DOCSLIB.ORG

A Simple Approach for Designing a Filter on Microstrip Lines

Total Page：16

File Type：pdf, Size：1020Kb

Download full-text PDF Read full-text
A Simple Approach for Designing a Filter on Microstrip Lines Applied Engineering Letters Vol.4, No.1, 19-23 (2019) e-ISSN: 2466-4847 A SIMPLE APPROACH FOR DESIGNING A FILTER ON MICROSTRIP LINES UDC: 621.372.543 Original scientific paper https://doi.org/10.18485/aeletters.2019.4.1.3 Ashish Kumar1 1Aryabhatta research institute of observational sciences (ARIES), Nainital, India Abstract: ARTICLE HISTORY This paper deals with the design and fabrication of edge-coupled band pass Received: 22.03.2019. filter (BPF) circuit (fifth order) on microwave laminate for 4.5 GHz ± 0.5 GHz Accepted: 26.03.2019. application. The design of filter is realized on a high quality RT/ duroid Available: 31.03.2019. laminate having the dielectric constant 10.5 and substrate thickness 1.27 mm. The relevant design specifications, simulation, and test results of the circuit is described. The numerical calculations and simulations are KEYWORDS performed in Linpar. The Printed Circuit Board (PCB) artwork is prepared in filter, microstrips, edge- coupled, linpar, CorelDraw, CorelDraw. A prototype of the design was manufactured and tested on microwave microwave network analyzer. Some offsets are observed between the theoretical and practical results, which may be attributed to the wide tolerance in the dielectric permittivity specified for the RT/ duroid substrate. 1. INTRODUCTION certain complexities. However, without entering into any design complexities, the present work is In electronic circuits, the filter is a network focussed on the basic steps involved in the design having non-uniform frequency response and fabrication of an edge-coupled BPF on characteristics in the desired frequency range. microstrip lines. Following the steps, one can They are used to manipulate the signal by realize any other microwave filters for their enhancing or attenuating certain frequency ranges frequency band of interests. or bands, and sometimes, for rejecting harmonics and excluding out-of-band signal. The ideal filter 2. THEORY network provides perfect transmission for all the 2.1 Coupled lines frequencies in certain passband region and infinite attenuation in stopband regions. Such ideal The coupled lines are formed when the two or characteristics can’t be achieved in practice. more unshielded transmission lines are placed in Therefore, filter design aims at approximating the close proximity to each other [3]. Likewise ideal characteristics within acceptable tolerances. transformers, the power at one transmission line At microwave frequency, instead of the lumped gets coupled to other. The level of coupling element inductors and capacitors, the transmission depends on mode and direction of electromagnetic line sections are used which behaves as inductors wave propagation, physical and electrical and capacitors. The microwave filters have a wide dimensions of the line, and frequency of operation. range of applications demanding high performance The coupled lines may be in symmetrical or at reduced size and production cost [1]. These asymmetrical form. The symmetrical coupled line filters are primarily used in wireless handsets, structures support odd and even mode excitations, satellite receivers and military systems [2]. The and the interaction between these modes induces filters with high performance characteristics is the coupling between the line conductors. The achieved when designed using sophisticated planar even and odd modes have different characteristics or waveguide architecture, but at the cost of CONTACT: A. Kumar, e-mail: [email protected] © 2019 Published by the Serbian Academic Center A. Kumar / Applied Engineering Letters Vol.4, No.1, 19-23 (2019) impedances (Zo_odd and Zo_even) from line to 2 F 2 ground and represents the in-phase and out of Zo ln 1 (2) 2 W// h W h phase characteristics of the driven source, eff respectively [4]. The terms, a and F are computed using the The theory of coupled line is utilized in the width-height ratio, W/h of the microstrip laminate. realization of numerous passive microwave The term, η is the wave impedance in free space. components like filters, directional couplers, In microstrip line configuration, the resonators, impedance transformers, and others, transmission line conductor of a typical N +1 of which the design of filters on the planar coupled section of coupled line filter takes the form shown transmission lines such as microstrip lines are the in Fig. 2a-b. most popular [2, 3, 5] due to its ease in fabrication using low-cost RT/ duroid laminates and processes (a) involved therein. The planar transmission lines at microwave frequencies are broadly classified in two categories: (i) the one that supports a Transverse Electromagnetic Mode (TEM) of propagation, like coaxial line, stripline etc., or the one that supports (b) quasi-TEM modes of propagation, and (ii) the one like hollow waveguides, dielectric guides etc. that does not support such modes of propagation. In this work, the planar coupled microstrip lines are used which supports the quasi- TEM of Fig. 2. Coupled line filter (a) layout of a typical N+1 propagation [6]. The microstrip line is best known section of coupled line band pass filter, and (b) its and widely used for microwave filter designs equivalent circuit. because of its inherent advantages like ease in integration with the active solid-state devices, 2.2 Filter parameters good heat sinking, low cost, compact design and good repeatability. Fig. 1 shows the cross-sectional When dealing with filters, the following view of a microstrip line [3, 6]. It contains a single parameters plays an important role [2-3, 8]: dielectric substrate of gallium arsenide (GaAs), Insertion Loss: The insertion loss quantifies the alumina (Al2O3) or teflon material having the amount below the 0 dB line the power amplitude dielectric constant as εr. response drops. Ideally, a perfect filter inserted into RF circuit path would introduce no power loss in the passband, or it would have zero insertion loss. In reality however, certain amount of power loss associated with the filter is expected. Mathematically, Insertion Loss (I.L.) = 2 10*log(Pin/PL) = -10*log(1- |RCin| ), where, PL= Fig. 1. Cross-sectional view of a microstrip line power delivered to the load, Pin = power from source, and |RCin| = reflection coefficient looking The height, h of the substrate is chosen to be into the filter. very smaller than its wavelength. At the top of the Ripple: It is the difference between maximum dielectric substrate, there is a conducting strip of and minimum amplitude response (in dB or width, w and thickness, t and the bottom surface is Nepers) or the flatness of signal in the passband. the ground plane. The transmission characteristic 3dB-Bandwidth: For any filter, it is the difference of the microstrip line is well described by its between upper and lower frequencies typically effective dielectric constant, εeff and its recorded at the 3dB attenuation points above the characteristic impedance, Zₒ expressed pass-band. mathematically as [3, 7]: Shape Factor: Shape factor defines the sharpness 0.053 r 0.9 0.564a of the filter response, by taking the ratio r 3 rr1110 eff 1 (1) between the 60 dB and the 3dB bandwidth. 2 2 (Wh / ) and, 20 A. Kumar / Applied Engineering Letters Vol.4, No.1, 19-23 (2019) Rejection: Attenuation level for the undesirable (d) Even and odd mode impedance calculation: The signal frequencies, however in reality an upper even and odd mode characteristics line impedance bound on this value called as rejection ratio, is is computed using: expected. Practically 60 dB is the rejection rate. 2 ZZZJZJo_odd i , i 1 o[1 o i , i 1 ( o i , i 1 ) ] , and 2 3. THEORY ZZZJZJo_evenii , 1 o[1 o ii , 1 ( oii , 1 ) ] (5) 3.1 Design specifications where, i, i + 1 refers to the overlapping of adjacent elements of coupled line filters. Zο is the The edge-coupled BPF is designed with the characteristics line impedance at the beginning specification as given in Table 1. and end of the filter structure. (e) Simulation using Linpar: Linpar [11] is a 2D Table 1. Design specification of filter Method of Moment (MoM) analysis package Parameters Values developed for numerical calculations involved in bandwidth 1 GHz the design of microwave circuits and transmission frequency range 4 - 5 GHz lines. Using Linpar, for the specified dielectric centre frequency (fo) 4.5 GHz constant and stripline dimensions, the separation s, order of filter Fifth Order and width w of the copper strips are determined to approximation Chebyshev meet the calculated even and odd mode ripple Factor 0.1 dB impedances. Generally, the width conforms to the dielectric constant 10.5 width of the other microstrip lines, therefore, the substrate thickness 1.27 mm separation is the most common parameter that can be varied to achieve the even and odd mode 3.2 Design steps impedances. The length of each coupled line segment has to be equal to λ/4 at the centre The series of steps that were followed in frequency. designing the filter, as detailed below [3, 8-10]: (f) Optimization of circuit parameters to meet the (a) Selection of standard filter coefficient: Based on desired specifications: Once the design is the type and order of the filter (generally completed, the circuit has to be simulated to Butterworth or Chebyshev) needed, an observe the characteristic response. If the appropriate filter coefficients g0, g1,…, gN, gN+1 from observed response deviates from the desired the standard tables are selected. In this work, the response, it is required to optimize the design by filter coefficients corresponding to fifth order varying the input parameters within the acceptable Chebyshev filter with 0.1 dB ripple is taken. range. Chebyshev filter is selected due to its narrow pass (g) Compensation for the length, width and band response. spacing: The precise design can be achieved by (b) Identification of normalized bandwidth, upper introducing the length correction to account for and lower cut-off frequencies: For the desired filter fringing field effects.
Load more

Recommended publications
  • A Broad Bandwidth Suspended Membrane Waveguide to Thinfilm
    A Broad Bandwidth Suspended Membrane Waveguide to Thinfilm Microstrip Transition J. W. Kooi California Institute of Technology, 320-47, Pasadena, CA 91125, USA. C. K. Walker University of Arizona, Dept. of Astronomy. J. Hesler University of Virginia, Dept. of Electrical Engineering. Abstract Excellent progress in the development of Submillimeter-wave SIS and HEB mixers has been demonstrated in recent years. At frequencies below 800 GHz these mixers are typically implemented using waveguide techniques, while above 800 GHz quasi-optical (open structure) methods are often used. In many instances though, the use of waveguide components offers certain advantages. For example, broadband corrugated feed-horns with well defined on axis Gaussian beam patterns. Over the years a number of waveguide to microstrip transitions have been proposed. Most of which are implemented in reduced height waveguide with RF bandwidth less than 35%. Unfortunately reducing the height makes machining of mixer components at terahertz frequencies rather difficult. It also increases RF loss as the current density in the waveguide goes up, and surface finish is degraded. An additional disadvantage of existing high frequency waveguide mixers is the way the active device (SIS, HEB, Schottky diode) is mounted in the waveguide. Traditionally the junction, and its supporting substrate, is mounted in a narrow channel across the guide. This structure forms a partially filled dielectric waveguide, whose dimensions must kept small to prevent energy from leaking out the channel. At frequencies approaching or exceeding a terahertz this mounting scheme becomes impractical. Because of these issues, quasi-optical mixers are typically used at these small wavelength. In this paper, we propose the use of suspended silicon (Si) and silicon nitride (Si3N4) membranes with silicon micro-machined backshort and feedhorn blocks.
    [Show full text]
  • A Survey on Microstrip Patch Antenna Using Metamaterial Anisha Susan Thomas1, Prof
    ISSN (Print) : 2320 – 3765 ISSN (Online): 2278 – 8875 International Journal of Advanced Research in Electrical, Electronics and Instrumentation Engineering (An ISO 3297: 2007 Certified Organization) Vol. 2, Issue 12, December 2013 A Survey on Microstrip Patch Antenna using Metamaterial Anisha Susan Thomas1, Prof. A K Prakash2 PG Student [Wireless Technology], Dept of ECE, Toc H Institute of Science and Technology, Cochin, Kerala, India 1 Professor, Dept of ECE, Toc H Institute of Science and Technology, Cochin, Kerala, India 2 ABSTRACT: Microstrip patch antennas are used for mobile phone applications due to their small size, low cost, ease of production etc. The MSA has proved to be an excellent radiator for many applications because of its several advantages, but it also has some disadvantages. Lower gain and narrow bandwidth are the major drawbacks of a patch antenna. In this paper, a survey on the existing solutions for the same which are developed through several years and an evolving technology metamaterial is presented. Metamaterials are artificial materials characterized by parameters generally not found in nature, but can be engineered. They differ from other materials due to the property of having negative permeability as well as permittivity. Metamaterial structure consists of Split Ring Resonators (SRRs) to produce negative permeability and thin wire elements to generate negative permittivity. Performance parameters especially bandwidth, of patch antennas which are usually considered as narrowband antennas can be improved using metamaterial. Metamaterials are also the basis of further miniaturization of microwave antennas. Keywords: Microstrip antenna, Metamaterial, Split Ring Resonator, Miniaturization, Narrowband antennas. I. INTRODUCTION Although the field of antenna engineering has a history of over 80 years it still remains as described in [1] “….
    [Show full text]
  • RF / Microwave PC Board Design and Layout
    RF / Microwave PC Board Design and Layout Rick Hartley L-3 Avionics Systems [email protected] 1 RF / Microwave Design - Contents 1) Recommended Reading List 2) Basics 3) Line Types and Impedance 4) Integral Components 5) Layout Techniques / Strategies 6) Power Bus 7) Board Stack-Up 8) Skin Effect and Loss Tangent 9) Shields and Shielding 10) PCB Materials, Fabrication and Assembly 2 RF / Microwave - Reading List PCB Designers – • Transmission Line Design Handbook – Brian C. Wadell (Artech House Publishers) – ISBN 0-89006-436-9 • HF Filter Design and Computer Simulation – Randall W. Rhea (Noble Publishing Corp.) – ISBN 1-884932-25-8 • Partitioning for RF Design – Andy Kowalewski - Printed Circuit Design Magazine, April, 2000. • RF & Microwave Design Techniques for PCBs – Lawrence M. Burns - Proceedings, PCB Design Conference West, 2000. 3 RF / Microwave - Reading List RF Design Engineers – • Microstrip Lines and Slotlines – Gupta, Garg, Bahl and Bhartia. Artech House Publishers (1996) – ISBN 0-89006-766-X • RF Circuit Design – Chris Bowick. Newnes Publishing (1982) – ISBN 0-7506-9946-9 • Introduction to Radio Frequency Design – Wes Hayward. The American Radio Relay League Inc. (1994) – ISBN 0-87259-492-0 • Practical Microwaves – Thomas S. Laverghetta. Prentice Hall, Inc. (1996) – ISBN 0-13-186875-6 4 RF / Microwave Design - Basics ) RF and Microwave Layout encompasses the Design of Analog Based Circuits in the range of Hundreds of Megahertz (MHz) to Many Gigahertz (GHz). ) RF actually in the 500 MHz - 2 GHz Band. (Design Above 100 MHz considered RF.) ) Microwave above 2 GHZ. 5 RF / Microwave Design - Basics ) Unlike Digital, Analog Signals can be at any Voltage and Current Level (Between their Min & Max), at any point in Time.
    [Show full text]
  • Tests of Microstrip Dispersion Formulas Presentation to Bring Them Into a Similar Formalism for Compari­ £ E(O) Is the Zero-Frequency, Or H
    IEFF. TRANSACTIONS ON MICROWAVE THEORY AND TECHNIQUES, VOL. 36, No.3, MARCH 1988 619 The most restrictive convergence plot is usually the one for the ranged from 2.3 percent to 4.1 percent of the seven formulas for <,,(j) propagation constant of the narrowest strip spacing at the lowest tested. A formula due to Kirschning and Jansen (10( showed the lowest frequency. This is due to the field having least space in terms of average deviation from measured values, although the differences between the predictions of their formuIa and others tested are of the order of the wavelength to adjust to the structure. However, when the odd error limits of the comparison process. It is concluded that the results mode is weakly bound at high frequencies, a small change in the indicate the suitability of relatively simple analytical expressons for the propagation constant changes the decay rate away from the strips computation for microstrip dispersion. dramatically. This greatly &ffects the power contained in the mode and hence the characteristic impedance. In this case the I. INTRODUCTION odd-mode impedance at high frequencies sets the number of modes required. Generally, there exists a relation between the The widespread use of micros trip transmission line for micro­ number of modes and the £2/£1 = £2/£3 dielectric step. Larger wave circuit construction has created a need for accurate and steps require more modes since the field has a more complicated practical computational algorithms for the values of microstrip structure in which to conform. line parameters. For this purpose, the micros trip line is modeled Numerical instabilities occur in the determinant calculation for as an equivalent TEM system at the operating frequency.
    [Show full text]
  • A Simple Linear-Type Negative Permittivity Metamaterials Substrate Microstrip Patch Antenna
    materials Article A Simple Linear-Type Negative Permittivity Metamaterials Substrate Microstrip Patch Antenna Wei-Hua Hui, Yao Guo and Xiao-Peng Zhao * Department of Applied Physics, School of Physical Science and Technology, Northwestern Polytechnical University, Xi’an 710129, China; [email protected] (W.-H.H.); [email protected] (Y.G.) * Correspondence: [email protected] Abstract: A microstrip patch antenna (MPA) loaded with linear-type negative permittivity metama- terials (NPMMs) is designed. The simple linear-type metamaterials have negative permittivity at 1–10 GHz. Four groups of antennas at different frequency bands are simulated in order to study the effect of linear-type NPMMs on MPA. The antennas working at 5.0 GHz are processed and measured. The measured results illustrate that the gain is enhanced by 2.12 dB, the H-plane half-power beam width (HPBW) is converged by 14◦, and the effective area is increased by 62.5%. It can be concluded from the simulation and measurements that the linear-type metamaterials loaded on the substrate of MAP can suppress surface waves and increase forward radiation well. Keywords: metamaterials; negative permittivity; microstrip patch antenna; gain 1. Introduction Citation: Hui, W.-H.; Guo, Y.; Zhao, Electromagnetic (EM) metamaterials are composed of periodic, subwavelength arti- X.-P. A Simple Linear-Type Negative ficial structures, which can be resonant or non-resonant units. A two-dimensional form Permittivity Metamaterials Substrate of metamaterials is called a metasurface. According to the uniform effective medium Microstrip Patch Antenna. Materials theory, the properties of these structures can be determined by the effective permittivity 2021, 14, 4398.
    [Show full text]
  • Reviewing the Basics of Microstrip
    DESIGN FEATURE Microstrip Lines Reviewing The Basics Of Microstrip An understanding of the fundamentals of Lines microstrip transmission lines can guide high- frequency designers in the proper application of this venerable circuit technology. Leo G. Maloratsky RINTED transmission lines are widely used, and for good reason. Principal Engineer They are broadband in frequency. They provide circuits that are Rockwell Collins, 2100 West Hibiscus Pcompact and light in weight. They are generally economical to pro- Blvd., Melbourne, FL 32901; (407) duce since they are readily adaptable to hybrid and monolithic inte- 953-1729, e-mail: lgmalora@ grated-circuit (IC) fabrication technologies at RF and microwave fre- mbnotes.collins.rockwell.com. quencies. To better appreciate printed transmission lines, and microstrip in particular, some of the basic principles of microstrip lines will be reviewed here. A number of different transmis- with respect to the others. In Fig. 1, sion lines are generally used for it should be noted that the substrate microwave ICs (MICs) as shown in materials are denoted by the dotted Fig. 1. Each type has its advantages areas and the conductors are indicat- ed by the bold lines. The microstrip line is a transmis- Basic lines Modifications sion-line geometry with a single con- W W t a ductor trace on one side of a dielectric H hhhW W substrate and a single ground plane line a h Suspended Inverted on the opposite side. Since it is an Microstrip Microstrip line Shielded microstrip line microstrip line microstrip line open structure, microstrip line has a t W W1 major fabrication advantage over b b t stripline.
    [Show full text]
  • Microstrip Solutions for Innovative Microwave Feed Systems
    Examensarbete LiTH-ITN-ED-EX--2001/05--SE Microstrip Solutions for Innovative Microwave Feed Systems Magnus Petersson 2001-10-24 Department of Science and Technology Institutionen för teknik och naturvetenskap Linköping University Linköpings Universitet SE-601 74 Norrköping, Sweden 601 74 Norrköping LiTH-ITN-ED-EX--2001/05--SE Microstrip Solutions for Innovative Microwave Feed Systems Examensarbete utfört i Mikrovågsteknik / RF-elektronik vid Tekniska Högskolan i Linköping, Campus Norrköping Magnus Petersson Handledare: Ulf Nordh Per Törngren Examinator: Håkan Träff Norrköping den 24 oktober, 2001 'DWXP $YGHOQLQJ,QVWLWXWLRQ Date Division, Department Institutionen för teknik och naturvetenskap 2001-10-24 Ã Department of Science and Technology 6SUnN 5DSSRUWW\S ,6%1 Language Report category BBBBBBBBBBBBBBBBBBBBBBBBBBBBBBBBBBBBBBBBBBBBBBBBBBBBB Svenska/Swedish Licentiatavhandling X Engelska/English X Examensarbete ISRN LiTH-ITN-ED-EX--2001/05--SE C-uppsats 6HULHWLWHOÃRFKÃVHULHQXPPHUÃÃÃÃÃÃÃÃÃÃÃÃ,661 D-uppsats Title of series, numbering ___________________________________ _ ________________ Övrig rapport _ ________________ 85/I|UHOHNWURQLVNYHUVLRQ www.ep.liu.se/exjobb/itn/2001/ed/005/ 7LWHO Microstrip Solutions for Innovative Microwave Feed Systems Title )|UIDWWDUH Magnus Petersson Author 6DPPDQIDWWQLQJ Abstract This report is introduced with a presentation of fundamental electromagnetic theories, which have helped a lot in the achievement of methods for calculation and design of microstrip transmission lines and circulators. The used software for the work is also based on these theories. General considerations when designing microstrip solutions, such as different types of transmission lines and circulators, are then presented. Especially the design steps for microstrip lines, which have been used in this project, are described. Discontinuities, like bends of microstrip lines, are treated and simulated.
    [Show full text]
  • Impact of Metamaterial in Antenna Design: a Review
    International Journal of Electronics and Communication Engineering. ISSN 0974-2166 Volume 8, Number 1 (2015), pp. 87-90 © International Research Publication House http://www.irphouse.com Impact of Metamaterial in Antenna Design: A Review Swagata B Sarkar Assistant Professor, Sri Sairam Engineering College, Chennai Abstract In this paper it is observed that how metamaterials can be used to improve the design parameters of antenna. Metamaterials are kind of structures through which negative permittivity and negative permeability can be obtained. This special property will improve some vital properties of antenna such as return loss, efficiency, size, bandwidth, multiband behavior, directivity, gain and specific absorption rate (SAR). In this paper some popular structures of metamaterial are highlighted after review. Key Words: Metamaterial, Antenna parameters, Negative permittivity, Negative permeability I. INTRODUCTION In recent days people are concentrating more about metamaterial based antenna design as it has lot of advantages. The metamaterial based antenna can be designed with improved antenna parameters. i) Return loss (RL): Return loss is the loss of power in the signal returned/reflected by a discontinuity in a transmission line. It is usually expressed as a ratio in decibels (dB). The metamaterial structure can decrease the return loss and make antenna to work with a better efficiency. ii) Efficiency: Antenna efficiency is radiation efficiency. It is a measure of the efficiency with which a radio antenna converts the radio-frequency power accepted at its terminals into radiated power. Efficiency can be increased with the metamaterial defect introduced in the antenna design. iii) Size: Physical size of the antenna can be decreased by using metamaterial structure as substrate, superstrate or any other position.
    [Show full text]
  • A Compact Multiband Metamaterial Based Microstrip Patch Antenna for Wireless Communication Applications
    Nikhil Kulkarni. Int. Journal of Engineering Research and Application www.ijera.com ISSN : 2248-9622, Vol. 7, Issue 1, ( Part -1) January 2017, pp.01-05 RESEARCH ARTICLE OPEN ACCESS A Compact Multiband Metamaterial based Microstrip Patch Antenna for Wireless communication Applications Nikhil Kulkarni*, G. B. Lohiya** *(Department of Electronic and Telecommunication, Mumbai University, India Email: [email protected]) ** (Department of Electronic and Telecommunication, Mumbai University, India Email: [email protected]) ABSTRACT In this paper, a metamaterial based compact multiband microstrip antenna is proposed which can give high gain and directivity. Metamaterials are periodic structures and have been intensively investigated due to the particular features such as ultra-refraction phenomenon and negative permittivity and/or permeability. A metamaterial- based microstrip patch antenna with enhanced characteristics and multi band operation will be investigated in this work. The multiple frequency operation will be achieved by varying the capacitance of the metamaterial structure with the help of metallic loadings placed in each metamaterial unit cells. The potential impacts will be miniaturization, reduced cost and reduced power consumption since multiple antennas operating at different frequencies are replaced by a single antenna which can operate at multiple frequencies. The proposed microstrip patch antenna will have its frequencies of operation in the L, S and C bands. The proposed structure is simulated using Agilent Advanced Design System (ADS) 2011.05. It is then fabricated on the FR4 substrate and the performance of the fabricated antenna is measured using the Vector Network Analyzer (VNA). Keywords – Metamaterial, Microstrip Antenna, Bandwidth, Tunability, Frequency Range, Gain I. Introduction thickness h [1].
    [Show full text]
  • Novel Hts Microstrip Resonator Configurations for Microwave Bandpass Filters
    Michael Reppel NOVEL HTS MICROSTRIP RESONATOR CONFIGURATIONS FOR MICROWAVE BANDPASS FILTERS Witten, Germany September 2000 NOVEL HTS MICROSTRIP RESONATOR CONFIGURATIONS FOR MICROWAVE BANDPASS FILTERS Vom Fachbereich Elektrotechnik und Informationstechnik der Bergischen Universitat¨ – Gesamthochschule Wuppertal angenommene Dissertation zur Erlangung des akademischen Grades eines Doktor–Ingenieurs von Diplom–Ingenieur Michael Reppel aus Witten Tag der mundlichen¨ Prufung:¨ 23.06.2000 Referenten: Prof. Dr.-Ing. Heinz Chaloupka Prof. Dr.-Ing. Volkert Hansen Contents Summary 1 1 Introduction 3 2 Planar Resonator Configurations 7 2.1 Distributed resonators . 7 2.2 Coupling of distributed resonators . 9 2.3 Lumped element resonators . 12 2.4 Novel doubly–symmetric microstrip resonator . 13 2.4.1 Resonator design and coupling between resonators . 13 2.4.2 Couplings of different natural phases . 15 2.4.3 Superior tuning of coupling coefficients . 17 3 HTS Microstrip Resonators 19 3.1 Loss contributions . 20 3.1.1 Conductor losses . 21 3.1.2 Dielectric losses . 25 3.1.3 Packaging and housing losses . 25 3.1.4 Analytic evaluation of losses in the housing cover . 31 3.2 Attainable unloaded quality factor . 34 4 Measurement Set–Ups 39 4.1 Measurement of the scattering parameters of a two–port device . 39 4.2 Measurement of the resonator quality factor . 40 4.3 Intermodulation measurement set–up . 43 5 Experimental Results for HTS Devices 45 5.1 Resonator and filter fabrication . 45 5.2 Unloaded quality factors of HTS resonators . 47 5.3 Bandpass filters . 49 5.3.1 Two–pole test filters . 49 i ii CONTENTS 5.3.2 Extremely narrow–band two–pole filter .
    [Show full text]
  • Broadband Transition from Microstrip Line to Waveguide Using a Radial Probe and Extended GND Planes for Millimeter-Wave Applications
    Progress In Electromagnetics Research Letters, Vol. 60, 95–100, 2016 Broadband Transition from Microstrip Line to Waveguide Using a Radial Probe and Extended GND Planes for Millimeter-Wave Applications Azzemi Ariffin*, Dino Isa, and Amin Malekmohammadi Abstract—A broadband microstrip line-to-waveguide (MSL-to-WG) transition is developed for E-band applications. In order to achieve a sufficient and broadband coupling between the microstrip line (MSL) and waveguide (WG), a radial electric probe at the end of the MSL and extended ground (GND) planes on the dielectric substrate are proposed. Results are compared against a simple transition (S-Tr) with a straight electric probe. For the case of operational bandwidth (BW) for an input return loss (S11) below −20 dB, the proposed transitions using the radial probe and extended GND planes show the BW enhancement of 33.8% and 61.9%, respectively, compared to the S-Tr. The proposed and simple transitions were fabricated on a low-loss liquid crystal polymer (LCP) dielectric substrate. The measured bandwidth (BW) for S11 below −10 dB of the proposed transition is over 28 GHz, which is satisfied at all test frequencies from 67 to 95 GHz. Its measured insertion loss can be analyzed as −1.33 and −1.41 dB per transition at 70 and 80 GHz, respectively, considering the loss contribution of the cable adapter and waveguide transition. 1. INTRODUCTION Millimeter-wave (MMW) technology has been recognized as having potential for emerging markets and developed for broadband ultra-high-speed wireless communication systems such as broadband radio links for the backhaul networking [1] of cellular base stations, Giga wireless LAN, Gigabit Ethernet networks, 77 GHz automotive radar systems [2] and inter-vehicle communications.
    [Show full text]
  • RF/Microwave PCB Fundamentals
    Fundamentals of RF/Microwave PCBs John Bushie and Anaya Vardya American Standard Circuits PEER REVIEWER This book has been reviewed for technical accuracy by the following expert from the PCB industry. Happy Holden Consulting Technical Editor, I-Connect007 Happy Holden is the retired director of electronics and innovations for Gentex Corporation. Happy is the former chief technical officer for the world’s largest PCB fabricator, Hon Hai Precision Indus- tries (Foxconn). Prior to Foxconn, Happy was the senior PCB technologist for Mentor Graphics and the advanced technology manager at Nan Ya/ Westwood Associates and Merix. Happy previ- ously worked at Hewlett-Packard for over 28 years as director of PCB R&D and manufacturing engineering manager. He has been involved in advanced PCB tech- nologies for over 47 years. MEET THE AUTHORS John Bushie Director of Technology at American Standard Circuits John has over 20 years of experience in the PCB in- dustry supplying and supporting the manufacture of PCBs as well as high-frequency RF/microwave circuit board laminates. He has provided product and design support to PCB and system design- ers throughout North America, Europe, and Asia. His extensive background in problem solving and process engineering has allowed him to support many customers through detailed and focused application engineering. It is this close relation- ship with customers that drives his passion for new product design and design for manufacturability. Anaya Vardya President and CEO of American Standard Circuits Anaya has over 33 years of experience in elec- tronics manufacturing, including in the United States, Canada, and the Far East.
    [Show full text]