CN103646126A - Design method of micro-strip array focusing antenna and micro-strip array focusing antenna - Google Patents
Design method of micro-strip array focusing antenna and micro-strip array focusing antenna Download PDFInfo
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Abstract
针对现有聚焦天线设计方法中聚焦效果不理想或具有大量旁瓣的缺陷,本发明提出了一种新型的微带阵列聚焦天线的设计方法及设计出的微带阵列聚焦天线,将天线单元的耦合效应已经考虑进去,得到的相位分布刚好可以满足设计聚焦天线所要求的二次球面波分布,同时可以将传输效率做到最大,设计出的聚焦天线几乎没有任何旁瓣且具有最佳幅度相位分布,有效聚焦距离和传输效率均有显著提高。
Aiming at the defects of unsatisfactory focusing effect or a large number of side lobes in the existing focusing antenna design method, the present invention proposes a new design method of microstrip array focusing antenna and the designed microstrip array focusing antenna, the antenna unit The coupling effect has been taken into account, and the obtained phase distribution can just meet the quadratic spherical wave distribution required by the design of the focusing antenna, and at the same time, the transmission efficiency can be maximized. The designed focusing antenna has almost no side lobes and has the best amplitude and phase distribution, effective focusing distance and transmission efficiency have all been significantly improved.
Description
技术领域 technical field
本发明属于平面天线设计技术领域,尤其是涉及一种精确度更高的聚焦天线的新型设计方法及通过该方法设计的微带阵列聚焦天线。 The invention belongs to the technical field of planar antenna design, and in particular relates to a novel design method of a focusing antenna with higher precision and a microstrip array focusing antenna designed by the method. the
背景技术 Background technique
微波作为一种信息传输的手段早已广为人知,并在近年来取得了飞速发展。微波作为功率传输的手段在19世纪首次被提出,并开展了初步的实验研究。微波作为功率传输的手段的优点是实现了功率传输的无线化,这在很多场合都有实用价值。上世纪50年代起人们就已经开始研究电磁能量的输运问题,并将电磁波作为能量的传输手段,这种无线输能方式从上世纪70年代起得到了飞速发展,例如美国加州理工学院的喷气实验室演示了工作于S波段的地面微波输电系统,以及靠微波供电的直升飞机。80年代后期,输能的重点转向了太空活动,工作频率也从S波段转向Ka波段和F波段。微波输能在太空的主要应用是将卫星或太空工作平台收集到的太阳能输给卫星或地面,这是一项耗资巨大的工程,但带来的经济效益也是十分可观的。 Microwaves have long been known as a means of information transmission and have developed rapidly in recent years. Microwave as a means of power transmission was first proposed in the 19th century, and preliminary experimental research was carried out. The advantage of microwave as a means of power transmission is that it realizes wireless power transmission, which has practical value in many occasions. Since the 1950s, people have begun to study the problem of electromagnetic energy transmission, and electromagnetic waves have been used as a means of energy transmission. This wireless energy transmission method has developed rapidly since the 1970s. For example, the California Institute of Technology's jet The laboratory demonstrated the ground microwave power transmission system working in the S-band, and the helicopter powered by microwave. In the late 1980s, the focus of energy transmission shifted to space activities, and the working frequency also shifted from S-band to Ka-band and F-band. The main application of microwave energy transmission in space is to transmit solar energy collected by satellites or space working platforms to satellites or the ground. This is a costly project, but the economic benefits it brings are also very considerable. the
为了保证电磁波能量在空间传输时不扩散,电磁波必须像光一样能聚焦到接收装置,从光的聚焦类比得知,为使电磁波聚焦,发射天线的口径的相位必须是球面分布。上个世纪60年代初期,Goubao,Shermen,Borigiotti等人对口径天线的聚焦问题做了大量的工作,奠定了电磁波输能的理论基础。电磁波聚焦的理论不仅可以用于微波输能,而且可以用于雷达和微波定向能武器。对微波定向能武器来说,其作用是使得目标在感兴趣的部分的电流分布达到最大;对雷达来说,其作用在于提高回波强度。同时可以应用于医学上的微波诱导高温,要将能量最大可能聚焦到癌变组织进行高温加热,而不对其周围的健康组织构成威胁。 In order to ensure that the electromagnetic wave energy does not spread during space transmission, the electromagnetic wave must be able to focus to the receiving device like light. From the analogy of light focusing, we know that in order to focus the electromagnetic wave, the phase of the aperture of the transmitting antenna must be spherically distributed. In the early 1960s, Goubao, Shermen, Borigiotti and others did a lot of work on the focusing of aperture antennas, and established the theoretical basis for electromagnetic wave energy transmission. The theory of electromagnetic wave focusing can be used not only for microwave energy transmission, but also for radar and microwave directed energy weapons. For microwave directed energy weapons, its function is to maximize the current distribution of the target in the interested part; for radar, its function is to increase the echo intensity. At the same time, microwave-induced high temperature, which can be applied in medicine, should focus the energy on cancerous tissue for high-temperature heating without posing a threat to the surrounding healthy tissue. the
传统的聚焦天线是通过在喇叭天线前放一个介电透镜,这类聚焦天线在聚焦平面附近有高的旁瓣,显然这类聚焦天线的结果并不是十分理想,而且这类聚焦天线通常体积都很大,而且设计非常困难,也不容易去实现,同时造价很高,不能满足工程的广泛应用。 The traditional focus antenna is by placing a dielectric lens in front of the horn antenna. This type of focus antenna has high side lobes near the focus plane. Obviously, the result of this type of focus antenna is not very ideal, and this type of focus antenna is usually small in size It is very large, and the design is very difficult, and it is not easy to realize. At the same time, the cost is very high, and it cannot meet the wide application of engineering. the
M.Bogosanovic给出了一种等幅不同相的设计方法,即相位满足二次球面波分布,而幅度保持不变,从实验效果来看,在聚焦位置附近有大量旁瓣,聚焦效果并不是十分理想。 M. Bogosanovic gave a design method with equal amplitude and different phases, that is, the phase satisfies the quadratic spherical wave distribution, while the amplitude remains unchanged. From the experimental results, there are a large number of side lobes near the focusing position, and the focusing effect is not good. Very ideal. the
Shaya Karimkashi给出了一种基于道尔夫———切尔雪夫分布的设计聚焦天线的方法,即不同幅不同相,其中幅度满足切尔雪夫分布,而相位满足二次球面波分布,从实验结果来看,这种设计方法将副瓣降到了-20dB以下,同时所得到的近场分布图也很好,但有一个明显的的不足,就是聚焦点的实际位置同仿真聚焦位置之间的误差比较大,理论上聚焦位置为200mm,而实际聚焦距离只达到了60mm,显然这样的设计方法仍然不够理想。因此,研究一种新型的微带阵列聚焦天线的设计方案非常必要且有相当重要的实际意义。 Shaya Karimkashi gave a method of designing a focusing antenna based on the Dolf-Chershev distribution, that is, different amplitudes and different phases, where the amplitude satisfies the Chershev distribution, and the phase satisfies the quadratic spherical wave distribution. From the experiment As a result, this design method reduces the sidelobe to below -20dB, and the obtained near-field distribution map is also very good, but there is an obvious shortcoming, that is, the difference between the actual position of the focus point and the simulated focus position The error is relatively large. The theoretical focus position is 200mm, but the actual focus distance is only 60mm. Obviously, this design method is still not ideal. Therefore, it is very necessary and of great practical significance to study a new design scheme of microstrip array focusing antenna. the
发明内容 Contents of the invention
针对现有聚焦天线设计方法中聚焦效果不理想并具有大量旁瓣的缺陷,本发明提出了一种新型的微带阵列聚焦天线的设计方法及微带阵列聚焦天线,设计出的聚焦天线几乎没有旁瓣且具有最佳幅度相位分布。 Aiming at the defects of unsatisfactory focusing effect and a large number of side lobes in the existing focusing antenna design method, the present invention proposes a novel microstrip array focusing antenna design method and a microstrip array focusing antenna, and the designed focusing antenna has almost no side lobes with optimal amplitude-phase distribution. the
为了达到上述目的,本发明提供如下技术方案: In order to achieve the above object, the present invention provides the following technical solutions:
一种微带阵列聚焦天线的设计方法,包括如下步骤: A design method for a microstrip array focusing antenna, comprising the steps of:
步骤1.将天线单元构成一个阵列作为发射天线,在预期聚焦位置放置一个同发射天线单元相同尺寸的天线作为接收天线,构造一个无线传输系统;
步骤2.定义所述无线传输系统的散射参数矩阵如下:
其中[at]=[a1,a2,...,an]T,[ar]=[an+1],[bt]=[b1,b2,...,bn]T,[br]=[bn+1],下标‘t’表示发射天线,‘r’表示接收天线,ai(i=1,2…n+1)表示归一化入射波,bi(i=1,2,…n+1)表示归一化反射波,Stt、Srt、Str、Srr表示各对应的S参数; Where [a t ]=[a 1 ,a 2 ,...,a n ] T , [a r ]=[a n+1 ], [b t ]=[b 1 ,b 2 ,..., b n ] T , [b r ]=[b n+1 ], the subscript 't' indicates the transmitting antenna, 'r' indicates the receiving antenna, a i (i=1,2…n+1) indicates the normalization Incident wave, b i (i=1,2,…n+1) represents the normalized reflected wave, S tt , S rt , S tr , S rr represent the corresponding S parameters;
步骤3.定义传输效率Tarray为接收天线的功率和发射天线的输入功率的比值:
步骤4.通过下述公式计算得到各个发射单元的激励幅度跟相位:
[A][at]=Tarray[B][at] [A][a t ]=T array [B][a t ]
其中[at]为发射天线阵各单元端口的激励; in [a t ] is the excitation of each unit port of the transmitting antenna array;
步骤5.通过电磁场仿真软件,得到天线阵列的相关散射参数,根据步骤4中的公式计算得到的各端口激励后进行馈电网络的设计,使得各端口的分配值同计算得到的值相一致。
作为微带阵列聚焦天线的设计方法的一种优选方案,所述阵列包括面阵列结构或线阵列结构。 As a preferred solution of the design method of the microstrip array focusing antenna, the array includes a planar array structure or a line array structure. the
作为微带阵列聚焦天线的设计方法的一种优选方案,所述电磁场仿真软件包括IE3D、HFSS或FEKO电磁仿真软件。 As a preferred solution of the design method of the microstrip array focusing antenna, the electromagnetic field simulation software includes IE3D, HFSS or FEKO electromagnetic simulation software. the
一种微带阵列聚焦天线,由阵列式分布的天线单元和连接天线单元之间的馈电网络构成,所述馈电网络通过下述步骤进行设计: A microstrip array focusing antenna is composed of antenna units distributed in an array and a feeding network connecting the antenna units, and the feeding network is designed through the following steps:
步骤1.在发射天线的预期聚焦位置放置一个同发射天线单元相同尺寸的天线作为接收天线,接收天线与发射天线构成一个无线传输系统;
步骤2.定义所述无线传输系统的散射参数矩阵如下:
其中[at]=[a1,a2,...,an]T,[ar]=[an+1],[bt]=[b1,b2,...,bn]T,[br]=[bn+1],下标‘t’表示发射天线,‘r’表示接收天线,ai(i=1,2…n+1)表示归一化入射波,bi(i=1,2,…n+1)表示归一化反射波,Stt、Srt、Str、Srr表示各对应的S参数; Where [a t ]=[a 1 ,a 2 ,...,a n ] T , [a r ]=[a n+1 ], [b t ]=[b 1 ,b 2 ,..., b n ] T , [b r ]=[b n+1 ], the subscript 't' indicates the transmitting antenna, 'r' indicates the receiving antenna, a i (i=1,2…n+1) indicates the normalization Incident wave, b i (i=1,2,…n+1) represents the normalized reflected wave, S tt , S rt , S tr , S rr represent the corresponding S parameters;
步骤3.定义传输效率Tarray为接收天线的功率和发射天线的输入功率的比值:
步骤4.通过下述公式计算得到各个发射单元的激励幅度跟相位:
[A][at]=Tarray[B][at] [A][a t ]=T array [B][a t ]
其中[at]为发射天线阵各单元端口的激励; in [a t ] is the excitation of each unit port of the transmitting antenna array;
步骤5.通过电磁场仿真软件,得到天线阵列的相关散射参数,根据步骤4中的公式计算得到的各端口激励后进行馈电网络的设计,使得各端口的分配值同计算得到的值相一致。
作为微带阵列聚焦天线的一种优选方案,所述馈电网络的馈电方式包括同轴馈电或边馈方式。 As a preferred solution of the microstrip array focusing antenna, the feeding mode of the feeding network includes a coaxial feeding mode or a side feeding mode. the
作为微带阵列聚焦天线的一种优选方案,所述阵列包括面阵列结构或线阵列结构。 As a preferred solution of the microstrip array focusing antenna, the array includes a planar array structure or a line array structure. the
与现有技术相比,本发明提供的新的聚焦天线的设计方法及根据该方法设计而成的聚焦天线,将天线单元的耦合效应已经考虑进去,得到的相位分布刚好可以满足设计聚焦天线所要求的二次球面波分布,同时可以将传输效率做到最大,有效聚焦距离和传输效率均有显著提高,几乎没有旁瓣。 Compared with the prior art, the new focusing antenna design method provided by the present invention and the focusing antenna designed according to the method have taken the coupling effect of the antenna unit into consideration, and the obtained phase distribution can just meet the requirements of designing the focusing antenna. The required quadratic spherical wave distribution can maximize the transmission efficiency at the same time, the effective focusing distance and transmission efficiency are significantly improved, and there are almost no side lobes. the
附图说明 Description of drawings
图1为发射天线阵列和接收天线形成的无线传输系统结构示意图; Figure 1 is a schematic structural diagram of a wireless transmission system formed by a transmitting antenna array and a receiving antenna;
图2为无线传输系统信号传输示意图; Fig. 2 is a schematic diagram of wireless transmission system signal transmission;
图3为单个天线单元示意图; Fig. 3 is a schematic diagram of a single antenna unit;
图4为馈电网络示意图,其中数字1,2,…,17表示各端口;
Figure 4 is a schematic diagram of the feed network, where
图5为发射天线示意图; Fig. 5 is a schematic diagram of transmitting antenna;
图6为天线阵列沿着Z方向的电场归一化图; Fig. 6 is the electric field normalization figure of antenna array along Z direction;
图7为天线在聚焦平面沿着X轴方向的电场分布图; Fig. 7 is the electric field distribution diagram along the X-axis direction of the antenna at the focal plane;
图8为天线在聚焦平面沿Y轴方向的电场分布图; Fig. 8 is the electric field distribution diagram of the antenna along the Y-axis direction in the focal plane;
图9是在最大电场强度密度所在平面的电场强度分布图。 Fig. 9 is a distribution diagram of the electric field intensity on the plane where the maximum electric field intensity density is located. the
具体实施方式 Detailed ways
以下将结合具体实施例对本发明提供的技术方案进行详细说明,应理解下述具体实施方式仅用于说明本发明而不用于限制本发明的范围。 The technical solutions provided by the present invention will be described in detail below in conjunction with specific examples. It should be understood that the following specific embodiments are only used to illustrate the present invention and are not intended to limit the scope of the present invention. the
聚焦天线设计面临的一个重要问题就是得到合适的近场辐射图,使之有较低的旁瓣,因为较高的旁瓣会影响聚焦的准确性以及传输效率,因此,合理的幅度相位分布是解决这一问题的关键。 An important problem in focusing antenna design is to obtain a suitable near-field radiation pattern so that it has lower side lobes, because higher side lobes will affect the accuracy of focusing and transmission efficiency. Therefore, a reasonable amplitude and phase distribution is key to solving this problem. the
具体地说,本发明采用新的聚焦天线的设计方法,包括如下步骤: Specifically, the present invention adopts the design method of new focusing antenna, comprises the following steps:
步骤1.基于无线功率传输系统,为了实现传输效率最大化,发射天线的发射能量聚焦在接收天线的位置,首先将天线单元构成一个阵列作为发射天线,在预期聚焦位置(与发射天线距离为D)放置一个同发射天线单元相同尺寸的天线作为接收天线,构造一个无线传输系统。发射天线中天线单元为阵列式分布,这里的阵列结构可以采用各类型的阵列天线结构,例如面阵列式、线阵列式结构、共形阵列结构等等。此时系统可以看成如图2所示的n+1端口网络,可以用(n+1)×(n+1)散射参数矩阵来表示。
例如我们以设计频率为2.45GHZ,基板材料为FR4,厚度为3mm,16个天线单元为例,16个天线单元为4*4的面阵列结构,单元之间的间距为60mm,预期聚焦距离为100mm,天线阵列和接收天线如图1所示放置,本发明采用如图3所示的微带贴片天线作为天线单元,但微带贴片天线不应作为本发明的限制,必须指出的是,业内常用的天线单元都可以满足本发明需求。整个系统可以看成16+1的端口网络,散射参数矩阵表示为: For example, we take the design frequency as 2.45GHZ, the substrate material as FR4, the thickness as 3mm, and 16 antenna elements as an example. The 16 antenna elements are a 4*4 area array structure, the distance between the elements is 60mm, and the expected focusing distance is 100mm, the antenna array and the receiving antenna are placed as shown in Figure 1, the present invention uses the microstrip patch antenna as shown in Figure 3 as the antenna unit, but the microstrip patch antenna should not be used as a limitation of the present invention, it must be pointed out that , antenna units commonly used in the industry can meet the requirements of the present invention. The whole system can be regarded as a 16+1 port network, and the scattering parameter matrix is expressed as:
其中[at]=[a1,a2,...,an]T,[ar]=[an+1],[bt]=[b1,b2,...,bn]T,[br]=[bn+1],下标‘t’表示发射天线,‘r’表示接收天线,ai(i=1,2…n+1)表示归一化入射波,bi(i=1,2,…n+1)表示归一化反射波,Stt、Srt、Str、Srr表示各对应的S参数; Where [a t ]=[a 1 ,a 2 ,...,a n ] T , [a r ]=[a n+1 ], [b t ]=[b 1 ,b 2 ,..., b n ] T , [b r ]=[b n+1 ], the subscript 't' indicates the transmitting antenna, 'r' indicates the receiving antenna, a i (i=1,2…n+1) indicates the normalization Incident wave, b i (i=1,2,…n+1) represents the normalized reflected wave, S tt , S rt , S tr , S rr represent the corresponding S parameters;
步骤2.定义传输效率Tarray为接收天线的功率和发射天线的输入功率的比值:
步骤3.通过下述公式计算得到各个发射单元的激励幅度跟相位:
[A][at]=Tarray[B][at] [A][a t ]=T array [B][a t ]
其中[at]为发射天线阵各单元端口的激励; in [a t ] is the excitation of each unit port of the transmitting antenna array;
步骤4.通过电磁场仿真软件(电磁场仿真软件可采用IE3D或HFSS、FEKO等常用电磁仿真软件),得到天线阵列的相关散射参数,进而根据系统间的传输效率得到最大效率值时所对应的端口最佳分布值,以本发明中的具体天线为例,通过运算得到的端口激励如表1所示:
表1 Table 1
步骤5.根据得到的端口值(发射单元的激励幅度跟相位),根据传输线的现有知识,充分利用阻抗变换器、功分器等相关知识,以宽度可以改变幅度,长度可以改变相位为基本原则,设计如图4、图5、图6所示的对应的馈电网络,使得各端口的分配值同之前计算得到的值相一致。其中各个与天线连接的端口(图4中的2,3,…,17,)用50欧姆输入阻抗替代,图4中1处为馈电处,本例中,馈电采用同轴馈电,根据需要,也可以采用其他馈电方式,如边馈方式。
馈电网络设计好以后,将馈电网络中所用的50欧姆输入阻抗替换成天线单元,从而将天线单元跟馈电网络组成一个整体。 After the feed network is designed, replace the 50-ohm input impedance used in the feed network with the antenna unit, so that the antenna unit and the feed network form a whole. the
我们通过电磁仿真软件和暗室近场测试得到本发明设计的天线阵列的电场归一化图(图6),天线在聚焦平面沿着X轴方向的电场分布图(图7)、天线在聚焦平面沿Y轴方向的电场分布图(图8)、最大电场强度密度所在平面的电场强度分布图(图9)。从图6中可以看出测试结果和仿真结果比较吻合,图7中看出主瓣到-35dB都没有出现旁瓣,图8中主瓣到-25dB 都没有出现旁瓣。从图9中可以看出采用本发明提供的设计方法设计的聚焦天线实际聚焦距离可以达到80mm,有效聚焦距离相较现有技术得到了显著提高,同时没有任何旁瓣,传输效率可以达到30%。 Through electromagnetic simulation software and darkroom near-field tests, we obtained the electric field normalization diagram of the antenna array designed by the present invention (Figure 6), the electric field distribution diagram of the antenna along the X-axis direction in the focal plane (Figure 7), and the antenna in the focal plane The electric field distribution diagram along the Y-axis direction (Figure 8), and the electric field intensity distribution diagram of the plane where the maximum electric field intensity density is located (Figure 9). It can be seen from Figure 6 that the test results are in good agreement with the simulation results. Figure 7 shows that there are no side lobes from the main lobe to -35dB, and no side lobes from the main lobe to -25dB in Figure 8. It can be seen from Fig. 9 that the actual focusing distance of the focusing antenna designed by the design method provided by the present invention can reach 80mm, and the effective focusing distance has been significantly improved compared with the prior art. At the same time, there is no side lobe, and the transmission efficiency can reach 30%. . the
本发明同样还公开了一种微带阵列聚焦天线,包括发射天线阵列,所述发射天线阵列由阵列式分布的发射单元构成,所述发射单元之间通过馈电网络连接,所述馈电网络及通过本发明提供的微带阵列聚焦天线的设计方法进行设计。 The present invention also discloses a microstrip array focusing antenna, which includes a transmitting antenna array, the transmitting antenna array is composed of transmitting units distributed in an array, and the transmitting units are connected through a feeding network, and the feeding network And design through the design method of the microstrip array focusing antenna provided by the present invention. the
本发明方案所公开的技术手段不仅限于上述实施方式所公开的技术手段,还包括由以上技术特征任意组合所组成的技术方案。应当指出,对于本技术领域的普通技术人员来说,在不脱离本发明原理的前提下,还可以做出若干改进和润饰,这些改进和润饰也视为本发明的保护范围。 The technical means disclosed in the solutions of the present invention are not limited to the technical means disclosed in the above embodiments, but also include technical solutions composed of any combination of the above technical features. It should be pointed out that for those skilled in the art, some improvements and modifications can be made without departing from the principle of the present invention, and these improvements and modifications are also regarded as the protection scope of the present invention. the
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Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN104485521A (en) * | 2014-12-19 | 2015-04-01 | 南京信息工程大学 | Planar array focusing antenna for microwave thermotherapy |
CN106992802A (en) * | 2017-06-02 | 2017-07-28 | 上海传英信息技术有限公司 | Signal receiving/transmission device, user terminal and method for transmitting signals for user terminal |
CN109586770A (en) * | 2018-11-20 | 2019-04-05 | 上海龙旗科技股份有限公司 | 5G mobile phone terminal antenna adjusting method and equipment |
CN109755762A (en) * | 2019-03-14 | 2019-05-14 | 南京信息工程大学 | A near-field adaptive focusing antenna and focusing method applied to RFID |
Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN102668408A (en) * | 2009-12-21 | 2012-09-12 | 高通股份有限公司 | Dynamic antenna selection in a wireless device |
CN103000977A (en) * | 2012-11-16 | 2013-03-27 | 北京航空航天大学 | Broadband novel microstrip line three-way power divider |
CN103200894A (en) * | 2010-09-06 | 2013-07-10 | It`Is基金会 | Electromagnetic field applicator array with integral field sensors for implicit correction of mutual coupling and mismatch |
-
2013
- 2013-11-01 CN CN201310535355.6A patent/CN103646126A/en active Pending
Patent Citations (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN102668408A (en) * | 2009-12-21 | 2012-09-12 | 高通股份有限公司 | Dynamic antenna selection in a wireless device |
CN103200894A (en) * | 2010-09-06 | 2013-07-10 | It`Is基金会 | Electromagnetic field applicator array with integral field sensors for implicit correction of mutual coupling and mismatch |
CN103000977A (en) * | 2012-11-16 | 2013-03-27 | 北京航空航天大学 | Broadband novel microstrip line three-way power divider |
Non-Patent Citations (2)
Title |
---|
FANGYI XIE等: "Optimal Design of an Antenna Array for Energy Harvesting", 《IEEE ANTENNAS AND WIRELESS PROPAGATION LETTERS》 * |
文舸一: "无线功率传输系统的优化设计", 《2013年全国微波毫米波会议论文集》 * |
Cited By (7)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
CN104485521A (en) * | 2014-12-19 | 2015-04-01 | 南京信息工程大学 | Planar array focusing antenna for microwave thermotherapy |
CN104485521B (en) * | 2014-12-19 | 2017-05-03 | 南京信息工程大学 | Planar array focusing antenna for microwave thermotherapy |
CN106992802A (en) * | 2017-06-02 | 2017-07-28 | 上海传英信息技术有限公司 | Signal receiving/transmission device, user terminal and method for transmitting signals for user terminal |
CN106992802B (en) * | 2017-06-02 | 2023-08-08 | 上海传英信息技术有限公司 | Signal receiving and transmitting device for user terminal, user terminal and signal transmission method |
CN109586770A (en) * | 2018-11-20 | 2019-04-05 | 上海龙旗科技股份有限公司 | 5G mobile phone terminal antenna adjusting method and equipment |
CN109755762A (en) * | 2019-03-14 | 2019-05-14 | 南京信息工程大学 | A near-field adaptive focusing antenna and focusing method applied to RFID |
CN109755762B (en) * | 2019-03-14 | 2023-12-01 | 南京信息工程大学 | A focusing method for near-field adaptive focusing antenna applied to RFID |
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