Lab #3: System Identification of the Torsional Disk System

Similar documents
Lab #2: Digital Simulation of Torsional Disk Systems in LabVIEW

Rotational Motion. Figure 1: Torsional harmonic oscillator. The locations of the rotor and fiber are indicated.

PHYSICS LAB Experiment 9 Fall 2004 THE TORSION PENDULUM

Rectilinear System. Introduction. Hardware

Inverted Pendulum System

Position Control Experiment MAE171a

EAS 535 Laboratory Exercise Weather Station Setup and Verification

MECHANICS LAB AM 317 EXP 4 TORSION OF CIRCULAR RODS

The Torsion Pendulum (One or two weights)

Physical Pendulum Torsion Pendulum

Coulomb s Law. Coloumb s law Appratus Assembly

Physical Pendulum, Torsion Pendulum

Lab 10 - Harmonic Motion and the Pendulum

Lab 9 - Harmonic Motion and the Pendulum

Experiment Two (2) Torsional testing of Circular Shafts

Lab M4: The Torsional Pendulum and Moment of Inertia

30th International Physics Olympiad. Padua, Italy. Experimental competition

Centripetal Force Lab

Lab 9. Rotational Dynamics

The Torsion Pendulum

Experiment A11 Chaotic Double Pendulum Procedure

Number of solutions of a system

Name Date: Course number: MAKE SURE TA & TI STAMPS EVERY PAGE BEFORE YOU START. Grade: EXPERIMENT 4

OSCILLATIONS OF A SPRING-MASS SYSTEM AND A TORSIONAL PENDULUM

Project 3: Pendulum. Physics 2300 Spring 2018 Lab partner

Lab 6 - Electron Charge-To-Mass Ratio

Parts II-V Sabbatical Leave Report

Lab 11: Rotational Dynamics

SHM Simple Harmonic Motion revised May 23, 2017

Week 14 The Simple Pendulum

Lab 9. Rotational Dynamics

NOTE To improve the TA to class ratio, two groups will perform this experiment at one time. Group times are listed on the class website.

Human Arm. 1 Purpose. 2 Theory. 2.1 Equation of Motion for a Rotating Rigid Body

Rotational Motion. 1 Purpose. 2 Theory 2.1 Equation of Motion for a Rotating Rigid Body

SRV02-Series Rotary Experiment # 1. Position Control. Student Handout

Physics 1020 Experiment 6. Equilibrium of a Rigid Body

ENERGY AND TIME CONSTANTS IN RC CIRCUITS By: Iwana Loveu Student No Lab Section: 0003 Date: February 8, 2004

EE 4443/5329. LAB 3: Control of Industrial Systems. Simulation and Hardware Control (PID Design) The Torsion Disks. (ECP Systems-Model: 205)

Experiment 6. Rotational Motion

Lab 5a: Magnetic Levitation (Week 1)

Lab 6 - ELECTRON CHARGE-TO-MASS RATIO

Experiment 14 It s Snow Big Deal

Structural Metals Lab 1.2. Torsion Testing of Structural Metals. Standards ASTM E143: Shear Modulus at Room Temperature

Experiment 5. Simple Harmonic Motion

A SHORT INTRODUCTION TO ADAMS

Measuring the Universal Gravitational Constant, G

Purpose: Materials: WARNING! Section: Partner 2: Partner 1:

The Cavendish Experiment

Lab 5 - ELECTRON CHARGE-TO-MASS RATIO

Lab 5 - ELECTRON CHARGE-TO-MASS RATIO

PHY 123 Lab 6 - Angular Momentum

Torsion Experiment. Encoder #3 ( 3 ) Third encoder/disk for Model 205a only. Figure 1: ECP Torsion Experiment

2: SIMPLE HARMONIC MOTION

Physics 4A Lab 11: MOMENT OF INERTIA Parts List

Dynamics Track. Magnetic Force Impulse and Momentum

Energy problems look like this: Momentum conservation problems. Example 8-1. Momentum is a VECTOR Example 8-2

SPH 4U Unit #1 Dynamics Topic #4: Experiment #2:Using an Inertial Balance (Teacher)

HW9 Concepts. Alex Alemi November 1, 2009

Rotational Inertia (Rotational Kinematics and Dynamics)

PHYSICS 107 FINAL EXAMINATION

Lab 11 - Free, Damped, and Forced Oscillations

Rotational Inertia (approximately 2 hr) (11/23/15)

Coupled Oscillators. 1 Introduction. 2 Theory. PHY 300 Lab 2 Fall 2012

Laboratory Manual Experiment NE02 - Rotary Motions Department of Physics The University of Hong Kong

Physics 2A Chapter 10 - Rotational Motion Fall 2018

LABORATORY 4: ROTATIONAL MOTION PLAYGROUND DYNAMICS: THE MERRY-GO-ROUND Written May-June 1993 by Melissa Wafer '95

Laboratory handouts, ME 340

Lab Exercise #3: Torsion

Laboratory handouts, ME 340

Department of Electrical and Computer Engineering. EE461: Digital Control - Lab Manual

LEP Coupled pendula

EXPERIMENT 7: ANGULAR KINEMATICS AND TORQUE (V_3)

Teacher s notes 35 Conservation of angular momentum (1)

Physics 8 Friday, October 20, 2017

Lab 6a: Pole Placement for the Inverted Pendulum

Hands-on Lab 3. System Identification with Experimentally Acquired Data

The student will experimentally determine the parameters to represent the behavior of a damped oscillatory system of one degree of freedom.

PHYS 2211L Final Examination Laboratory Simple Pendulum.

Kinematics. Become comfortable with the data aquisition hardware and software used in the physics lab.

Lecture PowerPoints. Chapter 10 Physics for Scientists and Engineers, with Modern Physics, 4 th edition Giancoli

Simple Harmonic Motion

Belt Tension Clamp. Drive Motor. Friction Brake. Load. Encoder 2. Drive. (4000 lines/rev incremental) Encoder 1. (4000 lines/rev incremental)

PHY 221 Lab 7 Work and Energy

Magnetic Torque Physics 2150 Experiment No. 11 University of Colorado

Calibration Routine. Store in HDD. Switch "Program Control" Ref 1/ Ref 2 Manual Automatic

Investigating Springs (Simple Harmonic Motion)

Uniform Circular Motion

LAB 01 Electrostatic Charge

Experiment 2 Random Error and Basic Statistics

Precalculations Individual Portion Correlation and Regression: Statistical Analysis of Trends

PS2 Lab 1: Measurement and Uncertainty Supplemental Fall 2013

a. Follow the Start-Up Procedure in the laboratory manual. Note the safety rules.

University of Utah Electrical & Computer Engineering Department ECE 3510 Lab 9 Inverted Pendulum

Rotary Motion Servo Plant: SRV02. Rotary Experiment #11: 1-DOF Torsion. 1-DOF Torsion Position Control using QuaRC. Student Manual

Physics 2001/2051 The Compound Pendulum Experiment 4 and Helical Springs

AERO 214. Lab II. Measurement of elastic moduli using bending of beams and torsion of bars

Lab 4 CAPACITORS & RC CIRCUITS

PHY 111L Activity 9 Moments of Inertia

Lecture PowerPoints. Chapter 8 Physics: Principles with Applications, 6 th edition Giancoli

Conservation of Linear Momentum

Transcription:

Chapter 1 Lab #3: System Identification of the Torsional Disk System Objective The purpose of this lab is to familiarize you with the functioning of the EPS Torsional Disk System (TDS) and learn how to perform a system identification on it. You have already done a somewhat heuristic version of this in the previous lab this time you will systematically identify the parameters in particular the parameters you cannot compute beforehand based on physical principles (e.g., the torsional spring constants, the inertia of the disk, and the dissipation constants). You will also need to establish the hardware gain for the system. Note that it will serve you well to be familiar with this process the four ECP units are somewhat different from each other and will typically change their parametric values over time, so you may find that you need to re-identify these systems as the lab progresses. (Hopefully you will not need to, however.) Note that this lab will be a two-week lab. Warning: Please do not break the TDS systems. If you have questions, or are unsure of a next step, please let us know. However, the most important things are: 1. never run the system while it is clamped down! If you follow this one rule, it is extremely unlikely (though sadly not impossible) that you will break the system; 2. do not twist the disks more than 30 degrees relative to each other as you can damage the torsional rod this way as well. 1

2CHAPTER 1. LAB #3: SYSTEM IDENTIFICATION OF THE TORSIONAL DISK SYSTEM 1.1 Pre-Lab Tasks These tasks must be completed and (the concrete portions) shown to either the TA or the instructor before you may use the hardware. Task: Read this entire document. Task: Read the software section of the lab manual (at this point you should have read the entire lab manual). Task: Model the bottom and top disk as second order systems assuming that the middle disk is clamped down. (You will clamp the middle disk while doing the system identification, so you will need this model.) Task: Write down the impulse response of the bottom disk and the top disk. What does this correspond to physically? Can you simulate it? Can you experimentally produce the impulse response? 1.2 Tasks 1.2.1 Task #1 Using the Hardware There are a number of tasks here that have to be done during the system identification process. The basic idea is that you will clamp the middle disk in order to separate the dynamics of the top disk from the bottom disk. You will then estimate the spring constants k 1 and k 2 by looking at the period of oscillation and you will estimate the dissipation constants by looking at the decay envelope of the system as oscillations die out. First, however, you need to be sure you can get data for the system. 1. Clamp the center disk and keep the hardware controller turned off. 2. Put four masses on the bottom disk and two masses on the top disk where the outer diameter of the masses touch 9.0 cm away from the center of the disk. (The rings in the disk are 1.0 cm apart.) 3. Test that you can read all three encoder values for a 10 second time period. 4. When you start the experiment in LabVIEW, the encoder should automatically zero so that all the encoders are at zero. Let us know if they don t. 5. Plot the output of one of the encoders. Keep in mind that the encoder will give you 16,000 counts for every revolution. (You should convert to radians.) 6. Save both the time data and encoder data for one of the encoders in a file. 7. Read your results back into LabVIEW and plot them.

1.2. TASKS 3 1.2.2 Task #2 Creating a System Identification Procedure There are several parameters you need to calculate to have a complete model of the ECP unit. These are: the inertias J 1, J 2, J 3 of the disks, the dissipation coefficients c 1, c 2, c 3, the spring constants k 1 and k 2, and lastly the hardware gain k hw that scales voltages from the FPGA to torque. For all that follows, assume that c 2 = c 3. Task: The inertia of each disk is equal to the inertia due to the brass weights plus the inertia of the unloaded disk. That is, J = J disk + nj brass where n is the number of weights on a given disk. For now, assume that J disk equals the value given in the lab manual. The brass weights have a mass (incl. bolt & nut) of 500g (±5g) and a diameter of 5.00cm (±0.02cm). Use this to calculate the inertia for the disks with the brass weights at the location described above. Task: Using the impulse response you calculated for both the bottom and top disk, how can you calculate the associated σ and ω d using experimental data? Task: Given σ and ω d, derive a formula for the dissipation constant c and the spring constant k for both the bottom disk and the top disk. This should now mean that you have a way to calculate J 1, J 2, J 3, c 1, c 3, and k 1, k 2. If you assume that c 2 = c 3 (which it roughly is), then you can calculate all these parameters from some data. 1.2.3 Task #3 System Identification Experiment Task: Discuss your system identification approach with the TA or instructor before taking data. Task: Clamp down the middle disk using the clamp provided. Task: Take the data you decided upon and calculate J 1, J 2, J 3, c 1, c 2, c 3, and k 1, k 2. Unclamp the ECP Unit NOW!!!!!

4CHAPTER 1. LAB #3: SYSTEM IDENTIFICATION OF THE TORSIONAL DISK SYSTEM 1.2.4 Task #4 System Identification Results Write down the values of the parameters you computed here. Variable J 1 J 2 J 3 c 1 c 2 c 3 k 1 k 2 Value This is probably a good potential stopping point for day one. 1.2.5 Task #5 Hardware Gain Task: Decide on a method of calculating the hardware gain k h. Discuss with the instructor or TA Task: Collect data from experiment authorized by the Instructor and calculate k h. Task: Is the relationship between voltage and output torque really a linear relationship? (I.e., is F really a constant?) If it is not linear, is it close enough to linear? Why/why V not? 1.2.6 Task #6 System Identification Analysis You now have a nominally identified system! The question is whether these parameters are enough to give you a good model of what the system actually does. Task: Use your model of the system to simulate the system with the correct parameters you have just computed. Task: Design two experiments that you can use to verify your model against the experiment. One should involve no applied torque (just setting the intial conditions) and the other should involve an applied torque. Task: We assumed the inertia J based on theory and given values rather than data and then calculated k and c using J. Design an experiment to calculate the values of all three J, k, and c using data or analytically justify why it is unnecessary. Task: How close is your model to the real system? Describe what differences there are. Can they be fixed? If not, how will they affect the controller design?

1.2. TASKS 5 This problem is open-ended. You need to justify to the best of your ability the fact that your model adequately represents the real system. Task: Lastly, decide on a way to approximate the error in your estimates for the parameters in the system (J i c i, k i, k hw ).