Microwave Filters
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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. -
Chapter 6 Two-Port Network Model
Chapter 6 Two-Port Network Model 6.1 Introduction In this chapter a two-port network model of an actuator will be briefly described. In Chapter 5, it was shown that an automated test setup using an active system can re- create various load impedances over a limited range of frequencies. This test set-up can therefore be used to automatically reproduce any load impedance condition (related to a possible application) and apply it to a test or sample actuator. It is then possible to collect characteristic data from the test actuator such as force, velocity, current and voltage. Those characteristics can then be used to help to determine whether the tested actuator is appropriate or not for the case simulated. However versatile and easy to use this test set-up may be, because of its limitations, there is some characteristic data it will not be able to provide. For this reason and the fact that it can save a lot of measurements, having a good linear actuator model can be of great use. Developed for transduction theory [29], the linear model presented in this chapter is 77 called a Two-Port Network model. The automated test set-up remains an essential complement for this model, as it will allow the development and verification of accuracy. This chapter will focus on the two-port network model of the 1_3 tube array actuator provided by MSI (Cf: Figure 5.5). 6.2 Theory of the Two–Port Network Model As a transducer converts energy from electrical to mechanical forms, and vice- versa, it can be modelled as a Two-Port Network that relates the electrical properties at one port to the mechanical properties at the other port. -
Analysis of Microwave Networks
! a b L • ! t • h ! 9/ a 9 ! a b • í { # $ C& $'' • L C& $') # * • L 9/ a 9 + ! a b • C& $' D * $' ! # * Open ended microstrip line V + , I + S Transmission line or waveguide V − , I − Port 1 Port Substrate Ground (a) (b) 9/ a 9 - ! a b • L b • Ç • ! +* C& $' C& $' C& $ ' # +* & 9/ a 9 ! a b • C& $' ! +* $' ù* # $ ' ò* # 9/ a 9 1 ! a b • C ) • L # ) # 9/ a 9 2 ! a b • { # b 9/ a 9 3 ! a b a w • L # 4!./57 #) 8 + 8 9/ a 9 9 ! a b • C& $' ! * $' # 9/ a 9 : ! a b • b L+) . 8 5 # • Ç + V = A V + BI V 1 2 2 V 1 1 I 2 = 0 V 2 = 0 V 2 I 1 = CV 2 + DI 2 I 2 9/ a 9 ; ! a b • !./5 $' C& $' { $' { $ ' [ 9/ a 9 ! a b • { • { 9/ a 9 + ! a b • [ 9/ a 9 - ! a b • C ) • #{ • L ) 9/ a 9 ! a b • í !./5 # 9/ a 9 1 ! a b • C& { +* 9/ a 9 2 ! a b • I • L 9/ a 9 3 ! a b # $ • t # ? • 5 @ 9a ? • L • ! # ) 9/ a 9 9 ! a b • { # ) 8 -
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] “…. -
Brief Study of Two Port Network and Its Parameters
© 2014 IJIRT | Volume 1 Issue 6 | ISSN : 2349-6002 Brief study of two port network and its parameters Rishabh Verma, Satya Prakash, Sneha Nivedita Abstract- this paper proposes the study of the various ports (of a two port network. in this case) types of parameters of two port network and different respectively. type of interconnections of two port networks. This The Z-parameter matrix for the two-port network is paper explains the parameters that are Z-, Y-, T-, T’-, probably the most common. In this case the h- and g-parameters and different types of relationship between the port currents, port voltages interconnections of two port networks. We will also discuss about their applications. and the Z-parameter matrix is given by: Index Terms- two port network, parameters, interconnections. where I. INTRODUCTION A two-port network (a kind of four-terminal network or quadripole) is an electrical network (circuit) or device with two pairs of terminals to connect to external circuits. Two For the general case of an N-port network, terminals constitute a port if the currents applied to them satisfy the essential requirement known as the port condition: the electric current entering one terminal must equal the current emerging from the The input impedance of a two-port network is given other terminal on the same port. The ports constitute by: interfaces where the network connects to other networks, the points where signals are applied or outputs are taken. In a two-port network, often port 1 where ZL is the impedance of the load connected to is considered the input port and port 2 is considered port two. -
Aperture-Coupled Stripline-To-Waveguide Transitions for Spatial Power Combining
ACES JOURNAL, VOL. 18, NO. 4, NOVEMBER 2003 33 Aperture-Coupled Stripline-to-Waveguide Transitions for Spatial Power Combining Chris W. Hicks∗, Alexander B. Yakovlev#,andMichaelB.Steer+ ∗Naval Air Systems Command, RF Sensors Division 4.5.5, Patuxent River, MD 20670 #Department of Electrical Engineering, The University of Mississippi, University, MS 38677-1848 +Department of Electrical and Computer Engineering, North Carolina State University, Raleigh, NC 27695-7914 Abstract power. However, tubes are bulky, costly, require high operating voltages, and have a short lifetime. As an A full-wave electromagnetic model is developed and alternative, solid-state devices offer several advantages verified for a waveguide transition consisting of slotted such as, lightweight, smaller size, wider bandwidths, rectangular waveguides coupled to a strip line. This and lower operating voltages. These advantages lead waveguide-based structure represents a portion of the to lower cost because systems can be constructed us- planar spatial power combining amplifier array. The ing planar fabrication techniques. However, as the fre- electromagnetic simulator is developed to analyze the quency increases, the output power of solid-state de- stripline-to-slot transitions operating in a waveguide- vices decreases due to their small physical size. There- based environment in the X-band. The simulator is fore, to achieve sizable power levels that compete with based on the method of moments (MoM) discretiza- those generated by vacuum tubes, several solid-state tion of the coupled system of integral equations with devices can be combined in an array. Conventional the piecewise sinusodial testing and basis functions in power combiners are effectively limited in the num- the electric and magnetic surface current density ex- ber of devices that can be combined. -
Lowpass Lumped-Element Coplanar Waveguide-To- Coplanar Stripline Transitions
LOWPASS LUMPED-ELEMENT COPLANAR WAVEGUIDE-TO- COPLANAR STRIPLINE TRANSITIONS Yo-Shen Lin1 and Chun Hsiung Chen2 1Department of Electrical Engineering, National Central University, Chungli 320, Taiwan, R.O.C. (email: [email protected]) 2Department of Electrical Engineering and Graduate Institute of Communication Engineering, National Taiwan University, Taipei 106, Taiwan, R.O.C. (email: [email protected]) ABSTRACT The lowpass coplanar waveguide-to-coplanar stripline transitions are proposed, using planar lumped-elements to realize the filter prototypes in the transition structures. The proposed transitions are very compact and can provide the combined functions of transition and filter. Simple equivalent-circuit models based on closed-form expressions are also established, from which the characteristics of various lowpass lumped-element transitions are investigated. INTRODUCTION Coplanar waveguide (CPW) and coplanar stripline (CPS) are widely used as building blocks in the design of uniplanar MMIC's [1]. To fully utilize the exclusive features of CPW and CPS, an effective interconnection between them is of crucial importance. This may allow the choice of different uniplanar line-based circuit elements in different parts of a system such that maximum circuit integration and optimal system performance may be accomplished. Various CPW-to-CPS transitions have been developed [2]-[7]. Most of these conventional transitions have bandpass behaviors [2]-[4]. The broadband transition [5] utilizing a slotline open structure has a lowpass frequency response but its insertion loss increases only gradually as the operating frequency increases. The ideally all-pass double-Y junction balun [2], in practice, also features a gradually increasing insertion loss with frequency. -
Classic Filters There Are 4 Classic Analogue Filter Types: Butterworth, Chebyshev, Elliptic and Bessel. There Is No Ideal Filter
Classic Filters There are 4 classic analogue filter types: Butterworth, Chebyshev, Elliptic and Bessel. There is no ideal filter; each filter is good in some areas but poor in others. • Butterworth: Flattest pass-band but a poor roll-off rate. • Chebyshev: Some pass-band ripple but a better (steeper) roll-off rate. • Elliptic: Some pass- and stop-band ripple but with the steepest roll-off rate. • Bessel: Worst roll-off rate of all four filters but the best phase response. Filters with a poor phase response will react poorly to a change in signal level. Butterworth The first, and probably best-known filter approximation is the Butterworth or maximally-flat response. It exhibits a nearly flat passband with no ripple. The rolloff is smooth and monotonic, with a low-pass or high- pass rolloff rate of 20 dB/decade (6 dB/octave) for every pole. Thus, a 5th-order Butterworth low-pass filter would have an attenuation rate of 100 dB for every factor of ten increase in frequency beyond the cutoff frequency. It has a reasonably good phase response. Figure 1 Butterworth Filter Chebyshev The Chebyshev response is a mathematical strategy for achieving a faster roll-off by allowing ripple in the frequency response. As the ripple increases (bad), the roll-off becomes sharper (good). The Chebyshev response is an optimal trade-off between these two parameters. Chebyshev filters where the ripple is only allowed in the passband are called type 1 filters. Chebyshev filters that have ripple only in the stopband are called type 2 filters , but are are seldom used. -
Introduction to Transmission Lines
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 ¤ Transmission lines ¤ Connectors ¨ As we transport energy energy gets lost ¤ Resistance of the wire à lossy cable ¤ Radiation (the energy radiates out of the wire à the wire is acting as an antenna We look at transmission lines and their characteristics Transmission Lines A transmission line connects a generator to a load – a two port network Transmission lines include (physical construction): • Two parallel wires • Coaxial cable • Microstrip line • Optical fiber • Waveguide (very high frequencies, very low loss, expensive) • etc. Types of Transmission Modes TEM (Transverse Electromagnetic): Electric and magnetic fields are orthogonal to one another, and both are orthogonal to direction of propagation Example of TEM Mode Electric Field E is radial Magnetic Field H is azimuthal Propagation is into the page Examples of Connectors Connectors include (physical construction): BNC UHF Type N Etc. Connectors and TLs must match! Transmission Line Effects Delayed by l/c At t = 0, and for f = 1 kHz , if: (1) l = 5 cm: (2) But if l = 20 km: Properties of Materials (constructive parameters) Remember: Homogenous medium is medium with constant properties ¨ Electric Permittivity ε (F/m) ¤ The higher it is, less E is induced, lower polarization ¤ For air: 8.85xE-12 F/m; ε = εo * εr ¨ Magnetic Permeability µ (H/m) Relative permittivity and permeability -
WAVEGUIDE ATTENUATORS : in Order to Control Power Levels in a Microwave System by Partially Absorbing the Transmitted Microwave Signal, Attenuators Are Employed
UNIT II MICROWAVE COMPONENTS Waveguide Attenuators- Resistive card, Rotary Vane types. Waveguide Phase Shifters : Dielectric, Rotary Vane types. Waveguide Multi port Junctions- E plane and H plane Tees, Magic Tee, Hybrid Ring. Directional Couplers- 2 hole, Bethe hole types. Ferrites-Composition and characteristics, Faraday Rotation. Ferrite components: Gyrator, Isolator, Circulator. S-matrix calculations for 2 port junction, E & H plane Tees, Magic Tee, Directional Coupler, Circulator and Isolator WAVEGUIDE ATTENUATORS : In order to control power levels in a microwave system by partially absorbing the transmitted microwave signal, attenuators are employed. Resistive films (dielectric glass slab coated with aquadag) are used in the design of both fixed and variable attenuators. A co-axial fixed attenuator uses the dielectric lossy material inside the centre conductor of the co-axial line to absorb some of the centre conductor microwave power propagating through it dielectric rod decides the amount of attenuation introduced. The microwave power absorbed by the lossy material is dissipated as heat. 1 In waveguides, the dielectric slab coated with aquadag is placed at the centre of the waveguide parallel to the maximum E-field for dominant TEIO mode. Induced current on the lossy material due to incoming microwave signal, results in power dissipation, leading to attenuation of the signal. The dielectric slab is tapered at both ends upto a length of more than half wavelength to reduce reflections as shown in figure 5.7. The dielectric slab may be made movable along the breadth of the waveguide by supporting it with two dielectric rods separated by an odd multiple of quarter guide wavelength and perpendicular to electric field. -
The Stripline Circulator Theory and Practice
The Stripline Circulator Theory and Practice By J. HELSZAJN The Stripline Circulator The Stripline Circulator Theory and Practice By J. HELSZAJN Copyright # 2008 by John Wiley & Sons, Inc. All rights reserved Published by John Wiley & Sons, Inc. Published simultaneously in Canada No part of this publication may be reproduced, stored in a retrieval system, or transmitted in any form or by any means, electronic, mechanical, photocopying, recording, scanning, or otherwise, except as permitted under Section 107 or 108 of the 1976 United States Copyright Act, without either the prior written permission of the Publisher, or authorization through payment of the appropriate per-copy fee to the Copyright Clearance Center, Inc., 222 Rosewood Drive, Danvers, MA 01923, (978) 750-8400, fax (978) 750-4470, or on the web at www.copyright.com. Requests to the Publisher for permission should be addressed to the Permissions Department, John Wiley & Sons, Inc., 111 River Street, Hoboken, NJ 07030, (201) 748-6011, fax (201) 748-6008, or online at http:// www.wiley.com/go/permission. Limit of Liability/Disclaimer of Warranty: While the publisher and author have used their best efforts in preparing this book, they make no representations or warranties with respect to the accuracy or completeness of the contents of this book and specifically disclaim any implied warranties of merchantability or fitness for a particular purpose. No warranty may be created or extended by sales representatives or written sales materials. The advice and strategies contained herein may not be suitable for your situation. You should consult with a professional where appropriate. Neither the publisher nor author shall be liable for any loss of profit or any other commercial damages, including but not limited to special, incidental, consequential, or other damages. -
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Lumped-element Sections for Modeling Coupling Between High-Speed Digital and I/O Lines W. Cui, H. Shi, X. Luo, F. Sha*, J.L. Drewniak, T.P. Van Doren and T. Anderson** ElectromagneticCompatibility Laboratory University of Missouri-Rolla Rolla, MCI 65401 * Northern Jiao Tong University EMC ResearchSection Beijing 100044,P.R.China * * HP-EEsof Division Hewlett-PackardCo. SantaRosa, CA 95403 Abstract: Lumped-elementsections are used for modeling designstage to estimateEM1 and minimize the noise coupling coupling betweenhigh-speed digital and I/O lines on printed to I/O lines on the PCB. As digital designs become more circuit boards (PCBs) in this paper. Radiatedelectromagnetic dense, flexibility in trace routing is reduced. Adherence to interference(EMI) is investigatedwhen the I/O line going off simple design maxims for avoiding adjacent segmentsof an the board is driven as an unintentional, but effective antenna. I/O line and a high-speeddigital line becomesmore difficult. Simulated results are compared with measurementsfor A meansfor estimatingEM1 at the design stageis desirableto coupled lines. A suitable number of lumped-elementsections maintainrouting flexibility while minimizing EM1 risk. for modeling is chosen based on the line length and the highestfrequency of interest. The three essentialcomponents for estimating EM1 resulting from coupling to I/O lines are suitable sourceand load models, a coupled transmission-line model, and an EM1 antenna I. INTR~DUC~~N model. Of particular interest at this stage are models for the coupled transmission lines, and the EM1 antenna. Two As the speed of digital designs continues to increase, approaches have been previously pursued for modeling unintentionalradiation from cablesattached to PCBs becomes coupled transmission-lines.One technique is to decouple the problematic.For clock speedsless than 50 MHz, a typical 1 m lines in the frequency domain by modal decomposition [l].