CN106684571A - Miura - Ori origami structure electromagnetic stealthl plate of loaded graphene metamaterial unit - Google Patents
Miura - Ori origami structure electromagnetic stealthl plate of loaded graphene metamaterial unit Download PDFInfo
- Publication number
- CN106684571A CN106684571A CN201710108086.3A CN201710108086A CN106684571A CN 106684571 A CN106684571 A CN 106684571A CN 201710108086 A CN201710108086 A CN 201710108086A CN 106684571 A CN106684571 A CN 106684571A
- Authority
- CN
- China
- Prior art keywords
- board
- electromagnetic
- cloaking
- electromagnetic cloaking
- metamaterial unit
- 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.)
- Pending
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q17/00—Devices for absorbing waves radiated from an antenna; Combinations of such devices with active antenna elements or systems
- H01Q17/007—Devices for absorbing waves radiated from an antenna; Combinations of such devices with active antenna elements or systems with means for controlling the absorption
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01Q—ANTENNAS, i.e. RADIO AERIALS
- H01Q17/00—Devices for absorbing waves radiated from an antenna; Combinations of such devices with active antenna elements or systems
-
- H—ELECTRICITY
- H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
- H05K—PRINTED CIRCUITS; CASINGS OR CONSTRUCTIONAL DETAILS OF ELECTRIC APPARATUS; MANUFACTURE OF ASSEMBLAGES OF ELECTRICAL COMPONENTS
- H05K9/00—Screening of apparatus or components against electric or magnetic fields
-
- H—ELECTRICITY
- H05—ELECTRIC TECHNIQUES NOT OTHERWISE PROVIDED FOR
- H05K—PRINTED CIRCUITS; CASINGS OR CONSTRUCTIONAL DETAILS OF ELECTRIC APPARATUS; MANUFACTURE OF ASSEMBLAGES OF ELECTRICAL COMPONENTS
- H05K9/00—Screening of apparatus or components against electric or magnetic fields
- H05K9/0073—Shielding materials
Landscapes
- Engineering & Computer Science (AREA)
- Microelectronics & Electronic Packaging (AREA)
- Shielding Devices Or Components To Electric Or Magnetic Fields (AREA)
Abstract
本发明为一种负载石墨烯超材料单元的Miura‑Ori折纸结构电磁隐身板,本发明的电磁隐身板,制备方法为:将基板浸入对苯二酚与氧化石墨烯混合液中,密封加热处理,使基板上附着吸波介质;取出清洗后,冷冻处理再干燥,得到石墨烯织布;石墨烯织布浸入环氧树脂前驱体溶液中浸渍后,铺平加热固化,得到电磁隐身板;将电磁隐身板按照Miura‑Ori折纸方法加工折痕,使电磁隐身板沿折痕伸缩变形;并在将电磁隐身板上板面粘固上述超材料单元。本发明通过折纸结构的变形设计,可以改变入射角和电磁波传播路径,实现调频隐身效果;通过超材料与吸波基体匹配,获得有效吸收更宽的吸收效率。
The present invention is a Miura-Ori origami structure electromagnetic cloaking board loaded with graphene metamaterial units. The preparation method of the electromagnetic cloaking board of the present invention is: immersing the substrate in a mixture of hydroquinone and graphene oxide, sealing and heat treatment , so that the substrate is attached with a wave-absorbing medium; after taking it out and cleaning it, freeze it and then dry it to obtain a graphene woven cloth; after dipping the graphene woven cloth in an epoxy resin precursor solution, lay it flat and heat and solidify it to obtain an electromagnetic stealth board; The electromagnetic cloaking board is creased according to the Miura-Ori origami method, so that the electromagnetic cloaking board stretches and deforms along the creases; and the above-mentioned metamaterial unit is glued on the surface of the electromagnetic cloaking board. Through the deformation design of the origami structure, the invention can change the incident angle and the electromagnetic wave propagation path to realize the frequency modulation stealth effect; through the matching of the metamaterial and the wave-absorbing matrix, a wider absorption efficiency can be effectively absorbed.
Description
技术领域technical field
本发明属于调频隐身材料与结构的设计与制备领域,特别涉及一种具有可调频吸波隐身性能的石墨烯/聚合物新复合结构电磁隐身板。The invention belongs to the field of design and preparation of frequency modulation stealth materials and structures, and in particular relates to a graphene/polymer new composite structure electromagnetic stealth board with adjustable frequency absorbing stealth performance.
背景技术Background technique
高性能电磁隐身材料(对电磁波具有强吸收与弱反射功能的材料)在探测、通信、航天、航空、先进装备等领域需求迫切。电磁隐身技术是通过利用电磁隐身材料与结构,减弱、抑制、吸收、偏转电磁波的强度,最大程度地降低(雷达电磁波)探测系统发现和识别(探测目标)的概率。随着信息时代的发展,高性能电磁隐身材料在探测、目标识别、电子对抗等诸多先进装备技术重要领域拥有巨大的应用潜力和发展空间,设计开发“轻、宽、薄、强”电磁隐身材料已经成为科技界与工业界的研究重点。[R.C.Che,L.M.Peng,X.F.Duan,Q.Chen,X.Liang,Adv.Mater.2004,16,401.Q.H.Liu Q.Cao,H.Bi,C.Y.Liang,K.P.Yuan,W.She,Y.J.Yang,R.C.Che,Adv.Mater.2016,28,486.]High-performance electromagnetic stealth materials (materials with strong absorption and weak reflection functions for electromagnetic waves) are in urgent demand in the fields of detection, communication, aerospace, aviation, and advanced equipment. Electromagnetic stealth technology uses electromagnetic stealth materials and structures to weaken, suppress, absorb, and deflect the intensity of electromagnetic waves to minimize the probability of (radar electromagnetic wave) detection system discovering and identifying (detecting targets). With the development of the information age, high-performance electromagnetic stealth materials have huge application potential and development space in many important fields of advanced equipment technology such as detection, target recognition, and electronic countermeasures. Design and develop "light, wide, thin, and strong" electromagnetic stealth materials It has become the research focus of science and technology circles and industrial circles. [R.C.Che, L.M.Peng, X.F.Duan, Q.Chen, X.Liang, Adv.Mater. Che, Adv. Mater. 2016, 28, 486.]
常规的吸波介质包括,介电损耗型、磁损耗型以及磁介耦合共损型,因在低频波段更易于拓宽有效吸收,磁介耦合共损型吸波介质一直受到关注。王钧等采用Fe50Ni50修饰的还原氧化石墨烯为磁损耦合吸波剂,获得了有效吸收带宽为8.8-13.1GHz的环氧树脂基的吸波介质[JOURNAL OF ALLOYS AND COMPOUNDS,Volume:653Pages:14-21,2015]。近期,车仁超等在制备了CoNi@SiO2@TiO2与CoNi@Air@TiO2多级微球结构的吸波介质填料,在2-18GHz范围内有效带宽能够达到8.1GHz,为发展新型磁电耦合吸波介质提出了新思路[Q.H.Liu Q.Cao,H.Bi,C.Y.Liang,K.P.Yuan,W.She,Y.J.Yang,R.C.Che,Adv.Mater.2016,28,486]。Conventional absorbing media include dielectric loss type, magnetic loss type, and magnetic-dielectric coupling loss type. Because it is easier to broaden the effective absorption in the low-frequency band, magnetic-dielectric coupling loss type absorbing media has always been concerned. Wang Jun et al. used Fe 50 Ni 50 modified reduced graphene oxide as a magnetic loss coupling absorber, and obtained an epoxy resin-based absorbing medium with an effective absorption bandwidth of 8.8-13.1 GHz [JOURNAL OF ALLOYS AND COMPOUNDS, Volume: 653 Pages: 14-21, 2015]. Recently, Che Renchao et al. have prepared CoNi@SiO 2 @TiO 2 and CoNi@Air@TiO 2 multi-level microsphere structure absorbing dielectric fillers. The effective bandwidth can reach 8.1 GHz in the range of 2-18 GHz. The magnetoelectric coupling absorbing medium puts forward a new idea [QHLiu Q.Cao, H.Bi, CYLiang, KPYuan, W.She, YJYang, RCChe, Adv.Mater.2016, 28, 486].
可调频隐身材料是解决隐身材料有效吸收带宽(反射损耗值<-10dB的频率宽度)偏窄突出问题的一种颠覆性手段。[H.T.Chen,J.F.O’Hara,A.K.Azad,A.J.Taylor,R.D.Averitt,D.B.Shrekenhamer,and W.J.Padilla,Nat.Photonics 2,295(2008).;H.T.Chen,W.J.Padilla,J.M.O.Zide,A.C.Gossard,A.J.Taylor,and R.D.Averitt,Nature(London)444,597(2006)]车仁超等通过调控隐身材料本征物理参数或者改变隐身超材料的图案结构,在多个频段实现谐振吸收峰的移动,对信号作出响应功能实现频率转变,改变隐身结构对外界目标电磁波频段的响应能力。设计具有碳纳米管阵列取向夹角的双层吸波介质,初始状态(夹角为0°)下有效吸波带宽为7.2~8.6GHz(反射损耗<-10dB的频带宽度),通过改变取向夹角(0~90°),最佳谐振峰频点位置由7.9GHz移动到11GHz,有效吸波带宽移动到10~12.2GHz,实现了7.2~12.2GHz范围内的可调控吸波带宽[Hao Sun,Renchao Che,Xiao You,Yishu Jiang,Zhibin Yang,Jue Deng,Longbin Qiu,and Huisheng Peng,Adv.Mater.2014,26,8120–8125]。因此,与传统隐身材料相比,相同条件下可调频电磁隐身材料拥有更加优异的吸波带宽与灵活性,极大地降低了隐身材料的厚度和重量,增强了隐身材料的宽频响应。Frequency-tunable stealth materials are a subversive means to solve the problem of narrow and prominent effective absorption bandwidth (frequency width of reflection loss value <-10dB) of stealth materials. [H.T.Chen, J.F.O'Hara, A.K.Azad, A.J.Taylor, R.D.Averitt, D.B.Shrekenhamer, and W.J.Padilla, Nat.Photonics 2, 295 (2008).; H.T.Chen, W.J.Padilla, J.M.O.Zide, A.C.Gossard, A.J.Taylor, and R.D.Averitt, Nature (London) 444,597 (2006)] Renchao Che et al. realized the movement of resonance absorption peaks in multiple frequency bands by adjusting the intrinsic physical parameters of stealth materials or changing the pattern structure of stealth metamaterials, and realized the function of responding to signals Frequency conversion, changing the response capability of the stealth structure to the frequency band of external target electromagnetic waves. Design a double-layer absorbing medium with a carbon nanotube array orientation angle. The effective absorption bandwidth is 7.2-8.6GHz (band width of reflection loss<-10dB) in the initial state (the angle is 0°). By changing the orientation angle Angle (0~90°), the best resonant peak frequency position moves from 7.9GHz to 11GHz, the effective absorbing bandwidth moves to 10~12.2GHz, and the adjustable absorbing bandwidth in the range of 7.2~12.2GHz is realized [Hao Sun , Renchao Che, Xiao You, Yishu Jiang, Zhibin Yang, Jue Deng, Longbin Qiu, and Huisheng Peng, Adv. Mater. 2014, 26, 8120–8125]. Therefore, compared with traditional stealth materials, frequency-tunable electromagnetic stealth materials have better absorbing bandwidth and flexibility under the same conditions, greatly reducing the thickness and weight of stealth materials, and enhancing the broadband response of stealth materials.
由于厚度方面的限制,通过调整吸波介质中的电磁参数,诱发有效吸收谐振频率及吸收强度的改变实现调频吸波介质,一直是研究热点。Due to the limitation of the thickness, it has been a research hotspot to realize the frequency modulation of the absorbing medium by adjusting the electromagnetic parameters in the absorbing medium to induce changes in the effective absorption resonance frequency and absorption strength.
(1)温度场调频:曹茂盛等研究了具有温度响应的介质材料,一维纳米钴链本征极化、电损耗及磁损耗会随着温度的升高,引起电磁参数大幅变化,当环境温度在50°~300°变化时,纳米钴链/二氧化硅复合材料可实现8.2-11GHz可调控吸收带宽[Liu J,CaoMS.ACS Appl.Mater.Interfaces 2016,8,22615-22622]。(1) Frequency modulation of temperature field: Cao Maosheng et al. have studied dielectric materials with temperature response. The intrinsic polarization, electrical loss and magnetic loss of one-dimensional nano-cobalt chains will cause large changes in electromagnetic parameters with the increase of temperature. When the environment When the temperature changes from 50° to 300°, nano-cobalt chains/silica composites can achieve 8.2-11GHz tunable absorption bandwidth [Liu J, CaoMS.ACS Appl.Mater.Interfaces 2016,8,22615-22622].
(2)极化方向调频:彭慧胜等通过调整两层阵列织物堆叠时的交互角度改变电磁波的极化方式与传播损耗方式,通过交互角度在0-90度中调整,实现了吸收峰在7.5-11GHz频率范围内的可控变换[Cross-Stacking Aligned Carbon-Nanotube Films to TuneMicrowave Absorption Frequencies and Increase AbsorptionIntensities.Adv.Mater.2014,26,8120.]。(2) Polarization direction frequency modulation: Peng Huisheng et al. changed the polarization mode and propagation loss mode of electromagnetic waves by adjusting the interaction angle when the two-layer array fabric was stacked. By adjusting the interaction angle from 0 to 90 degrees, the absorption peak was achieved at 7.5- Controllable transformation in the 11GHz frequency range [Cross-Stacking Aligned Carbon-Nanotube Films to TuneMicrowave Absorption Frequencies and Increase Absorption Intensities. Adv. Mater. 2014, 26, 8120.].
在可调频超材料吸波材料中,江建军团队设计了含PIN二极管的有源频率选择表面的超材料隐身结构,通过调节结构中的偏置电压改变谐振特性,在5.3-13GHz实现最佳宽度隐身性能[Chen Q,Jiang JJ,et al.Acta Phys.Sin.2011,60,074202]。In the frequency-tunable metamaterial absorbing material, Jiang Jianjun’s team designed a metamaterial stealth structure with an active frequency-selective surface containing PIN diodes. By adjusting the bias voltage in the structure to change the resonance characteristics, the optimal width stealth was achieved at 5.3-13GHz Performance [Chen Q, Jiang JJ, et al. Acta Phys. Sin. 2011, 60, 074202].
尽管可调频隐身材料在近期取得了重要进展,但是依然存在两个问题:(1)可调参数有限且可调频段狭窄。目前实现的调频技术中通常只针对某个单一参数在一个有限的范围内(几个GHz范围内)进行调控,所能够实现的可调频段范围狭窄,实现宽带调频依然面临挑战。(2)可调维度空间单一(吸波调控维度)其理论模型有待完善。目前研究的可调频方式设计大多依托在单一平面内改变材料物理性能参数,对于在依托结构变形的多维空间调频实验与理论研究依然较少,对多维空间中超材料隐身结构的调频规律的认识依然有限。Although tunable stealth materials have made important progress recently, there are still two problems: (1) The tunable parameters are limited and the tunable frequency band is narrow. Currently implemented frequency modulation technology usually only regulates a single parameter within a limited range (in the range of several GHz), and the range of adjustable frequency bands that can be realized is narrow, and the realization of broadband frequency modulation is still facing challenges. (2) The theoretical model of the single adjustable dimension space (wave absorbing control dimension) needs to be improved. Most of the currently researched frequency-tunable methods rely on changing the physical performance parameters of materials in a single plane. There are still few experimental and theoretical studies on frequency modulation in multi-dimensional space based on structural deformation, and the understanding of the frequency modulation laws of metamaterial stealth structures in multi-dimensional space is still limited. .
发明内容Contents of the invention
本发明目的是为了解决了调频带宽范围与机理有局限性以及调频维度空间单一的问题,而提供一种负载石墨烯超材料单元的Miura-Ori折纸结构电磁隐身板。The purpose of the present invention is to solve the problems of limited frequency modulation bandwidth range and mechanism and single frequency modulation dimension space, and provide a Miura-Ori origami structure electromagnetic stealth board loaded with graphene metamaterial units.
本发明的目的是通过以下技术方案实现的:The purpose of the present invention is achieved through the following technical solutions:
本发明的一种电磁隐身板,具体制备步骤如下:A kind of electromagnetic stealth board of the present invention, specific preparation steps are as follows:
步骤1:将氧化石墨烯溶于水配置成浓度为1.0~9.0mg/ml氧化石墨烯水溶液,将对苯二酚加入氧化石墨烯水溶液中,搅拌均匀;对苯二酚与氧化石墨烯质量比为0.1~10;Step 1: Dissolve graphene oxide in water to prepare a graphene oxide aqueous solution with a concentration of 1.0-9.0 mg/ml, add hydroquinone into the graphene oxide aqueous solution, and stir evenly; the mass ratio of hydroquinone to graphene oxide 0.1 to 10;
步骤2:将基板浸入上述混合液中,并将其密封;在70-120℃的条件下保温处理2~20h,使基板上附着吸波介质;所述基板为聚合物织物或者聚合物泡沫;基板厚度为1~10mm;Step 2: immerse the substrate in the above mixture, and seal it; heat preservation treatment at 70-120°C for 2-20 hours, so that the substrate is attached with a wave-absorbing medium; the substrate is polymer fabric or polymer foam; Substrate thickness is 1~10mm;
步骤3:将附着有吸波介质的基板从混合液中取出,用水浸泡清洗后,平铺成直板后在-20~-60℃的条件下冷冻2~100h,再置于常温下干燥2~100h,得到石墨烯织布;Step 3: Take the substrate with the absorbing medium out of the mixture, soak it in water and wash it, spread it into a straight plate, freeze it at -20~-60℃ for 2~100 hours, and then dry it at room temperature for 2~ 100h, obtain graphene weaving;
步骤4:将环氧树脂与环氧树脂固化剂按1:1~1:3的质量比混合,配制成形成环氧树脂前驱体溶液;将步骤3得到的石墨烯织布浸入环氧树脂前驱体溶液中浸渍1h以上,取出后铺平,在70~150℃下加热固化2~10小时,得到电磁隐身板。Step 4: Mix epoxy resin and epoxy resin curing agent at a mass ratio of 1:1 to 1:3 to form an epoxy resin precursor solution; immerse the graphene woven fabric obtained in step 3 into the epoxy resin precursor Immerse in the body solution for more than 1 hour, take it out, pave it flat, heat and cure it at 70-150°C for 2-10 hours, and obtain an electromagnetic stealth board.
为提高电磁隐身板的可调隐身性能,本发明还提供一种负载超材料单元结构的电磁隐身板,包括上述方法制备的电磁隐身板,以及粘固在电磁隐身板上板面的超材料单元,所述超材料单元为通过上述方法制备的电磁隐身板剪切而成的正方形、圆形、十字形、回字形薄片结构,超材料单元的外边长为5~40mm,超材料单元的厚度与所粘固的电磁隐身板的厚度相同;同一电磁隐身板上粘固的所有超材料单元外形相同,且各个超材料单元在电磁隐身板上板面呈等间距分布。In order to improve the adjustable stealth performance of the electromagnetic cloaking board, the present invention also provides an electromagnetic cloaking board with a metamaterial unit structure, including the electromagnetic cloaking board prepared by the above method, and the metamaterial unit glued on the surface of the electromagnetic cloaking board , the metamaterial unit is a square, circular, cross-shaped, back-shaped sheet structure cut from the electromagnetic cloaking plate prepared by the above method, the outer length of the metamaterial unit is 5-40 mm, and the thickness of the metamaterial unit is the same as The thickness of the electromagnetic cloaking boards bonded is the same; all metamaterial units bonded on the same electromagnetic cloaking board have the same shape, and each metamaterial unit is distributed at equal intervals on the surface of the electromagnetic cloaking board.
为提高电磁隐身板的可调隐身性能,本发明还提供一种可伸缩变形的电磁隐身板,将上述方法制备的电磁隐身板剪切为符合Miura-Ori折纸方法的长宽比为5:7的矩形板,再将电磁隐身板的一侧板面按照Miura-Ori折纸方法加工折痕,使电磁隐身板沿折痕伸缩变形。In order to improve the adjustable stealth performance of the electromagnetic cloaking board, the present invention also provides a scalable and deformable electromagnetic cloaking board, and the electromagnetic cloaking board prepared by the above method is cut into a Miura-Ori origami method with an aspect ratio of 5:7 A rectangular plate, and then crease one side of the electromagnetic cloaking plate according to the Miura-Ori origami method, so that the electromagnetic cloaking plate stretches and deforms along the creases.
进一步的,可将可伸缩变形的电磁隐身板上板面粘固上述超材料单元,且超材料单元在电磁隐身板的上板面呈等间距分布。Further, the above-mentioned metamaterial units can be glued to the upper surface of the expandable and deformable electromagnetic cloaking plate, and the metamaterial units are distributed at equal intervals on the upper surface of the electromagnetic cloaking plate.
有益效果Beneficial effect
(1)通过折纸结构的变形设计,可以改变入射角和电磁波传播路径,实现调频隐身效果。(1) Through the deformation design of the origami structure, the incident angle and the electromagnetic wave propagation path can be changed to achieve the FM stealth effect.
(2)通过织物为基体,制备石墨烯基织物复合材料,石墨烯能够稳定地固定在三维织物骨架中,形成可变形的复合材料。(2) The graphene-based fabric composite material is prepared by using the fabric as the matrix, and the graphene can be stably fixed in the three-dimensional fabric skeleton to form a deformable composite material.
(3)通过超材料与吸波基体匹配,匹配耦合多个四分之一谐振峰获得有效吸收更宽的吸收效率。通过耦合变形的效果,变形前平铺状态,在8-18GHz测试,最小反射损耗值为-10.2dB;将隐身结构按照折叠变形,在8-18GHz测试,最小反射损耗值为-27.1dB,在8~18GHz内反射损耗值低于-10dB(低于-10dB等于对电磁波的吸收>90%,可以近似等于雷达上被识别的物体体积缩小90%,满足隐身条件)的频带为12.3-17.5GHz。(3) By matching the metamaterial and the absorbing matrix, multiple quarter-resonant peaks are matched and coupled to obtain effective absorption and wider absorption efficiency. Through the effect of coupling deformation, the flat state before deformation, the minimum reflection loss value is -10.2dB when tested at 8-18GHz; the stealth structure is deformed according to folding, and the minimum reflection loss value is -27.1dB when tested at 8-18GHz. 8-18GHz internal reflection loss value is lower than -10dB (lower than -10dB equals to the absorption of electromagnetic waves>90%, which can be approximately equal to the reduction of 90% of the volume of the object recognized on the radar, and the frequency band is 12.3-17.5GHz .
附图说明Description of drawings
图1负载石墨烯超材料单元的Miura-Ori折纸结构电磁隐身板的平铺示意图;Figure 1. Schematic diagram of the tiled Miura-Ori origami-structured electromagnetic cloaking plate loaded with graphene metamaterial units;
图2实施例1的反射损耗性能,实线为平铺状态性能,虚线为折叠状态性能;The reflection loss performance of Fig. 2 embodiment 1, the solid line is the flat state performance, and the dotted line is the folded state performance;
图3实施例2的反射损耗性能,实线为平铺状态性能,虚线为折叠状态性能;The reflection loss performance of Fig. 3 embodiment 2, the solid line is the flat state performance, and the dotted line is the folded state performance;
图4实施例3的反射损耗性能,实线为平铺状态性能,虚线为折叠状态性能。Figure 4 shows the reflection loss performance of Example 3, the solid line is the performance in the flat state, and the dotted line is the performance in the folded state.
具体实施方式detailed description
下面结合具体实施例对本发明的内容做进一步说明。The content of the present invention will be further described below in conjunction with specific embodiments.
实施例1Example 1
步骤1:将氧化石墨烯溶于水配置成浓度为7.5mg/ml氧化石墨烯水溶液,将对苯二酚加入氧化石墨烯水溶液中,搅拌均匀;对苯二酚与氧化石墨烯质量比为5;Step 1: Dissolve graphene oxide in water to prepare a graphene oxide aqueous solution with a concentration of 7.5 mg/ml, add hydroquinone to the graphene oxide aqueous solution, and stir evenly; the mass ratio of hydroquinone to graphene oxide is 5 ;
步骤2:将基板浸入上述混合液中,并将其密封;在100℃的条件下保温处理10h,使基板上附着吸波介质;所述基板为聚合物织物或者聚合物泡沫;基板厚度为2mm;Step 2: Immerse the substrate in the above mixed solution, and seal it; heat preservation treatment at 100°C for 10 hours, so that the absorbing medium is attached to the substrate; the substrate is polymer fabric or polymer foam; the thickness of the substrate is 2mm ;
步骤3:将附着有吸波介质的基板从混合液中取出,用水浸泡清洗后,平铺成直板后在-40℃的条件下冷冻10h,再置于常温下干燥48h,得到石墨烯织布;Step 3: Take the substrate with the absorbing medium out of the mixture, soak it in water and wash it, spread it into a straight plate, freeze it at -40°C for 10 hours, and dry it at room temperature for 48 hours to obtain a graphene woven fabric ;
步骤4:将环氧树脂与环氧树脂固化剂按1:3的质量比混合,配制成形成环氧树脂前驱体溶液;将步骤3得到的石墨烯织布浸入环氧树脂前驱体溶液中浸渍4h,取出后铺平,在120℃下加热固化8小时,得到电磁隐身板。Step 4: Mix epoxy resin and epoxy resin curing agent in a mass ratio of 1:3 to form an epoxy resin precursor solution; dip the graphene fabric obtained in step 3 into the epoxy resin precursor solution After 4 hours, take it out and pave it flat, heat and cure it at 120°C for 8 hours to obtain an electromagnetic stealth board.
步骤5:将步骤4得到的电磁隐身板剪切为符合Miura-Ori折纸方法的长宽比为300×375mm的矩形板,再将电磁隐身板的一侧板面按照Miura-Ori折纸方法加工折痕,其中折纸结构中的平行四边形的边长分别为60.45mm与51mm,梯形单元的长边与短边分别为54mm与51mm,高为60mm。使电磁隐身板沿折痕伸缩变形。同时将裁剪矩形板后剩余部分剪切成140块16×16mm正方形薄片;Step 5: Cut the electromagnetic cloaking plate obtained in step 4 into a rectangular plate with an aspect ratio of 300×375mm conforming to the Miura-Ori origami method, and then process and fold one side of the electromagnetic cloaking plate according to the Miura-Ori origami method The side lengths of the parallelogram in the origami structure are 60.45mm and 51mm respectively, the long side and short side of the trapezoidal unit are 54mm and 51mm respectively, and the height is 60mm. The electromagnetic cloaking board is stretched and deformed along the crease. At the same time, cut the remaining part after cutting the rectangular plate into 140 square slices of 16×16mm;
步骤6:将步骤5得到的正方形薄片均粘固在步骤5得到的电磁隐身板上板面,且使各个正方形薄片在电磁隐身板上板面呈等间距分布,得到负载超材料单元的可伸缩变形电磁隐身板。Step 6: Glue the square sheets obtained in step 5 to the surface of the electromagnetic cloaking board obtained in step 5, and distribute the square sheets at equal intervals on the surface of the electromagnetic cloaking board to obtain a scalable load metamaterial unit. Deformable electromagnetic cloaking board.
将实施例得到的负载超材料单元的可伸缩变形电磁隐身板进行吸波性能测试,具体测试条件为:采用自由空间法,通过8-18GHz的信号源向电池隐身板输出电磁波型号,测试电磁隐身板变形前后的反射损耗值(单位dB)。The wave-absorbing performance test is carried out on the stretchable and deformable electromagnetic cloaking board loaded with metamaterial units obtained in the embodiment. The specific test conditions are: adopt the free space method, output the electromagnetic wave model to the battery cloaking board through a signal source of 8-18 GHz, and test the electromagnetic cloaking Reflection loss value (in dB) before and after plate deformation.
测试结果为:变形前平铺状态,测试最小反射损耗值为-10.2dB;按照折叠变形,在8-18GHz测试,最小反射损耗值为-27.1dB,在8~18GHz内反射损耗值低于-10dB的频带为12.3-17.5GHz。The test results are: in the flat state before deformation, the minimum reflection loss value of the test is -10.2dB; according to the folding deformation, the minimum reflection loss value is -27.1dB when tested at 8-18GHz, and the reflection loss value is lower than - The frequency band of 10dB is 12.3-17.5GHz.
实施例2Example 2
步骤1:将氧化石墨烯溶于水配置成浓度为4mg/ml氧化石墨烯水溶液,将对苯二酚加入氧化石墨烯水溶液中,搅拌均匀;对苯二酚与氧化石墨烯质量比为2;Step 1: dissolving graphene oxide in water to prepare a graphene oxide aqueous solution with a concentration of 4 mg/ml, adding hydroquinone to the graphene oxide aqueous solution, and stirring evenly; the mass ratio of hydroquinone to graphene oxide is 2;
步骤2:将基板浸入上述混合液中,并将其密封;在120℃的条件下保温处理8h,使基板上附着吸波介质;所述基板为聚合物织物或者聚合物泡沫;基板厚度为2mm;Step 2: Immerse the substrate in the above mixture, and seal it; heat preservation treatment at 120°C for 8 hours to attach the absorbing medium to the substrate; the substrate is polymer fabric or polymer foam; the thickness of the substrate is 2mm ;
步骤3:将附着有吸波介质的基板从混合液中取出,用水浸泡清洗后,平铺成直板后在-40℃的条件下冷冻12h,再置于常温下干燥36h,得到石墨烯织布;Step 3: Take the substrate with the absorbing medium out of the mixture, soak it in water and wash it, spread it into a straight plate, freeze it at -40°C for 12 hours, and then dry it at room temperature for 36 hours to obtain a graphene woven fabric ;
步骤4:将环氧树脂与环氧树脂固化剂按1:3的质量比混合,配制成形成环氧树脂前驱体溶液;将步骤3得到的石墨烯织布浸入环氧树脂前驱体溶液中浸渍4h,取出后铺平,在100℃下加热固化8小时,得到电磁隐身板。Step 4: Mix epoxy resin and epoxy resin curing agent in a mass ratio of 1:3 to form an epoxy resin precursor solution; dip the graphene fabric obtained in step 3 into the epoxy resin precursor solution After 4 hours, take it out and pave it flat, heat and cure it at 100°C for 8 hours to obtain an electromagnetic stealth board.
步骤5:将步骤4得到的电磁隐身板剪切为符合Miura-Ori折纸方法的长宽比为300×375mm的矩形板,再将电磁隐身板的一侧板面按照Miura-Ori折纸方法加工折痕,其中折纸结构中的平行四边形的边长分别为60.45mm与51mm,梯形单元的长边与短边分别为54mm与51mm,高为60mm。使电磁隐身板沿折痕伸缩变形。同时将裁剪矩形板后剩余部分剪切成140块16×16mm正方形薄片;Step 5: Cut the electromagnetic cloaking plate obtained in step 4 into a rectangular plate with an aspect ratio of 300×375mm conforming to the Miura-Ori origami method, and then process and fold one side of the electromagnetic cloaking plate according to the Miura-Ori origami method The side lengths of the parallelogram in the origami structure are 60.45mm and 51mm respectively, the long side and short side of the trapezoidal unit are 54mm and 51mm respectively, and the height is 60mm. The electromagnetic cloaking board is stretched and deformed along the crease. At the same time, cut the remaining part after cutting the rectangular plate into 140 square slices of 16×16mm;
步骤6:将步骤5得到的正方形薄片均粘固在步骤5得到的电磁隐身板上板面,且使各个正方形薄片在电磁隐身板上板面呈等间距分布,得到负载超材料单元的可伸缩变形电磁隐身板。Step 6: Glue the square sheets obtained in step 5 to the surface of the electromagnetic cloaking board obtained in step 5, and distribute the square sheets at equal intervals on the surface of the electromagnetic cloaking board to obtain a scalable load metamaterial unit. Deformable electromagnetic cloaking board.
将实施例得到的负载超材料单元的可伸缩变形电磁隐身板进行吸波性能测试,具体测试条件为:采用自由空间法,通过8-18GHz的信号源向电池隐身板输出电磁波型号,测试电磁隐身板变形前后的反射损耗值(单位dB)。The wave-absorbing performance test is carried out on the stretchable and deformable electromagnetic cloaking board loaded with metamaterial units obtained in the embodiment. The specific test conditions are: adopt the free space method, output the electromagnetic wave model to the battery cloaking board through a signal source of 8-18 GHz, and test the electromagnetic cloaking Reflection loss value (in dB) before and after plate deformation.
测试结果为:变形前平铺状态,测试最小反射损耗值为-7.8dB;按照折叠变形,在8-18GHz测试,最小反射损耗值为-17.1dB,在8~18GHz内反射损耗值低于-10dB的频带为13.9-17.4GHz。The test results are: in the flat state before deformation, the minimum reflection loss value of the test is -7.8dB; according to the folding deformation, the minimum reflection loss value is -17.1dB when tested at 8-18GHz, and the reflection loss value is lower than - The frequency band of 10dB is 13.9-17.4GHz.
实施例3Example 3
步骤1:将氧化石墨烯溶于水配置成浓度为2mg/ml氧化石墨烯水溶液,将对苯二酚加入氧化石墨烯水溶液中,搅拌均匀;对苯二酚与氧化石墨烯质量比为1;Step 1: Dissolving graphene oxide in water to prepare a graphene oxide aqueous solution with a concentration of 2 mg/ml, adding hydroquinone to the graphene oxide aqueous solution, and stirring evenly; the mass ratio of hydroquinone to graphene oxide is 1;
步骤2:将基板浸入上述混合液中,并将其密封;在100℃的条件下保温处理8h,使基板上附着吸波介质;所述基板为聚合物织物或者聚合物泡沫;基板厚度为2mm;Step 2: Immerse the substrate in the above mixture, and seal it; heat preservation treatment at 100°C for 8 hours, so that the absorbing medium is attached to the substrate; the substrate is polymer fabric or polymer foam; the thickness of the substrate is 2mm ;
步骤3:将附着有吸波介质的基板从混合液中取出,用水浸泡清洗后,平铺成直板后在-40℃的条件下冷冻10h,再置于常温下干燥30h,得到石墨烯织布;Step 3: Take out the substrate attached with the absorbing medium from the mixture, soak it in water and wash it, spread it into a straight plate, freeze it at -40°C for 10 hours, and then dry it at room temperature for 30 hours to obtain a graphene woven fabric ;
步骤4:将环氧树脂与环氧树脂固化剂按1:3的质量比混合,配制成形成环氧树脂前驱体溶液;将步骤3得到的石墨烯织布浸入环氧树脂前驱体溶液中浸渍4h,取出后铺平,在110℃下加热固化5小时,得到电磁隐身板。Step 4: Mix epoxy resin and epoxy resin curing agent in a mass ratio of 1:3 to form an epoxy resin precursor solution; dip the graphene fabric obtained in step 3 into the epoxy resin precursor solution After 4 hours, take it out and pave it flat, heat and cure it at 110°C for 5 hours to obtain an electromagnetic stealth board.
步骤5:将步骤4得到的电磁隐身板剪切为符合Miura-Ori折纸方法的长宽比为300×375mm的矩形板,再将电磁隐身板的一侧板面按照Miura-Ori折纸方法加工折痕,其中折纸结构中的平行四边形的边长分别为60.45mm与51mm,梯形单元的长边与短边分别为54mm与51mm,高为60mm。使电磁隐身板沿折痕伸缩变形。同时将裁剪矩形板后剩余部分剪切成140块16×16mm正方形薄片;Step 5: Cut the electromagnetic cloaking plate obtained in step 4 into a rectangular plate with an aspect ratio of 300×375mm conforming to the Miura-Ori origami method, and then process and fold one side of the electromagnetic cloaking plate according to the Miura-Ori origami method The side lengths of the parallelogram in the origami structure are 60.45mm and 51mm respectively, the long side and short side of the trapezoidal unit are 54mm and 51mm respectively, and the height is 60mm. The electromagnetic cloaking board is stretched and deformed along the crease. At the same time, cut the remaining part after cutting the rectangular plate into 140 square slices of 16×16mm;
步骤6:将步骤5得到的正方形薄片均粘固在步骤5得到的电磁隐身板上板面,且使各个正方形薄片在电磁隐身板上板面呈等间距分布,得到负载超材料单元的可伸缩变形电磁隐身板。Step 6: Glue the square sheets obtained in step 5 to the surface of the electromagnetic cloaking board obtained in step 5, and distribute the square sheets at equal intervals on the surface of the electromagnetic cloaking board to obtain a scalable load metamaterial unit. Deformable electromagnetic cloaking board.
将实施例得到的负载超材料单元的可伸缩变形电磁隐身板进行吸波性能测试,具体测试条件为:采用自由空间法,通过8-18GHz的信号源向电池隐身板输出电磁波型号,测试电磁隐身板变形前后的反射损耗值(单位dB)。The wave-absorbing performance test is carried out on the stretchable and deformable electromagnetic cloaking board loaded with metamaterial units obtained in the embodiment. The specific test conditions are: adopt the free space method, output the electromagnetic wave model to the battery cloaking board through a signal source of 8-18 GHz, and test the electromagnetic cloaking Reflection loss value (in dB) before and after plate deformation.
测试结果为:变形前平铺状态,测试最小反射损耗值为-6.2dB;按照折叠变形,在8-18GHz测试,最小反射损耗值为-13.6dB,在8~18GHz内反射损耗值低于-10dB的频带为14.3-18GHz。The test results are: in the flat state before deformation, the minimum reflection loss value of the test is -6.2dB; according to the folding deformation, the minimum reflection loss value is -13.6dB when tested at 8-18GHz, and the reflection loss value is lower than - The frequency band of 10dB is 14.3-18GHz.
Claims (6)
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201710108086.3A CN106684571A (en) | 2017-02-27 | 2017-02-27 | Miura - Ori origami structure electromagnetic stealthl plate of loaded graphene metamaterial unit |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
CN201710108086.3A CN106684571A (en) | 2017-02-27 | 2017-02-27 | Miura - Ori origami structure electromagnetic stealthl plate of loaded graphene metamaterial unit |
Publications (1)
Publication Number | Publication Date |
---|---|
CN106684571A true CN106684571A (en) | 2017-05-17 |
Family
ID=58862041
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
CN201710108086.3A Pending CN106684571A (en) | 2017-02-27 | 2017-02-27 | Miura - Ori origami structure electromagnetic stealthl plate of loaded graphene metamaterial unit |
Country Status (1)
Country | Link |
---|---|
CN (1) | CN106684571A (en) |
Cited By (10)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN108357161A (en) * | 2017-12-14 | 2018-08-03 | 北京理工大学 | Graphene-based electromagnetism stealth and shielding integrated material and preparation method |
CN108494354A (en) * | 2018-06-07 | 2018-09-04 | 北京汉能光伏投资有限公司 | A kind of slab method for folding, device and device of solar generating |
CN108504038A (en) * | 2018-03-19 | 2018-09-07 | 天津大学 | A kind of absorbing meta-material and preparation method of graphite paper epoxy resin |
CN110772890A (en) * | 2018-07-30 | 2020-02-11 | 天津大学 | Ferroferric oxide-loaded SiC foamed ceramic and preparation method and application thereof |
KR102129791B1 (en) * | 2019-07-19 | 2020-07-03 | 중앙대학교 산학협력단 | Method for producing apparatus of absorbing and/or reflecting using metamaterial |
CN111987452A (en) * | 2020-09-01 | 2020-11-24 | 中国科学院光电技术研究所 | A metamaterial with switchable transmission/reflection and tunable amplitude |
CN112490681A (en) * | 2020-11-24 | 2021-03-12 | 中国人民解放军空军工程大学 | Three-dimensional paper-cut metamaterial adjustable wave absorber and design method thereof |
CN113594707A (en) * | 2021-07-23 | 2021-11-02 | 浙江大学 | Tunable terahertz filter based on folded paper metamaterial |
CN113594649A (en) * | 2021-08-09 | 2021-11-02 | 苏州星航综测科技有限公司 | Electric control micro-disturbance electromagnetic filtering structure, regulation and control method and equipment |
US11700763B2 (en) | 2020-04-10 | 2023-07-11 | The Hong Kong University Of Science And Technology | Curved display and lighting device based on a Miura-Ori structure |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN102161785A (en) * | 2011-03-10 | 2011-08-24 | 四川大学 | Preparation method of graphene/polymer nano composite material |
CN103249290A (en) * | 2013-05-13 | 2013-08-14 | 电子科技大学 | Single-layered composite element wideband periodic wave-absorbing structure |
CN105757438A (en) * | 2014-12-13 | 2016-07-13 | 刘国权 | Panel capable of being quickly folded and unfolded |
-
2017
- 2017-02-27 CN CN201710108086.3A patent/CN106684571A/en active Pending
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN102161785A (en) * | 2011-03-10 | 2011-08-24 | 四川大学 | Preparation method of graphene/polymer nano composite material |
CN103249290A (en) * | 2013-05-13 | 2013-08-14 | 电子科技大学 | Single-layered composite element wideband periodic wave-absorbing structure |
CN105757438A (en) * | 2014-12-13 | 2016-07-13 | 刘国权 | Panel capable of being quickly folded and unfolded |
Cited By (13)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN108357161A (en) * | 2017-12-14 | 2018-08-03 | 北京理工大学 | Graphene-based electromagnetism stealth and shielding integrated material and preparation method |
CN108504038A (en) * | 2018-03-19 | 2018-09-07 | 天津大学 | A kind of absorbing meta-material and preparation method of graphite paper epoxy resin |
CN108494354A (en) * | 2018-06-07 | 2018-09-04 | 北京汉能光伏投资有限公司 | A kind of slab method for folding, device and device of solar generating |
CN108494354B (en) * | 2018-06-07 | 2023-12-12 | 东君新能源有限公司 | Thick plate folding method and device and solar power generation device |
CN110772890B (en) * | 2018-07-30 | 2021-11-19 | 天津大学 | Ferroferric oxide-loaded SiC foamed ceramic and preparation method and application thereof |
CN110772890A (en) * | 2018-07-30 | 2020-02-11 | 天津大学 | Ferroferric oxide-loaded SiC foamed ceramic and preparation method and application thereof |
KR102129791B1 (en) * | 2019-07-19 | 2020-07-03 | 중앙대학교 산학협력단 | Method for producing apparatus of absorbing and/or reflecting using metamaterial |
US11700763B2 (en) | 2020-04-10 | 2023-07-11 | The Hong Kong University Of Science And Technology | Curved display and lighting device based on a Miura-Ori structure |
CN111987452A (en) * | 2020-09-01 | 2020-11-24 | 中国科学院光电技术研究所 | A metamaterial with switchable transmission/reflection and tunable amplitude |
CN112490681A (en) * | 2020-11-24 | 2021-03-12 | 中国人民解放军空军工程大学 | Three-dimensional paper-cut metamaterial adjustable wave absorber and design method thereof |
CN112490681B (en) * | 2020-11-24 | 2022-04-12 | 中国人民解放军空军工程大学 | Three-dimensional kirigami metamaterial tunable absorber and its design method |
CN113594707A (en) * | 2021-07-23 | 2021-11-02 | 浙江大学 | Tunable terahertz filter based on folded paper metamaterial |
CN113594649A (en) * | 2021-08-09 | 2021-11-02 | 苏州星航综测科技有限公司 | Electric control micro-disturbance electromagnetic filtering structure, regulation and control method and equipment |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
CN106684571A (en) | Miura - Ori origami structure electromagnetic stealthl plate of loaded graphene metamaterial unit | |
CN107994353B (en) | Broadband metamaterial terahertz wave absorber | |
CN202259698U (en) | Fractal structure-based multi-tape polarization insensitive terahertz metamaterial absorber | |
Ma et al. | Strong magnetic–dielectric synergistic gradient metamaterials for boosting superior multispectral ultra‐broadband absorption with low‐frequency compatibility | |
CN105647468A (en) | Wave-absorbing material based on grapheme and preparation method thereof | |
CN104099062B (en) | Compounded wave-absorbing material of grapheme/four-pin zinc oxide whisker and preparation method thereof | |
Lai et al. | A high-performance ultra-broadband transparent absorber with a patterned ITO metasurface | |
CN103730739A (en) | Rotating unit type double-frequency circular polarization reflective array antenna | |
Shater et al. | Radar cross section reduction of microstrip antenna using dual-band metamaterial absorber | |
Choudhary et al. | Broadband millimeter-wave absorbers: a review | |
CN108365306A (en) | Novel Bipolar lower passband suction type frequency selecting structures | |
CN109687157A (en) | The super surface of controllable suction wave and polarization conversion function based on electric field triggering | |
CN108610590B (en) | Microwave absorbing material and preparation method thereof | |
Lan et al. | Design of miniaturized wideband microwave absorber loaded with lumped resistance | |
CN107611575A (en) | A kind of end-on-fire antenna based on surface wave guide Yu super surface absorber composite construction | |
Xiong et al. | Compact ultra-wideband microstrip antenna with metamaterials | |
Liu et al. | 3D flower-branch hierarchical carbon nanofiber/ZnO/TiO2/Ti3C2Tx composites for dramatically enhanced electromagnetic absorbing properties | |
CN206180102U (en) | Miniaturized broadband antenna based on fold metal period structure | |
Cong et al. | Polarization-independent wide-angle ultrathin double-layered metamaterial absorber for broadband application | |
CN103922716B (en) | Zinc-doped W type barium ferrite composite wave-absorption material and preparation method thereof | |
Sitara et al. | A multi-band polarization insensitive metasurface based microwave absorber using square and circular loop with lumped elements | |
Yang et al. | Design of a P-band absorber based on metamaterial and magnetic material | |
Ayop et al. | Double layer circular ring metamaterial absorber for dual-directional application at 10 GHz | |
CN108483508B (en) | Porous flaky Fe3O4Electromagnetic wave absorbing agent and preparation method thereof | |
Nie et al. | A tunable absorber based on plasma composite material with dual-channel and broadband properties |
Legal Events
Date | Code | Title | Description |
---|---|---|---|
PB01 | Publication | ||
PB01 | Publication | ||
SE01 | Entry into force of request for substantive examination | ||
SE01 | Entry into force of request for substantive examination | ||
WD01 | Invention patent application deemed withdrawn after publication | ||
WD01 | Invention patent application deemed withdrawn after publication |
Application publication date: 20170517 |