Development of a Novel Tuning Approach of the Notch Filter of the Servo Feed Drive System

Total Page:16

File Type:pdf, Size:1020Kb

Development of a Novel Tuning Approach of the Notch Filter of the Servo Feed Drive System Journal of Manufacturing and Materials Processing Article Development of a Novel Tuning Approach of the Notch Filter of the Servo Feed Drive System Chung-Ching Liu 1,* , Meng-Shiun Tsai 2, Mao-Qi Hong 2 and Pu-Yang Tang 1 1 Department of Mechanical Engineering, National Chung Cheng University, Chiayi 62102, Taiwan; [email protected] 2 Department of Mechanical Engineering, National Taiwan University, Taipei 10617, Taiwan; [email protected] (M.-S.T.); [email protected] (M.-Q.H.) * Correspondence: [email protected] Received: 23 January 2020; Accepted: 2 March 2020; Published: 5 March 2020 Abstract: To alleviate the vibration effect of the feed drive system, a traditional approach is to apply notch filters to suppress vibrations in the velocity loop. The current approach is to adjust the notch filter parameters such as the center frequency, damping and depth based on observing the frequency response diagram of servo velocity closed loop. In addition, the notch filters are generally provided in the velocity loop control for the commercialized controllers such as FANUC, Siemens, etc. However, the resonance of the transmission system also appears in the position loop when the linear scale is used as the position feedback. The notch filter design without consideration of the resonance behavior of the position loop might cause degradation of performance. To overcome this problem, the paper proposes an innovative method which could automatically determine the optimal parameters of the notch filter under the consideration of resonance behavior of position loop. With the optimal parameters, it is found that both the gains of position and velocity loop controller could be increased such that the bandwidths of the position/velocity loops are higher. Based on the simulation results, the rising time is improved by 33% and the time for reaching the steady state is improved by 72% as comparing the cases of using the optimal approach and traditional approach. Keywords: notch filter; auto-tuning; feed drive system 1. Introduction High-speed machine tools are widely used in manufacturing the parts for aviation, automotive, mold, and other industrial fields. The design objectives of machine tools are to obtain high efficiency, high precision and high surface quality. However, vibrations of machine structure may be excited when the machine is under high speed and acceleration condition, and the surface quality would also be affected. To avoid the vibration effects, many factors should be considered. One of the most critical factors is how to adjust the servo control parameters. The vibrations could deteriorate the manufacturing qualities and performances [1–3]. To suppress the structural vibration of the feed drive system, many scholars have proposed different approaches. For example, motion commands are filtered before entering the servo controller [4–6]. Some scholars have also proposed strategies that adopted active damping of structural vibrations inside the control loop [7–9]. In the modern time, there are many various ways to control vibration behavior, such as neural networks [10,11], fuzzy control [12,13], and sliding mode control [14,15]. These methods can achieve higher control bandwidth by applying notch filters in the control loop. However, the design of such controllers could be difficult because higher-order plant models need to be considered in order to include the vibration modes into the dynamic model. For commercialized controllers, the control loops are designed by three main loops: current, velocity and position loops. J. Manuf. Mater. Process. 2020, 4, 21; doi:10.3390/jmmp4010021 www.mdpi.com/journal/jmmp J. Manuf. Mater. Process. 2020, 4, x FOR PEER REVIEW 2 of 11 commercialized controllers, the control loops are designed by three main loops: current, velocity and J. Manuf. Mater. Process. 2020, 4, 21 2 of 11 position loops. The commercial controllers generally apply the notch filters in velocity loop to alleviate the vibration signal near the resonance frequency [16] such that the bandwidth of the control Theloop commercial could be increased. controllers However, generally the apply traditional the notch method filters of in adjusting velocity loopthe notch to alleviate filter only the vibrationconsiders signalthe resonance near the resonancebehavior frequencyof the velocity [16] such loop. that The the resonance bandwidth behaviors of the control of the loop components could be increased. located However,outside the the velocity traditional loop methodhave not of been adjusting considered. the notch The filterresearch only of considers how to design the resonance the notch behavior filter by ofconsidering the velocity both loop. the Thevelocity resonance and position behaviors loop of dynamics the components is still an located open issue. outside In this the paper, velocity a novel loop haveapproach not been which considered. could determine The research the optimal of how parameters to design the of notchthe notch filter filter by considering is proposed. both In thethe velocityapproach, and the position vibration loop effects dynamics in velocity is still anand open position issue. loops In this are paper, considered a novel, approachand the parameters which could of determinenotch filters the could optimal automatically parameters ofbe the adjusted. notch filter The is paper proposed. is arranged In the approach, as follows. the In vibration Section e2,ffects the indynamics velocity andof the position feed system loops areand considered, the traditional and theapproach parameters are introduced. of notch filters Then, could the automaticallynovel optimal beapproach adjusted. is proposed The paper in isSection arranged 3. The as Bode follows. plots In velocity Section and2, the position dynamics loop of of the using feed traditional system and and theoptimal traditional approaches approach are arecompared introduced. in Section Then, 4. the The novel servo optimal performances approach using is proposed the traditional in Section and3. Theoptimal Bode approaches plots velocity for and the position step input loop and of usingthe trajectory traditional are and compared. optimal approaches Finally, Section are compared 5 gives the in Sectionconclusion.4. The servo performances using the traditional and optimal approaches for the step input and the trajectory are compared. Finally, Section5 gives the conclusion. 2. The Dynamic Model of the Feed Drive System 2. The Dynamic Model of the Feed Drive System In this section, the dynamic model of the feed drive system is first derived. Then, the dynamic modelIn thisis simplified section, theto explain dynamic the model parameter of the tuning feed drive process. system is first derived. Then, the dynamic model is simplified to explain the parameter tuning process. 2.1. The Derivation of the Feed Drive System 2.1. The Derivation of the Feed Drive System To describe the dynamic behavior of feed drive system, this paper utilizes the model proposed by theTo paper describe [4]. the The dynamic model includes behavior the of feeddynamics drive effects system, of this couplings, paper utilizes ball-screws, the model structure proposed base, byand the servo paper loop [4]. controls. The model The includes schematic the diagram dynamics of eaff feedects ofdrive couplings, system ball-screws,is shown in structureFigure 1a. base, The androtary servo motion loop controls.of the motor The drives schematic the platform diagram ofthrough a feed drivethe coupling system isand shown the ball in Figure-screw.1a. The The rotation rotary motionof the motor of the motorcan be drives measured the platform by the throughencoder themounted coupling on andthe themotor. ball-screw. The linear The rotationmotion of thethe motorplatform can can be measuredbe measured by theby encoderthe optical mounted linear scale on the on motor. the platform. The linear The motion feed drive of the system platform can can be besimplified measured as bya mass the optical-damper linear-spring scale (MCK) on the system platform. as shown The feed in Figure drive system1b. can be simplified as a mass-damper-spring (MCK) system as shown in Figure1b. (a) (b) FigureFigure 1.1. TheThe feedfeed drive drive system. system. ( a()a) The The schematic schematic of of the the feed feed drive drive system. system. (b )(b The) The 2 DOF 2 DOF diagram diagram of theof the feed feed drive drive system. system. InIn Figure1 1,, thethe parameters parameters could could be be defined defined as as the the following. following. isX thet is displacement the displacement of the of table, the table, is theXl isdisplacement the displacement of the ofball the-screw ball-screw,, and and is theXb displacementis the displacement of the base. of the base. and θl and are θthem are the ball-screw and motor rotation angle. Jl and Jm are the inertia of the ball-screw and motor. J.J. Manuf. Manuf. Mater. Mater. Process. Process. 20202020, ,44, ,x 21 FOR PEER REVIEW 33 of of 11 11 ball-screw and motor rotation angle. and are the inertia of the ball-screw and motor. and Mt arande theM bmassare theof table mass and of tablebase. and , base. andC t, C arel and theC dampingb are the of damping guideway, of guideway, ball-screw ball-screwand base, respectively.and base, respectively. , andK b, Kareg and the Kstiffnesst are the of sti base,ffness coupling of base, stiffness coupling and sti longitudinalffness and longitudinal stiffness of ballstiff-nessscrew, of respectively. ball-screw, respectively. The rotary Themotion rotary of motionthe ball of-screw, the ball-screw, , is transmittedθl, is transmitted to the linear to the displacement,linear displacement, , throughXl, through the converting the converting ratio, ratio, . Risl. givenRl is given as / as2 P , /where2π, where is Ptheis pitch the pitch of the of ballthe- ball-screw.screw. AfterAfter the the integration integration of of the the feed feed drive drive syste systemm and and servo servo loop loop control control system, system, the the complete complete system system cancan be be expressed expressed as asthe the block block diagram diagram shown shown in Figure in Figure 2 and2 isand named is named as the asservo the feed servo drive feed system drive.
Recommended publications
  • Lesson 22: Determining Control Stability Using Bode Plots
    11/30/2015 Lesson 22: Determining Control Stability Using Bode Plots 1 ET 438A AUTOMATIC CONTROL SYSTEMS TECHNOLOGY lesson22et438a.pptx Learning Objectives 2 After this presentation you will be able to: List the control stability criteria for open loop frequency response. Identify the gain and phase margins necessary for a stable control system. Use a Bode plot to determine if a control system is stable or unstable. Generate Bode plots of control systems the include dead-time delay and determine system stability. lesson22et438a.pptx 1 11/30/2015 Bode Plot Stability Criteria 3 Open loop gain of less than 1 (G<1 or G<0dB) at Stable Control open loop phase angle of -180 degrees System Oscillatory Open loop gain of exactly 1 (G=1 or G= 0dB) at Control System open loop phase angle of -180 degrees Marginally Stable Unstable Control Open loop gain of greater than 1 (G>1 or G>0dB) System at open loop phase angle of -180 degrees lesson22et438a.pptx Phase and Gain Margins 4 Inherent error and inaccuracies require ranges of phase shift and gain to insure stability. Gain Margin – Safe level below 1 required for stability Minimum level : G=0.5 or -6 dB at phase shift of 180 degrees Phase Margin – Safe level above -180 degrees required for stability Minimum level : f=40 degree or -180+ 40=-140 degrees at gain level of 0.5 or 0 dB. lesson22et438a.pptx 2 11/30/2015 Determining Phase and Gain Margins 5 Define two frequencies: wodB = frequency of 0 dB gain w180 = frequency of -180 degree phase shift Open Loop Gain 0 dB Gain Margin -m180 bodB Phase Margin -180+b0dB -180o Open Loop w w Phase odB 180 lesson22et438a.pptx Determining Phase and Gain Margins 6 Procedure: 1) Draw vertical lines through 0 dB on gain and -180 on phase plots.
    [Show full text]
  • EE C128 Chapter 10
    Lecture abstract EE C128 / ME C134 – Feedback Control Systems Topics covered in this presentation Lecture – Chapter 10 – Frequency Response Techniques I Advantages of FR techniques over RL I Define FR Alexandre Bayen I Define Bode & Nyquist plots I Relation between poles & zeros to Bode plots (slope, etc.) Department of Electrical Engineering & Computer Science st nd University of California Berkeley I Features of 1 -&2 -order system Bode plots I Define Nyquist criterion I Method of dealing with OL poles & zeros on imaginary axis I Simple method of dealing with OL stable & unstable systems I Determining gain & phase margins from Bode & Nyquist plots I Define static error constants September 10, 2013 I Determining static error constants from Bode & Nyquist plots I Determining TF from experimental FR data Bayen (EECS, UCB) Feedback Control Systems September 10, 2013 1 / 64 Bayen (EECS, UCB) Feedback Control Systems September 10, 2013 2 / 64 10 FR techniques 10.1 Intro Chapter outline 1 10 Frequency response techniques 1 10 Frequency response techniques 10.1 Introduction 10.1 Introduction 10.2 Asymptotic approximations: Bode plots 10.2 Asymptotic approximations: Bode plots 10.3 Introduction to Nyquist criterion 10.3 Introduction to Nyquist criterion 10.4 Sketching the Nyquist diagram 10.4 Sketching the Nyquist diagram 10.5 Stability via the Nyquist diagram 10.5 Stability via the Nyquist diagram 10.6 Gain margin and phase margin via the Nyquist diagram 10.6 Gain margin and phase margin via the Nyquist diagram 10.7 Stability, gain margin, and
    [Show full text]
  • I Introduction and Background
    Final Design Report Platform Motion Measurement System ELEC 492 A Senior Design Project, 2005 Between University of San Diego And Trex Enterprises Submitted to: Dr. Lord at USD Prepared by: YAZ Zlatko Filipovic Yoshitaka Yano August 12, 2005 University of San Diego Final Design Report USD August 12, 2005 Platform Motion Measurement System Table of Contents I. Acknowledgments…………...…………………………………………………………4 II. Executive Summary……..…………………………………………………………….5 III. Introduction and Background…...………………………...………………………….6 IV. Project Requirements…………….................................................................................8 V. Methodology of Design Plan……….…..……………..…….………….…..…….…..11 VI. Testing….……………………………………..…..…………………….……...........21 VII. Deliverables and Project Results………...…………...…………..…….…………...24 VIII. Budget………………………………………...……..……………………………..25 IX. Personnel…………………..………………………………………....….……….......28 X. Design Schedule………….…...……………………………….……...…………........29 XI. Reference and Bibliography…………..…………..…………………...…………….31 XII. Summary…………………………………………………………………………....32 Appendices Appendix 1. Simulink Simulations…..………………………….…….33 Appendix 2. VisSim Simulations..........……………………………….34 Appendix 3. Frequency Response and VisSim results……………......36 Appendix 4. Vibration Measurements…………..………………….….38 Appendix 5. PCB Layout and Schematic……………………………..39 Appendix 6. User’s Manual…………………………………………..41 Appendix 7. PSpice Simulations of Hfilter…………………………….46 1 Final Design Report USD August 12, 2005 Platform Motion Measurement System
    [Show full text]
  • Meeting Design Specifications
    NDSU Meeting Design Specs using Bode Plots ECE 461 Meeting Design Specs using Bode Plots When designing a compensator to meet design specs including: Steady-state error for a step input Phase Margin 0dB gain frequency the procedure using Bode plots is about the same as it was for root-locus plots. Add a pole at s = 0 if needed (making the system type-1) Start cancelling zeros until the system is too fast For every zero you added, add a pole. Place these poles so that the phase adds up. When using root-locus techniques, the phase adds up to 180 degrees at some spot on the s-plane. When using Bode plot techniques, the phase adds up to give you your phase margin at some spot on the jw axis. Example 1: Problem: Given the following system 1000 G(s) = (s+1)(s+3)(s+6)(s+10) Design a compensator which result in No error for a step input 20% overshoot for a step input, and A settling time of 4 second Solution: First, convert to Bode Plot terminology No overshoot means make this a type-1 system. Add a pole at s = 0. 20% overshoot means ζ = 0.4559 Mm = 1.2322 GK = 1∠ − 132.120 Phase Margin = 47.88 degrees A settling time of 4 seconds means s = -1 + j X s = -1 + j2 (from the damping ratio) The 0dB gain frequency is 2.00 rad/sec In short, design K(s) so that the system is type-1 and 0 (GK)s=j2 = 1∠ − 132.12 JSG 1 rev June 22, 2016 NDSU Meeting Design Specs using Bode Plots ECE 461 Start with s+1 K(s) = s At 4 rad/sec 1000 0 GK = s(s+3)(s+6)(s+10) = 2.1508∠ − 153.43 s=j2 There is too much phase shift, so start cancelling zeros.
    [Show full text]
  • Applications Academic Program Distributing Vissim Models
    VISSIM VisSim is a visual block diagram language for simulation of dynamical systems and Model Based Design of embedded systems. It is developed by Visual Solutions of Westford, Massachusetts. Applications VisSim is widely used in control system design and digital signal processing for multidomain simulation and design. It includes blocks for arithmetic, Boolean, and transcendental functions, as well as digital filters, transfer functions, numerical integration and interactive plotting. The most commonly modeled systems are aeronautical, biological/medical, digital power, electric motor, electrical, hydraulic, mechanical, process, thermal/HVAC and econometric. Academic program The VisSim Free Academic Program allows accredited educational institutions to site license VisSim v3.0 for no cost. The latest versions of VisSim and addons are also available to students and academic institutions at greatly reduced pricing. Distributing VisSim models VisSim viewer screenshot with sample model. The free Vis Sim Viewer is a convenient way to share VisSim models with colleagues and clients not licensed to use VisSim. The VisSim Viewer will execute any VisSim model, and allows changes to block and simulation parameters to illustrate different design scenarios. Sliders and buttons may be activated if included in the model. Code generation The VisSim/C-Code add-on generates efficient, readable ANSI C code for algorithm acceleration and real-time implementation of embedded systems. The code is more efficient and readable than most other code generators. VisSim's author served on the X3J11 ANSI C committee and wrote several C compilers, in addition to co-authoring a book on C. [2] This deep understanding of ANSI C, and the nature of the resulting machine code when compiled, is the key to the code generator's efficiency.
    [Show full text]
  • Frequency Response and Bode Plots
    1 Frequency Response and Bode Plots 1.1 Preliminaries The steady-state sinusoidal frequency-response of a circuit is described by the phasor transfer function Hj( ) . A Bode plot is a graph of the magnitude (in dB) or phase of the transfer function versus frequency. Of course we can easily program the transfer function into a computer to make such plots, and for very complicated transfer functions this may be our only recourse. But in many cases the key features of the plot can be quickly sketched by hand using some simple rules that identify the impact of the poles and zeroes in shaping the frequency response. The advantage of this approach is the insight it provides on how the circuit elements influence the frequency response. This is especially important in the design of frequency-selective circuits. We will first consider how to generate Bode plots for simple poles, and then discuss how to handle the general second-order response. Before doing this, however, it may be helpful to review some properties of transfer functions, the decibel scale, and properties of the log function. Poles, Zeroes, and Stability The s-domain transfer function is always a rational polynomial function of the form Ns() smm as12 a s m asa Hs() K K mm12 10 (1.1) nn12 n Ds() s bsnn12 b s bsb 10 As we have seen already, the polynomials in the numerator and denominator are factored to find the poles and zeroes; these are the values of s that make the numerator or denominator zero. If we write the zeroes as zz123,, zetc., and similarly write the poles as pp123,, p , then Hs( ) can be written in factored form as ()()()s zsz sz Hs() K 12 m (1.2) ()()()s psp12 sp n 1 © Bob York 2009 2 Frequency Response and Bode Plots The pole and zero locations can be real or complex.
    [Show full text]
  • MT-033: Voltage Feedback Op Amp Gain and Bandwidth
    MT-033 TUTORIAL Voltage Feedback Op Amp Gain and Bandwidth INTRODUCTION This tutorial examines the common ways to specify op amp gain and bandwidth. It should be noted that this discussion applies to voltage feedback (VFB) op amps—current feedback (CFB) op amps are discussed in a later tutorial (MT-034). OPEN-LOOP GAIN Unlike the ideal op amp, a practical op amp has a finite gain. The open-loop dc gain (usually referred to as AVOL) is the gain of the amplifier without the feedback loop being closed, hence the name “open-loop.” For a precision op amp this gain can be vary high, on the order of 160 dB (100 million) or more. This gain is flat from dc to what is referred to as the dominant pole corner frequency. From there the gain falls off at 6 dB/octave (20 dB/decade). An octave is a doubling in frequency and a decade is ×10 in frequency). If the op amp has a single pole, the open-loop gain will continue to fall at this rate as shown in Figure 1A. A practical op amp will have more than one pole as shown in Figure 1B. The second pole will double the rate at which the open- loop gain falls to 12 dB/octave (40 dB/decade). If the open-loop gain has dropped below 0 dB (unity gain) before it reaches the frequency of the second pole, the op amp will be unconditionally stable at any gain. This will be typically referred to as unity gain stable on the data sheet.
    [Show full text]
  • A Note on Stability Analysis Using Bode Plots
    ChE classroom A NOTE ON STABILITY ANALYSIS USING BODE PLOTS JUERGEN HAHN, THOMAS EDISON, THOMAS F. E DGAR The University of Texas at Austin • Austin, TX 78712-1062 he Bode plot is an important tool for stability analysis amplitude ratio greater than unity for frequencies where f = of closed-loop systems. It is based on calculating the -180∞-n*360∞, where n is an integer. These conditions can T amplitude and phase angle for the transfer function occur when the process includes time delays, as shown in the following example. GsGsGs 1 OL( ) = C( ) P ( ) ( ) for s = jw Juergen Hahn was born in Grevenbroich, Ger- many, in 1971. He received his diploma degree where GC(s) is the controller and GP(s) is the process. The in engineering from RWTH Aachen, Germany, Bode stability criterion presented in most process control text- in 1997, and his MS degree in chemical engi- neering from the University of Texas, Austin, in books is a sufficient, but not necessary, condition for insta- 1998. He is currently a PhD candidate working bility of a closed-loop process.[1-4] Therefore, it is not pos- as a research assistant in chemical engineer- sible to use this criterion to make definitive statements about ing at the University of Texas, Austin. His re- search interests include process modeling, non- the stability of a given process. linear model reduction, and nonlinearity quanti- fication. Other textbooks[5,6] state that this sufficient condition is a necessary condition as well. That statement is not correct, as Thomas Edison is a lecturer at the University of Texas, Austin.
    [Show full text]
  • Lecture 45 Bode Plots of Transfer Functions A. Goals
    Lecture 45 Bode Plots of Transfer Functions A. Goals : Design Oriented Analysis 1. Design Oriented Analysis Overview 2. Inspection of T(s) in normalized form 3. Five points in design oriented analysis B. Review of Bode Plots 1. db values 2. Log - Log Slopes vs f 3. Normalized Form 1 + s/w a. Regular Pole b. Right Half Plane Zero flyback / Buck - Boost c. Inverted Forms 1 + w/s 1. Pole d. Complex T(s) Plots versus Frequency 4. Low-Pass Filter Resonant Circuit 5. Series Resonant R-L-C Circuit 1 Lecture 45 Bode Plots of Transfer Functions A. Goal : Design Oriented Analysis 1. Design Oriented Analysis Our aim in design is to always keep the whole system view at hand so that we can alter some parts of the system and immediately see the results of the change in other parts of the system. The keystone will be the Bode plots of each part of the system that comprise the open loop response. From the open loop response Bode plots various design changes may be explored. We seek simple intuitive understanding of a transfer function via Bode Plots vs f 2. Inspection of T(s) in normalized form to: a. Guess / estimate pole and zero location b. Determine asymptotic behaviors 2 3. The five points in design oriented analysis we will emphasize are given below: Before we can do this we need to review how to construct and make Bode plots as they are the key to our design oriented approach. Asymptotic approximations to the full Bode plots are key to rapid design and analysis.
    [Show full text]
  • Transfer Function G(S) S =Jω Frequency Response G(Jω)
    FREQUENCY RESPONSES Signals and System Analysis Transfer function G(s) s =jω Frequency response G(jω) Frequency (strictly angular frequency) ω Magnitude |G(jω)| Phase ∠G(jω) Signals and System Analysis Significance of the frequency response It indicates how much the system responds to a sinusoidal input at different frequencies Frequency response G(jω) Mmagnitude |G(jω)| Phase ∠G(jω) Signals and System Analysis There are several ways of plotting frequency responses but the two most common are: Direct plotting |G|-ω ∠G-ω Bode diagrams |G| - ω in log scale ∠G- ω in log scale Nyquist (or polar) plot Real(G) -Imag(G) Signals and System Analysis Any transfer function can be plotted 1. using the Control Kit in MATLAB. or 2. write a program using MATLAB codes Signals and System Analysis The Bode diagram consists of two graphs: 1. |G(jω)| against ω on a log scale The gain in dB, that is 20log10 |G(jω)|, is plotted on a linear scale 2. ∠G(jω) against ω on a log scale The Nyquist plot is a locus with ω as a parameter showing |G(jω)| and ∠G(jω as a curve as ω varies. Signals and System Analysis Bode plots of the following transfer functions K – a gain 1/sT – an integrator 1/(1+sT) – a time constant or first order system 2 2 2 ω0 /(s +2ζsω0+ω0 ) – a complex pole pair or second order system. Signals and System Analysis K – a gain G(s)=K G(jω)=K G( jω) = K 0 ∠G( jω) = tan −1 = 0 K Signals and System Analysis - K – a negative gain G(s)=-K G(jω)=-K G( jω) = K 0 ∠G( jω) = tan −1 =180o − K Signals and System Analysis Plot Frequency Response for K gain 2
    [Show full text]
  • And Elliptic Filter for Speech Signal Analysis Design And
    Design and Implementation of Butterworth, Chebyshev-I and Elliptic Filter for Speech Signal Analysis Prajoy Podder Md. Mehedi Hasan Md.Rafiqul Islam Department of ECE Department of ECE Department of EEE Khulna University of Khulna University of Khulna University of Engineering & Technology Engineering & Technology Engineering & Technology Khulna-9203, Bangladesh Khulna-9203, Bangladesh Khulna-9203, Bangladesh Mursalin Sayeed Department of EEE Khulna University of Engineering & Technology Khulna-9203, Bangladesh ABSTRACT and IIR filter. Analog electronic filters consisted of resistors, In the field of digital signal processing, the function of a filter capacitors and inductors are normally IIR filters [2]. On the is to remove unwanted parts of the signal such as random other hand, discrete-time filters (usually digital filters) based noise that is also undesirable. To remove noise from the on a tapped delay line that employs no feedback are speech signal transmission or to extract useful parts of the essentially FIR filters. The capacitors (or inductors) in the signal such as the components lying within a certain analog filter have a "memory" and their internal state never frequency range. Filters are broadly used in signal processing completely relaxes following an impulse. But after an impulse and communication systems in applications such as channel response has reached the end of the tapped delay line, the equalization, noise reduction, radar, audio processing, speech system has no further memory of that impulse. As a result, it signal processing, video processing, biomedical signal has returned to its initial state. Its impulse response beyond processing that is noisy ECG, EEG, EMG signal filtering, that point is exactly zero.
    [Show full text]
  • S-DOMAIN ANALYSIS: POLES, ZEROS, and BODE PLOTS
    APPENDIX F s-DOMAIN ANALYSIS: POLES, ZEROS, AND BODE PLOTS In analyzing the frequency response of an amplifier, most of the work involves finding the amplifier voltage gain as a function of the complex frequency s. In this s-domain analysis, a capacitance C is replaced by an admittance sC, or equivalently an impedance 1/sC, and an inductance L is replaced by an impedance sL. Then, using usual circuit-analysis techniques, ( ) ≡ ( )/ ( ) one derives the voltage transfer function T s Vo s Vi s . EXERCISE F.1 ( ) ≡ ( )/ ( ) Find the voltage transfer function T s Vo s Vi s for the STC network shown in Fig. EF.1. R1 ϩ Vi Ϫ ϩ C R2 Vo Ϫ Figure EF.1 1/CR Ans. T(s) = 1 + / s 1 C R1 R2 Once the transfer function T(s) is obtained, it can be evaluated for physical frequencies by replacing s by jω. The resulting transfer function T( jω) is in general a complex quantity whose magnitude gives the magnitude response (or transmission) and whose angle gives the phase response of the amplifier. In many cases it will not be necessary to substitute s = jω and evaluate T(jω); rather, the form of T(s) will reveal many useful facts about the circuit performance. In general, for all the circuits dealt with in this book, T(s) can be expressed in the form − a sm + a sm 1 + ... + a T(s) = m m−1 0 (F.1) n + n−1 + ... + s bn−1s b0 F-1 ©2015 Oxford University Press Reprinting or distribution, electronically or otherwise, without the express written consent of Oxford University Press is prohibited.
    [Show full text]