Application Guide MSO5000 Series Digital Oscilloscope
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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. -
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 -
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 -
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. -
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. -
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. -
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. -
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. -
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. -
Loop Stability Compensation Technique for Continuous-Time Common-Mode Feedback Circuits
Loop Stability Compensation Technique for Continuous-Time Common-Mode Feedback Circuits Young-Kyun Cho and Bong Hyuk Park Mobile RF Research Section, Advanced Mobile Communications Research Department Electronics and Telecommunications Research Institute (ETRI) Daejeon, Korea Email: [email protected] Abstract—A loop stability compensation technique for continuous-time common-mode feedback (CMFB) circuits is presented. A Miller capacitor and nulling resistor in the compensation network provide a reliable and stable operation of the fully-differential operational amplifier without any performance degradation. The amplifier is designed in a 130 nm CMOS technology, achieves simulated performance of 57 dB open loop DC gain, 1.3-GHz unity-gain frequency and 65° phase margin. Also, the loop gain, bandwidth and phase margin of the CMFB are 51 dB, 27 MHz, and 76°, respectively. Keywords-common-mode feedback, loop stability compensation, continuous-time system, Miller compensation. Fig. 1. Loop stability compensation technique for CMFB circuit. I. INTRODUCTION common-mode signal to the opamp. In Fig. 1, two poles are The differential output amplifiers usually contain common- newly generated from the CMFB loop. A dominant pole is mode feedback (CMFB) circuitry [1, 2]. A CMFB circuit is a introduced at the opamp output and the second pole is located network sensing the common-mode voltage, comparing it with at the VCMFB node. Typically, the location of these poles are a proper reference, and feeding back the correct common-mode very close which deteriorates the loop phase margin (PM) and signal with the purpose to cancel the output common-mode makes the closed loop system unstable. -
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. -
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