Planar Transmission Line Method for Char- Acterization of Printed Circuit Board Di- Electrics
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Design and Analysis of Band Pass Filter for Wireless Communication Viswavardhan Reddy
Volume III, Issue VI, June 2014 IJLTEMAS ISSN 2278 - 2540 Design and Analysis of Band Pass Filter for Wireless Communication Viswavardhan Reddy. K1, Mausumi Dutta2, Maumita Dutta3 1,2Department of Telecommunication Engineering, RV College of Engineering, Bangalore - 560059 [email protected], [email protected],[email protected] Abstract— There are applications in wireless communications, where a particular band of frequencies are needed to be filtered full sections can be used to increase the filter roll-off factor. from a wider range of mixed signals. Filter circuits can be Method [4] includes equal-ripple and maximally flat passband designed to accomplish this task by combining the properties of filters with general stopbands, as well as equal-ripple low-pass filter and high-pass filter into a single filter which is stopband filters with general passbands. To solve the referred as band-pass filter. A band-pass filter works to screen out frequencies that are too low or too high, giving easy passage approximation problem and to improve numerical only to certain frequencies within a specific range. At high conditioning, the design is carried out exclusively in terms of frequencies, the behavior of the discrete components changes. one or two transformed frequency variables. Hence discrete components are replaced by microstrip transmission lines. Microstrip transmission line is the most used II. LITERATURE SURVEY planar transmission line in Radio Frequency (RF) applications. A microstrip transmission line consists of a thin conductor strip The concept of coupling coefficients has been a very useful over a dielectric substrate along with a ground plate at the one in the design of small-to-moderate bandwidth microwave bottom of the dielectric. -
Development of Planar Microstrip Resonators for Electron Spin Resonance Spectroscopy 2 Per Cladding Is Present on Either Side of the Substrate
Development of planar microstrip resonators for electron spin resonance spectroscopy Preprint, compiled April 2, 2020 Subhadip Roy1, a, Sagnik Saha1, a, Jit Sarkar1, and Chiranjib Mitra1 1Department of Physical Sciences, Indian Institute of Science Education And Research Kolkata,India. Abstract This work focuses on the development of planar microwave resonators which are to be used in electron spin resonance spectroscopic studies. Two half wavelength microstrip resonators of different geometrical shapes, namely straight ribbon and omega, are fabricated on commercially available copper clad microwave laminates. Both resonators have a characteristic impedance of 50 Ω.We have performed electromagnetic field simulations for the two microstrip resonators and have extracted practical design parameters which were used for fabrica- tion. The effect of the geometry of the resonators on the quasi-transverse electromagnetic (quasi-TEM) modes of the resonators is noted from simulation results. The fabrication is done using optical lithography technique in which laser printed photomasks are used. This rapid prototyping technique allows us to fabricate resonators in a few hours with accuracy up to 6 mils. The resonators are characterized using a Vector Network Analyzer. The fabricated resonators are used to standardize a home built low-temperature continuous wave electron spin resonance (CW-ESR) spectrometer which operates in S-band, by capturing the absorption spectrum of the free radical DPPH, at both room temperature and 77 K. The measured value of g-factor using our resonators is consistent with the values reported in literature. The designed half wavelength planar resonators will be even- tually used in setting up a pulsed electron spin resonance spectrometer by suitably modifying the CW-ESR spectrometer. -
Equivalent-Circuit Models for Split-Ring Resonators And
IEEE TRANSACTIONS ON MICROWAVE THEORY AND TECHNIQUES, VOL. 53, NO. 4, APRIL 2005 1451 Equivalent-Circuit Models for Split-Ring Resonators and Complementary Split-Ring Resonators Coupled to Planar Transmission Lines Juan Domingo Baena, Jordi Bonache, Ferran Martín, Ricardo Marqués Sillero, Member, IEEE, Francisco Falcone, Txema Lopetegi, Member, IEEE, Miguel A. G. Laso, Member, IEEE, Joan García–García, Ignacio Gil, Maria Flores Portillo, and Mario Sorolla, Senior Member, IEEE Abstract—In this paper, a new approach for the development expected for left-handed metamaterials (LHMs); namely, inver- of planar metamaterial structures is developed. For this pur- sion of the Snell law, inversion of the Doppler effect, and back- pose, split-ring resonators (SRRs) and complementary split-ring ward Cherenkov radiation. It is also worth mentioning the con- resonators (CSRRs) coupled to planar transmission lines are investigated. The electromagnetic behavior of these elements, as troversy originated four years ago from the paper published by well as their coupling to the host transmission line, are studied, Pendry [2], where amplification of evanescent waves in LHMs and analytical equivalent-circuit models are proposed for the is pointed out [3]–[6]. isolated and coupled SRRs/CSRRs. From these models, the In spite of these interesting properties, it was not until 2000 stopband/passband characteristics of the analyzed SRR/CSRR that the first experimental evidence of left-handedness was loaded transmission lines are derived. It is shown that, in the long wavelength limit, these stopbands/passbands can be interpreted as demonstrated [7]. Following this seminal paper, other artifi- due to the presence of negative/positive values for the effective cially fabricated structures exhibiting a left-handed behavior and of the line. -
Basic PCB Material Electrical and Thermal Properties for Design Introduction
1 Basic PCB material electrical and thermal properties for design Introduction: In order to design PCBs intelligently it becomes important to understand, among other things, the electrical properties of the board material. This brief paper is an attempt to outline these key properties and offer some descriptions of these parameters. Parameters: The basic ( and almost indispensable) parameters for PCB materials are listed below and further described in the treatment that follows. dk, laminate dielectric constant df, dissipation factor Dielectric loss Conductor loss Thermal effects Frequency performance dk: Use the design dk value which is assumed to be more pertinent to design. Determines such things as impedances and the physical dimensions of microstrip circuits. A reasonable accurate practical formula for the effective dielectric constant derived from the dielectric constant of the material is: -1/2 εeff = [ ( εr +1)/2] + [ ( εr -1)/2][1+ (12.h/W)] Here h = thickness of PCB material W = width of the trace εeff = effective dielectric constant εr = dielectric constant of pcb material df: The dissipation factor (df) is a measure of loss-rate of energy of a mode of oscillation in a dissipative system. It is the reciprocal of quality factor Q, which represents the Signal Processing Group Inc., technical memorandum. Website: http://www.signalpro.biz. Signal Processing Gtroup Inc., designs, develops and manufactures analog and wireless ASICs and modules using state of the art semiconductor, PCB and packaging technologies. For a free no obligation quote on your product please send your requirements to us via email at [email protected] or through the Contact item on the website. -
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. -
Agilent Basics of Measuring the Dielectric Properties of Materials
Agilent Basics of Measuring the Dielectric Properties of Materials Application Note Contents Introduction ..............................................................................................3 Dielectric theory .....................................................................................4 Dielectric Constant............................................................................4 Permeability........................................................................................7 Electromagnetic propagation .................................................................8 Dielectric mechanisms ........................................................................10 Orientation (dipolar) polarization ................................................11 Electronic and atomic polarization ..............................................11 Relaxation time ................................................................................12 Debye Relation .................................................................................12 Cole-Cole diagram............................................................................13 Ionic conductivity ............................................................................13 Interfacial or space charge polarization..................................... 14 Measurement Systems .........................................................................15 Network analyzers ..........................................................................15 Impedance analyzers and LCR meters.........................................16 -
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. -
Application Note: ESR Losses in Ceramic Capacitors by Richard Fiore, Director of RF Applications Engineering American Technical Ceramics
Application Note: ESR Losses In Ceramic Capacitors by Richard Fiore, Director of RF Applications Engineering American Technical Ceramics AMERICAN TECHNICAL CERAMICS ATC North America ATC Europe ATC Asia [email protected] [email protected] [email protected] www.atceramics.com ATC 001-923 Rev. D; 4/07 ESR LOSSES IN CERAMIC CAPACITORS In the world of RF ceramic chip capacitors, Equivalent Series Resistance (ESR) is often considered to be the single most important parameter in selecting the product to fit the application. ESR, typically expressed in milliohms, is the summation of all losses resulting from dielectric (Rsd) and metal elements (Rsm) of the capacitor, (ESR = Rsd+Rsm). Assessing how these losses affect circuit performance is essential when utilizing ceramic capacitors in virtually all RF designs. Advantage of Low Loss RF Capacitors Ceramics capacitors utilized in MRI imaging coils must exhibit Selecting low loss (ultra low ESR) chip capacitors is an important ultra low loss. These capacitors are used in conjunction with an consideration for virtually all RF circuit designs. Some examples of MRI coil in a tuned circuit configuration. Since the signals being the advantages are listed below for several application types. detected by an MRI scanner are extremely small, the losses of the Extended battery life is possible when using low loss capacitors in coil circuit must be kept very low, usually in the order of a few applications such as source bypassing and drain coupling in the milliohms. Excessive ESR losses will degrade the resolution of the final power amplifier stage of a handheld portable transmitter image unless steps are taken to reduce these losses. -
Dielectric Loss
Dielectric Loss - εr is static dielectric constant (result of polarization under dc conditions). Under ac conditions, the dielectric constant is different from the above as energy losses have to be taken into account. - Thermal agitation tries to randomize the dipole orientations. Hence dipole moments cannot react instantaneously to changes in the applied field Æ losses. - The absorption of electrical energy by a dielectric material that is subjected to an alternating electric field is termed dielectric loss. - In general, the dielectric constant εr is a complex number given by where, εr’ is the real part and εr’’ is the imaginary part. Dept of ECE, National University of Singapore Chunxiang Zhu Dielectric Loss - Consider parallel plate capacitor with lossy dielectric - Impedance of the circuit - Thus, admittance (Y=1/Z) given by Dept of ECE, National University of Singapore Chunxiang Zhu Dielectric Loss - The admittance can be written in the form The admittance of the dielectric medium is equivalent to a parallel combination of - Note: compared to parallel an ideal lossless capacitor C’ with a resistance formula. relative permittivity εr’ and a resistance of 1/Gp or conductance Gp. Dept of ECE, National University of Singapore Chunxiang Zhu Dielectric Loss - Input power: - Real part εr’ represents the relative permittivity (static dielectric contribution) in capacitance calculation; imaginary part εr’’ represents the energy loss in dielectric medium. - Loss tangent: defined as represents how lossy the material is for ac signals. Dept of ECE, National University of Singapore Chunxiang Zhu Dielectric Loss The dielectric loss per unit volume: Dept of ECE, National University of Singapore Chunxiang Zhu Dielectric Loss - Note that the power loss is a function of ω, E and tanδ. -
A Comprehensive Guide to Selecting the Right Capacitor for Your Specific Application
CAPACITOR FUNDAMENTALS EBOOK A Comprehensive Guide to Selecting the Right Capacitor for Your Specific Application 2777 Hwy 20 (315) 655-8710 [email protected] Cazenovia, NY 13035 knowlescapacitors.com CAPACITOR FUNDAMENTALS EBOOK TABLE OF CONTENTS Introduction .................................. 2 The Key Principles of Capacitance and How a Basic Capacitor Works .............................. 3 How Capacitors are Most Frequently Used in Electronic Circuits ............................. 6 Factors Affecting Capacitance .................. 9 Defining Dielectric Polarization .................. 11 Dielectric Properties ........................... 15 Characteristics of Ferroelectric Ceramics ......................... 19 Characteristics of Linear Dielectrics .............. 22 Dielectric Classification ......................... 24 Test Parameters and Electrical Properties .......... 27 Industry Test Standards Overview. 32 High Reliability Testing .......................... 34 Visual Standards For Chip Capacitors ............. 37 Chip Attachment and Termination Guidelines ...... 42 Dissipation Factor and Capacitive Reactance ..... 49 Selecting the Right Capacitor for Your Specific Application Needs ............................ 51 1 CAPACITOR FUNDAMENTALS EBOOK INTRODUCTION At Knowles Precision Devices, our expertise in capacitor technology helps developers working on some of the world’s most demanding applications across the medical device, military and aerospace, telecommunications, and automotive industries. Thus, we brought together our top engineers -
United States Patent (19) 11 Patent Number: 4,503,404 Racy 45) Date of Patent: Mar
United States Patent (19) 11 Patent Number: 4,503,404 Racy 45) Date of Patent: Mar. 5, 1985 54 PRIMED MICROWAVE OSCILLATOR cludes a single tank conductor (16) coupled to a cou 75 Inventor: Joseph E. Racy, Hudson, N.H. pling conductor (17) by an interdigitated coupler (26). The coupling conductor (17) is connected to the cath 73 Assignee: Sanders Associates, Inc., Nashua, ode of an IMPATT diode (22) which is triggered by the N.H. application of a back-biasing trigger pulse that biases it 21 Appl. No.: 473,173 into its negative-resistance region. When a keying pulse is applied to the IMPATT diode (22), the diode couples 22 Filed: Mar. 7, 1983 power through the interdigitated coupler (26) to the 51) Int. Cl. .......................... H03B5/00; H03B 7/00 tank circuit (16) to cause oscillations that are initially in 52 U.S. Cl. ............................... 331/96; 331/107 SL; phase with any incoming signals, but the frequency of 331/107 G; 330/287 the oscillations is determined by the configuration of 58 Field of Search ................. 331/55, 56, 96, 107 G, the tank circuit (16), not by the frequency of the incom 331/107 DP, 107 SL, 173; 330/286, 287 ing signal. If the incoming signal is near enough to the 56) References Cited resonant frequency, and if the duration of the keying pulses is short enough, the output of the primed oscilla U.S. PATENT DOCUMENTS tor appears to a band-limited receiver to be an amplified 4,056,784 11/1977 Cohn ................................... 330/287 version of the input signal. -
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.