Department of Mechanical Engineering

Similar documents
ME 3210 Mechatronics II Laboratory Lab 4: DC Motor Characteristics

2.004 Dynamics and Control II Spring 2008

Quanser NI-ELVIS Trainer (QNET) Series: QNET Experiment #02: DC Motor Position Control. DC Motor Control Trainer (DCMCT) Student Manual

DcMotor_ Model Help File

Rotary Motion Servo Plant: SRV02. Rotary Experiment #01: Modeling. SRV02 Modeling using QuaRC. Student Manual

3 Lab 3: DC Motor Transfer Function Estimation by Explicit Measurement

FEEDBACK CONTROL SYSTEMS

Experiment 5. Simple Harmonic Motion

Manufacturing Equipment Control

Positioning Servo Design Example

Prepare for this experiment!

Laboratory 11 Control Systems Laboratory ECE3557. State Feedback Controller for Position Control of a Flexible Joint

ECE 5670/6670 Lab 8. Torque Curves of Induction Motors. Objectives

Experiment A11 Chaotic Double Pendulum Procedure

MECHATRONICS ENGINEERING TECHNOLOGY. Modeling a Servo Motor System

Solved Problems. Electric Circuits & Components. 1-1 Write the KVL equation for the circuit shown.

Prepare for this experiment!

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

Lab 3: Quanser Hardware and Proportional Control

Mechatronic System Case Study: Rotary Inverted Pendulum Dynamic System Investigation

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

Experiment AM Angular Momentum

Inverted Pendulum System

Class #12: Experiment The Exponential Function in Circuits, Pt 1

Laboratory Exercise M-2 Power measurements

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

EDEXCEL NATIONALS UNIT 5 - ELECTRICAL AND ELECTRONIC PRINCIPLES. ASSIGNMENT No. 3 - ELECTRO MAGNETIC INDUCTION

2002 Prentice Hall, Inc. Gene F. Franklin, J. David Powell, Abbas Emami-Naeini Feedback Control of Dynamic Systems, 4e

Mechatronics Engineering. Li Wen

Physics 1020 Experiment 6. Equilibrium of a Rigid Body

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

1. Write the symbolic representation and one possible unit for angular velocity, angular acceleration, torque and rotational inertia.

MATHEMATICAL MODELING OF OPEN LOOP PMDC MOTOR USING MATLAB/SIMULINK

PHYSICS 122 Lab EXPERIMENT NO. 6 AC CIRCUITS

Texas A & M University Department of Mechanical Engineering MEEN 364 Dynamic Systems and Controls Dr. Alexander G. Parlos

DC motors. 1. Parallel (shunt) excited DC motor

Lab 11: Rotational Dynamics

Coupled Drive Apparatus Modelling and Simulation

Pre-Lab Exercise Full Name:

Prepare for this experiment!

EXPERIMENT 7: ANGULAR KINEMATICS AND TORQUE (V_3)

Control of Manufacturing Processes

Dynamic Characterization Results. Table of Contents. I. Introduction

System Parameters and Frequency Response MAE 433 Spring 2012 Lab 2

Experiment 4. RC Circuits. Observe and qualitatively describe the charging and discharging (decay) of the voltage on a capacitor.

In this experiment, a motor-generator combination serves as a first-order system with a voltage input V in and a voltage output V out.

MCE380: Measurements and Instrumentation Lab. Chapter 5: Electromechanical Transducers

M61 1 M61.1 PC COMPUTER ASSISTED DETERMINATION OF ANGULAR ACCELERATION USING TORQUE AND MOMENT OF INERTIA

Model of a DC Generator Driving a DC Motor (which propels a car)

LAB 8: ROTATIONAL DYNAMICS

Automatic Control Systems. -Lecture Note 15-

Lab 4 RC Circuits. Name. Partner s Name. I. Introduction/Theory

Lab 9. Rotational Dynamics

Overview of motors and motion control

THE REACTION WHEEL PENDULUM

PHY 123 Lab 6 - Angular Momentum

Physics 401 Classical Physics Laboratory. Experiment 5. Transients and Oscillations in RLC Circuits. I. Introduction II. Theory...

Elementary Theory of DC Permanent Magnet Motors

Dynamic Self Assembly of Magnetic Colloids

Mechatronics II Laboratory EXPERIMENT #1: FORCE AND TORQUE SENSORS DC Motor Characteristics Dynamometer, Part I

Center of Gravity Pearson Education, Inc.

Driven Harmonic Oscillator

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

ENSC387: Introduction to Electromechanical Sensors and Actuators LAB 3: USING STRAIN GAUGES TO FIND POISSON S RATIO AND YOUNG S MODULUS

Lab 9 - Rotational Dynamics

A METHOD FOR EVALUATION OF THE CHAIN DRIVE EFFICIENCY

LAB 11: FREE, DAMPED, AND FORCED OSCILLATIONS

Torques and Static Equilibrium

Modeling and Simulation Revision III D R. T A R E K A. T U T U N J I P H I L A D E L P H I A U N I V E R S I T Y, J O R D A N

The basic principle to be used in mechanical systems to derive a mathematical model is Newton s law,

POLYTECHNIC UNIVERSITY Electrical Engineering Department. EE SOPHOMORE LABORATORY Experiment 2 DC circuits and network theorems

Revision Guide for Chapter 15

A FORCE BALANCE TECHNIQUE FOR MEASUREMENT OF YOUNG'S MODULUS. 1 Introduction

Newton s Second Law. Computer with Capstone software, motion detector, PVC pipe, low friction cart, track, meter stick.

Mechanical Oscillations

6) Motors and Encoders

DC-motor modelling and parameter identification

Capacitance Measurement

Mathematical Modeling and Dynamic Simulation of DC Motors using MATLAB/Simulink Environment

PHYSICS LAB Experiment 9 Fall 2004 THE TORSION PENDULUM

2.010 Fall 2000 Solution of Homework Assignment 1

13-Nov-2015 PHYS Rotational Inertia

DC Motor Position: System Modeling

(a) Torsional spring-mass system. (b) Spring element.

State Feedback Controller for Position Control of a Flexible Link

1 M62 M62.1 CONSERVATION OF ANGULAR MOMENTUM FOR AN INELASTIC COLLISION

SRV02-Series Rotary Experiment # 7. Rotary Inverted Pendulum. Student Handout

Lab 7: EC-5, Faraday Effect Lab Worksheet

Never switch on the equipment without the assistants explicit authorization!

The Control of an Inverted Pendulum

UNIVERSITY OF WASHINGTON Department of Aeronautics and Astronautics

Practical 1 RC Circuits

Example: DC Motor Speed Modeling

Lab 11 Simple Harmonic Motion A study of the kind of motion that results from the force applied to an object by a spring

E102. Study of the magnetic hysteresis

τ = (Force)(lever arm) #

QNET DC Motor Control

Magnetic Fields INTRODUCTION. The Hall Effect

ECE 220 Laboratory 4 Volt Meter, Comparators, and Timer

WHAT A SINGLE JOINT IS MADE OF RA

Transcription:

Department of Mechanical Engineering 2.010 CONTROL SYSTEMS PRINCIPLES Laboratory 2: Characterization of the Electro-Mechanical Plant Introduction: It is important (for future lab sessions) that we have anadequate model, and numerical values for the parameters of the electro-mechanical motor/load plant at your lab station. In this session your goal is make measurements on the various components of the system and to determine the parameters. The specifc objectives are: To measure the gain K a of the servo-amplifier. To measure the motor torque constant K m. To estimate and measure the shaft/load moment of inertia J. To investigate and characterize the the rotational friction characteristics of the motor shaft and bearings. To measure the tachometer gain constant K t. Preparation: Review the Aerotech 1135 DC servomotor specifications. Also you can save time in the lab by sketching the step responses asked for in part (a) of the Mechanical Properties section below - Is the shaft friction viscous? Measurements: Amplifier Gain Constant K a : The servo-amplifier is a voltage-controlled current-source, that is it generates an output current that is proportional to the voltage that is applied at the BNC input connector. The amplifier will adjust its output voltage to maintain the output current (up to its saturation limits of ±40 volts). Within the linear range the input/output relationship is I out (t) =KaVin(t) The task is to measure the gain constant K a. 1

Procedure: Use the Virtual Bench Function Generator to generate a steady (dc) voltage by using the Offset control. Connect the D/A output to the servo-amplfier input. Make sure the amplifier is turned off and disconnect the servo-motor from the red and black terminals. Connect the Wavetek DMM using its 20 amp current input terminal. Set the meter to the AMP range and press the yellow button to select dc measurements. Note: Be careful making these connections you can damage the DVM and/or the amplifier through incorrect connections. The nominal amplifier gain is K a = 2 A/V, and the maximum sustained current that the amplifier can supply is 5 A. Select an appropriate input voltage and turn on the function generator. Measure the current and calculate the gain constant in the space below. The Motor Torque Constant For a permanent-magnet dc motor the torque produced is proportional to the armature current: T (t) = K m I(t) The task is to measure the torque constant K m. (Note that the Aerotech spec sheet calls this quantity K t.) Procedure Reconnect the motor to the servo-amp. You are given a digital postage scale and a lever arm that clamps on to the aluminum inertial load. The function generator may be used to generate a given motor current, and the indicated mass shown on the scale may be used to calculate the force applied by the lever arm, and hence the torque. 2

Note: In measurements such as this it is common to apply a dither signal to overcome any stiction in the bearings or the scale. We suggest that you set the function generator to add a 0.25 volt sinusoid at approximately 30 Hz to the dc value you use in order to minimize stiction effects. Use the function generator to measure the indicated mass at output voltages of 0, -1, -2, -3, -4 volts. Note: Be very careful about the polarity of the voltage a positive voltage will cause the motor to rotate in the wrong direction. On your Windows NT desktop you will find afolder named 2.010 Files. Open the folder and then open the Lab 2 folder. Open the Excel file Motor Calibration and enter your data into the spreadsheet, which will plot the torque/current relationship and fit a sraight line to it. The slope of the line is the torque constant K m. Print the spreadsheet and graph on a single page (attach it) and enter the result below. Compare your measured value with the manufacturer s quoted value from the data sheet. The Tachometer Gain Constant The tachometer serves as the angular velocity sensor for closed-loop control. It is an electromagnetic transducer that generates a voltage that is directly proportional to the angular velocity Ω of the shaft. v t = K t Ω(t) The task is to measure the constant K t for your motor. Procedure: With the setup as before, remove the torque monitoring lever arm and connect your DMM to the tachometer BNC connector on the motor terminal box. Apply a small dc voltage using the function generator and let the motor spin. The lab instructor will help you to measure the angular velocity with a non-contacting optical 3

tachometer. Record both the measured speed and the tachometer voltage and compute the gain constant K t. Compare your measured value with the manufacturer s quoted value from the data sheet. Motor Mechanical Properties (Shaft Inertia and Friction) Our analyses of motor behavior have assumed a linear lumped parameter model of the mechanical system (moment of inerta J and viscous friction B). We now test the assumption of viscous friction and make measurements of the parameters. (a) Is the shaft friction viscous? Consider two possibilities, (i) the frictional torque T f is viscous in nature, that is T f = BΩ, in which case the differential equation describing the angular velocity is: J dω dt + BΩ = T (t) (1) where J is the shaft moment of inertia, B is the viscous coefficient, and T is the motor torque, or (ii) the friction is Coulomb (or static) in nature, that is T f = sgn(ω)k f and depends only on the sign of the shaft velocity. (The signum function sgn() ensures that the the frictional torque opposes the motion.) In this case J dω dt = T (t) T f (2) In the space below make sketches of the form of the angular velocity response you would expect from a step in the applied torque T for each of the two cases. 4

5

Procedure: Set up the function generator to generate a 10% duty cycle, 1 volt unipolar square wave with a 2 second period as follows: Frequency 0.5 Hz Duty Cycle 10 15% Amplitude 0.5 V Offset 0.5 V Use the square wave to drive the motor, and record the square wave on Ch. 1 of the oscilloscope, and the angular velocity Ω from the tachometer on Ch. 2 of the scope. Adjust the duty cycle to ensure that the motor comes to rest between pulses. Which model of the friction best describes the observed velocity response? Write your answer with reasons below: (b) Determine the Moment of Inertia: Assume from this point that the shaft friction is purely Coulomb in nature, that is the system is described by Eq. (2). Our task is to estimate J and T f from the measured angular velocity response. 6

Consider the two regions of the response. In the first the generator voltage is 1 Volt, the shaft is accelerating and the equation of motion is Ω 1 = dω dt = 1 J (K ak m V T f ) (3) where V is the volltage (1 Volt). In the second ( coast-down ) region where the voltage is zero there is no applied torque and the equation becomes Eqs. (3) and (4) may be combined to solve for J Ω 2 = dω dt = 1 J T f (4) J = K ak m V Ω 1 Ω 2 (5) Use the oscilloscope to measure the slopes of the two regions of the response. (We suggest you use the cursors and the dv and dt measuremnts). Calculate the value of J below: To verify your estimate of J, calculate the value from the dimensions of the aluminumwheelandthemotorshaftasfollows: Thediameterofthewheelis76mm, its length is 76 mm, and the density of aluminum is 2600 kg/m 3. The moment of inertia of a disk is J disk = mr 2 /2. The total inertia is J = J disk + J shaft where J shaft isspecified in the specification sheet. Compute the shaft inertia in the space below: 7

(c) Determine the Coulomb Friction Torque: Use Eq. (2) to estimate the friction torque T f from your measurements. Compare the value with that given in the spec sheet. 8

Summary: Summarize your measured values of the electo-mechanical plant parameters below (with units): Amplifier Gain Constant (K a ): Motor Torque Constant (K m ): Load Inertia (J): Coulomb Friction Torque (T f ): Tahometer Gain Constant (K t ): 9