Lipparini* anazysis which compare favourabzy with experimentaz results. The same modez. described. It is shown that the discrepancies between computed
|
|
- Letitia Edith King
- 5 years ago
- Views:
Transcription
1 ACCURATE ANALYSIS AND DESIGN OF MICROSTRIP INTERDIGITATED COUPLERS Vittorio Rizzoli*- Alessandro Lipparini* Abstract. The ezectricaz behaviour of interdigitated directionaz coupzers in an inhomogeneous diezectric medium is anazyzed. Thanks to the symmetry properties of the device, the concepts of even and odd networks can be appzied, Zeading to simpze, closed-form expressions for coupzer anazysis which compare favourabzy with experimentaz results. The same modez azzows the most important parasitic effects to be understood and quantitativezy described. It is shown that the discrepancies between computed and experimentaz data can be accurately expzained in terms of the parasiticsarising from junction discontinuities. FinaZZy, design data for azumina-microstrip interdigitated couplers are presented in graphic form. INTRODUCTION In the last few years, considerable attention has been devoted in literature to the problem of predicting microstrip interdigitated coupler behaviour on a quantitative basis. Analyses based on the homogeneous-dielectric assumption have been presented first {f1,2}, showing the theoretical equivalence between the interdigitated device and the conventional twowire one {2}. More recently, the same concept has been extended to the microstrip case {3}, leading to the definition of equivalent even and odd modes of propagation. These approximate approaches are usually adequate for computing the coupling coefficient and are generally suitable for obtaining qualitative information of technical interest about coupler performance and feasibility. On the other hand, if a complete and accurate characterization of coupler behaviour is required, a rigorous analysis should be carried out. This is particularly true when coupler directivity is concerned. In fact, the amount of power being coupled to the insulated port arises from the interference of nearly in-phase and nearly equal-amplitude waves, which must be carefully evaluated if directivity is to be accurately found. Such a rigorous analysis is attempted in this paper. COUPLER ANALYSIS AND DESIGN Let us consider a microstrip interdigitated coupler in the "unfolded" configuration as described in ref. {4} and schematically shown in fig. 1. This device basically consists of a length of an axially uniform fourmicrostrip system whose alternate conductors are short-circuited at both ends of the coupled section to yield the interdigitated topology. The reactances of the bonding wires will be assumed to be negligible, as is actually the case at microwave frequencies up to about 12 GHz. The strips will be further assumed to be equal and equally spaced since this is the most commonly encountered configuration. Thus the only two design parameters are strip width (w) and spacing Cs), apart from substrate thickness and permittivity. As a first step of the analysis procedure, the device is modelled as a *Istituto di Elettronica, University of Bologna, Villa Griffone, Pontecchio Marconi, 444 Bologna, ITALY. 642
2 //t// z FIG. I loss-free, inhomogeneous, quasi-tem four-wire line and any parasitic effects are neglected. If this is the case, the normal modes of propagation are defined by the following eigenvector matrix: 1 1 OC 3 c -ai1 a2-1 M al a a3 -a4 where the a's are dependent on coupler geometry. From (1) the network is seen to support two even and two odd modes with respect to the axial plane of symmetry. Thus, despite of the interdigitated topology, one can take advantage of the concepts of even and odd networks {5} and reduce the analysis problem to one of two independent two-port networks. In turn, each one of these simply consists of a couple of independent trasmission lines, since only the even (odd) modes are fed in the case of even (odd) excitation. This allows simple, explicit analysis formulae to be derived in a straightforward way. The latter are not reported here for the sake of brevity. To show the validity of this approach, in fig. 2 the measured and computed performances of an alumina 3-dB coupler having w=7 pm and s=5 pm are compared. Though the agreement is not perfect, it is evident that the coupler operation, including directivity, can be predicted with practically significant accuracy. In the simple schematization considered so far, the scattering matrix of the coupler depends on frequency only through the product f$, where i is the length of the coupled section. Thus a universal (i. e., frequencyindependent) design chart can be drawn for any given substrate characteris tics. Such a chart for.635 mm alumina is given in fig. 3, where constant coupling and directivity curves are plotted in the w-s plane. All coupling and directivity values refer to center band, which is defined as the value of the product fk yielding minimum coupling (in de3). Only the region corresponding to a VSWR less than 1.2 is shown in the figure. The center band value of ft typically ranges from in/sec to 3.1*16 m/sec for e =1 alumina. From fig. 2 it is evidqnt that coupling values between 2 and 6 db with good directivities and technically significant strip widths and spacings can be realised by this technique. In particular, it is in- 643
3 EXPERIMENT THEORY (NO PRRASITICS) THEORY [INCLUOING PRERSITICS) a.,: C3 (1) 'm - I? C:, Q L) oi _ C? S.5 9 FREQUENCY [GHZ) Ct C3? C)i \ I~~~~~~~~~~~~~~~~~~~~~~~~~~~ \ X 11~~~~~~~~~~~~ "I~~~~~~~' 'NN N a TI - - -r- T -r I- I- - I I I I I _ N "I z,.. ns z / :;~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~~i 2 lt 1I - --I FItG 2 644
4 a %*C(DB) - D(DB) z V5WR<1.2 -a ( B a85. 9 S W (M ICRONS) FIG. 3 teresting to observe that coupling essentially depends on strip spacing only (at least, as far as the limitation V/SWR<1.2 is retained) and, for any given coupling value, there exists an optimum strip width, yielding maximum directivity..in order to refine the analytical model of the coupler and t;o improve accuracy between theory and experiment, additional effects such as discontinuity parasitics i conductor losses and dispersion shou ld be taken into account. UJnfortunately,n when these are considered it is no longer possible to draw a frequency-independent design chart such as fig. 3. since the coupler scattering matrix no lonlger contains frequency in the fq combination only. Thus, for a practical design this chart would be best used to find a reasonable starting point for a local optimization to be carried out by a more sophisticated model. As an example, the effects of junction discontinuity parasitics will be briefely discussed here. Let us separately consider the even and odd networks. For each one of these, the electrical situation at both ends of the coupled section is much the same as due to an impedance step in a conventional microstrip. Thus launching parasitics can be modelled as lumped LC low-pass ladder networks which are cascade connected at the input and out- 645
5 put ports of both networks {6,7}. Fig. 2 clearly shows that these effects are mainly responsible for the previously observed discrepancies between theoretical and experimental results. The only fact that this model is still unable to describe is the.4 db 'insertion loss of the coupler. To predict the latter, conductor losses in microstrip should be obviously taken into account. CONCLUSION It has been shown that the quasi-tem analysis is adequate for describing microstrip interdigitated coupler behaviour up to 12 GHz, provided that the TEM mode distribution be accurately taken into account. Making use of the even- and odd-network concepts, analysis bec:omes simple and may be carried out by explicit formulae. The latter can be used to generate design charts yielding good starting points for optimization of practical designs. REFERENCES 11} W. P. Ou, "Design equations for interdigitated directional couplers", IEEE Trans., NTT-23, pp , Febr (2} V. Rizzoli, "Stripline interdigitated couplers: analysis and design considerations", Electron. Lett., vol. /11, pp , Aug {31 S. J. Hewitt and R. S. Pengelly, "Design data for interdigital directional couplers", Electron. Lett., vol. 12, pp , Febr (4} R. Waugh and D. La Combe, "Unfolding the Lange coupler", IEEE Trans., NTT-2, pp , Nov {5} J. Reed and G. J. Wheeler, "A method of analysis of symnetrical fourport networks", IRE Trans., MTT-4, pp , Oct {6} A. F. Thomson and A. Gopinath, "Calculation of microstrip discontinuity inductances", IEEE Trans., MTT-23, pp , Aug {7} P. Benedek and P. Silvester, "Equivalent capacitances for microstrip gaps and steps", IEEE Trans., MTT-2, pp , Nov This work was partially sponsored by the Italian National Research Council (CNR). 646
TC 412 Microwave Communications. Lecture 6 Transmission lines problems and microstrip lines
TC 412 Microwave Communications Lecture 6 Transmission lines problems and microstrip lines RS 1 Review Input impedance for finite length line Quarter wavelength line Half wavelength line Smith chart A
More informationARTIFICIAL TRANSMISSION LINE WITH LEFT/RIGHT-HANDED BEHAVIOR BASED ON WIRE BONDED INTERDIGITAL CAPACITORS
Progress In Electromagnetics Research B, Vol. 11, 245 264, 29 ARTIFICIAL TRANSMISSION LINE WITH LEFT/RIGHT-HANDED BEHAVIOR BASED ON WIRE BONDED INTERDIGITAL CAPACITORS J. J. Sánchez-Martínez, E. Márquez-Segura,
More informationSpectral Domain Analysis of Open Planar Transmission Lines
Mikrotalasna revija Novembar 4. Spectral Domain Analysis of Open Planar Transmission Lines Ján Zehentner, Jan Mrkvica, Jan Macháč Abstract The paper presents a new code calculating the basic characteristics
More informationMicrostrip Coupler with Complementary Split-Ring Resonator (CSRR)
Microstrip Coupler with Complementary Split-Ring Resonator (CSRR) E-242 Course Project Report Submitted by, EMIL MATHEW JOSEPH 4810-411-091-07049 Guided by, Prof. K J VINOY Department of Electrical and
More informationMicrowave Engineering 3e Author - D. Pozar
Microwave Engineering 3e Author - D. Pozar Sections 3.6 3.8 Presented by Alex Higgins 1 Outline Section 3.6 Surface Waves on a Grounded Dielectric Slab Section 3.7 Stripline Section 3.8 Microstrip An Investigation
More informationHow to measure complex impedance at high frequencies where phase measurement is unreliable.
Objectives In this course you will learn the following Various applications of transmission lines. How to measure complex impedance at high frequencies where phase measurement is unreliable. How and why
More informationECE 546 Lecture 13 Scattering Parameters
ECE 546 Lecture 3 Scattering Parameters Spring 08 Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois jesa@illinois.edu ECE 546 Jose Schutt Aine Transfer Function Representation
More informationNon-Sinusoidal Waves on (Mostly Lossless)Transmission Lines
Non-Sinusoidal Waves on (Mostly Lossless)Transmission Lines Don Estreich Salazar 21C Adjunct Professor Engineering Science October 212 https://www.iol.unh.edu/services/testing/sas/tools.php 1 Outline of
More informationModule 2 : Transmission Lines. Lecture 1 : Transmission Lines in Practice. Objectives. In this course you will learn the following
Objectives In this course you will learn the following Point 1 Point 2 Point 3 Point 4 Point 5 Point 6 Point 7 Point 8 Point 9 Point 10 Point 11 Point 12 Various Types Of Transmission Line Explanation:
More informationSTUB BASED EQUIVALENT CIRCUIT MODELS FOR EVEN/ODD MODE DUAL CRLH UNIT CELLS. Faculty of Engineering, Ain Shams University, Cairo, Egypt
Progress In Electromagnetics Research M, Vol. 3, 95 9, 3 STUB BASED EQUIVALENT CIRCUIT MODELS FOR EVEN/ODD MODE DUAL CRLH UNIT CELLS Amr M. E. Safwat, *, Amr A. Ibrahim, Mohamed A. Othman, Marwah Shafee,
More informationARTIFICIAL DIELECTRIC SUBSTRATE FOR MICROWAVE APPLICATIONS
ARTIFICIAL DIELECTRIC SUBSTRATE FOR MICROWAVE APPLICATIONS DOC. ING. JAN MACHÁČ, DRSC. PROF. ING. JÁN ZEHENTNER, DRSC. Abstract: This paper presents a new version of an artificial dielectric substrate.
More informationRana Pratap Yadav *, Sunil Kumar, and S. V. Kulkarni Institute for Plasma Research, Bhat, Gandhinagar , India
Progress In Electromagnetics Research B, Vol. 56, 5 49, 013 AN ANALYSIS OF JUNCTION DISCONTINUITY EF- FECTS IN THE MULTI-ELEMENT COUPLED LINES AND ITS DIMINUTION AT DESIGNING STAGE Rana Pratap Yadav *,
More informationECE 598 JS Lecture 06 Multiconductors
ECE 598 JS Lecture 06 Multiconductors Spring 2012 Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois jesa@illinois.edu 1 TELGRAPHER S EQUATION FOR N COUPLED TRANSMISSION LINES
More informationTransmission-Line Essentials for Digital Electronics
C H A P T E R 6 Transmission-Line Essentials for Digital Electronics In Chapter 3 we alluded to the fact that lumped circuit theory is based on lowfrequency approximations resulting from the neglect of
More informationDESIGN AND OPTIMIZATION OF EQUAL SPLIT BROADBAND MICROSTRIP WILKINSON POWER DI- VIDER USING ENHANCED PARTICLE SWARM OPTI- MIZATION ALGORITHM
Progress In Electromagnetics Research, Vol. 118, 321 334, 2011 DESIGN AND OPTIMIZATION OF EQUAL SPLIT BROADBAND MICROSTRIP WILKINSON POWER DI- VIDER USING ENHANCED PARTICLE SWARM OPTI- MIZATION ALGORITHM
More informationThis section reviews the basic theory of accuracy enhancement for one-port networks.
Vector measurements require both magnitude and phase data. Some typical examples are the complex reflection coefficient, the magnitude and phase of the transfer function, and the group delay. The seminar
More informationDesign of all-pole microwave filters. Giuseppe Macchiarella Polytechnic of Milan, Italy Electronic and Information Department
Design of all-pole microwave filters Giuseppe Macchiarella Polytechnic of Milan, Italy Electronic and Information Department In-line filters with all-equal resonators R L eq, f L eq, f L eq, f L eq, f
More informationCLOSED-FORM DESIGN METHOD OF AN N-WAY DUAL-BAND WILKINSON HYBRID POWER DIVIDER
Progress In Electromagnetics Research, PIER 101, 97 114, 2010 CLOSED-FORM DESIGN METHOD OF AN N-WAY DUAL-BAND WILKINSON HYBRID POWER DIVIDER Y. L. Wu, Y. A. Liu, S. L. Li, C. P. Yu, and X. Liu School of
More informationECE 497 JS Lecture -07 Planar Transmission Lines
ECE 497 JS Lecture -07 Planar Transmission Lines Spring 2004 Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois jose@emlab.uiuc.edu 1 Microstrip ε Z o w/h < 3.3 2 119.9 h h =
More informationTransmission-Reflection Method to Estimate Permittivity of Polymer
Transmission-Reflection Method to Estimate Permittivity of Polymer Chanchal Yadav Department of Physics & Electronics, Rajdhani College, University of Delhi, Delhi, India Abstract In transmission-reflection
More informationECE 451 Transmission Lines & Packaging
Transmission Lines & Packaging Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois jose@emlab.uiuc.edu 1 Radio Spectrum Bands The use of letters to designate bands has long ago
More informationTransmission Lines. Plane wave propagating in air Y unguided wave propagation. Transmission lines / waveguides Y. guided wave propagation
Transmission Lines Transmission lines and waveguides may be defined as devices used to guide energy from one point to another (from a source to a load). Transmission lines can consist of a set of conductors,
More informationMATHEMATICAL MODEL BASED TRANSMISSION PARAMETERS OF AN ISOLATED MICROSTRIPLINE STRUCTURE
International Journal of Research in Engineering, Technology and Science, Volume VI, Issue VIII, August 2016 www.ijrets.com, editor@ijrets.com, ISSN 2454-1915 MATHEMATICAL MODEL BASED TRANSMISSION PARAMETERS
More informationMEASURE THE COMPLEX PERMEABILITY OF FER- ROMAGNETIC THIN FILMS: COMPARISON SHORTED MICROSTRIP METHOD WITH MICROSTRIP TRANS- MISSION METHOD
Progress In Electromagnetics Research Letters, Vol. 11, 173 181, 2009 MEASURE THE COMPLEX PERMEABILITY OF FER- ROMAGNETIC THIN FILMS: COMPARISON SHORTED MICROSTRIP METHOD WITH MICROSTRIP TRANS- MISSION
More informationNEW CAD MODEL OF THE MICROSTRIP INTERDIGITAL CAPACITOR
Active and Passive Electronic Components December 2004, Vol. 27, pp. 237 245 NEW CAD MODEL OF THE MICROSTRIP INTERDIGITAL CAPACITOR NIHAD DIB a, *,y, QIU ZHANG b and ULRICH ROHDE c a Electrical Engineering
More informationCoplanar Microwave Integrated Circuits
Ingo Wolff Coplanar Microwave Integrated Circuits Verlagsbuchhandlung Dr. Wolff GmbH Content Chapter I. 1.1 Chapter II. II. 1 n.1.1 n.1.2 n.1.3 n.1.3.1 n.1.3.2 n.2 n.2.1 n.2.2 n.2.3 n.2.4 n.2.5 n.2.6 n.2.7
More informationAnalyzing of Coupling Region for CRLH/RH TL Coupler with Lumped-elements
PIERS ONLINE, VOL. 3, NO. 5, 27 564 Analyzing of Coupling Region for CRLH/RH TL Coupler with Lumped-elements Y. Wang 2, Y. Zhang, 2, and F. Liu 2 Pohl Institute of Solid State Physics, Tongji University,
More informationA Method to Extract Dielectric Parameters from Transmission Lines with Conductor Surface Roughness at Microwave Frequencies
Progress In Electromagnetics Research M, Vol. 48, 1 8, 2016 A Method to Extract Dielectric Parameters from Transmission Lines with Conductor Surface Roughness at Microwave Frequencies Binke Huang * and
More informationPHY3128 / PHYM203 (Electronics / Instrumentation) Transmission Lines
Transmission Lines Introduction A transmission line guides energy from one place to another. Optical fibres, waveguides, telephone lines and power cables are all electromagnetic transmission lines. are
More informationECE 451 Advanced Microwave Measurements. TL Characterization
ECE 451 Advanced Microwave Measurements TL Characterization Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois jesa@illinois.edu ECE 451 Jose Schutt-Aine 1 Maxwell s Equations
More informationA GENERALIZED COUPLED-LINE DUAL-BAND WILKINSON POWER DIVIDER WITH EXTENDED PORTS
Progress In Electromagnetics Research, Vol. 19, 197 14, 1 A GENERALIZED COUPLED-LINE DUAL-BAND WILKINSON POWER DIVIDER WITH EXTENDED PORTS J. C. Li *, Y. L. Wu, Y. A. Liu, J. Y. Shen, S. L. Li, and C.
More informationCOPLANAR STRIPLINE (CPS) COMPONENTS. Previous Page. lower-frequency regions, without affecting the radiation pattern. 3. TRIANGULAR (BOWTIE) ANTENNAS
Previous Page 78 COPLANAR STRIPLINE (CPS) COMPONENTS Directivity gain (dbi) 8 6 4 4 lower-frequency regions, without affecting the radiation pattern. 3. TRIANGULAR (BOWTIE) ANTENNAS A triangular plate
More informationSolutions to Problems in Chapter 6
Appendix F Solutions to Problems in Chapter 6 F.1 Problem 6.1 Short-circuited transmission lines Section 6.2.1 (book page 193) describes the method to determine the overall length of the transmission line
More informationDUAL-BAND COMPOSITE RIGHT/LEFT-HANDED RING ANTENNA WITH LINEAR/CIRCULAR POLARIZATION CAPABILITY
DUAL-BAND COMPOSITE IGHT/LEFT-HANDED ING ANTENNA WITH LINEA/CICULA POLAIZATION CAPABILITY A. ennings (), S. Otto (), T. Liebig (), C. Caloz (), I. Wolff () () IMST GmbH, Carl-Friedrich-Gauß-Str., D-47475
More informationCAD modeling of coplanar waveguide (CPW) air-bridges
International Journal of Electronics, Vol. 92, No. 7, July 2005, 417 426 CAD modeling of coplanar waveguide (CPW) air-bridges NIHAD I. DIB*y and AMJAD A. OMARz ydepartment of Electrical Engineering, Jordan
More informationTransmission Line Basics II - Class 6
Transmission Line Basics II - Class 6 Prerequisite Reading assignment: CH2 Acknowledgements: Intel Bus Boot Camp: Michael Leddige Agenda 2 The Transmission Line Concept Transmission line equivalent circuits
More informationA UNEQUAL COUPLED-LINE WILKINSON POWER DI- VIDER FOR ARBITRARY TERMINATED IMPEDANCES
Progress In Electromagnetics Research, Vol. 117, 181 194, 211 A UNEQUAL COUPLED-LINE WILKINSON POWER DI- VIDER FOR ARBITRARY TERMINATED IMPEDANCES Y. Wu * and Y. Liu School of Electronic Engineering, Beijing
More informationAnalysis of Frequency Behavior of Microstrip Lines on Anisotropic Substrates with Slots in Ground Plane
18 Analysis of Frequency Behavior of Microstrip Lines on Anisotropic Substrates with Slots in Ground Plane Sachin Singh and Banmali S. Rawat* Department of Electrical Engineering University of Nevada,
More informationAN EQUIVALENT CIRCUIT FOR EMI PREDICTION IN PRINTED CIRCUIT BOARDS FEATURING A STRAIGHT-TO-BENT MICROSTRIP LINE COUPLING
Progress In Electromagnetics Research B, Vol. 5, 107 118, 2008 AN EQUIVALENT CIRCUIT FOR EMI PREDICTION IN PRINTED CIRCUIT BOARDS FEATURING A STRAIGHT-TO-BENT MICROSTRIP LINE COUPLING P. Bernardi and R.
More informationModeling of Signal and Power Integrity in System on Package Applications
Modeling of Signal and Power Integrity in System on Package Applications Madhavan Swaminathan and A. Ege Engin Packaging Research Center, School of Electrical and Computer Engineering, Georgia Institute
More informationEquivalent Circuit Model Extraction for Interconnects in 3D ICs
Equivalent Circuit Model Extraction for Interconnects in 3D ICs A. Ege Engin Assistant Professor, Department of ECE, San Diego State University Email: aengin@mail.sdsu.edu ASP-DAC, Jan. 23, 213 Outline
More informationExperiment 06 - Extraction of Transmission Line Parameters
ECE 451 Automated Microwave Measurements Laboratory Experiment 06 - Extraction of Transmission Line Parameters 1 Introduction With the increase in both speed and complexity of mordern circuits, modeling
More informationSPIN MATRIX EXPONENTIALS AND TRANSMISSION MATRICES*
25 SPIN MATRIX EXPONENTIALS AND TRANSMISSION MATRICES* BY L. YOUNG Stanford Research Institute Abstract. The three Pauli spin matrices
More informationANTENNAS and MICROWAVES ENGINEERING (650427)
Philadelphia University Faculty of Engineering Communication and Electronics Engineering ANTENNAS and MICROWAVES ENGINEERING (65427) Part 2 Dr. Omar R Daoud 1 General Considerations It is a two-port network
More informationand Ee = E ; 0 they are separated by a dielectric material having u = io-s S/m, µ, = µ, 0
602 CHAPTER 11 TRANSMISSION LINES 11.10 Two identical pulses each of magnitude 12 V and width 2 µs are incident at t = 0 on a lossless transmission line of length 400 m terminated with a load. If the two
More informationMicrowave Network Analysis
Prof. Dr. Mohammad Tariqul Islam titareq@gmail.my tariqul@ukm.edu.my Microwave Network Analysis 1 Text Book D.M. Pozar, Microwave engineering, 3 rd edition, 2005 by John-Wiley & Sons. Fawwaz T. ILABY,
More informationRobust magnon-photon coupling in a planar-geometry hybrid of. inverted split-ring resonator and YIG film
SUPPLEMENTARY MATERIALS Robust magnon-photon coupling in a planar-geometry hybrid of inverted split-ring resonator and YIG film Bianath Bhoi, Bosung Kim, Junhoe Kim, Young-Jun Cho and Sang-Koog Kim a)
More informationSupplementary Information
S1 Supplementary Information S2 Forward Backward Forward Backward Normalized to Normalized to Supplementary Figure 1 Maximum local field ratio and transmission coefficient. Maximum local field ratio (green
More informationTransmission lines. Shouri Chatterjee. October 22, 2014
Transmission lines Shouri Chatterjee October 22, 2014 The transmission line is a very commonly used distributed circuit: a pair of wires. Unfortunately, a pair of wires used to apply a time-varying voltage,
More informationINTRODUCTION TO TRANSMISSION LINES DR. FARID FARAHMAND FALL 2012
INTRODUCTION TO TRANSMISSION LINES DR. FARID FARAHMAND FALL 2012 http://www.empowermentresources.com/stop_cointelpro/electromagnetic_warfare.htm RF Design In RF circuits RF energy has to be transported
More informationIN order to characterize the
D E S G N F E A T U R E VERFY WAFER-PROBE REFERENCE PLANES FOR MMC TESTNG Three techniques for verification of planar calibration standards agree within ko.1 ps of electrical length. N order to characterize
More informationAccurate Modeling of Spiral Inductors on Silicon From Within Cadence Virtuoso using Planar EM Simulation. Agilent EEsof RFIC Seminar Spring 2004
Accurate Modeling of Spiral Inductors on Silicon From Within Cadence Virtuoso using Planar EM Simulation Agilent EEsof RFIC Seminar Spring Overview Spiral Inductor Models Availability & Limitations Momentum
More informationElectromagnetic Modeling and Signal Integrity Simulation of Power/Ground Networks in High Speed Digital Packages and Printed Circuit Boards
Electromagnetic Modeling and Signal Integrity Simulation of Power/Ground Networks in High Speed Digital Packages and Printed Circuit Boards Frank Y. Yuan Viewlogic Systems Group, Inc. 385 Del Norte Road
More informationElectromagnetic-Thermal Analysis Study Based on HFSS-ANSYS Link
Syracuse University SURFACE Electrical Engineering and Computer Science Technical Reports College of Engineering and Computer Science 5-9-2011 Electromagnetic-Thermal Analysis Study Based on HFSS-ANSYS
More informationCase Study: Parallel Coupled- Line Combline Filter
MICROWAVE AND RF DESIGN MICROWAVE AND RF DESIGN Case Study: Parallel Coupled- Line Combline Filter Presented by Michael Steer Reading: 6. 6.4 Index: CS_PCL_Filter Based on material in Microwave and RF
More informationIPC-TM-650 TEST METHODS MANUAL
ASSOCIATION CONNECTING ELECTRONICS INDUSTRIES 3000 Lakeside Drive, Suite 309S Bannockburn, IL 60015-1219 TEST METHODS MANUAL Number High Frequency Testing to Determine Permittivity and Loss Originating
More informationPaper V. Acoustic Radiation Losses in Busbars. J. Meltaus, S. S. Hong, and V. P. Plessky J. Meltaus, S. S. Hong, V. P. Plessky.
Paper V Acoustic Radiation Losses in Busbars J. Meltaus, S. S. Hong, and V. P. Plessky 2006 J. Meltaus, S. S. Hong, V. P. Plessky. V Report TKK-F-A848 Submitted to IEEE Transactions on Ultrasonics, Ferroelectrics,
More informationEffects from the Thin Metallic Substrate Sandwiched in Planar Multilayer Microstrip Lines
Progress In Electromagnetics Research Symposium 2006, Cambridge, USA, March 26-29 115 Effects from the Thin Metallic Substrate Sandwiched in Planar Multilayer Microstrip Lines L. Zhang and J. M. Song Iowa
More informationCoplanar Waveguides Loaded with Symmetric and Asymmetric MultiSection Stepped Impedance Resonators (SIRs): Modeling and Potential.
This is the accepted version of the following article: Su, Lijuan, et al. "Coplanar waveguides loaded with symmetric and asymmetric multisection stepped impedance resonators : modeling and potential applications"
More information3294 IEEE TRANSACTIONS ON MICROWAVE THEORY AND TECHNIQUES, VOL. 59, NO. 12, DECEMBER 2011
3294 IEEE TRANSACTIONS ON MICROWAVE THEORY AND TECHNIQUES, VOL. 59, NO. 12, DECEMBER 2011 A Rigorous Solution to the Low-Frequency Breakdown in Full-Wave Finite-Element-Based Analysis of General Problems
More informationSYNTHESIS OF MICROWAVE RESONATOR DIPLEX- ERS USING LINEAR FREQUENCY TRANSFORMATION AND OPTIMIZATION
Progress In Electromagnetics Research, Vol. 24, 44 4, 22 SYNTHESIS OF MICROWAVE RESONATOR DIPLEX- ERS USING LINEAR FREQUENCY TRANSFORMATION AND OPTIMIZATION R. Wang *, J. Xu, M.-Y. Wang, and Y.-L. Dong
More informationAdvancements in mm-wave On-Wafer Measurements: A Commercial Multi-Line TRL Calibration Author: Leonard Hayden Presenter: Gavin Fisher
Advancements in mm-wave On-Wafer Measurements: A Commercial Multi-Line TRL Calibration Author: Leonard Hayden Presenter: Gavin Fisher The title of this section is A Commercial Multi-Line TRL Calibration
More informationDetermining the effective electromagnetic properties of negative-refractive-index metamaterials from internal fields
Determining the effective electromagnetic properties of negative-refractive-index metamaterials from internal fields Bogdan-Ioan Popa* and Steven A. Cummer Department of Electrical and Computer Engineering,
More informationProgress In Electromagnetics Research M, Vol. 20, 73 80, 2011
Progress In Electromagnetics Research M, Vol. 20, 73 80, 2011 COPLANAR METAMATERIAL MICRO-RESONATOR S. Nemer 1, 2, *, B. Sauviac 1, B. Bayard 1, J. J. Rousseau 1, C. Nader 2, J. Bechara 2, and A. Khoury
More informationGeneralized network formulation for symmetric double-step waveguide discontinuities
INT. J. ELECTRONICS, 1989, VOL. 67, NO. 3, 427-435 Generalized network formulation for symmetric double-step waveguide discontinuities A. K. HAMIDt, I. R. CIRICt and M. HAMIDH The equivalence principle
More informationLecture 12. Microwave Networks and Scattering Parameters
Lecture Microwave Networs and cattering Parameters Optional Reading: teer ection 6.3 to 6.6 Pozar ection 4.3 ElecEng4FJ4 LECTURE : MICROWAE NETWORK AND -PARAMETER Microwave Networs: oltages and Currents
More informationApplication of EM- Simulators for Extraction of Line Parameters
Chapter - 2 Application of EM- Simulators for Extraction of Line Parameters 2. 1 Introduction The EM-simulators-2D, 2.5D and 3D, are powerful tools for the analysis of the planar transmission lines structure.
More informationModeling frequency-dependent conductor losses and dispersion in serial data channel interconnects
Modeling frequency-dependent conductor losses and dispersion in serial data channel interconnects Yuriy Shlepnev Simberian Inc., www.simberian.com Abstract: Models of transmission lines and transitions
More informationEfficiency and Bandwidth Improvement Using Metamaterial of Microstrip Patch Antenna
Efficiency and Bandwidth Improvement Using Metamaterial of Microstrip Patch Antenna Aakash Mithari 1, Uday Patil 2 1Student Department of Electronics Technology Engg., Shivaji University, Kolhapur, Maharashtra,
More informationMICROSTRIP NONUNIFORM IMPEDANCE RESONATORS
Progress In Electromagnetics Research, PIER 67, 329 339, 2007 MICROSTRIP NONUNIFORM IMPEDANCE RESONATORS M. Khalaj-Amirhosseini College of Electrical Engineering Iran University of Science and Technology
More informationOmar M. Ramahi University of Waterloo Waterloo, Ontario, Canada
Omar M. Ramahi University of Waterloo Waterloo, Ontario, Canada Traditional Material!! Electromagnetic Wave ε, μ r r The only properties an electromagnetic wave sees: 1. Electric permittivity, ε 2. Magnetic
More informationBoundary and Excitation Training February 2003
Boundary and Excitation Training February 2003 1 Why are They Critical? For most practical problems, the solution to Maxwell s equations requires a rigorous matrix approach such as the Finite Element Method
More informationELECTROMAGNETIC ENVIRONMENT GENERATED IN A TEM CELL FOR BIOLOGICAL DOSIMETRY APPLICATIONS
ISEF 2007 XIII International Symposium on Electromagnetic Fields in Mechatronics, Electrical and Electronic Engineering Prague, Czech Republic, September 13-15, 2007 ELECTROMAGNETIC ENVIRONMENT GENERATED
More informationAnalysis of Charge Distribution on Rectangular Microstrip Structures
Vol. 119 (2011) ACTA PHYSICA POLONICA A No. 4 Physical Aspects of Microwave and Radar Applications Analysis of Charge Distribution on Rectangular Microstrip Structures E. Metlevskis and V. Urbanavicius
More informationCausal Modeling and Extraction of Dielectric Constant and Loss Tangent for Thin Dielectrics
Causal Modeling and Extraction of Dielectric Constant and Loss Tangent for Thin Dielectrics A. Ege Engin 1, Abdemanaf Tambawala 1, Madhavan Swaminathan 1, Swapan Bhattacharya 1, Pranabes Pramanik 2, Kazuhiro
More informationMutual Couplings between EMI Filter Components
Mutual Couplings between EMI Filter Components G. Asmanis, D.Stepins, A. Asmanis Latvian Electronic Equipment Testing Centre Riga, Latvia asmanisgundars@inbox.lv, deniss.stepins@rtu.lv L. Ribickis, Institute
More informationUnderstanding EMC Basics
1of 7 series Webinar #1 of 3, February 27, 2013 EM field theory, and 3 types of EM analysis Webinar Sponsored by: EurIng CEng, FIET, Senior MIEEE, ACGI AR provides EMC solutions with our high power RF/Microwave
More informationTASK A. TRANSMISSION LINE AND DISCONTINUITIES
TASK A. TRANSMISSION LINE AND DISCONTINUITIES Task A. Transmission Line and Discontinuities... 1 A.I. TEM Transmission Line... A.I.1. Circuit Representation of a Uniform Transmission Line... A.I.. Time
More informationDIRECTIONAL COUPLERS
DIRECTIONAL COUPLERS Ing. rvargas@inictel.gob.pe INICTEL Abstract This paper analyzes two types of Directional Couplers. First, magnetic coupling between a transmission line and a secondary circuit is
More informationInternational Distinguished Lecturer Program
U 005-006 International Distinguished Lecturer Program Ken-ya Hashimoto Chiba University Sponsored by The Institute of Electrical and Electronics Engineers (IEEE) Ultrasonics, Ferroelectrics and Frequency
More informationUNIT I ELECTROSTATIC FIELDS
UNIT I ELECTROSTATIC FIELDS 1) Define electric potential and potential difference. 2) Name few applications of gauss law in electrostatics. 3) State point form of Ohm s Law. 4) State Divergence Theorem.
More informationConventional Paper I (a) (i) What are ferroelectric materials? What advantages do they have over conventional dielectric materials?
Conventional Paper I-03.(a) (i) What are ferroelectric materials? What advantages do they have over conventional dielectric materials? (ii) Give one example each of a dielectric and a ferroelectric material
More informationThe Effect of Cooling Systems on HTS Microstrip Antennas
PIERS ONLINE, VOL. 4, NO. 2, 28 176 The Effect of Cooling Systems on HTS Microstrip Antennas S. F. Liu 1 and S. D. Liu 2 1 Xidian University, Xi an 7171, China 2 Xi an Institute of Space Radio Technology,
More informationElectrodynamics and Microwaves 17. Stub Matching Technique in Transmission Lines
1 Module 17 Stub Matching Technique in Transmission Lines 1. Introduction 2. Concept of matching stub 3. Mathematical Basis for Single shunt stub matching 4.Designing of single stub using Smith chart 5.
More informationECE 497 JS Lecture -03 Transmission Lines
ECE 497 JS Lecture -03 Transmission Lines Spring 2004 Jose E. Schutt-Aine Electrical & Computer Engineering University of Illinois jose@emlab.uiuc.edu 1 MAXWELL S EQUATIONS B E = t Faraday s Law of Induction
More informationFinite Element Method Analysis of Symmetrical Coupled Microstrip Lines
International Journal of Computing and Digital Systems ISSN (20-142X) Int. J. Com. Dig. Sys. 3, No.3 (Sep-2014) Finite Element Method Analysis of Symmetrical Coupled Microstrip Lines Sarhan M. Musa and
More informationECE Spring Prof. David R. Jackson ECE Dept. Notes 6
ECE 6341 Spring 2016 Prof. David R. Jackson ECE Dept. Notes 6 1 Leaky Modes v TM 1 Mode SW 1 v= utan u ε R 2 R kh 0 n1 r = ( ) 1 u Splitting point ISW f = f s f > f s We will examine the solutions as the
More informationComparison of MLCC and X2Y Technology for Use in Decoupling Circuits
Comparison of MLCC and X2Y Technology for Use in Decoupling Circuits Dale L. Sanders James P. Muccioli Anthony A. Anthony X2Y Attenuators, LLC 37554 Hills Tech Dr. Farmington Hills, MI 48331 248-489-0007
More informationMicrostrip Antennas. Prof. Girish Kumar Electrical Engineering Department, IIT Bombay. (022)
Microstrip Antennas Prof. Girish Kumar Electrical Engineering Department, IIT Bombay gkumar@ee.iitb.ac.in (022) 2576 7436 Rectangular Microstrip Antenna (RMSA) Y Top View W x X L Side View r Ground plane
More informationPassive Coplanar Circulator with the Yig Thin Films
Passive Coplanar Circulator with the Yig Thin Films Rahmouna El-Bouslemti 1,1, Faouzi Salah-Belkhodja 1, 1 LTTNS Laboratory, Department of Electronic, University of Djillali Liabès, Sidi Bel Abbés, Algeria
More informationProgress In Electromagnetics Research C, Vol. 33, , 2012
Progress In Electromagnetics Research C, Vol. 33, 213 227, 2012 MAXIMUM BANDWIDTH PERFORMANCE FOR AN IDEAL LUMPED-ELEMENT CIRCULATOR H. Dong *, J. L. Young, J. R. Smith, and B. Aldecoa Department of Electrical
More informationMicrowave Network Analysis
Microwave Network Analysis S R Zinka zinka@hyderabadbits-pilaniacin Department of Electrical & Electronics Engineering BITS Pilani, Hyderbad Campus May 7, 2015 RF & Microwave Engineering, Dept of EEE,
More informationTopic 5: Transmission Lines
Topic 5: Transmission Lines Profs. Javier Ramos & Eduardo Morgado Academic year.13-.14 Concepts in this Chapter Mathematical Propagation Model for a guided transmission line Primary Parameters Secondary
More informationGHZ ELECTRICAL PROPERTIES OF CARBON NANOTUBES ON SILICON DIOXIDE MICRO BRIDGES
GHZ ELECTRICAL PROPERTIES OF CARBON NANOTUBES ON SILICON DIOXIDE MICRO BRIDGES SHENG F. YEN 1, HAROON LAIS 1, ZHEN YU 1, SHENGDONG LI 1, WILLIAM C. TANG 1,2, AND PETER J. BURKE 1,2 1 Electrical Engineering
More informationECE 107: Electromagnetism
ECE 107: Electromagnetism Set 2: Transmission lines Instructor: Prof. Vitaliy Lomakin Department of Electrical and Computer Engineering University of California, San Diego, CA 92093 1 Outline Transmission
More informationSupplementary Figure 1: SAW transducer equivalent circuit
Supplementary Figure : SAW transducer equivalent circuit Supplementary Figure : Radiation conductance and susceptance of.6um IDT, experiment & calculation Supplementary Figure 3: Calculated z-displacement
More informationA COMPACT PI-STRUCTURE DUAL BAND TRANSFORMER
Progress In Electromagnetics Research, PIER 88, 121 134, 2008 A COMPACT PI-STRUCTURE DUAL BAND TRANSFORMER Y. Wu, Y. Liu, and S. Li School of Electronic Engineering Beijing University of Posts and Telecommunications
More informationN. Sarikaya Department of Aircraft Electrical and Electronics Civil Aviation School Erciyes University Kayseri 38039, Turkey
Progress In Electromagnetics Research B, Vol. 6, 225 237, 2008 ADAPTIVE NEURO-FUZZY INFERENCE SYSTEM FOR THE COMPUTATION OF THE CHARACTERISTIC IMPEDANCE AND THE EFFECTIVE PERMITTIVITY OF THE MICRO-COPLANAR
More informationEfficient Calculation of Surface Impedance for Rectangular Conductors. Emre Tuncer and Dean P. Neikirk
Efficient Calculation of Surface Impedance for Rectangular Conductors Emre Tuncer and Dean P. Neikirk Electrical and Computer Engineering Department University of Texas at Austin Austin, Texas 78712 Abstract
More informationTransmission Line Basics
Transmission Line Basics Prof. Tzong-Lin Wu NTUEE 1 Outlines Transmission Lines in Planar structure. Key Parameters for Transmission Lines. Transmission Line Equations. Analysis Approach for Z and T d
More information