Artificial Neural Network Modeling of Damaged Aircraft

Total Page:16

File Type:pdf, Size:1020Kb

Artificial Neural Network Modeling of Damaged Aircraft Calhoun: The NPS Institutional Archive Theses and Dissertations Thesis Collection 1994-03 Artificial neural network modeling of damaged aircraft Brunger, Clifford A. Monterey, California. Naval Postgraduate School http://hdl.handle.net/10945/42931 AD-A283IlIIhIiIhIIm IhIhili 227 . , NAVAL POSTGRADUATE SCHOOL Monterey, California DTIC AUG 11994 THESIS b, 7- ARTIFICIAL NEURAL NETWORK MODELING OF DAMAGED AIRCRAFT _• by Clifford A. Bnmger March, 1994 Thesis Advisor: Daniel J. Collins Approved for public release; distribution is unlimited. 94 8 10 002 Unclassified SECURITY CLASSIFICATION OF T-IS PAGE "I r oForm Approved,, REPORT DOCUMENTATION PAGE NMo Oils I& KkMiKr /5kLULU1 ICLAeJ"-ILAIgJIN lb. Kkb1IbL-Vk"MAICMNLgJ Unclassified 2& SECUU[[Y LA SU WATIU NiAUTUOIUTY 3. LDII 1R WUTI4AVAILA/U1 TY KZ" OTUKI __________________________________________ Approved for public release; ULU.A W.L.IU^.U~a,•wNU IU •JULL distribution is unlimited. 4. YW~tUiJMMNU UK(,AXZ142-AAIUf k¶KI I'4MUM~bK) 5. NMUNI MMI( 0K~iANUAIIUt XMMlIJ 4UhMAkRI) 6*NAM1 UP FtPELCMIU UKUANJAW-CIUN *. UiMk bymDsL U* NAME~ OF MONITUKINa UKRiADUA1UN Naval Posgraduate School I AA/PL Naval Postgraduate School MWontMaUy. 3 Er CBS50) I. AIMonte riey. 3-C934 L-50r Monterey. CA 93943-5000 Mont CA-. 93943-5000 NAREOF FORRM071MRrlj 16. UFmLB ITSMUU V. IKUMAULi 243 KlibQ2I LulNiIEILA1iN NummL OROANA•1ON (If aWhoebe) 5ce. AL)DKJXS (City. State, and•LW ie 10. .UKL;V" UP tPuN'X~lRF NUL/Mbb,", ACCESON NO. SNO. NO. Artificial Neural Network Modeling of Damaged Aircraft 14. IIMMNAL AUWHUK(b) Clifford A. Brunger IS. I TR• (R KKI 1*u. -IWm=* uu 14. VAIB Ur ROU (IfhlJy) VAL&"OUNI Master's Thesis I 01M92DI0M9 March 1994 - 7 109 l6r7PUEMXLKY NVI[AIRIM The views expressed in this thesis are those of the author and do not reflect the official policy or position of the Department of Defense or the U.S. Government. L;UbAII tULX5 I&. bumLI 11MMl (LaaMe aU swe•e wy Ideiualy by bilack SUnaa) K"UA UKUUP Ig KU Neural Network, Parallel Processors UlnuereIa IFl=n by b10" metw) Aircraft design and control techniques rely on the proper modeling of the aircraft's equations of motion. Many of the variables used in these equations are aerodynamic coefficients which are obtained from scale models in wind tunnel tests. In order to model damaged aircraft, every aerodynamic coefficient must be determined for every possible damage mechanism in every flight coutdition. Designing a controller for a damaged aircraft is particularly burdensome because knowledge of the effect of each damage mechanism on the model is required bafoM the controller can be designed. Also, a monitoring system must be employed to decide when and how much damage has occurred in order to re configure the controller. Recent advances in artificial intelligence have made parallel distributed processors (artificial neural networks) feasible. Modeled on the human brain, the artificial neural network's strength lies in its ability to generalize from a given model. This thesis examines the robustness of the artificial neural network as a model for damaged aircraft. [E tNDAsz6JIEIU Q s Amsmrr. Q zncwas Unclassified Daniel J. Collins (408) 656 - 2311 fC S/N 0102-LX-014-6603 Unclassified Approved for public release; distribution is unlimited. Artificial Neural Network Modeling of Damaged Aircraft by Clifford A. Brunger Lieutenant, United States Navy B.S.E.E., United States Naval Academy, 1984 Submitted in partial fulfillment of the requirements for the degree of MASTER OF SCIENCE IN AERONAUTICAL ENGINEERING from the NAVAL POSTGRADUATE SCHOOL MARCH 1994 Author: Approved by: J. Colli, Thesis Advisor Richard M. Howard, Second Reader Daniel J. $llins, Chairman Department of Aeronautics and Astronautics ii ABSTRACT Aircraft design and control techniques rely on the proper modeling of the aircraft's equations of motion. Many of the variables used in these equations are aerodynamic coefficients which are obtained from scale models in wind tunnel tests. In order to model damaged aircraft, every aerodynamic coefficient must be determined for every possible damage mechanism in every flight condition. Designing a controller for a damaged aircraft is particularly burdensome because knowledge of the effect of each damage mechanism on the model is required before the controller can be designed. Also, a monitoring system must be employed to decide when and how much damage has occurred in order to re configure the controller. Recent advances in artificial intelligence have made parallel distributed processors (artificial neural networks) feasible. Modeled on the human brain, the artificial neural network's strength lies in its ability to generalize from a given model. This thesis examines the robustness of the artificial neural network as a model for damaged aircraft. Acoession For DTIC T.1.3 Unanuo,-a=o'wed 0 Just if tenion By- iii Dist TABLE OF CONTENTS 1. INTRODUCTION ......................................................................... I II. NEURAL NETWORK FUNDAMENTALS ....................................... 4 A. BIOL.OGICAL. NEURONS ................................................................................ 4 B. PROCESSING ELEMENTS ............................................................................. 6 C. ARTIFICIAL NEURAL NETWORKS ......................................................... 1 2 D. ARTIFICIAL NEURAL NETWORK OPERATION .................................... 13 1. L.earig ............................................................................................... 14 a. Supervised Lea ng ............................................................... 14 2. Tes g ................................................................................................. 16 3. Learning Algorithm ........................................................................ 17 E BACK-PROPAGATION ............................................................................... 17 1. Generalized Delta Rule ........................................................... 18 I I I. EXPERIMENTAL PROCEDURE .......................... ................... 2 2 A. HARDWARE-SOFTWARE .................................................................... 22 B. OVERVIEW .............................................................................................. 23 CL SETUP SPECIFICS ............................................................................... 23 1. Modeling of A-4D Longitudinal Motion .............................. 23 2. Generation of Learn and Test Files ................................... 28 a. Random Binary Sequence ................................................ 28 b. A-4D Learn and Test Data .............................................. 32 c. Damaged A-4D Learn and Test Data ........................... 33 3. Neural Network Configuration .............................................. 37 4. Network Validation ................................................................. 39 iv I V. RESULTS ................................................................................. 5 0 A. INTERPOLATION BETWEEN DAMAGE MECHANISMS ....................... 50 B. EXTRAPOLATING FROM A DAMAGED AIRCRAFT ........................ 59 C, DETECTING AND RESPONDING TO DAMAGE ................................ 61 V . CONCLUSIONS ......................................................................... 7 5 APPENDIX A: MATLAB PROGRAMS ............................................. 7 6 APPENDIX B: NEURALWORKS SETUP SPECIFICS ...................... 9 8 LIST OF REFERENCES ................................................................ 100 INITIAL DISTRIBUTION LIST ................................................... 102 V To my beautiful wife Joie, who makes life enjoyable. vi I. INTRODUCTION Designing modem aircraft controllers requires advance knowledge of aircraft dynamics. In order to determine these dynamics, the aircraft is usually modeled. First, the equations of motion (based on Newton's second law) are derived. Neglecting higher order derivatives and making small angle approximations, these equations are linearized around a trim position. The aircraft's equations of motion can then be written in the following state space format: X(t) = Ax(t) + Bu(t) Y(t) = Cx(t) + Du(t) where, x(t) = state vector u(t) = input vector Y(t) = output vector Although the previous steps can be carried out to a high degree of accuracy, the aerodynamicist's job is still daunting. Using wind tunnel tests on scale models, the numerous partial derivatives must be obtained in order to compute the state space matrices (A, B, C and D). Since a simple model of an aircraft is at least eighth order, and some models reach more than fiftieth order, this makes determining the partial derivatives an arduous task. Once the derivatives are known, the transfer functions can be computed and, therefore, the static and dynamic response of the aircraft can be determined. These responses, however, are valid only around the trimmed position. In order for the controller to function throughout the aircraft's entire flight regime, several other trim positions, or flight conditions, must be defined, the equations of motion must be linearized around these new trim positions, and the new aerodynamic derivatives must be determined or estimated. This results in additional A, B, C, and D matrices. The more trim positions selected, the more schedules or plants the controller has to pick from and, therefore, the more robust the controller. A problem arises, however, when the aircraft is damaged. The controller is hard-wired with the
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]
  • 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.
    [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]