TW575980B - Reflector antenna edge design with feed-horn equi-illumination pattern - Google Patents
Reflector antenna edge design with feed-horn equi-illumination pattern Download PDFInfo
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- TW575980B TW575980B TW91135891A TW91135891A TW575980B TW 575980 B TW575980 B TW 575980B TW 91135891 A TW91135891 A TW 91135891A TW 91135891 A TW91135891 A TW 91135891A TW 575980 B TW575980 B TW 575980B
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Description
575980575980
詳細說明 面種;;馈送器等能量分佈場形設計反射 送器等能種可切除部分反射面面積之饋 t裔寻此量分佈場形設計方法。 計用於高增益雷達微波系統中’其基本設 周圍= ; = :造關係、’天線外觀較為方正。因此天線 部份能量分:=!送器=分佈較低,而反射面邊緣中央 示,天線姆艺回以致旁波辨略咼,經測試電性規格顯 線面積夠:ii 低很難達到理想的配合,雖然天 及射®違不到應有的功能,整體而言饋送器饋送至 efficien 佈效率(aPertUre ⑽以訂 distribution eiriciency) μ φ ^ r .,, 〆、/现出值(spill over value)並不理想。 其外型多與結構有關’其周界邊緣與饋送 ° 等強度分佈有一些差距,以至於反射面完成時 與馈送器場形能量分佈並不吻合,天線性 化之效果。 %』取Ί王 為解決上述之缺失,以下將說明本發明之方法及其特| 了般在天線規格訂定後,即可設計反射面與饋送器之關 係’其中饋送器場形能量分佈可由分析或測試獲得。本發Detailed description of the surface type ;; energy distribution field shape design of the feeder and other reflections; the energy source field design of the feeder can cut off part of the reflection surface area of the feed; Designed to be used in high-gain radar microwave systems, its basic design is around =; =: fabrication relationship, and the antenna appearance is more square. Therefore, the energy of the antenna part is: =! Transmitter = low distribution, and the edge of the reflecting surface is shown in the center. The antenna ’s antenna is designed so that the side wave is discerned. After testing the electrical specifications, the area of the display line is sufficient. Although the Tianhe She ® does not function as it should, overall the feeder feeds to efficien cloth efficiency (aPertUre ⑽ to order distribution eiriciency) μ φ ^ r. ,, 〆, / spill value value) is not ideal. Its appearance is mostly related to the structure. Its peripheral edge is slightly different from the intensity distribution of the feed, so that when the reflection surface is completed, it does not match the field-shaped energy distribution of the feeder, and the effect of antennaization. To solve the above-mentioned shortcomings, take the "King Wang". The method and features of the present invention will be explained below. After the antenna specifications are set, the relationship between the reflective surface and the feeder can be designed. Obtained through analysis or testing. The hair
第4頁 575980Page 4 575980
明反射面天線邊緣用饋送器等能量分佈場形設計 係依照饋送器等能量分佈曲線設計製作反射面外 將不需要部份予以切除,可減少天線體積重量與 時達到反射面能量分佈效率最佳效果。 特點之一 圍邊緣, ,同 在配合需求設計搜索雷達天線時,當天線規格訂定後, Π 反射面與饋送器之關係’饋送器至反射面橫軸涵【 約144度,縱軸涵蓋約35度。計算饋送器之3])場形等能旦 曲線為近似橢圓。一般反射面天線邊緣能量分佈約 至-15db,本發明反射面天線邊緣用饋送器等能量分佈广 形設計另一特點係在反射面與饋送器結構關係固定後,ζ 中心頻率-12db同能量分佈曲線,依照相關位置投射至反牙 射面,其反射面周界即照-12db等能量分佈曲線涵蓋 設計製作。 固 因規格需求所没计反射面為圓柱抛物面,縱面為直面 饋 送器能量經反射面反射後’部份電磁波會被饋送器及輸送 線遮蔽,因此,本發明反射面天線邊緣用饋送器^能量分 佈場形設計另一特點即將饋送器向上傾斜,也丨l=μ二 α钟,例如向上傾斜 10度,反射面向下傾斜,例如5度,(成為〇^36士 reflector),以便將遮蔽效應降低。 本發明反射面天線邊緣用饋送器等能量分佈場形設計另. 特點係應用饋送器約-12 db等能量分佈曲線對應至&反射面The energy distribution field shape design of the antenna on the edge of the clear reflector is designed according to the energy distribution curve of the feeder and so on. The outside of the reflector will not need to be cut away, which can reduce the antenna volume and weight and achieve the best energy distribution efficiency on the reflector. effect. One of the characteristics is to surround the edge. When designing a search radar antenna to meet the needs, when the antenna specifications are set, the relationship between the reflective surface and the feeder 'the horizontal axis of the feeder to the reflective surface [about 144 degrees, the vertical axis covers about 35 degrees. Calculating the feeder 3]) The isoform of the field shape is approximately ellipse. Generally, the energy distribution of the edge of the reflective surface antenna is about -15db. The wide-shaped design of the energy distribution of the reflective surface antenna of the present invention uses a feeder and the like. Another feature is that after the fixed relationship between the reflective surface and the feeder structure, the ζ center frequency is -12db with the same energy distribution. The curve is projected on the anti-ejection surface according to the relevant position, and the perimeter of the reflective surface is according to the energy distribution curve such as -12db, which covers the design and production. Due to the specification requirements, the reflecting surface is a cylindrical paraboloid, and the longitudinal surface is a straight-faced feeder. After the energy is reflected by the reflecting surface, part of the electromagnetic waves will be shielded by the feeder and the transmission line. Therefore, the feeder for the edge of the reflective surface antenna of the present invention ^ Another feature of the energy distribution field shape design is that the feeder is tilted upwards, also l = μ 2 alpha clock, for example, tilted 10 degrees upwards, and the reflection tilted downwards, such as 5 degrees, (become ^ 36 ± reflector) in order to shield The effect is reduced. The energy distribution field design of the reflector for the edge of the reflective surface antenna of the present invention is another. The characteristic is that the energy distribution curve of the feeder is about -12 db and the corresponding to the &
575980 五、發明說明(3) 之範圍,依照此周界設計製作碳纖維反射面外圍,其中饋 送器不等能量分佈(-lldb至Odb)曲線可從反射面座標顯示 出〇 本發明反射面天線邊緣用饋送器等能量分佈場形設計之優 點可利用搜索雷達天線場形用物理光學分析,經過等能量 分佈曲線製作將外圍將切除面積約有28%,其反射面能量 分佈效率約由41%增加至48 ·5%,溢出值約由13 .2%增加 至 14 · 5% 〇 上述本 方法中 距離不多,反 主要電 瓣變化 應用本 將搜索 試值, 外型流 用。 發明反射面 ,其反射面 等而有不同 射面外圍切 性規格,如 甚微小。 發明反射面 雷達反射面 不但符合該 線美觀。目 天線邊緣用饋送器等能量分# 能量分佈因饋送器至反射面不 ,但其能量分佈因距離不等而 除前與切除後其場形理論計# 增益、水平波束寬、垂直波束 天線邊緣用饋送器等能量分# 天線部分切除後,其製作完成 型天線各樣電性之規格需求, 前該雷達反射面天線已通過系 场形設计 同位置因 變化並不 值顯示其 寬、旁波 場形設計 之電性測 且製作之 統驗證使575980 5. The scope of the description of the invention (3). According to this perimeter, the outer surface of the carbon fiber reflective surface is designed and manufactured. The unequal energy distribution (-lldb to Odb) curve of the feeder can be displayed from the reflective surface coordinates. The edge of the reflective surface antenna of the present invention. The advantages of using energy distribution field shape design such as feeder can be used to search the radar antenna field shape using physical optics analysis. After iso energy distribution curve is made, the cut-off area of the periphery will be about 28%, and its reflection surface energy distribution efficiency will increase from about 41%. To 48 · 5%, the overflow value increased from 13.2% to 14 · 5%. 〇 In the above method, there is not much distance. The anti-main flap change application will search for the test value, and the appearance is used. Invented reflective surface, the reflective surface, etc. have different specifications of the external surface cut, such as very small. Invented reflective surface Radar reflective surface not only meets the beauty of the line. The energy distribution of the antennas such as the feeder at the edge of the antenna # The energy distribution varies from the feeder to the reflective surface, but its energy distribution is divided by the difference in distance from the front and the cut after the field shape theory # Gain, horizontal beam width, vertical beam antenna edge After the antenna is partially cut off with the feeder and other energy, all the electrical specifications of the completed antenna are required. The radar reflective surface antenna has been designed in the same field shape, and its width and side are not displayed due to changes in position. Electrical verification of wave field shape design
575980 圖式簡單說明 以下以圖示說明本發明反射面天線邊緣用饋送器等能量分 佈場形設計。 第1 a圖係傳統饋送器計算之H-p lane場形。 第1 b圖係傳統饋送器計算之E-plane場形。 第1 c圖係傳統饋送器計算之3D場形。 第1 d圖係傳統饋送器計算之能量分佈圖。 第2 a圖係饋送器入射反射面垂直向量能量分佈圖。 第2 b圖係饋送器入射反射面水平向量能量分佈圖。 第2 c圖係饋送器入射反射面能量分佈侧視圖。575980 Brief description of the drawings The following illustrates the design of energy distribution fields such as the feeder for the edge of the reflective surface antenna of the present invention. Figure 1a is the H-p lane field shape calculated by the traditional feeder. Figure 1b is the E-plane field shape calculated by the traditional feeder. Figure 1c is the 3D field shape calculated by the traditional feeder. Figure 1d shows the energy distribution calculated by the traditional feeder. Figure 2a is the vertical vector energy distribution diagram of the incident reflecting surface of the feeder. Figure 2b is the horizontal vector energy distribution of the incident reflecting surface of the feeder. Figure 2c is a side view of the energy distribution of the incident reflecting surface of the feeder.
第2 d圖係饋送器入射反射面能量分佈立體圖。 第3 a圖係搜索雷達天線切割前水平場形分析值。 第3 b圖係搜索雷達天線切割後水平場形分析值。 第3 c圖係搜索雷達天線切割前垂直場形分析值。 第3 d圖係搜索雷達天線切割後垂直場形分析值。 第3 e圖係搜索雷達天線切割前之3 D場形。 第3 f圖係搜索雷達天線切割後之3 D場形。 第4 a圖係搜索雷達天線切割後之水平場形測試值。 第4 b圖係搜索雷達天線切割後之垂直場形測試值。Figure 2d is a perspective view of the energy distribution of the incident reflecting surface of the feeder. Figure 3a shows the analysis of the horizontal field shape before the radar antenna is cut. Figure 3b shows the horizontal field shape analysis value after the radar antenna is cut. Figure 3c shows the analysis of the vertical field shape before the radar antenna is cut. Figure 3d shows the analysis of the vertical field shape after the radar antenna is cut. Figure 3e shows the 3D field shape before the radar antenna is cut. Figure 3f shows the 3D field shape of the searched radar antenna. Figure 4a is the horizontal field shape test value after the radar antenna is cut. Figure 4b is the vertical field shape test value after the radar antenna is cut.
第5 a圖係本發明反射面天線邊緣用饋送器等能量分佈場 形設計之反射面雷達天線立體圖。 第5 b圖係本發明反射面天線邊緣用饋送器等能量分佈場 形設計之反射面雷達天線之系統驗證實況。 第1 a 、1 b 、1 c及1 d圖係分別說明一般傳統饋送器Figure 5a is a perspective view of a reflective radar antenna with an energy distribution field design such as a feeder for the edge of a reflective antenna of the present invention. Fig. 5b shows the system verification of a reflective radar antenna with an energy distribution field design such as a feeder for the edge of the reflective antenna of the present invention. Figures 1a, 1b, 1c, and 1d illustrate the conventional conventional feeders, respectively
第7頁 575980 圖式簡單說明 計算之H-plane、E-plane、3D場形及能量周線圖。 第2a、2b圖係分別說明饋送器入射反射面之垂直及 水平向量能量分佈圖。 第2 c及2 d圖係分別說明饋送器入射反射面能量分佈 之侧視及立體圖。 第3 a及3 b圖係分別說明搜索雷達天線切割前及切割 後之水平場形分析值,其切割前後之電性規格變化甚小。 第3 c及3 d圖係分別說明搜索雷達天線切割前及切割後 之垂直場形分析值,其切割前後之電性規格變化甚小。 第3 e及3 f圖係分別說明搜索雷達天線切割前及切割後 之3D場形。 ° 第4 a圖係說明搜索雷達天線切割後之水平場形測試值, 其增益、波束寬及旁波瓣變化甚小。 第4 b圖係說明搜索雷達天線切割後之垂直 其增益、波束寬及旁波瓣變化甚小。 第5 a圖係說明本發明反射面天線邊緣用饋送器等能量八 佈場形設計之反射面雷達天線立體圖。 ° i刀 圖係說明本發明反射面天線邊緣用饋送器等能量 佈易形設計之反射面雷達天線之系統驗證實況。 說明可以瞭解本發明反射面天線邊緣用饋送器等 ί二ΐ場形設計係依照饋送器等能量分佈曲線設計製ΐ 射面外圍邊緣,可將不需要部份予以切除,、= 積重量與風阻,同時達到反射面能量分佈效率最=線Page 7 575980 Schematic description of the calculated H-plane, E-plane, 3D field shape and energy cycle diagram. Figures 2a and 2b illustrate the vertical and horizontal vector energy distribution diagrams of the incident reflecting surface of the feeder, respectively. Figures 2c and 2d are side and perspective views illustrating the energy distribution of the incident reflecting surface of the feeder, respectively. Figures 3a and 3b show the horizontal field shape analysis values of the search radar antenna before and after cutting, respectively. The electrical specifications before and after the cutting have little change. Figures 3c and 3d show the vertical field shape analysis values of the search radar antenna before and after cutting, respectively. The electrical specifications before and after the cutting have very little change. Figures 3e and 3f show the 3D field shape of the search radar antenna before and after cutting, respectively. ° Figure 4a shows the horizontal field shape test value of the search radar antenna after cutting. Its gain, beam width, and side lobe are very small. Figure 4b shows the vertical variation of the search radar antenna after cutting, its gain, beam width and side lobe are very small. Fig. 5a is a perspective view illustrating a reflective surface radar antenna having an eight-field layout design such as a feeder for the edge of the reflective surface antenna of the present invention. ° i The figure shows the system verification of the reflective surface radar antenna designed with energy-distribution such as the feeder for the edge of the reflective surface antenna of the present invention. It can be understood that the field-shaped design of the feeder such as the feeder for the edge of the reflective surface of the present invention is designed according to the energy distribution curve of the feeder and the like. The outer edge of the transmitting surface can be cut away. , While achieving the most efficient energy distribution on the reflecting surface = line
第8頁 575980Page 8 575980
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