CN102904057A - A new artificial electromagnetic material - Google Patents
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Abstract
Description
【技术领域】 【Technical field】
本发明涉及电磁领域,更具体的说,涉及一种新型人工电磁材料。The invention relates to the electromagnetic field, and more specifically, relates to a novel artificial electromagnetic material.
【背景技术】 【Background technique】
人工电磁材料,俗称超材料,是一种新型人工合成材料,是由非金属材料制成的基板和附着在基板表面上或嵌入在基板内部的多个人造微结构构成的。基板可以虚拟地划分为矩形阵列排布的多个方形基板单元,每个基板单元上附着有一个人造微结构从而形成一个超材料单元,整个超材料即是由数十万、百万甚至上亿的这样的超材料单元组成的,就像晶体是由无数的晶格按照一定的排布构成的。每个超材料单元上的人造微结构相同或者不完全相同。人造微结构是组成一定几何图形的圆柱形或扁平状金属丝,例如组成圆环形、工字型的金属丝等。Artificial electromagnetic material, commonly known as metamaterial, is a new type of artificial synthetic material, which is composed of a substrate made of non-metallic materials and multiple artificial microstructures attached to the surface of the substrate or embedded in the interior of the substrate. The substrate can be virtually divided into multiple square substrate units arranged in a rectangular array. Each substrate unit is attached with an artificial microstructure to form a metamaterial unit. The entire metamaterial is composed of hundreds of thousands, millions or even hundreds of millions of It is composed of such metamaterial units, just like a crystal is composed of countless lattices according to a certain arrangement. The artificial microstructures on each metamaterial unit are identical or not identical. Artificial microstructures are cylindrical or flat metal wires that form a certain geometric figure, such as ring-shaped, I-shaped metal wires, etc.
由于人造微结构的存在,每个超材料单元具有不同于基板本身的等效介电常数和等效磁导率,因此所有的超材料单元构成的超材料对电场和磁场呈现出特殊的响应特性;同时,对人造微结构设计不同的具体结构和形状,可改变其单元的等效介电常数和等效磁导率,进而改变整个超材料的响应特性。Due to the existence of artificial microstructures, each metamaterial unit has an equivalent permittivity and an equivalent magnetic permeability different from the substrate itself, so all metamaterial units composed of metamaterials exhibit special response characteristics to electric and magnetic fields ; At the same time, designing different specific structures and shapes for artificial microstructures can change the equivalent dielectric constant and equivalent magnetic permeability of its units, and then change the response characteristics of the entire metamaterial.
介电常数是以绝缘材料为介质与以真空为介质制成同尺寸电容器的电容量之比值,通常使用希腊字母ε表示,其表示在单位电场中,单位体积内积蓄的静电能量的大小。介电常数表征电介质极化并储存电荷的能力。如果有高介电常数的材料放在电场中,电场的强度会在电介质内有可观的下降。在高介电常数材料中,电磁波波长很短,可以大大缩小射频及微波器件的尺寸。现有的材料绝大多数介电常数的变化范围都很小,且通常为大于零的介电常数。The dielectric constant is the ratio of the capacitance of a capacitor of the same size made of an insulating material as a medium and a vacuum as a medium. It is usually represented by the Greek letter ε, which indicates the amount of electrostatic energy accumulated in a unit volume in a unit electric field. The dielectric constant characterizes the ability of a dielectric to polarize and store charge. If a material with a high dielectric constant is placed in the electric field, the strength of the electric field will drop appreciably within the dielectric. In high dielectric constant materials, the wavelength of electromagnetic waves is very short, which can greatly reduce the size of radio frequency and microwave devices. The variation range of the dielectric constant of most existing materials is very small, and the dielectric constant is usually greater than zero.
现有的人工电磁材料设计生产工艺中通常采用工字型人造微结构去改变空间中的介电常数分布。这种结构产生的介电常数分布通常在关注的频率段内只产生一次协振,因而介电常数变化范围比较小,且通常都是从一个比较大的值开始变化,然而实际应用中通常需要从零开始变化的介电常数。In the existing artificial electromagnetic material design and production process, I-shaped artificial microstructures are usually used to change the dielectric constant distribution in space. The distribution of permittivity produced by this structure usually produces only one resonant resonance in the frequency band of interest, so the range of permittivity change is relatively small, and usually starts to change from a relatively large value. However, practical applications usually require Dielectric constant varying from zero.
【发明内容】 【Content of invention】
本发明实施例的目的在于提供一种新型人工电磁材料,该材料在一定的频段内具有宽频高介电常数且在另一频段内具有由零开始逐渐增大的介电常数分布。本发明实施例是这样实现的,一种新型人工电磁材料,所述材料包括:The purpose of the embodiments of the present invention is to provide a new type of artificial electromagnetic material, which has a wide-band high dielectric constant in a certain frequency band and a dielectric constant distribution that gradually increases from zero in another frequency band. The embodiment of the present invention is achieved in this way, a novel artificial electromagnetic material, said material comprising:
片状基板,附着在所述片状基板上的人造微结构,所述人造微结构有至少一对,每对人造微结构包括附着在所述基板上的第一人造微结构和第二人造微结构。A sheet substrate, an artificial microstructure attached to the sheet substrate, the artificial microstructure has at least one pair, each pair of artificial microstructures includes a first artificial microstructure and a second artificial microstructure attached to the substrate structure.
本发明实施例通过两个不同的人造微结构得到两个谐振峰,使得在所述两个谐振峰之间能够实现ε从零开始平滑渐变,并且由仿真图比较可知,改变人造微结构的尺寸大小可以使得谐振峰在一定频段内前移或后移,进而调节ε从零开始平滑渐变的频段,具体的变化规律为:减小微结构的尺寸,能够使ε所述频段带宽变宽,谐振峰会后移;增加微结构的尺寸,能够使ε所述频段带宽变宽,谐振峰会前移,并且所述人工电磁材料在第一个谐振峰的前面具有宽频高介电常数,可以满足特定场合的需求。The embodiment of the present invention obtains two resonant peaks through two different artificial microstructures, so that ε can be smoothly and gradually changed from zero between the two resonant peaks, and it can be seen from the comparison of the simulation diagrams that changing the size of the artificial microstructure It can make the resonance peak move forward or backward within a certain frequency band, and then adjust the frequency band where ε smoothly and gradually changes from zero. The specific change law is: reducing the size of the microstructure can widen the bandwidth of the frequency band described by ε, and the resonance peak Move back; increasing the size of the microstructure can broaden the bandwidth of the frequency band described by ε, and move the resonance peak forward, and the artificial electromagnetic material has a wide frequency and high dielectric constant in front of the first resonance peak, which can meet the requirements of specific occasions. need.
【附图说明】 【Description of drawings】
图1所示为本发明优选实施例一提供的人工电磁材料的结构图;Fig. 1 shows the structural diagram of the artificial electromagnetic material provided by preferred embodiment one of the present invention;
图2所示为本发明优选实施例二提供的人工电磁材料的结构图;Fig. 2 shows the structural diagram of the artificial electromagnetic material provided by the second preferred embodiment of the present invention;
图3所示为本发明优选实施例一提供的人工电磁材料介电常数的仿真示意图;Fig. 3 shows the simulation schematic diagram of the dielectric constant of the artificial electromagnetic material provided by the preferred embodiment of the present invention;
图4所示为本发明优选实施例二提供的人工电磁材料介电常数的仿真示意图;Fig. 4 shows the simulation schematic diagram of the dielectric constant of the artificial electromagnetic material provided by the
图5所示为本发明实施例提供的第一人造微结构的又一实施例;Figure 5 shows another embodiment of the first artificial microstructure provided by the embodiment of the present invention;
图6所示为本发明实施例一提供的人造微结构对应的数据。FIG. 6 shows data corresponding to the artificial microstructure provided by Embodiment 1 of the present invention.
【具体实施方式】 【Detailed ways】
为了使本发明的目的、技术方案及优点更加清楚明白,以下结合附图及实施例,对本发明进行进一步详细说明。应当理解,此处所描述的具体实施例仅仅用以解释本发明,并不用于限定本发明。In order to make the object, technical solution and advantages of the present invention clearer, the present invention will be further described in detail below in conjunction with the accompanying drawings and embodiments. It should be understood that the specific embodiments described here are only used to explain the present invention, not to limit the present invention.
本发明实施例通过两个不同的人造微结构得到两个谐振峰,使得在所述两个谐振峰之间能够实现ε从零开始平滑渐变,并且由仿真图比较可知,改变人造微结构的尺寸大小可以使得谐振峰在一定频段内前移或后移,进而调节ε从零开始平滑渐变的频段,具体的变化规律为:减小微结构的尺寸,能够使ε所述频段带宽变宽,谐振峰会后移;增加微结构的尺寸,能够使ε所述频段带宽变宽,谐振峰会前移,并且所述电磁材料在第一个谐振峰的前面具有宽频高介电常数,可以满足特定场合的需求。The embodiment of the present invention obtains two resonant peaks through two different artificial microstructures, so that ε can be smoothly and gradually changed from zero between the two resonant peaks, and it can be seen from the comparison of the simulation diagrams that changing the size of the artificial microstructure It can make the resonance peak move forward or backward within a certain frequency band, and then adjust the frequency band where ε smoothly and gradually changes from zero. The specific change law is: reducing the size of the microstructure can widen the bandwidth of the frequency band described by ε, and the resonance peak Move back; increasing the size of the microstructure can widen the bandwidth of the frequency band described by ε, and move the resonance peak forward, and the electromagnetic material has a wide frequency and high dielectric constant in front of the first resonance peak, which can meet the needs of specific occasions .
如图1所示为本发明优选实施例一提供的人工电磁材料的结构图,为了便于说明,仅示出与本发明实施例相关的部分,包括:As shown in Figure 1, it is a structural diagram of the artificial electromagnetic material provided by the preferred embodiment of the present invention. For the convenience of description, only the parts related to the embodiment of the present invention are shown, including:
片状基板1,附着在所述基板1上的人造微结构2。A
在本发明实施例中,基板通常选用环氧树脂、聚四氟乙烯、陶瓷等材料制成,人造微结构为银线或铜线等金属丝线构成的具有一定几何图案的平面结构。每个基板可虚拟地划分为多个长度和宽度分别相等的方体形网格,每个网格的厚度等于基板的厚度,长度和宽度则不大于将要响应的入射电磁波波长的十分之一。每一个方体形网格为一个基板单元,每个基板单元及其表面上附着的人造微结构构成一个材料单元,每个材料片层可以看作是由这些材料单元以一个材料单元的宽度为行间距、长度为列间距进行阵列得到的。In the embodiment of the present invention, the substrate is usually made of materials such as epoxy resin, polytetrafluoroethylene, ceramics, etc., and the artificial microstructure is a planar structure with a certain geometric pattern composed of metal wires such as silver wires or copper wires. Each substrate can be virtually divided into a plurality of cube-shaped grids with equal length and width, the thickness of each grid is equal to the thickness of the substrate, and the length and width are not greater than one-tenth of the wavelength of the incident electromagnetic wave to be responded. Each cube-shaped grid is a substrate unit, and each substrate unit and the artificial microstructure attached to its surface constitute a material unit. Each material sheet can be regarded as a row of these material units with the width of a material unit. The spacing and length are obtained by arraying the column spacing.
每个基板单元附着至少一对人造微结构,包括:第一人造微结构和第二人造微结构,所述第一、第二人造微结构组合成一个新的人造微结构,以使介质基板1表现出不同的介电常数。并且第一、第二人造微结构为尺寸不同的两个ELC结构。并且所述第一人造微结构、第二人造微结构可以互换。Each substrate unit is attached with at least one pair of artificial microstructures, including: a first artificial microstructure and a second artificial microstructure, and the first and second artificial microstructures are combined to form a new artificial microstructure, so that the
如图1所示,第一人造微结构是由两个工字型金属环呈90°相交构成的雪花结构。第二人造微结构与第一人造微结构1相似,除了由两个工字型金属环呈90°相交外,还包括自每个工字型的横边弯折向交点延伸但不接触的金属线。As shown in FIG. 1 , the first artificial microstructure is a snowflake structure formed by two I-shaped metal rings intersecting at 90°. The second artificial microstructure is similar to the first
需要指出的是,所述第二人造微结构工字型横边的弯折包括但不限于:呈一定度数向交点弯折,呈圆弧状向交点弯折;如图5所示所述工字型的横边的端线可以为直线也可以为圆弧;另外所述第一人造微结构和第二人造微结构可以互换。It should be pointed out that the bending of the I-shaped transverse side of the second artificial microstructure includes but is not limited to: bending toward the intersection point at a certain degree, bending toward the intersection point in an arc shape; The end line of the transverse side of the font can be a straight line or an arc; in addition, the first artificial microstructure and the second artificial microstructure can be interchanged.
如图2所示,为本发明的优选实施例二提供的人工电磁材料的结构图,在优选实施例二中第一人造微结构的工字型横边延长了尺寸,即变大了第一人造微结构的横边尺寸。As shown in Figure 2, the structural diagram of the artificial electromagnetic material provided for the preferred embodiment two of the present invention, in the preferred embodiment two, the I-shaped lateral side of the first artificial microstructure has extended the size, that is, the first one has been enlarged. The lateral dimension of the artificial microstructure.
需要指出的是,优选实施例一、二提供的第二人造微结构的尺寸与第一人造微结构的尺寸相同,并且所述第二人造微结构的中心点位于第一人造微结构中心点的水平或垂直延长线上。It should be pointed out that the size of the second artificial microstructure provided by
图3所示为本发明优选实施例一提供的人工电磁材料的介电常数的仿真示意图,各仿真参数如图6所示,其中S2为0.1mm,S3为0.7mm,S4为1mm,第二微结构弯折的角度为45°,S5为2.1mm,S6为0.7mm,S7为0.4mm。由图3可知优选实施例一提供的人工电磁材料在f1为9.4GHZ出现第一个谐振峰,在f2为12.5GHZ出现第二个谐振峰,在两个谐振峰之间的f3为10.4GHZ出现了ε为零的情况,并且在f为10.4~11GHZ频段,介电常数从零开始缓慢变化,带宽为0.6GHZ。Fig. 3 shows the simulation schematic diagram of the dielectric constant of the artificial electromagnetic material that preferred
图4所示为本发明优选实施例二提供的人工电磁材料的介电常数的仿真示意图,其对应的数据与图6相同,仅把S3改为2mm。由图4可知优选实施例二提供的人工电磁材料在f4为9.2GHZ出现第一个谐振峰,在f5为10.5GHZ出现第二个谐振峰,在两个谐振峰之间f6为10GHZ出现了ε为零的情况。Fig. 4 is a simulation schematic diagram of the dielectric constant of the artificial electromagnetic material provided by the
由图3和图4的仿真示意图可知,本发明实施例通过两个不同的人造微结构得到两个谐振峰,使得在所述两个谐振峰之间能够实现ε从零开始平滑渐变,并且由仿真图比较可知,改变人造微结构的尺寸大小可以使得谐振峰在一定频段内前移或后移,进而调节ε从零开始平滑渐变的频段,具体的:减小微结构的尺寸,能够使ε频段带宽变宽,谐振峰会后移;增加微结构的尺寸,能够使ε频段带宽变宽,谐振峰会前移。It can be seen from the simulation schematic diagrams of Fig. 3 and Fig. 4 that the embodiment of the present invention obtains two resonant peaks through two different artificial microstructures, so that ε can be smoothly and gradually changed from zero between the two resonant peaks, and by the simulation It can be seen from the comparison of the figures that changing the size of the artificial microstructure can make the resonance peak move forward or backward within a certain frequency band, and then adjust the frequency band where ε changes smoothly and gradually from zero. Specifically: reducing the size of the microstructure can make the ε frequency band When the bandwidth is widened, the resonance peak moves backward; increasing the size of the microstructure can widen the bandwidth of the ε frequency band, and the resonance peak moves forward.
在上述实施例中,仅对本发明进行了示范性描述,但是本领域技术人员在阅读本专利申请后可以在不脱离本发明的精神和范围的情况下对本发明进行各种修改。In the above embodiments, the present invention is only described as an example, but those skilled in the art can make various modifications to the present invention without departing from the spirit and scope of the present invention after reading this patent application.
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| CN104638351A (en) * | 2013-11-13 | 2015-05-20 | 深圳光启创新技术有限公司 | Antenna baffle board and high-gain antenna |
| CN104638351B (en) * | 2013-11-13 | 2018-09-28 | 深圳光启创新技术有限公司 | Antenna-reflected plate and high-gain aerial |
| CN104916918A (en) * | 2015-04-28 | 2015-09-16 | 电子科技大学 | High-gain horn antenna based on metamaterial loading |
| CN104916918B (en) * | 2015-04-28 | 2018-05-25 | 电子科技大学 | A kind of high-gain horn antenna based on Meta Materials loading |
| CN110112569A (en) * | 2019-05-13 | 2019-08-09 | 佛山市粤海信通讯有限公司 | A kind of manufacturing method of magnetoelectric composites |
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