On a Class of Low-Reflection Transmission-Line Quasi- Gaussian Low-Pass Filters and Their Lumped-Element Approximations
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
MPA15-16 a Baseband Pulse Shaping Filter for Gaussian Minimum Shift Keying
A BASEBAND PULSE SHAPING FILTER FOR GAUSSIAN MINIMUM SHIFT KEYING 1 2 3 3 N. Krishnapura , S. Pavan , C. Mathiazhagan ,B.Ramamurthi 1 Department of Electrical Engineering, Columbia University, New York, NY 10027, USA 2 Texas Instruments, Edison, NJ 08837, USA 3 Department of Electrical Engineering, Indian Institute of Technology, Chennai, 600036, India Email: [email protected] measurement results. ABSTRACT A quadrature mo dulation scheme to realize the Gaussian pulse shaping is used in digital commu- same function as Fig. 1 can be derived. In this pap er, nication systems like DECT, GSM, WLAN to min- we consider only the scheme shown in Fig. 1. imize the out of band sp ectral energy. The base- band rectangular pulse stream is passed through a 2. GAUSSIAN FREQUENCY SHIFT lter with a Gaussian impulse resp onse b efore fre- KEYING GFSK quency mo dulating the carrier. Traditionally this The output of the system shown in Fig. 1 can b e describ ed is done by storing the values of the pulse shap e by in a ROM and converting it to an analog wave- Z t form with a DAC followed by a smo othing lter. g d 1 y t = cos 2f t +2k c f This pap er explores a fully analog implementation 1 of an integrated Gaussian pulse shap er, which can where f is the unmo dulated carrier frequency, k is the c f result in a reduced power consumption and chip mo dulating index k =0:25 for Gaussian Minimum Shift f area. Keying|GMSK[1] and g denotes the convolution of the rectangular bit stream bt with values in f1; 1g 1. -
Advanced Electronic Systems Damien Prêle
Advanced Electronic Systems Damien Prêle To cite this version: Damien Prêle. Advanced Electronic Systems . Master. Advanced Electronic Systems, Hanoi, Vietnam. 2016, pp.140. cel-00843641v5 HAL Id: cel-00843641 https://cel.archives-ouvertes.fr/cel-00843641v5 Submitted on 18 Nov 2016 (v5), last revised 26 May 2021 (v8) HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. advanced electronic systems ST 11.7 - Master SPACE & AERONAUTICS University of Science and Technology of Hanoi Paris Diderot University Lectures, tutorials and labs 2016-2017 Damien PRÊLE [email protected] Contents I Filters 7 1 Filters 9 1.1 Introduction . .9 1.2 Filter parameters . .9 1.2.1 Voltage transfer function . .9 1.2.2 S plane (Laplace domain) . 11 1.2.3 Bode plot (Fourier domain) . 12 1.3 Cascading filter stages . 16 1.3.1 Polynomial equations . 17 1.3.2 Filter Tables . 20 1.3.3 The use of filter tables . 22 1.3.4 Conversion from low-pass filter . 23 1.4 Filter synthesis . 25 1.4.1 Sallen-Key topology . 25 1.5 Amplitude responses . 28 1.5.1 Filter specifications . 28 1.5.2 Amplitude response curves . -
CHAPTER 3 ADC and DAC
CHAPTER 3 ADC and DAC Most of the signals directly encountered in science and engineering are continuous: light intensity that changes with distance; voltage that varies over time; a chemical reaction rate that depends on temperature, etc. Analog-to-Digital Conversion (ADC) and Digital-to-Analog Conversion (DAC) are the processes that allow digital computers to interact with these everyday signals. Digital information is different from its continuous counterpart in two important respects: it is sampled, and it is quantized. Both of these restrict how much information a digital signal can contain. This chapter is about information management: understanding what information you need to retain, and what information you can afford to lose. In turn, this dictates the selection of the sampling frequency, number of bits, and type of analog filtering needed for converting between the analog and digital realms. Quantization First, a bit of trivia. As you know, it is a digital computer, not a digit computer. The information processed is called digital data, not digit data. Why then, is analog-to-digital conversion generally called: digitize and digitization, rather than digitalize and digitalization? The answer is nothing you would expect. When electronics got around to inventing digital techniques, the preferred names had already been snatched up by the medical community nearly a century before. Digitalize and digitalization mean to administer the heart stimulant digitalis. Figure 3-1 shows the electronic waveforms of a typical analog-to-digital conversion. Figure (a) is the analog signal to be digitized. As shown by the labels on the graph, this signal is a voltage that varies over time. -
Whiguqzgdrjracxb.Pdf
Analog Filters Using MATLAB Lars Wanhammar Analog Filters Using MATLAB 13 Lars Wanhammar Department of Electrical Engineering Division of Electronics Systems Linkoping¨ University SE-581 83 Linkoping¨ Sweden [email protected] ISBN 978-0-387-92766-4 e-ISBN 978-0-387-92767-1 DOI 10.1007/978-0-387-92767-1 Springer Dordrecht Heidelberg London New York Library of Congress Control Number: 2008942084 # Springer ScienceþBusiness Media, LLC 2009 All rights reserved. This work may not be translated or copied in whole or in part without the written permission of the publisher (Springer ScienceþBusiness Media, LLC, 233 Spring Street, New York, NY 10013, USA), except for brief excerpts in connection with reviews or scholarly analysis. Use in connection with any form of information storage and retrieval, electronic adaptation, computer software, or by similar or dissimilar methodology now known or hereafter developed is forbidden. The use in this publication of trade names, trademarks, service marks, and similar terms, even if they are not identified as such, is not to be taken as an expression of opinion as to whether or not they are subject to proprietary rights. Printed on acid-free paper Springer is part of Springer ScienceþBusiness Media (www.springer.com) Preface This book was written for use in a course at Linkoping¨ University and to aid the electrical engineer to understand and design analog filters. Most of the advanced mathematics required for the synthesis of analog filters has been avoided by providing a set of MATLAB functions that allows sophisticated filters to be designed. Most of these functions can easily be converted to run under Octave as well. -
Loudspeaker Parameters
Loudspeaker Parameters D. G. Meyer School of Electrical & Computer Engineering Outline • Review of How Loudspeakers Work • Small Signal Loudspeaker Parameters • Effect of Loudspeaker Cable • Sample Loudspeaker • Electrical Power Needed • Sealed Box Design Example How Loudspeakers Work How Loudspeakers Are Made Fundamental Small Signal Mechanical Parameters 2 • Sd – projected area of driver diaphragm (m ) • Mms – mass of diaphragm (kg) • Cms – compliance of driver’s suspension (m/N) • Rms – mechanical resistance of driver’s suspension (N•s/m) • Le – voice coil inductance (mH) • Re – DC resistance of voice coil ( Ω) • Bl – product of magnetic field strength in voice coil gap and length of wire in magnetic field (T•m) Small Signal Parameters These values can be determined by measuring the input impedance of the driver, near the resonance frequency, at small input levels for which the mechanical behavior of the driver is effectively linear. • Fs – (free air) resonance frequency of driver (Hz) – frequency at which the combination of the energy stored in the moving mass and suspension compliance is maximum, which results in maximum cone velocity – usually it is less efficient to produce output frequencies below F s – input signals significantly below F s can result in large excursions – typical factory tolerance for F s spec is ±15% Measurement of Loudspeaker Free-Air Resonance Small Signal Parameters These values can be determined by measuring the input impedance of the driver, near the resonance frequency, at small input levels for which the -
Characteristic Impedance of Lines on Printed Boards by TDR 03/04
Number 2.5.5.7 ASSOCIATION CONNECTING Subject ELECTRONICS INDUSTRIES ® Characteristic Impedance of Lines on Printed 2215 Sanders Road Boards by TDR Northbrook, IL 60062-6135 Date Revision 03/04 A IPC-TM-650 Originating Task Group TEST METHODS MANUAL TDR Test Method Task Group (D-24a) 1 Scope This document describes time domain reflectom- b. The value of characteristic impedance obtained from TDR etry (TDR) methods for measuring and calculating the charac- measurements is traceable to a national metrology insti- teristic impedance, Z0, of a transmission line on a printed cir- tute, such as the National Institute of Standards and Tech- cuit board (PCB). In TDR, a signal, usually a step pulse, is nology (NIST), through coaxial air line standards. The char- injected onto a transmission line and the Z0 of the transmis- acteristic impedance of these transmission line standards sion line is determined from the amplitude of the pulse is calculated from their measured dimensional and material reflected at the TDR/transmission line interface. The incident parameters. step and the time delayed reflected step are superimposed at the point of measurement to produce a voltage versus time c. A variety of methods for TDR measurements each have waveform. This waveform is the TDR waveform and contains different accuracies and repeatabilities. information on the Z0 of the transmission line connected to the d. If the nominal impedance of the line(s) being measured is TDR unit. significantly different from the nominal impedance of the Note: The signals used in the TDR system are actually rect- measurement system (typically 50 Ω), the accuracy and angular pulses but, because the duration of the TDR wave- repeatability of the measured numerical valued will be form is much less than pulse duration, the TDR pulse appears degraded. -
Unit – I Filters
EC6503 Transmission lines and Waveguides Department of ECE 2018 - 2019 EC6503 TRANSMISSION LINES AND WAVEGUIDES UNIT –I TRANSMISSION LINE THEORY PART A - C303.1 1. Distinguish lumped parameters and distributed parameters. Lumped parameters are individually concentrated or lumped at discrete points in the circuit and can be identified definitely as representing a particular parameter. Distributed parameters are distributed along the circuit, each elemental length of the circuit having its own values and concentration of the individual parameters is not possible. 2. What are the different types of transmission lines? The different types of transmission lines are 1.Open wire line 2. Cable 3. Coaxial line 4. Waveguide 3. Describe the different parameters of a transmission line. (1)The parameters include resistance, which is uniformly distributed along the length of the conductors. Since current will be present, the conductors will be surrounded and linked by magnetic flux, and this phenomena will demonstrate its effect in distributed inductance along the line.(2)The conductors are separated by insulating dielectric, so that capacitance will be distributed along the conductor length.(3)The dielectric or the insulators of the open wire line may not be perfect, a leakage current will flow, and leakage conductance will exist between the conductors. 4. Give the general equations of a transmission line. The general equations are, E = ERcosh√ZY s + IRZosinh √ZY s I = IRcosh√ZY s + ( ER / Zo ) sinh √ZY s where Z= R + jωL = series impedance, ohms per unit length of line and Y = G + j ωC = shunt admittance, mhos per unit length of line. 5. -
1.1 Transmission Line Basic Concepts: Introduction to Narrow-Band Matching Networks
European Master of Research on Information Technology Design and Analysis of RF and Microwave Systems 1.1 Transmission line basic concepts: Introduction to narrow-band matching networks March 2010 Francesc Torres, Lluís Pradell, Jorge Miranda European Master of Research on Information Technology Design and Analysis of RF and Microwave Systems Voltage and current in the transmission line V For any lossless transmission line: L IL V (z) V (z) V (z) V(z V+(z) Z ≠ Z 1 Z0 I(z) - L 0 I(z) V (z) V (z) V (z) Z0 -z z=0 where At z=0 Periodicity of V(z) and I(z): wavelength jz (z z) z n2 , z n2 V (z) V0 e V (0) V0 V0 VL 1 jz I(0) V V I 2 V (z) V0 e Z L z n n 0 Impedance: load Reflection coefficient: load V V V V V 1 V Z Z Z L Z Z L Z L L 0 L 0 0 0 L I L V V V LV 1 L V Z L Z0 1 European Master of Research on Information Technology Design and Analysis of RF and Microwave Systems Reflection coefficient in the transmission line At any point z of the transmission line the impedance is computed as: V (z) 1 (z) Z(z) Z0 Z(z) Z0 (z) Z0 I(z) 1 (z) Z(z) Z0 At any point z of the transmission line the reflection coefficient is: V (z) V 2 jz 2 jz 2 jz (z) e (0)e Le V (z) V 2 jz Modulus (z) Le L Constant in z 180º 2z rad 2z deg Phase 2z 2 (z z) n2 , 2z n2 Linear n n Increasing with +z (towards load) z n Periodicity: half a wavelength 2 2 European Master of Research on Information Technology Design and Analysis of RF and Microwave Systems The transmission line as impedance transformer () L 2 j (z) L 2 jz Z0, β ZL≠ Z0 |Γ(z) |=|ΓL| i () z z=0 Example: Compute the input impedance Zi of a circuit formed by a transmission line of length is λ/8 and loaded with ZL=0 (sc). -
521Fmelectronic 1..14
Radio-Frequency and Microwave Communication Circuits: Analysis and Design Devendra K. Misra Copyright # 2001 John Wiley & Sons, Inc. ISBNs: 0-471-41253-8 (Hardback); 0-471-22435-9 (Electronic) RADIO-FREQUENCY AND MICROWAVE COMMUNICATION CIRCUITS RADIO-FREQUENCY AND MICROWAVE COMMUNICATION CIRCUITS ANALYSIS AND DESIGN DEVENDRA K. MISRA A WILEY±INTERSCIENCE PUBLICATION JOHN WILEY & SONS, INC. New York Chichester Weinheim Brisbane Singapore Toronto Designations used by companies to distinguish their products are often claimed as trademarks. In all instances where John Wiley & Sons, Inc., is aware of a claim, the product names appear in initial capital or ALL CAPITAL LETTERS. Readers, however, should contact the appropriate companies for more complete information regarding trademarks and registration. Copyright # 2001 by John Wiley & Sons, Inc. All rights reserved. No part of this publication may be reproduced, stored in a retrieval system or transmitted in any form or by any means, electronic or mechanical, including uploading, downloading, printing, decompiling, recording or otherwise, except as permitted under Sections 107 or 108 of the 1976 United States Copyright Act, without the prior written permission of the Publisher. Requests to the Publisher for permission should be addressed to the Permissions Department, John Wiley & Sons, Inc., 605 Third Avenue, New York, NY 10158-0012, (212) 850-6011, fax (212) 850-6008, E-Mail: PERMREQ@ WILEY.COM. This publication is designed to provide accurate and authoritative information in regard to the subject matter covered. It is sold with the understanding that the publisher is not engaged in rendering professional services. If professional advice or other expert assistance is required, the services of a competent professional person should be sought. -
Microwave Connectors
O30E.pdf Mar. 19,2021 Microwave Connectors !Note • Please read rating and !CAUTION (for storage, operating, rating, soldering, mounting and handling) in this catalog to prevent smoking and/or burning, etc. O30E.pdf • This catalog has only typical specifications. Therefore, please approve our product specifications or transact the approval sheet for product specifications before ordering. Mar. 19,2021 EU RoHS Compliant • All the products in this catalog comply with EU RoHS. • EU RoHS is "the European Directive 2011/65/EU on the Restriction of the Use of Certain Hazardous Substances in Electrical and Electronic Equipment." • For more details, please refer to our web page, "Murata's Approach for EU RoHS" (https://www.murata.com/en-eu/support/ compliance/rohs). !Note • Please read rating and !CAUTION (for storage, operating, rating, soldering, mounting and handling) in this catalog to prevent smoking and/or burning, etc. O30E.pdf • This catalog has only typical specifications. Therefore, please approve our product specifications or transact the approval sheet for product specifications before ordering. Mar. 19,2021 1 Contents Product specifications are as of February 2021. 2 Part Numbering p2 Type of Connectors p3 1 Microwave Coaxial Connectors with Switch SWD Type p5 SWF Type p7 SWG Type p9 SWH Type p11 SWH-2Way Type p13 SWJ Type p15 2 Microwave Multi Line Connectors MLF Type p17 Notice (Design) p22 Notice (Engagement/Disengagement) p23 Type of Probes p24 Electrical Performance Measurement System (Insertion Loss, VSWR) p25 Mechanical Performance Measurement System (Engagement/Disengagement Force) p26 Notice p27 Please check the MURATA website (https://www.murata.com/) if you cannot find a part number in this catalog. -
Acoustic Interface Design Guide
Acoustic Interface Design Guide MEMS MICROPHONES ECMs SPECIALTY MICROPHONES SPECIALTY SPEAKERS CUSTOM ASSEMBLIES ACOUSTIC SOFTWARE MICROPHONE AND SPEAKER BASICS Discover your next acoustic interface solution. Knowles Acoustics offers you a full spectrum of MEMS microphones, electret condenser microphones, specialty microphones, balanced armature speakers, custom assemblies, and sound conditioning software. This application guide will help you select the right acoustic interface solution. Knowles reserves the right to change designs and specifications without prior notice. Should a safety concern arise regarding this product, please contact us immediately for technical consultation. Knowles cannot assume responsibility for any problems arising out of the use of this product. This information does not convey any license by any implication under any patents or other right. 2 www.knowles.com We can help you every step of the way. It all starts with your application. Or it starts with an idea you may have. For support from concept to design to sub-assembly, or any step along the way, just call us. Or visit us at www.knowles.com Table of Contents MICROPHONES - MEMS . 4-5 MICROPHONES - ECMs . 6-8 SPECIALTY TRANSDUCERS - MICROPHONES . 9-14 ACCELEROMETERS & DAMPERS . 14 SPECIALTY TRANSDUCERS - SPEAKERS . 15-23 CUSTOM ASSEMBLIES . 24 ACOUSTIC SOFTWARE . 25 MICROPHONE AND SPEAKER BASICS . 26-27 www.knowles.com 3 MICROPHONES – MEMS SiSonic™ MEMS Microphones The SiSonic™ MEMS microphone series is entering its fourth generation of development, with product shipments exceeding 400 million units to date. The proven and evolving design series continues to support high-performance, high-density innovation in such applications as cell phones, digital still cameras, portable music players, premium earbuds and other portable electronic devices. -
Sections 5-1 to 5-4: Analog Filters
ANALOG FILTERS H Op Amp History 1 Op Amp Basics 2 Specialty Amplifiers 3 Using Op Amps with Data Converters ◆ 4 Sensor Signal Conditioning ◆ 5 Analog Filters 1 Introduction 2 The Transfer Function 3 Time Domain Response 4 Standard Responses 5 Frequency Transformations 6 Filter Realizations 7 Practical Problems in Filter Implementation 8 Design Examples 6 Signal Amplifiers 7 Hardware and Housekeeping Techniques OP AMP APPLICATIONS ANALOG FILTERS INTRODUCTION CHAPTER 5: ANALOG FILTERS Hank Zumbahlen SECTION 5-1: INTRODUCTION Filters are networks that process signals in a frequency-dependent manner. The basic concept of a filter can be explained by examining the frequency dependent nature of the impedance of capacitors and inductors. Consider a voltage divider where the shunt leg is a reactive impedance. As the frequency is changed, the value of the reactive impedance changes, and the voltage divider ratio changes. This mechanism yields the frequency dependent change in the input/output transfer function that is defined as the frequency response. Filters have many practical applications. A simple, single pole, lowpass filter (the integrator) is often used to stabilize amplifiers by rolling off the gain at higher frequencies where excessive phase shift may cause oscillations. A simple, single pole, highpass filter can be used to block DC offset in high gain amplifiers or single supply circuits. Filters can be used to separate signals, passing those of interest, and attenuating the unwanted frequencies. An example of this is a radio receiver, where the signal you wish to process is passed through, typically with gain, while attenuating the rest of the signals.