【正文】
此處,截止頻率可由式()求得如下: () 。 () 當(dāng)藕合線段長(zhǎng)為λ/4( θ=π/2 )時(shí),鏡像阻抗簡(jiǎn)化為 () 這是一個(gè)正實(shí)數(shù),因?yàn)?。在這種情況下,==0,所以四端口阻抗矩陣方程式簡(jiǎn)化為 () ()式中,由式()給出。正如在表中所指明的那樣,各種電路有不同的頻率響應(yīng),包括低通、帶通、全通和全阻。根據(jù)對(duì)稱性,一旦第一行已知,則所有其他矩陣元都能求出。若其他端開路,在端口1或端口2看到的阻抗是 () 在每個(gè)導(dǎo)體上的電壓可以表示為 () 則在端口1和端口2的電壓為 用這個(gè)結(jié)果和式(),可把式()改寫成用i2表示為 () 同樣,由電流源i4驅(qū)動(dòng)線上奇模的電壓是 () 現(xiàn)在在端口1的總電壓是 () 使用公式(),(),()和()中的結(jié)果,且θ=β。通過(guò)疊加,我們看到總端口電流I可以用耦模和奇模電流表示為: = + , () = , () = , () = + . () 首先考慮用i1電流源在耦模下驅(qū)動(dòng)此線。所以。 耦合線段的濾波器特性(a)顯示了平行耦合線段,且?guī)в卸丝陔妷汉碗娏鞯亩x。我們首先研究耽擱四分之一波長(zhǎng)耦合線段的濾波器的特性,然后說(shuō)明如何用這些耦合線段設(shè)計(jì)貸通濾波器[7]。要制作帶寬小于20%的微帶線型多節(jié)帶通或帶阻耦合線濾波器實(shí)際上是容易辦到的。附錄A 外文文獻(xiàn)COUPLED LINE FILTERSThe parallel coupled transmission lines discussed in Section (for directional couplers) can be used to construct many types of filters. Fabrication of multisection bandpass or bandstop coupled line filters is particularly easy in microstrip or stripline form for band widths less than about 20%. Wider bandwidth filters generally require very tightly coupled lines, which are difficult to fabricate. We will first study the filter characteristics of a single quarterwave coupled line section, and then show how these sections can be used to design a bandpass filter [7]. Other filter designs using coupled lines can be found in reference [1]. Filter Properties of a Coupled Line Section A parallel coupled line section is shown in Figure , with port voltage and current definitions. We will derive the opencircuit impedance matrix for this fourport network by considering the superposition of even and oddmode excitations [8], which are shown in Figure . Thus, the current sources and drive the line in the even mode, while and drive the line in the odd mode. By superposition, we see that the total port currents, , can be expressed in terms of the even and oddmode currents as = + , () = , () = , () = + . () First consider the line as being driven in the even mode by the current sources. If the other ports are opencircuited, the impedance seen at port 1 or 2 is () The voltage on either conductor can be expressed as () so the voltage at port 1 or 2 is This result and () can be used to rewrite () in terms of i1 as () (a) (b) (c)FIGURE Definitions pertaining to a coupled line filter section. (a) A parallel coupled line section with port voltage and current definitions. (b) A parallel coupled line section with even and oddmode current sources. (c) A twoport coupled line section having a bandpass response. Similarly, the voltages due to current sources driving the line in the even mode are () Now consider the line as being driven in the odd mode by current . If the other ports are opencircuited, the impedance seen at port 1 or 2 is () The voltage on either conductor can be expressed as () Then the voltage at port 1 or port 2 is This result and () can be used to rewrite () in terms ofas () Similarly, the voltages due to current driving the line in the odd mode are () The total voltage at port 1 is () where the results of (), (), (), and () were used, and θ = β .Next, we solve () for the i j in terms of the I s: =(+), () =(-), () =(+), () =(-), () and use these results in (): () This result yields the top row of the opencircuit impedance matrix [Z ] that describes the coupled line section. From symmetry, all other matrix elements can be found once the rst row is known. The matrix elements are then () () () () A twoport network can be formed from a coupled line section by terminating two of the four ports with either open or short circuits, or by connecting two ends。這是我的大學(xué)最后的一個(gè)學(xué)期,隨著畢業(yè)設(shè)計(jì)工作的完成,我的大學(xué)生涯也馬上將要結(jié)束。在這次畢業(yè)設(shè)計(jì)中也有好多同學(xué)給我很大的幫助。他以其嚴(yán)謹(jǐn)?shù)膶W(xué)術(shù)態(tài)度、和善的待人態(tài)度、獨(dú)到的專業(yè)見解給予我精心的指導(dǎo)和幫助,所以我要衷心感謝我的指導(dǎo)老師賈建科老師,在此向老師表示深深的謝意!我還要感謝我的同學(xué)在四年的大學(xué)學(xué)習(xí)期間,我們共同度過(guò)了美好又充滿歡笑的大學(xué)生活。在本次畢業(yè)設(shè)計(jì)中,賈老師給了我很大的幫助,本篇論文是在賈老師的悉心指導(dǎo)下完成的。參考文獻(xiàn)[1][2]徐興福. ADS2011射頻電路設(shè)計(jì)與仿真實(shí)例[M]. 電子工業(yè)出版社,2014.[3]雷振亞. 射頻/微波電路導(dǎo)論[M]. 西安電子科技大學(xué)出版社,2005.[4]甘本祓,吳萬(wàn)春.現(xiàn)代微波濾波器的結(jié)構(gòu)與設(shè)計(jì)[M].北京科學(xué)出版社,1973.[5]欒秀珍,房少軍.微波工程基礎(chǔ)[M].大連海事大學(xué)出版社,2001:139.165.[6]H.Miyake,S.Kitazawa,T.Ishizaki,T.Yamada,and Y.Nagatom.Aminiaturized monolithic dual band fiiter using ceramic lamination technique for dual mode portable telephones.IEEE MTT—S Int Dig,v01.2,Jun.1997[7]鐘淼,劉成國(guó),黎楊.雙頻微帶帶通濾波器的設(shè)計(jì)與仿真[J].電子元器件應(yīng)用,2009:6264.[8]GL.Matt.had,L.Young,E.M.TJones.Microwave Filters Impedance—Matching Network and coupling Structures.Norwood,MA:Artech House,1980:766—766.[9]J.S.Hong and M.J.Lancaster.Microstrip Filters for RF/Mierowave Applications,John Wiley amp。至此,本次設(shè)計(jì)的過(guò)程基本完成,但因個(gè)人能力和濾波器本身的一些原因,雖然實(shí)現(xiàn)了雙頻帶通濾波器的設(shè)計(jì),但對(duì)于兩個(gè)中心頻率的處理還存在一定的誤差,這是本次設(shè)計(jì)的不足。并用微帶線結(jié)構(gòu)實(shí)現(xiàn)了雙頻濾波器電路,設(shè)計(jì)了一個(gè)工作于在GPS兩個(gè)波段的中心頻率處的雙頻段帶通濾波器。在綜合設(shè)計(jì)理論的基礎(chǔ)上,探究?jī)纱晤l率變換后得到雙頻濾波器的理論。同時(shí)給出了設(shè)計(jì)濾波器的設(shè)計(jì)實(shí)例以及對(duì)一些公式作了推導(dǎo)工作。 本篇論文以研究濾波器為基礎(chǔ),深入展開微波雙頻帶通濾波器的結(jié)構(gòu),從而較深層次地分析微帶線系列濾波器的設(shè)計(jì)、軟件優(yōu)化等方面的內(nèi)容。人們?nèi)找嬖鲩L(zhǎng)的通信需求需要占用更多的通信頻段,雙頻甚至多頻通信系統(tǒng)的設(shè)計(jì)引起了廣泛的關(guān)注。 版圖生成5 總結(jié)與展望 伴隨著微波通信領(lǐng)域技術(shù)的飛速發(fā)展,未來(lái)的濾波器需要從現(xiàn)在通信系統(tǒng)的工作頻率向更短波長(zhǎng),主要是毫米波段轉(zhuǎn)變,以避免在低頻段的擁擠的問題, 微帶線濾波器因其體積小,結(jié)構(gòu)簡(jiǎn)單,加工方便,成本低等優(yōu)點(diǎn)更會(huì)被人們選擇。這時(shí)彈出“Status of Layout Generation