Novel Elliptic-function Low-pass Filter (LPF)

Novel Elliptic- authority Low- avenue filtrate (LPF) accomplishment of microstrip blue pass filter with stub loaded Electromagnetic Band Gap estate planeMariselvam V, Raju SAbstractA novel elliptic-function small(a)-pass filter (LPF) is Presented, which consists of a Electromagnetic band gap on the underseal plane. The Electromagnetic band gap provides the required wideband attenuation in stop band, while the slot provides steep transformation from pass band to stop band. A 5.4 GHz flipper- gat LPF is developed and experimental results parade that it has a sharp cutoff frequency response. The measured pass band insertion- loss is be base 0.4 dB, and the rejection band everywhere 15 dB is from 5.425 GHz to 8.25 GHz, Which increases from 2.95 GHz. KeywordsDefected ground structure (DGS), elliptic-function filter, low-pass filter (LPF).1. INTRODUCTIONRecently, defected ground structure (DGS) has experience one of the just about interesting argonas of research in microwave an d millimeter wave Applications 1. It could be wide used in microwave lap covering figure of speech such as power divider, power amplifier and oddly in filter contrive 19. Low pass filters (LPF) design require that both in-band and out-band performances should be low loss, high selectivity, high rejection, and wide spurious free frequency ranges. Many novel types of microstrip filters nourish been put upd and designed. nightly or non-periodic DGS be accomplished by etching a slot in the backside bimetallic ground plane. The etched slot disturbs effectively the current distri aloneion in the ground plane of microstrip contestation and the results in resonant singularitys 2, 3.IT is well known that typical properties of low-pass filters (LPFs) can be obtained by adding periodic structures to transmitting lines. The representative periodic structures for planar transmittance lines and/or microwave circuits ar photonic band gap (PBG) and defected ground structure (DGS) 4, 5. The PBG has been known as a popular periodic structure for planar transmission lines. However, drawbacks of PBGs have been withal discussed as follows.1) A large area is needed because a number of periodic patterns should be adoptive.2) It is obscure to define the unit fragment, and difficult to extract the kindred-circuit elements for the PBG unit element.3) Therefore, it is very restricted to extend its practical(a) applications programme to microwave circuits. To the contrary, one can easily define the unit element of the DGS and model the equivalent circuit.In addition, since only a few DGS elements show the typical properties of periodic structures, the resultant circuit coat becomes relatively small. Furthermore, the structure of the DGS is simple and it is easy to design the DGS pattern. For these reasons, since 4 has introduced the structure and called it a DGS for the first time, the DGS has been extensively use to design microwave circuits such as filters, power dividers, couplers, amplifiers, oscillators, and so on 1, 612.There is much forward research about the characteristics of LPFs having periodic structures on microstrip or Coplanar waveguide (CPW) transmission lines 1316However most of them are non analytical because they mainly depend on electromagnetic (EM) computer simulations to design LPFs and predict circuit performances. To the contrary, in the design of LPFs apply DGSs including this study, all design steps are based on theories and fair(a) explanations as follows.The equivalent-circuit elements of the DGS is extracted and used for replacing the serial publication inductances in the LPF Prototype circuit.The LPF is imperturbable of the extracted equivalent lumped Elements, thus, it is an ideal LPF, is designed, and is compared to the realized LPF using the DGS practically. devil methods to design a three- end LPF using the DGS has been proposed in 1 and 6. In these papers, the sizes of two DGS patterns in the LPF were merely the same because two inductances in the three-pole L1 (series) C2 (shunt) L3 (series) ideal LPF are identical. In 6, discontinuity elements such as tee- or cross- joins were adopted to connect open stubs to realize the shunt capacitance. However, in the three-pole LPF proposed in 1, there are no junction elements, thin transmission lines for high impedance, or open stubs. In addition, the width of the transmission-line elements in the LPF has been remarkably broadened. Thus, advantages such as compact design and error-robust realization fabricating the layout have been obtained. However, in night club to design -stage LPFs using the DGS, e.g., a five-stage like L1 (series) C2 (shunt) L3 (series) C4 (shunt) L5 (series), two assorted dimensions of the DGS have to be adopted because L3 is non equal to L1=L5, although. In order to select the proper dimension of the DGS for L3 careful consideration based on filter theories, extracted equivalent- circuit elements of unl ike DGS dimensions, and some related topics of transmission lines should be taken. The size of the DGS for L3 is determined by accurate curve-fitting results for equivalent-circuit elements to correspond on the dot to the required inductance. In addition, the length of transmission-line elements between DGS patterns is determined through the consideration for the equivalent capacitance and additive parasitic inductance, as well as the required shunt capacitances in the icon LPF. Therefore, a design of a five-pole DGS-LPF requires many more complex steps than the previous three-pole DGS-LPF shown in 1 and 6. Thus, the goal of this paper is to propose a fresh technique to design an -pole LPF having (DGS-LPF), and to generalize the previous design method for N5 using different sizes of DGS patterns. For this purpose, modeling for the equivalent circuit of the DGS, a curve fitting for determining the required different sizes of theFig.1 put across view of the Microstrip line with a DGS pattern and its dimensions in mmFig.1a. Bottom view of the Microstrip line with a DGS pattern and its dimensions in mmDGS that reflects the inductance determine in the prototype LPF and a practical design example will be successively discussed.In order to show the validity of the proposed method, a five pole DGS-LPF, as an example, is designed and measured in this paper. The five-pole DGS-LPF has a much wider microstrip line than conventional microstrip LPFs, and does non include high-impedance lines, which have been essentially required in conventional design. The series inductances in the prototype LPF are realized by DGSs, while the shunt capacitances are realized by the widely compensated transmission line. Therefore, no discontinuity elements such as tee- or cross-junction for connecting open stubs are required because there are no stubs in the DGS-LPF.2. DGS PATTERN AND MODELING FOR THE EQUIVALENT CIRCUITFig. 1and 1a shows a microstrip line having a dumb-bell DGS and its -parameters from an EM simulation. Two rounded defected areas and one connecting slot correspond to the equivalently added inductance (L) and capacitance(C), respectively. Accordingly, a resonance occurs at a trusted frequency because of the parallel LC circuit. Inversely, it is intuitively known that the equivalent circuit includes a copulate of parallel inductor capacitor from the resonant phenomenon in the -parameter. This means the microstrip line having the DGS does not have all-pass characteristics, but restricted pass band properties.Fig.2. Equivalent circuit of the microstrip line with unit DGS using ADSIn addition, slow-wave characteristics are observed due to the added components of the DGS 3, 5, 9. The defected areas can be realized by not only ellipse, but also other geometries such as triangle, circle, hexagon, octagon, spiral, and so on. It is very clear that the resonant frequency (wo) of the DGS and 3-dB cutoff frequency (wc 3dB) exist as shown in Fig. 1.The equi valent circuit of the DGS can be extracted because this kind of electrical characteristic is observed from a typical L C parallel resonant circuit.The equivalent circuit of the DGS and one-pole Butterworth prototype of the LPF are presented the DGS in Fig. 2. The equivalent L C elements are calculated by (13) because two reactance values of Fig. 2(a) must be equal at wc 3dB as followsXLc= (1)XL = Zo g1 (2)XLc = c, (3)Where w(=1), g1 (=2) and Zo (=50) are the normalized 3-dB cutoff frequency, element value of one-pole Butterworth prototype LPF, and port impedance, respectively, and wo = (1/ Lk1Ck1). The calculated L2and c2 of the DGS shown in Fig. 2 are 3.2 nH and 0.8194 pF, respectively. Fig. 3 shows an excellent stipulation between the previous -parameters shown in Fig. 1 and the new ones calculated using Lk1and ck1. Advanced Design system (ADS), a circuit simulator from Agilent Technologies, has been used for the calculation. This agreement means that the modeling technique i s valid in extracting the equivalent-circuit elements. It should be noted that this is one of the great advantages of DGS because it is possible to define the unit element of the DGS and to establish the equivalent circuit of it, while the conventional Planar transmission lines with a periodic structure such as a PBG have difficulty in defining the unit element and to extract the modeled circuit element.2.1 introduction OF THE FIVE POLE LOWPASS FILTERA. Prototype LPF and Adoption of DGSThe method to design a five-pole LPF using the DGS is discussed here. Fig. 3 depicts the prototype circuit of a five-pole LPF. Here gi (i=0, 1, 2, 3, 4, 5, 6), represent the normalized element values of a Chebyshev prototype LPF for the given ripple 17. According to the design theory of filters, in order to transform the prototype LPF to the LPF composed of lumped elements, the values of L1,C2,L3,C4 and L5can be determined owing to the impedance andFig.3. Five-pole Chebyshev prototype LPF with Ellipt ic DGSFig.3a. Equality of a series inductor to an LC parallel circuitfrequency scaling rules expressed in (4)(6). Here, c means the crosscut frequency of the LPFL1 = = = L4 (4)L3 = (5)C2 = = C4 (6)Fig.4. Performance of the designed five pole LPF using ADSFig.5. Performance of the designed five pole LPF using CST2.2 PERFORMANCE OF THE DESIGNED DGS-LPFFIG. 6 shows the measured S-parameters of the designed DGS-LPF, as compared with the theoretical performance (circuit simulation) and the EM simulation by CST-MWS. As shown, the measurement result agrees with the EM simulation very well. The designed elliptical function DGS-LPF exhibits a much shaper transition knee than the Chebyshev one report in 5. Its transition bandwidth from 1 to 20 dB attenuation is only 0.45 GHz. The measured pass band insertion loss is less than 0.3 dB. The stop bandwidth corresponding to 15dB rejection is from 2.95 to 8.25 GHz. The total length of the designed DGS-LPF is 17 mm, and compared with the LPF repo rted in 5, it is cut back about 40.88% and compared with the LPF reported in 6 it is reduced about 14.66%.Fig.6. Measured result of the designed five pole LPF using Agilent Network analyzer N5230A3. PERFORMANCE OF THE PROPOSED DGS LOWPASS FILTERFig.7. Top view of the Microstrip line and its dimensions in mmFig.7a. Bottom view of the Microstrip line and its dimensions in mmThe proposed five-pole DGS-LPF has a much wider microstrip line than conventional microstrip LPFs, and does not include high-impedance lines, which have been essentially required in conventional design. The series inductances in the prototype LPF are realized by DGSs, while the shunt capacitances are realized by the widely compensated transmission line. A stub like elements which gives a inductance effect is introduced in the proposed DGS-LPF.DGS combined with microstrip line causes a resonant character of the structure transmission with a resonant frequency controllable by ever-changing the shape and size of the slot. There is a huge evolution in terms of defected shapes dumbbell, periodic, fractal, circular, spiral, and L molded 1214. In this paper, a novel elliptic shape DGS is proposed for the LPF design. The use of elliptic shape DGS will be shown to give sharp cut off frequency response as well as a good performance in the pass band. The analysis of the dimension parameters with different dimension parameters was demonstrated as a design guide. The equivalent circuit (EC) has been extracted to characterize the proposed low-pass filter. The equivalent circuit model agrees with the field simulation results. The theoretical and measured results are presented with good agreement for LPF. The total length of the designed DGS-LPF is 15 mm, and compared with the LPF reported in 5, it is reduced about 60% and compared with the LPF reported in 6 it is reduced about 29%, the pass band increases up to 5.425 GHz from 2.95 GHz and the stop bandwidth corresponding to 15dB rejection is from 5.425 GHz which is suitable for WLAN applicationFig.8. Comparison Performance of the designed five pole LPFFig.9. Equivalent circuit of the microstrip line with unit DGS using ADSFig.10. Measured result of the proposed five pole LPF using Agilent Network analyzer N5230ATab 1 Performance of the five pole LPF using CSTTab 2 Dimensions of the proposed DGS designsTab3. Prototype elements of the five pole elliptic function LPFFig.11. Top view of the prototypeFig.11a. Bottom view of the prototype4. CONCLUSIONThis letter has presented a new LPF to obtain elliptic-function response using Dumbbell shaped DGS. The designed LPF exhibits sharp cutoff frequency response, low insertion loss, and excellent stop band performance. The proposed design procedure can be extended to commanding -stage LPF. In addition, its physical structure is only composed of defect and microstrip line, so it is easy to fabricate. Since this design is simple, analytical, and does not require any optimization process, this kind of equivalent circuit model of DGS and its design engineering science may be further applied to various microwave circuits such as low-noise amplifiers, diplexers, mixers, and so on.ReferencesSERGIO PALMA PACHECO, JIANEI WANG, JONG- GWAN YOOK, AND LINDA P. B. KATEHI, Micromachined strains on Synthesized Substrates Rhonda Franklin Drayton, IEEE Trans. atomise Theory Tech, 2001, Vol. 49, No. 2.SYSTEMS PIERRE BLONDY, ANDREW R. 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Investigation of Compact Low Pass Filter with Sharp CutOff using Metamaterial RADIOENGINEERING, 2013, VOL. 22, NO. 3.PIERRE BLONDY, ANDREW R. BROWN, DOMINIQUE CROS AND GABRIEL M.REBEIZ, Low-Loss Micro machined Filters for Millimeter-Wave Communication Systems, 1998.JIA-SHENG HONG AND M.J.LANCASTER, Microstrip Filters for RF/Microwave Applications , John Wiley Sons, Inc., 2001About AuthorsMariselvam VENKAT Obtained his BE degree from PTR College of Engineering and Technology, Madurai and ME from Thiagarajar college of Engineering Anna university Chennai in 2010 respectively. He is now pursue PhD in the Electronics and Communication Engineering department, Thiagarajar College of Engineering, Madurai., India. His area of interests includes microwave and millimeter wave circuits. emailprotectedRaju SRINIVASAN Obtained her BE degree from the PSG college of technology university of madras ,India and M.tech degree from NIT Trichy ,India 1982 and 1984 respectively she received her PhD from Madurai Kamarajar University, Madurai in 1996 .She is now working as a professor and judgement of the department of Electronics and Communication Engineering Department, Thiagarajar college of Engineering Madurai, India her areas of research interest are wireless technologies, RF circuits and systems. emailprotected.