Paper Title (use style: paper title) 2018 International Conference on Sensor Network and Computer Engineering (ICSNCE 2018) 69 The Comparison on the Side Feed Mode of Micro-strip Patch Wen Dang Department of Communication and Information Xi'an Technology University Lane 78, Yanta Road, Beilin District, Xian, China e-mail: 13637863650@163.com Xinliang Liu Department of Communication and Information Xi'an Technology University Lane 78, Yanta Road, Beilin District, Xian, China e-mail: 84829562@qq.com Abstract—The feeding of the micro-strip patch is flexible and complex, especially side feeding. In this paper, a single micro- strip patch antenna with a center frequency of 2.45GHZ is taken as an example to explore the performance of the slotted feed and non-slotted feed and verified in HFSS15.0. Combined with HFSS15.0 software simulation and theoretical calculation, the corresponding conclusions can be obtained. The theoretical value and simulation results will be shown that: the required 1/4 converter sizes of the non-slotted side feed and slotted side feed are different. By contrasting with sizes of two feeding modes, electrical size of the slotted feed is smaller. It can be known that all performances of the slotted feed are more superior. Keywords-HFSS Simulation; Micro-strip Patch; Side-feed; Slot; Matching I. INTRODUCTION Antenna is a necessary component for radiating and receiving radio waves in engineering systems such as wireless communications, radio and television, navigation, satellite, radar and other engineering systems. The micro- strip patch is simple and easy to plastic, its feeding modes are flexible and changeable. The stability of the antenna can be also affected by micro-strip patch feeding mode. The different feeding mode has different properties. The design of the feeding system determines the current distribution of the radiation patch. The more consistent the current direction is, the higher the gain is, the greater the energy is, and the better the directivity is [3]. Therefore, in an antenna system, it is especially important that how the feeding system should design, which determines the stability of the system and the quality of microwave devices. In this paper, two different side feed modes of the radiation patch are analyzed and compared. By simulating the cell structure of the micro-strip patch antenna with the center frequency f at 2.45GHZ in HFSS15.0, the corresponding sizes of the 1/4 impedance converter and intrinsic impedance are different, when the feeding position is not the same place, which has been validated in HFSS15.0. The mode following the theoretical sizes calculated by given equations is simulated in HFSS15.0. The simulation results have been drawn the followings. For the non-slotted side feed, the radiation impedance is caused by the edge impedance of the patch. The theoretical calculated 1/4 converter has a large error between the length and width values. To achieve the minimum S11 at the center frequency, it is necessary to optimize the micro-strip line parameters for several times. For the slotted side feed, the radiation impedance is produced by the edge impedance of the patch and the edge impedance of the groove. The theoretical value of the 1/4 converter has a higher accuracy. The best performance of the center frequency can be achieved by adjusting the width and depth of the slotted feeding. Based on the above conditions, the minimum value of the antenna S11 can be obtained, the smaller the reflection energy is, the greater the transmission efficiency is. II. DESIGN AND ANALYSIS OF RADIATION PATCH UNIT In this paper, the radiation patch of the center frequency f = 2.45GHZ would be used as an example, the thickness h of the substrate with Rogers5880 is 1.5mm, its dielectric constant is 2.2. According to the formula (1) – (5) [8] - [9] , it can be obtained that the width w, length L were 40mm and 48.4mm respectively, as well as the input impedance. The width w of radiation patch is the following: 2 1 2 1 2          r f c w   Where c is the speed of free space wave. Taking into account the edge shortening effect, the actual length L of the radiation patch should be expressed as: L f c L e  2 2   Where e  is the effective permittivity, L is the length of the equivalent radiation gap, they can be calculated by using the following formulas respectively. 2 1 e 121 2 1 2 1             w h rr    2018 International Conference on Sensor Network and Computer Engineering (ICSNCE 2018) 70      8.0258.0 264.03.0 412.0 e    hw hw hL e    The input impedance can be obtained as following:    )(cos 2 2 z G zY in    Where G is the radiation conductance, β is the phase constant in the medium, and z is the distance from the feed point to the radiation patch edge. It can be concluded that the different input impedance can be obtained by selecting different feeding point positions. A. Radiation Patch Unit The length and width of the radiation patch can be calculated by formulas (1)-(4). The edge impedance of the radiation patch can be obtained by formula (5). The length and width of the 1/4 impendence converter can be known by the edge impedance. The width and length of the 50Ω intrinsic impedance can be also counted. According to the optimum sizes, the model can be built in hfss15.0 shown in Fig.1. The size of the slotted micro-strip patch can be also calculated by the same method. The optimum sizes can be obtained after many optimizations, it can be built in hfss15.0 shown in Fig.2. Figure 1. Slotted patch antenna After hfss15.0 simulation, the results are obtained in TableⅠ. The simulation results obtained by the two feeding methods are basically the same. The theoretical sizes of the slotted feed is closer to the simulated ones, even almost identical, and its electrical size is smaller. When optimizing in the way of the slotted feed, the workloads can be greatly reduced and the efficiency can be improved. B. Verification In order to verify the rationality of the above conclusions, the input port can be excited by the wave port with a 50 Ω load. when the width of the micro-strip line is w0 and the medium thickness is h, the height of the wave port is generally set to 6 ~ 10h. When there is w0>h, the width of the wave port is set to 10w0. When there is w0