate, 7 represents the absorption surface, 8 represents the metal square ring structure, 9 represents the concentrated resistance element, and 10 represents the open gap metal planar structure , 11 represents the external incident wave, and 12 represents the outgoing wave. The specific implementation process is as follows:
(1)利用传统光刻工艺,在一张介电常数3.38,长宽为60mm×60mm,厚度为3.25mm的双面覆铜的微波PCB板(型号Rogers4003)金属层上旋涂光刻胶、烘干固化、曝光、显影、烘干坚膜、湿法腐蚀金属层等步骤,在微波PCB板的正面制作出周期个数为5×5的四边带开口的金属方环结构,同时在反面制作出周期5×5的开口缝隙金属平面结构,然后在金属方环结构四个开口中个焊接一个集中电阻元件;每个单元形状为图1中的金属方环结构、加载的集中电阻和开口缝隙金属平面结构所示的形状。上述微波PCB板(型号Rogers4003)为正反两面不同反射率的人工结构材料的介质基板6。本实例采取的参数尺寸为:金属方环结构8和开口缝隙金属平面结构10的周期p为12mm,金属方环结构8的边长b为7mm,金属方环结构8的宽w1为0.5mm,金属方环结构8四边中心开口宽度g为1mm,金属方环结构8四边中加载的集中电阻9的电阻值为110Ω。开口缝隙金属平面结构10中的缝隙宽带w2为0.15mm,缝隙长度l为8mm,缝隙沿x轴方向的周期d为4mm。(1) Using the traditional photolithography process, spin-coat photoresist on the metal layer of a double-sided copper-clad microwave PCB board (model Rogers4003) with a dielectric constant of 3.38, a length and width of 60mm×60mm, and a thickness of 3.25mm. Drying and curing, exposure, development, drying and hardening, wet etching of the metal layer and other steps, a metal square ring structure with a cycle number of 5×5 four sides with openings is produced on the front side of the microwave PCB board, and at the same time, it is produced on the back side A metal planar structure with open gaps of period 5×5 is produced, and then a concentrated resistance element is welded in the four openings of the metal square ring structure; the shape of each unit is the metal square ring structure in Figure 1, the loaded concentrated resistance and the open gap The shape shown in the metal planar structure. The above-mentioned microwave PCB board (model Rogers4003) is a dielectric substrate 6 of artificial structural materials with different reflectivity on the front and back sides. The parameter size taken in this example is: the period p of the metal square ring structure 8 and the open gap metal plane structure 10 is 12mm, the side length b of the metal square ring structure 8 is 7mm, and the width w1 of the metal square ring structure 8 is 0.5mm , the central opening width g of the four sides of the metal square ring structure 8 is 1mm, and the resistance value of the concentrated resistor 9 loaded on the four sides of the metal square ring structure 8 is 110Ω. The gap width w 2 in the open gap metal planar structure 10 is 0.15 mm, the gap length l is 8 mm, and the period d of the gap along the x-axis direction is 4 mm.
(2)利用传统光刻工艺,在一张介电常数2.5,长宽为60mm×60mm,厚度为1.524mm的单面覆铜的微波PCB板(型号Arlon AD250)正面金属层上旋涂光刻胶、烘干固化、曝光、显影、烘干坚膜、湿法腐蚀金属层等步骤,在微波PCB板的正面中心制作出一个金属方片结构作为微带贴片3。该微波PCB板(型号ArlonAD250)作为微带贴片的介质板4,微带贴片3的参数尺寸为:13.8mm×13.8mm。(2) Using the traditional photolithography process, spin-coat photolithography on the front metal layer of a single-sided copper-clad microwave PCB board (model Arlon AD250) with a dielectric constant of 2.5, a length and width of 60mm×60mm, and a thickness of 1.524mm. Gluing, drying and curing, exposure, development, drying and hardening, wet etching of the metal layer and other steps, a metal square structure is produced on the front center of the microwave PCB board as a microstrip patch 3. The microwave PCB board (model ArlonAD250) is used as the dielectric board 4 of the microstrip patch, and the parameter size of the microstrip patch 3 is: 13.8mm×13.8mm.
(3)用一张长宽为60mm×60mm,厚度为6mm的金属铝板紧贴着微带贴片的介质板4作为天线的金属接地板3。金属接地板3距离正反两面不同反射率的人工结构材料1为13mm。(3) A metal aluminum plate with a length and width of 60mm×60mm and a thickness of 6mm is used as the metal ground plate 3 of the antenna, which is closely attached to the dielectric plate 4 of the microstrip patch. The distance between the metal ground plate 3 and the artificial structural material 1 with different reflectivity on the front and back sides is 13 mm.
本发明的基于人工电磁结构材料的高增益、低RCS平板天线中的具有不同反射率人工结构材料,通过时域有限差分法(FDTD)仿真结果如图1所示,该图中的纵坐标的单位为分贝,横坐标为频率,图中实线表示的是电场方向平行于x轴的线极化波的透过率,可见在11.5GHz附近有一定的透过率,而在6-10.5GHz的透过率小于-10分贝。部分反射表面在6-12GHz有较高的反射率,特别是在工作频率11.5GHz附近的反射率均大于-2.5分贝,可以用来构造高增益F-P谐振腔。吸波表面在6.5-11GHz的反射率小于-10分贝,可见在该频带对电磁波有很好的吸收性能。The artificial structural materials with different reflectivity in the high-gain, low RCS panel antenna based on artificial electromagnetic structural materials of the present invention are simulated by the finite difference time domain method (FDTD) as shown in Figure 1, and the vertical coordinates in the figure The unit is decibel, and the abscissa is frequency. The solid line in the figure indicates the transmittance of the linearly polarized wave whose electric field direction is parallel to the x-axis. It can be seen that there is a certain transmittance near 11.5GHz, while that of The transmittance is less than -10 decibels. The partially reflective surface has high reflectivity at 6-12GHz, especially the reflectivity near the operating frequency of 11.5GHz is greater than -2.5 decibels, and can be used to construct a high-gain F-P resonant cavity. The reflectivity of the absorbing surface at 6.5-11GHz is less than -10 decibels, which shows that it has good absorption performance for electromagnetic waves in this frequency band.
本发明的基于人工电磁结构材料的高增益、低RCS平板天线,通过FDTD仿真结果如图2所示,该图中的纵坐标为回波损耗,横坐标为频率,在11.5GHz附近天线回波损耗小于-10分贝,天线可以正常工作。The high-gain, low-RCS planar antenna based on the artificial electromagnetic structure material of the present invention is shown in Figure 2 by the FDTD simulation result, and the ordinate in this figure is the return loss, and the abscissa is the frequency, and the antenna echo near 11.5GHz If the loss is less than -10dB, the antenna can work normally.
本发明的基于人工电磁结构材料的高增益、低RCS平板天线和没有覆盖正反两面不同反射特性的周期性人工结构材料的天线,通过FDTD仿真结果如图3所示,该图中的纵坐标为天线增益,横坐标为角度,图中实线表示的是基于人工电磁结构材料的高增益、低RCS平板天线E面的远场方向图;虚线为没有覆盖正反两面不同反射特性的周期性人工结构材料的天线E面远场方向图。可见,覆盖材料后天线增益从7分贝提高到了14分贝,同时波束宽度得到了缩减。图4中实线表示的是基于人工电磁结构材料的高增益、低RCS平板天线H面的远场方向图;虚线为没有覆盖正反两面不同反射特性的周期性人工结构材料的天线H面远场方向图。The high-gain, low RCS planar antenna based on artificial electromagnetic structural materials of the present invention and the antenna of periodic artificial structural materials that do not cover the different reflection characteristics of the front and back sides are as shown in Figure 3 through FDTD simulation results, and the vertical coordinates in the figure is the antenna gain, and the abscissa is the angle. The solid line in the figure represents the far-field pattern of the E-plane of the high-gain, low-RCS panel antenna based on artificial electromagnetic structure materials; the dotted line represents the periodicity that does not cover the different reflection characteristics of the front and back sides Antenna E-plane far-field pattern of artificial structural materials. It can be seen that the antenna gain is increased from 7dB to 14dB after covering the material, and the beam width is reduced at the same time. The solid line in Figure 4 shows the far-field pattern of the H-plane of the high-gain, low-RCS panel antenna based on artificial electromagnetic structure materials; field pattern.
本发明的基于人工电磁结构材料的高增益、低RCS平板天线和没有覆盖正反两面不同反射特性的周期性人工结构材料的天线,通过FDTD仿真结果如图6所示,该图中的纵坐标为天线的RCS,横坐标为角度,图中实线表示的是基于人工电磁结构材料的高增益、低RCS平板天线的RCS;虚线为没有覆盖正反两面不同反射特性的周期性人工结构材料的天线RCS。可见,覆盖材料后天线的RCS在6-14GHz都得到了显著的缩减。The high-gain, low RCS planar antenna based on the artificial electromagnetic structural material of the present invention and the antenna of the periodic artificial structural material that do not cover the different reflection characteristics of the front and back sides are as shown in Figure 6 through the FDTD simulation results, and the ordinate in the figure is the RCS of the antenna, and the abscissa is the angle. The solid line in the figure represents the RCS of a high-gain, low-RCS panel antenna based on artificial electromagnetic structural materials; Antenna RCS. It can be seen that the RCS of the antenna has been significantly reduced at 6-14GHz after covering the material.
本发明未详细阐述部分属于本领域技术人员的公知技术。Parts not described in detail in the present invention belong to the known techniques of those skilled in the art.
Claims (3)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201310030029.XA CN103078185B (en) | 2013-01-25 | 2013-01-25 | High-gain low-radar cross section panel antenna based on artificial electromagnetic structural material |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201310030029.XA CN103078185B (en) | 2013-01-25 | 2013-01-25 | High-gain low-radar cross section panel antenna based on artificial electromagnetic structural material |
Publications (2)
Publication Number | Publication Date |
---|---|
CN103078185A CN103078185A (en) | 2013-05-01 |
CN103078185B true CN103078185B (en) | 2014-11-12 |
Family
ID=48154641
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201310030029.XA Active CN103078185B (en) | 2013-01-25 | 2013-01-25 | High-gain low-radar cross section panel antenna based on artificial electromagnetic structural material |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN103078185B (en) |
Families Citing this family (16)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN104852153B (en) * | 2015-04-15 | 2017-10-10 | 北京航空航天大学 | It is a kind of that RCS composites are reduced based on the broadband for intersecting bowtie-shaped AMC |
CN105514619A (en) * | 2016-01-13 | 2016-04-20 | 武汉科技大学 | Ultra wideband material microwave absorber loaded with chip resistor |
CN107181056B (en) * | 2017-05-16 | 2022-08-30 | 叶云裳 | Microwave attenuation type GNSS measurement type antenna and equipment |
CN107611575B (en) * | 2017-08-29 | 2020-03-27 | 电子科技大学 | End-fire antenna based on surface wave waveguide and super surface absorber composite structure |
CN108682952B (en) * | 2018-03-15 | 2021-02-09 | 杭州电子科技大学 | Double-layer cascade dual-polarization broadband band-absorption type frequency selection surface |
CN108565549A (en) * | 2018-03-23 | 2018-09-21 | 南京航空航天大学 | A kind of medium incorporating high gain low section Fabry-Perot resonant antennas |
CN108521018B (en) * | 2018-03-23 | 2020-02-21 | 西安电子科技大学 | A circularly polarized F-P resonant cavity antenna with high gain and low RCS |
CN109560374B (en) * | 2018-11-22 | 2021-01-05 | 西安电子科技大学 | High-gain low-radar-section Fabry-Perot antenna |
CN109713457B (en) * | 2019-01-23 | 2021-01-26 | 西北大学 | Wave-absorbing/wave-transmitting super surface design method based on tantalum nitride material and application thereof |
CN111293441B (en) * | 2020-02-17 | 2021-05-25 | 南京航空航天大学 | Wave absorbing and transmitting integrated wave absorber |
CN111697335B (en) * | 2020-07-15 | 2021-07-20 | 盛纬伦(深圳)通信技术有限公司 | Radar antenna housing with mixed absorption and diffuse scattering |
CN111883934B (en) * | 2020-08-10 | 2021-06-01 | 西安电子科技大学 | Low RCS Antenna Based on Ultra-Broadband Miniaturized Absorber |
CN111987452B (en) * | 2020-09-01 | 2021-06-18 | 中国科学院光电技术研究所 | Transmission/reflection switchable and amplitude-adjustable metamaterial |
CN112086756B (en) * | 2020-09-04 | 2022-07-05 | 重庆大学 | Integrated electric/magnetic alternative wave absorbing device and antenna array multi-state mutual coupling suppression method |
CN113285237B (en) * | 2021-05-18 | 2022-06-14 | 重庆邮电大学 | Broadband high-gain Fabry-Perot resonant cavity antenna |
CN114843772B (en) * | 2022-04-25 | 2025-02-18 | 深圳万知达技术转移中心有限公司 | A dual-frequency, dual-circularly polarized, high-isolation Fabry-Perot cavity MIMO antenna and its processing method |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2006093301A1 (en) * | 2005-03-03 | 2006-09-08 | National University Corporation Yamaguchi University | Left-handed medium using no via |
CN101924572A (en) * | 2009-06-09 | 2010-12-22 | 美国博通公司 | Communication means and communication system |
CN102117971A (en) * | 2011-01-06 | 2011-07-06 | 西安电子科技大学 | Low-scattering plane-reflective array antenna |
-
2013
- 2013-01-25 CN CN201310030029.XA patent/CN103078185B/en active Active
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2006093301A1 (en) * | 2005-03-03 | 2006-09-08 | National University Corporation Yamaguchi University | Left-handed medium using no via |
CN101924572A (en) * | 2009-06-09 | 2010-12-22 | 美国博通公司 | Communication means and communication system |
CN102117971A (en) * | 2011-01-06 | 2011-07-06 | 西安电子科技大学 | Low-scattering plane-reflective array antenna |
Non-Patent Citations (2)
Title |
---|
Design of a Patch Antenna With Dual-band Radar Cross Section Reduction;Zhilong Miao等;《2012 International Conference on Microwave and Millimeter Wave Technology (ICMMT)》;20120508;第5卷;全文 * |
Zhilong Miao等.Design of a Patch Antenna With Dual-band Radar Cross Section Reduction.《2012 International Conference on Microwave and Millimeter Wave Technology (ICMMT)》.2012,第5卷1-3. * |
Also Published As
Publication number | Publication date |
---|---|
CN103078185A (en) | 2013-05-01 |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN103078185B (en) | High-gain low-radar cross section panel antenna based on artificial electromagnetic structural material | |
Jia et al. | Low-RCS, high-gain, and wideband mushroom antenna | |
Huang et al. | Wideband radar cross-section reduction of a stacked patch array antenna using metasurface | |
Ge et al. | Broadband and high‐gain printed antennas constructed from Fabry–Perot resonator structure using EBG or FSS cover | |
CN102227040A (en) | Array Antennas for Radar Cross Section Reduction | |
Liu et al. | RCS reduction of a patch array antenna based on microstrip resonators | |
Sun et al. | Low-RCS reflectarray antenna based on frequency selective rasorber | |
CN109713457B (en) | Wave-absorbing/wave-transmitting super surface design method based on tantalum nitride material and application thereof | |
CN106935970B (en) | Metamaterial structure, radome, antenna system and method for forming sandwich structure | |
CN111883932B (en) | Low radar cross section reflectarray antenna based on artificial surface plasmon | |
Shater et al. | Radar cross section reduction of microstrip antenna using dual-band metamaterial absorber | |
CN112467393A (en) | Dual-band RCS reduction super surface based on FSS and polarization rotation super surface | |
Jiang et al. | Polarization conversion metasurface for broadband radar cross section reduction | |
Jidi et al. | X-band and circularly polarized antenna with inborn RCS reduction | |
Zheng et al. | Ultrawideband and polarization-independent radar-cross-sectional reduction with composite artificial magnetic conductor surface | |
CN107611575B (en) | End-fire antenna based on surface wave waveguide and super surface absorber composite structure | |
CN112701495A (en) | Frustum-mounted two-dimensional conformal low-scattering ultra-wideband phased array based on strong coupling effect | |
Zhang et al. | A low-scattering Vivaldi antenna array with slits on nonradiating edges | |
Li et al. | A reflectarray antenna backed on FSS for low RCS and high radiation performances | |
CN103268979A (en) | A Dual Frequency High Gain Coaxial Feed Patch Antenna | |
Zhu et al. | An integrated antenna array with broadband, low-RCS, and high-gain characteristics | |
Zheng et al. | A new method for designing low RCS patch antenna using frequency selective surface | |
Panda et al. | Mushroom-like EBG structures for reducing RCS of patch antenna arrays | |
Sima et al. | Out-of-band RCS Reduction of a Dipole Antenna Based on Frequency-Selective Metasurface | |
Cong et al. | A new design method for patch antenna with low RCS and high gain performance |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
C06 | Publication | ||
PB01 | Publication | ||
C10 | Entry into substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
C14 | Grant of patent or utility model | ||
GR01 | Patent grant |