Manufacturing Equipment Modeling
|
|
|
- Basil Tyler
- 9 years ago
- Views:
Transcription
1 QUESTION 1 For a linear axis actuated by an electric motor complete the following: a. Derive a differential equation for the linear axis velocity assuming viscous friction acts on the DC motor shaft, leadscrew, and linear axis (i.e., B m 0, B l 0, and b a 0) and that the motor has velocity feedback such that the input voltage to the amplifier is e(t) = e c (t) K tach ω m (t). Include the axis disturbance force, but do not include motor electrical dynamics or Coulomb friction torques acting on the motor shaft or leadscrew. b. Determine the time constant for this system. c. For a constant command voltage with magnitude E c and a constant disturbance load with magnitude F L, determine the steady state velocity. d. Determine the steady state gains from axis velocity to command voltage and from axis velocity to load force. e. Draw a block diagram of the electric linear axis system. QUESTION 2 For a spindle actuated by an electric motor complete the following: a. Derive a differential equation for the spindle angular velocity assuming viscous friction acts on the motor and spindle and that the motor has velocity feedback such that the input
2 voltage to the amplifier is e(t) = e c (t) K tach ω m (t). Include the spindle load torque, but do not include motor electrical dynamics or nonlinear friction torques. b. Determine the spindle system time constant. c. For a constant command voltage with magnitude E c and a constant load torque with magnitude T L, determine the steady state angular velocity. d. Determine the steady state gains from spindle angular velocity to command voltage and from spindle angular velocity to load torque. e. Draw a block diagram of the electric spindle system. QUESTION 3 Two trials are run for a spindle system. The outputs are given in Figure 1. Approximate the spindle system model parameters (i.e., τ, K, and K d ) for the model given in equation (1). () t + ω ( t) = Ke ( t) K T ( t) τω (1) s s c d d Page 2
3 spindle speed (rad/s) T d = 0 N m T d = 25 N m time (s) Figure 1: Spindle System Output with e c (t) = 8 V. QUESTION 4 For a rotational axis actuated by a hydraulic motor complete the following: a. Derive differential equations relating rotational axis angular velocity and load pressure to valve displacement, disturbance torque, and motor shaft Coulomb friction. Include motor shaft and fluid viscous friction, fluid Coulomb friction, leakage effects, and rotational axis disturbance torque. b. For a constant command voltage, disturbance torque, and motor Coulomb friction torque, determine the steady state angular velocity and load pressures. c. Determine the steady state gains from axis angular velocity to command voltage, disturbance torque, and motor Coulomb friction. d. Determine the steady state gains from load pressure to command voltage, disturbance torque, and motor Coulomb friction. Page 3
4 e. Draw a block diagram of the hydraulic rotational axis system. QUESTION 5 A spindle has a mass moment of inertia of J s = kg m 2 and is connected to a DC motor having the following parameters: J m = kg m 2, R = 5 Ω, K t = 0.7 N m/a, K v = 0.7 V/(rad/s), and K a = 30. The maximum command voltage is e c = 10 V. Complete the following: a. Select the gear gain K s such that the maximum steady state spindle speed, without disturbance, will be ω ss 250 rad/s and the maximum change in spindle speed due to a disturbance torque of 10 N m will be 10 rad/s. b. Determine the time constant. QUESTION 6 For a linear axis actuated by an electric motor complete the following a. Derive a differential equation relating linear axis velocity to command voltage, disturbance force, DC motor shaft Coulomb friction, and leadscrew Coulomb friction. Include motor shaft, leadscrew, and linear axis viscous friction and axis disturbance force, but do not include motor electrical dynamics. b. Determine the linear axis system time constant. c. For a constant command voltage, disturbance force, and Coulomb friction torques, determine the steady state velocity. Page 4
5 d. Determine the steady state gains from axis velocity to command voltage, disturbance force, motor Coulomb friction, and leadscrew Coulomb friction. e. Draw a block diagram of the electric linear axis system. QUESTION 7 A hydraulic rotational axis has the following parameters: J m = 0.6 kg m 2, J r = 10 kg m 2, V 0 = 0.2 m 3, β = 10 9 N/m 2, D m = 10 2 m 3 /rad, K r = 0.2, K c = 10 8 m 5 /(N s), and K q = 3 m 2 /s. Complete the following: a. Using the Euler method, derive first order difference equations for the axis angular position, axis angular velocity, and load pressure. b. For a constant valve displacement of 10 mm and a disturbance torque of 10 4 sin(100t) N m, where t is time in s, create a numerical simulation and, on separate graphs, plot the axis angular position, axis angular velocity, load pressure, and load flow versus time. All initial conditions are zero. QUESTION 8 A hydraulic rotational axis system has the following parameters: J m = 0.6 kg m 2, B m = 4 N m/(rad/s), V 0 = 0.5 m 3, β = 10 9 N/m 2, D m = 10 4 m 3 /rad, K c = 10 8 m 5 /(N s), K q = 30 m 2 /s, J r = 10 3 kg m 2, B r = 1 N m/(rad/s), and K r = 0.7. Complete the following: a. Using the Euler method, derive first order difference equations for the axis angular position, axis angular velocity, and load pressure. Page 5
6 b. For the valve displacement shown in Figure 1 and a constant disturbance torque of 50 N m, create a numerical simulation and, on separate graphs, plot the axis angular position, axis angular velocity, load pressure, and load flow versus time. All initial conditions are zero. x v 5 mm 0 mm 0 s 1 s t Figure 1 QUESTION 9 An electric drive spindle has the following parameters: J m = 10 2 kg m 2, R = 5 Ω, K t = 0.5 N m/a, K v = 0.5 V/(rad/s), K a = 30, L = 0.1 H, J s = 4 kg m 2, and K s = 0.1. The current is limited to ±10 A. Complete the following: a. Symbolically derive a differential equation relating spindle angular velocity to command voltage and disturbance torque, a transfer function relating spindle angular velocity to command voltage, and a transfer function relating spindle angular velocity to disturbance torque. Ignore all sources of viscous friction and Coulomb friction acting on the motor shaft. Page 6
7 b. Calculate the time constants numerically. c. Using the Euler method, symbolically derive difference equations to simulate the spindle angular velocity and current. d. Simulate the electric spindle system for e c (t) = 4 + sin(5t) V and T d = 0. On separate graphs, plot the spindle angular velocity and current versus time. All initial conditions are zero. QUESTION 10 An electric linear axis has the following parameters: J m = 10 3 kg m 2, R a = 7.5 Ω, K t = 0.9 N m/a, K v = 0.9 V/(rad/s), K a = 55, L a = H, J l = kg m 2, K l = 1, p = 20/(2000π) m/rad, m = 1000 kg. The current is limited to ±10 A. Complete the following: a. Symbolically derive a differential equation relating axis position to command voltage and load force, a transfer function relating axis position to command voltage, and a transfer function relating axis position to load force. Ignore all sources of viscous and nonlinear friction. b. Calculate the time constants numerically. c. Using the Euler method, symbolically derive difference equations to simulate the axis position, axis velocity, and armature current. d. Simulate the system for a square command voltage signal with an amplitude of 2 V and a frequency of 0.25 Hz, and and f L = 0. Run the simulation for 2 cycles and plot the axis position, axis velocity, motor torque, and armature current versus time on separate Page 7
8 graphs. A square signal may be generated by the function Asgn(sin(2πft)), where A is the amplitude and f is the frequency in Hz. All initial conditions are zero. QUESTION 11 A hydraulic rotational axis has the following parameters: J m = 0.6 kg m 2, J r = 10 kg m 2, V 0 = 0.2 m 3, and β = 10 9 N/m 2. Select the gear gain, volumetric displacement, flow gain, and flow pressure coefficient such that that system has a damping ratio of 2, a natural frequency of 100 rad/s, the angular velocity will change by 0.6 rad/s for a change in valve displacement of 10 mm, and the angular velocity will change by 1 rad/s for a change in disturbance torque applied to the rotational axis of 2500 N m. Neglect viscous damping in the motor and rotational axis. QUESTION 12 An empirical model of a powder feeder is given in equations (1) and (2). The unit of motor angular velocity is rpm and the unit of nozzle powder flow rate is gpm. Complete the following: a. Ignoring the nonlinear friction, symbolically determine a differential equation relating the powder flow rate to the command voltage. b. Ignoring the nonlinear friction, symbolically determine a transfer function relating the powder flow rate to the command voltage. c. The powder feeder has the following parameters: τ m = s, k m = 158 rpm/v, ω f = 98.8 rpm, τ p = s, k p = gpm/rpm, and t d = 1.98 s. Determine a set of difference equations, using Euler s method, to simulate the powder feeder. Simulate the powder Page 8
9 feeder for a command voltage e c (t) = 2sin(t). Plot the motor angular velocity and nozzle mass flow rate on separate graphs. All initial conditions are zero and e c (t) = 0 for t < 0. d. Ignoring the nonlinear friction, plot the magnitude and phase frequency plots for the transfer function derived in part b. () t + ( t) = sgn ( ) + k e ( t) τ ω ω ω ω (1) m m m f m m c ( ) + ( ) = ω ( ) τ mt mt k t t (2) p p m d QUESTION 13 For a spindle actuated by an electric motor complete the following: a. Derive a differential equation relating spindle angular velocity to command voltage, disturbance torque, and DC motor shaft Coulomb friction. Include motor shaft and spindle viscous friction and spindle disturbance torque, but do not include motor electrical dynamics. b. Determine the spindle system time constant. c. For a constant command voltage, disturbance torque, and Coulomb friction torque, determine the steady state angular velocity. d. Determine the steady state gain from spindle angular velocity to command voltage, disturbance torque, and motor Coulomb friction. e. Draw a block diagram of the spindle system. Page 9
DCMS DC MOTOR SYSTEM User Manual
DCMS DC MOTOR SYSTEM User Manual release 1.3 March 3, 2011 Disclaimer The developers of the DC Motor System (hardware and software) have used their best efforts in the development. The developers make
EDUMECH Mechatronic Instructional Systems. Ball on Beam System
EDUMECH Mechatronic Instructional Systems Ball on Beam System Product of Shandor Motion Systems Written by Robert Hirsch Ph.D. 998-9 All Rights Reserved. 999 Shandor Motion Systems, Ball on Beam Instructional
Active Vibration Isolation of an Unbalanced Machine Spindle
UCRL-CONF-206108 Active Vibration Isolation of an Unbalanced Machine Spindle D. J. Hopkins, P. Geraghty August 18, 2004 American Society of Precision Engineering Annual Conference Orlando, FL, United States
INSTRUMENTATION AND CONTROL TUTORIAL 2 ELECTRIC ACTUATORS
INSTRUMENTATION AND CONTROL TUTORIAL 2 ELECTRIC ACTUATORS This is a stand alone tutorial on electric motors and actuators. The tutorial is of interest to any student studying control systems and in particular
Motor Selection and Sizing
Motor Selection and Sizing Motor Selection With each application, the drive system requirements greatly vary. In order to accommodate this variety of needs, Aerotech offers five types of motors. Motors
DC motors: dynamic model and control techniques
DC motors: dynamic model and control techniques Luca Zaccarian Contents 1 Magnetic considerations on rotating coils 1 1.1 Magnetic field and conductors.......................... 1 1.2 The magneto-motive
Chapter 11 SERVO VALVES. Fluid Power Circuits and Controls, John S.Cundiff, 2001
Chapter 11 SERVO VALVES Fluid Power Circuits and Controls, John S.Cundiff, 2001 Servo valves were developed to facilitate the adjustment of fluid flow based on the changes in the load motion. 1 Typical
Controller Design in Frequency Domain
ECSE 4440 Control System Engineering Fall 2001 Project 3 Controller Design in Frequency Domain TA 1. Abstract 2. Introduction 3. Controller design in Frequency domain 4. Experiment 5. Colclusion 1. Abstract
Power Electronics. Prof. K. Gopakumar. Centre for Electronics Design and Technology. Indian Institute of Science, Bangalore.
Power Electronics Prof. K. Gopakumar Centre for Electronics Design and Technology Indian Institute of Science, Bangalore Lecture - 1 Electric Drive Today, we will start with the topic on industrial drive
EE 402 RECITATION #13 REPORT
MIDDLE EAST TECHNICAL UNIVERSITY EE 402 RECITATION #13 REPORT LEAD-LAG COMPENSATOR DESIGN F. Kağan İPEK Utku KIRAN Ç. Berkan Şahin 5/16/2013 Contents INTRODUCTION... 3 MODELLING... 3 OBTAINING PTF of OPEN
Practice Exam Three Solutions
MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics Physics 8.01T Fall Term 2004 Practice Exam Three Solutions Problem 1a) (5 points) Collisions and Center of Mass Reference Frame In the lab frame,
Slide 10.1. Basic system Models
Slide 10.1 Basic system Models Objectives: Devise Models from basic building blocks of mechanical, electrical, fluid and thermal systems Recognize analogies between mechanical, electrical, fluid and thermal
Harmonic Drive acutator P r e c i s i o n G e a r i n g & M o t i o n C o n t r o l
D C S e r v o S y s t e m s RH Mini Series Total Motion Control Harmonic Drive acutator P r e c i s i o n G e a r i n g & M o t i o n C o n t r o l Precision Gearing & Motion Control DC SERVO ACTUATORS
Lab Session 4 Introduction to the DC Motor
Lab Session 4 Introduction to the DC Motor By: Professor Dan Block Control Systems Lab Mgr. University of Illinois Equipment Agilent 54600B 100 MHz Ditizing Oscilloscope (Replacement model: Agilent DSO5012A
Electric Motors and Drives
EML 2322L MAE Design and Manufacturing Laboratory Electric Motors and Drives To calculate the peak power and torque produced by an electric motor, you will need to know the following: Motor supply voltage,
ANALYTICAL METHODS FOR ENGINEERS
UNIT 1: Unit code: QCF Level: 4 Credit value: 15 ANALYTICAL METHODS FOR ENGINEERS A/601/1401 OUTCOME - TRIGONOMETRIC METHODS TUTORIAL 1 SINUSOIDAL FUNCTION Be able to analyse and model engineering situations
Physics 1A Lecture 10C
Physics 1A Lecture 10C "If you neglect to recharge a battery, it dies. And if you run full speed ahead without stopping for water, you lose momentum to finish the race. --Oprah Winfrey Static Equilibrium
226 Chapter 15: OSCILLATIONS
Chapter 15: OSCILLATIONS 1. In simple harmonic motion, the restoring force must be proportional to the: A. amplitude B. frequency C. velocity D. displacement E. displacement squared 2. An oscillatory motion
AP Physics C. Oscillations/SHM Review Packet
AP Physics C Oscillations/SHM Review Packet 1. A 0.5 kg mass on a spring has a displacement as a function of time given by the equation x(t) = 0.8Cos(πt). Find the following: a. The time for one complete
dspace DSP DS-1104 based State Observer Design for Position Control of DC Servo Motor
dspace DSP DS-1104 based State Observer Design for Position Control of DC Servo Motor Jaswandi Sawant, Divyesh Ginoya Department of Instrumentation and control, College of Engineering, Pune. ABSTRACT This
Unit - 6 Vibrations of Two Degree of Freedom Systems
Unit - 6 Vibrations of Two Degree of Freedom Systems Dr. T. Jagadish. Professor for Post Graduation, Department of Mechanical Engineering, Bangalore Institute of Technology, Bangalore Introduction A two
Objectives. Electric Current
Objectives Define electrical current as a rate. Describe what is measured by ammeters and voltmeters. Explain how to connect an ammeter and a voltmeter in an electrical circuit. Explain why electrons travel
Brush DC Motor Basics. by Simon Pata Business Unit Manager, Brushless DC
thinkmotion Brush DC Motor Basics by Simon Pata Business Unit Manager, Brushless DC Ironless DC Motor Basics Technical Note Brushed DC ironless motors are found in a large variety of products and applications
Torque and Rotary Motion
Torque and Rotary Motion Name Partner Introduction Motion in a circle is a straight-forward extension of linear motion. According to the textbook, all you have to do is replace displacement, velocity,
Magnetic electro-mechanical machines
Magnetic electro-mechanical machines Lorentz Force A magnetic field exerts force on a moving charge. The Lorentz equation: f = q(e + v B) f: force exerted on charge q E: electric field strength v: velocity
11. Rotation Translational Motion: Rotational Motion:
11. Rotation Translational Motion: Motion of the center of mass of an object from one position to another. All the motion discussed so far belongs to this category, except uniform circular motion. Rotational
Precise Modelling of a Gantry Crane System Including Friction, 3D Angular Swing and Hoisting Cable Flexibility
Precise Modelling of a Gantry Crane System Including Friction, 3D Angular Swing and Hoisting Cable Flexibility Renuka V. S. & Abraham T Mathew Electrical Engineering Department, NIT Calicut E-mail : [email protected],
Drivetech, Inc. Innovations in Motor Control, Drives, and Power Electronics
Drivetech, Inc. Innovations in Motor Control, Drives, and Power Electronics Dal Y. Ohm, Ph.D. - President 25492 Carrington Drive, South Riding, Virginia 20152 Ph: (703) 327-2797 Fax: (703) 327-2747 [email protected]
D660 Series Servo-Proportional Control Valves with Integrated Electronics ISO 4401 Size 05 to 10
D660 Series Servo-Proportional Control Valves with Integrated Electronics ISO 4401 Size 05 to 10 OVERVIEW D660 Section Page MOOG SERVO-PROPORTIONAL CONTROL VALVES Overview 2 3 Technical Data 4 5 Electronics
Applications of Second-Order Differential Equations
Applications of Second-Order Differential Equations Second-order linear differential equations have a variety of applications in science and engineering. In this section we explore two of them: the vibration
Servo Motor Selection Flow Chart
Servo otor Selection Flow Chart START Selection Has the machine Been Selected? YES NO Explanation References etermine the size, mass, coefficient of friction, and external forces of all the moving part
Electro-Hydraulic Servo Valve Construction, Models and Use
Electro-Hydraulic Servo Valve Construction, Models and Use From Merritt, H. E., Hydraulic Control Systems, J. Wiley, 1967. The input to an electro-hydraulic (EH) servovalve is typically a current or a
EXPERIMENT: MOMENT OF INERTIA
OBJECTIVES EXPERIMENT: MOMENT OF INERTIA to familiarize yourself with the concept of moment of inertia, I, which plays the same role in the description of the rotation of a rigid body as mass plays in
Electric Rotary Actuator - On/Off or programmable control actuator
Electric Rotary Actuator - On/Off or programmable control actuator Direct mounting on quarter-turn valves Manual override standard Corrosion resistant Adjustable limit switches Multi-voltage version Type
PHYS 101-4M, Fall 2005 Exam #3. MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.
PHYS 101-4M, Fall 2005 Exam #3 Name MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question. 1) A bicycle wheel rotates uniformly through 2.0 revolutions in
Center of Gravity. We touched on this briefly in chapter 7! x 2
Center of Gravity We touched on this briefly in chapter 7! x 1 x 2 cm m 1 m 2 This was for what is known as discrete objects. Discrete refers to the fact that the two objects separated and individual.
SYNCHRONOUS MACHINES
SYNCHRONOUS MACHINES The geometry of a synchronous machine is quite similar to that of the induction machine. The stator core and windings of a three-phase synchronous machine are practically identical
Physical Quantities, Symbols and Units
Table 1 below indicates the physical quantities required for numerical calculations that are included in the Access 3 Physics units and the Intermediate 1 Physics units and course together with the SI
Rotational Inertia Demonstrator
WWW.ARBORSCI.COM Rotational Inertia Demonstrator P3-3545 BACKGROUND: The Rotational Inertia Demonstrator provides an engaging way to investigate many of the principles of angular motion and is intended
Chapter 10 Rotational Motion. Copyright 2009 Pearson Education, Inc.
Chapter 10 Rotational Motion Angular Quantities Units of Chapter 10 Vector Nature of Angular Quantities Constant Angular Acceleration Torque Rotational Dynamics; Torque and Rotational Inertia Solving Problems
SOLID MECHANICS TUTORIAL MECHANISMS KINEMATICS - VELOCITY AND ACCELERATION DIAGRAMS
SOLID MECHANICS TUTORIAL MECHANISMS KINEMATICS - VELOCITY AND ACCELERATION DIAGRAMS This work covers elements of the syllabus for the Engineering Council exams C105 Mechanical and Structural Engineering
D634-P Series Direct Drive Proportional Valve with Integrated 24 V Electronics ISO 4401 Size 05
D634-P Series Direct Drive Proportional Valve with Integrated 24 V Electronics ISO 4401 Size 05 GENERAL SECTION PAGE MOOG SERVO- AND PROPORTIONAL CONTROL VALVES General 2 enefits and Functionality 3 General
Chapter 11. h = 5m. = mgh + 1 2 mv 2 + 1 2 Iω 2. E f. = E i. v = 4 3 g(h h) = 4 3 9.8m / s2 (8m 5m) = 6.26m / s. ω = v r = 6.
Chapter 11 11.7 A solid cylinder of radius 10cm and mass 1kg starts from rest and rolls without slipping a distance of 6m down a house roof that is inclined at 30 degrees (a) What is the angular speed
! n. Problems and Solutions Section 1.5 (1.66 through 1.74)
Problems and Solutions Section.5 (.66 through.74).66 A helicopter landing gear consists of a metal framework rather than the coil spring based suspension system used in a fixed-wing aircraft. The vibration
Application Information
Moog Components Group manufactures a comprehensive line of brush-type and brushless motors, as well as brushless controllers. The purpose of this document is to provide a guide for the selection and application
Advantages of Auto-tuning for Servo-motors
Advantages of for Servo-motors Executive summary The same way that 2 years ago computer science introduced plug and play, where devices would selfadjust to existing system hardware, industrial motion control
Physics 231 Lecture 15
Physics 31 ecture 15 Main points of today s lecture: Simple harmonic motion Mass and Spring Pendulum Circular motion T 1/f; f 1/ T; ω πf for mass and spring ω x Acos( ωt) v ωasin( ωt) x ax ω Acos( ωt)
Motors. 13/16 Siemens PM 21 2013
Motors Motor selection The is selected on the basis of the required torque, which is defined by the application, e.g. traveling drives, hoisting drives, test stands, centrifuges, paper and rolling mill
2.6. In-Laboratory Session. 2.6.1. QICii Modelling Module. Modelling. 2.6.1.1. Module Description
2.6. In-Laboratory Session 2.6.1. QICii Modelling Module 2.6.1.1. Module Description The main tool for this lab is the front panel of the module entitled Modelling in the QICii software, which should be
AP1 Oscillations. 1. Which of the following statements about a spring-block oscillator in simple harmonic motion about its equilibrium point is false?
1. Which of the following statements about a spring-block oscillator in simple harmonic motion about its equilibrium point is false? (A) The displacement is directly related to the acceleration. (B) The
Linear Motion vs. Rotational Motion
Linear Motion vs. Rotational Motion Linear motion involves an object moving from one point to another in a straight line. Rotational motion involves an object rotating about an axis. Examples include a
Motors and Generators
Motors and Generators Electro-mechanical devices: convert electrical energy to mechanical motion/work and vice versa Operate on the coupling between currentcarrying conductors and magnetic fields Governed
CORRECTION OF DYNAMIC WHEEL FORCES MEASURED ON ROAD SIMULATORS
Pages 1 to 35 CORRECTION OF DYNAMIC WHEEL FORCES MEASURED ON ROAD SIMULATORS Bohdan T. Kulakowski and Zhijie Wang Pennsylvania Transportation Institute The Pennsylvania State University University Park,
What Is Regeneration?
What Is Regeneration? Braking / Regeneration Manual Regeneration Overview Revision 1.0 When the rotor of an induction motor turns slower than the speed set by the applied frequency, the motor is transforming
Tips For Selecting DC Motors For Your Mobile Robot
Tips For Selecting DC Motors For Your Mobile Robot By AJ Neal When building a mobile robot, selecting the drive motors is one of the most important decisions you will make. It is a perfect example of an
Tennessee State University
Tennessee State University Dept. of Physics & Mathematics PHYS 2010 CF SU 2009 Name 30% Time is 2 hours. Cheating will give you an F-grade. Other instructions will be given in the Hall. MULTIPLE CHOICE.
Angular acceleration α
Angular Acceleration Angular acceleration α measures how rapidly the angular velocity is changing: Slide 7-0 Linear and Circular Motion Compared Slide 7- Linear and Circular Kinematics Compared Slide 7-
ACTUATOR DESIGN FOR ARC WELDING ROBOT
ACTUATOR DESIGN FOR ARC WELDING ROBOT 1 Anurag Verma, 2 M. M. Gor* 1 G.H Patel College of Engineering & Technology, V.V.Nagar-388120, Gujarat, India 2 Parul Institute of Engineering & Technology, Limda-391760,
PHYS 211 FINAL FALL 2004 Form A
1. Two boys with masses of 40 kg and 60 kg are holding onto either end of a 10 m long massless pole which is initially at rest and floating in still water. They pull themselves along the pole toward each
Modeling Mechanical Systems
chp3 1 Modeling Mechanical Systems Dr. Nhut Ho ME584 chp3 2 Agenda Idealized Modeling Elements Modeling Method and Examples Lagrange s Equation Case study: Feasibility Study of a Mobile Robot Design Matlab
Simple Harmonic Motion
Simple Harmonic Motion 1 Object To determine the period of motion of objects that are executing simple harmonic motion and to check the theoretical prediction of such periods. 2 Apparatus Assorted weights
Chapter 7 Homework solutions
Chapter 7 Homework solutions 8 Strategy Use the component form of the definition of center of mass Solution Find the location of the center of mass Find x and y ma xa + mbxb (50 g)(0) + (10 g)(5 cm) x
Review of First- and Second-Order System Response 1
MASSACHUSETTS INSTITUTE OF TECHNOLOGY DEPARTMENT OF MECHANICAL ENGINEERING 2.151 Advanced System Dynamics and Control Review of First- and Second-Order System Response 1 1 First-Order Linear System Transient
Pumps: Convert mechanical energy (often developed from electrical source) into hydraulic energy (position, pressure and kinetic energy).
HYDRAULIC MACHINES Used to convert between hydraulic and mechanical energies. Pumps: Convert mechanical energy (often developed from electrical source) into hydraulic energy (position, pressure and kinetic
Physics 9e/Cutnell. correlated to the. College Board AP Physics 1 Course Objectives
Physics 9e/Cutnell correlated to the College Board AP Physics 1 Course Objectives Big Idea 1: Objects and systems have properties such as mass and charge. Systems may have internal structure. Enduring
WINDER SYSTEMS GE Industrial Control Systems
WINDER SYSTEMS Systems Concepts Terminology GE Industrial Control Systems APPLICATION TECHNIQUES With a smooth metal surface material, a paper liner is sometimes wound with a coil. The paper is lightweight
D.C. Motors. Products and specifications subject to change without notice.
D.C. Motors Order/Technical Support - Tel: (8) 677-5 / FAX: (8) 677-865 / www.crouzet-usa.com / DC Motors Selection guide Gearbox Speed Torque max (Nm).5. Type of Gearbox 8 8 8. Power usable (w) Torque
Midterm Solutions. mvr = ω f (I wheel + I bullet ) = ω f 2 MR2 + mr 2 ) ω f = v R. 1 + M 2m
Midterm Solutions I) A bullet of mass m moving at horizontal velocity v strikes and sticks to the rim of a wheel a solid disc) of mass M, radius R, anchored at its center but free to rotate i) Which of
1115 4G SERIES GOVERNOR. 4-20 ma ANALOGUE DIGITAL SPEED SETTING
1115 4G SERIES GOVERNOR with 4-20 ma ANALOGUE & DIGITAL SPEED SETTING PO Box 28, 9300AA Roden, The Netherlands Tel: +31 505019888 Fax: +31 505013618 E-mail: [email protected] 1115 4G
Columbia University Department of Physics QUALIFYING EXAMINATION
Columbia University Department of Physics QUALIFYING EXAMINATION Monday, January 13, 2014 1:00PM to 3:00PM Classical Physics Section 1. Classical Mechanics Two hours are permitted for the completion of
Mathematical Modeling and Dynamic Simulation of a Class of Drive Systems with Permanent Magnet Synchronous Motors
Applied and Computational Mechanics 3 (2009) 331 338 Mathematical Modeling and Dynamic Simulation of a Class of Drive Systems with Permanent Magnet Synchronous Motors M. Mikhov a, a Faculty of Automatics,
Equivalent Spring Stiffness
Module 7 : Free Undamped Vibration of Single Degree of Freedom Systems; Determination of Natural Frequency ; Equivalent Inertia and Stiffness; Energy Method; Phase Plane Representation. Lecture 13 : Equivalent
System Modeling and Control for Mechanical Engineers
Session 1655 System Modeling and Control for Mechanical Engineers Hugh Jack, Associate Professor Padnos School of Engineering Grand Valley State University Grand Rapids, MI email: [email protected] Abstract
Problem Set 12: Kinetic Theory; Mechanical Equivalent of Heat Solutions
MASSACHUSETTS INSTITUTE OF TECHNOLOGY Department of Physics Physics 8.01T Fall Term 2004 Problem Set 12: Kinetic Theory; Mechanical Equivalent of Heat Solutions Problem 1: Isothermal Ideal Gas Atmosphere
FUZZY Based PID Controller for Speed Control of D.C. Motor Using LabVIEW
FUZZY Based PID Controller for Speed Control of D.C. Motor Using LabVIEW SALIM, JYOTI OHRI Department of Electrical Engineering National Institute of Technology Kurukshetra INDIA [email protected] [email protected]
Solution Derivations for Capa #11
Solution Derivations for Capa #11 1) A horizontal circular platform (M = 128.1 kg, r = 3.11 m) rotates about a frictionless vertical axle. A student (m = 68.3 kg) walks slowly from the rim of the platform
3600 s 1 h. 24 h 1 day. 1 day
Week 7 homework IMPORTANT NOTE ABOUT WEBASSIGN: In the WebAssign versions of these problems, various details have been changed, so that the answers will come out differently. The method to find the solution
EDEXCEL NATIONAL CERTIFICATE/DIPLOMA UNIT 5 - ELECTRICAL AND ELECTRONIC PRINCIPLES NQF LEVEL 3 OUTCOME 4 - ALTERNATING CURRENT
EDEXCEL NATIONAL CERTIFICATE/DIPLOMA UNIT 5 - ELECTRICAL AND ELECTRONIC PRINCIPLES NQF LEVEL 3 OUTCOME 4 - ALTERNATING CURRENT 4 Understand single-phase alternating current (ac) theory Single phase AC
MECHANICAL PRINCIPLES OUTCOME 4 MECHANICAL POWER TRANSMISSION TUTORIAL 1 SIMPLE MACHINES
MECHANICAL PRINCIPLES OUTCOME 4 MECHANICAL POWER TRANSMISSION TUTORIAL 1 SIMPLE MACHINES Simple machines: lifting devices e.g. lever systems, inclined plane, screw jack, pulley blocks, Weston differential
Experiment # 3: Pipe Flow
ME 05 Mechanical Engineering Lab Page ME 05 Mechanical Engineering Laboratory Spring Quarter 00 Experiment # 3: Pipe Flow Objectives: a) Calibrate a pressure transducer and two different flowmeters (paddlewheel
Fluid. Flu. Fluid Fluid. uid Power d Power P. Fluid Power P. Fluid Power. Fluid Power Power. d Power. Directional Cetop Valves DCV 03.
Catalogue Directional Cetop Valves DCV 03 Power Flu uid Power d Power P wer Power Power Power Power Power d Power Power Power ower Power Power wer Power Power P Power Power Powe d Power Power Power Power
MCE380: Measurements and Instrumentation Lab. Chapter 9: Force, Torque and Strain Measurements
MCE380: Measurements and Instrumentation Lab Chapter 9: Force, Torque and Strain Measurements Topics: Elastic Elements for Force Measurement Dynamometers and Brakes Resistance Strain Gages Holman, Ch.
ENERGY TRANSFER SYSTEMS AND THEIR DYNAMIC ANALYSIS
ENERGY TRANSFER SYSTEMS AND THEIR DYNAMIC ANALYSIS Many mechanical energy systems are devoted to transfer of energy between two points: the source or prime mover (input) and the load (output). For chemical
Series TMM Axial Piston Motor. Technical Information
Series TMM Axial Piston Motor Technical Information General Description GENERAL DESCRIPTION These motors are designed primarily to be combined with other products in closed circuit systems to transfer
HITACHI INVERTER SJ/L100/300 SERIES PID CONTROL USERS GUIDE
HITACHI INVERTER SJ/L1/3 SERIES PID CONTROL USERS GUIDE After reading this manual, keep it for future reference Hitachi America, Ltd. HAL1PID CONTENTS 1. OVERVIEW 3 2. PID CONTROL ON SJ1/L1 INVERTERS 3
Available online at www.sciencedirect.com Available online at www.sciencedirect.com
Available online at www.sciencedirect.com Available online at www.sciencedirect.com Procedia Procedia Engineering Engineering () 9 () 6 Procedia Engineering www.elsevier.com/locate/procedia International
Quadcopter Dynamics, Simulation, and Control Introduction
Quadcopter Dynamics, Simulation, and Control Introduction A helicopter is a flying vehicle which uses rapidly spinning rotors to push air downwards, thus creating a thrust force keeping the helicopter
PowerFlex Dynamic Braking Resistor Calculator
Application Technique PowerFlex Dynamic Braking Resistor Calculator Catalog Numbers 20A, 20B, 20F, 20G, 22A, 22B Important User Information Solid-state equipment has operational characteristics differing
Lecture 17. Last time we saw that the rotational analog of Newton s 2nd Law is
Lecture 17 Rotational Dynamics Rotational Kinetic Energy Stress and Strain and Springs Cutnell+Johnson: 9.4-9.6, 10.1-10.2 Rotational Dynamics (some more) Last time we saw that the rotational analog of
Loudspeaker Parameters. D. G. Meyer School of Electrical & Computer Engineering
Loudspeaker Parameters D. G. Meyer School of Electrical & Computer Engineering Outline Review of How Loudspeakers Work Small Signal Loudspeaker Parameters Effect of Loudspeaker Cable Sample Loudspeaker
APPENDIX A CONTROL VALVE TESTING PROCEDURES AND EQUATIONS FOR LIQUID FLOWS
APPENDIX A CONTROL VALVE TESTING PROCEDURES AND EQUATIONS FOR LIQUID FLOWS Section A.1. Flow Coefficients Definition The flow coefficient or pressure loss coefficient is used to relate the pressure loss
Machine Design II Prof. K.Gopinath & Prof. M.M.Mayuram. Module 2 - GEARS. Lecture 17 DESIGN OF GEARBOX
Module 2 - GEARS Lecture 17 DESIGN OF GEARBOX Contents 17.1 Commercial gearboxes 17.2 Gearbox design. 17.1 COMMERCIAL GEARBOXES Various commercial gearbox designs are depicted in Fig. 17.1 to 17.10. These
Dynamics of Offshore Wind Turbines
Proceedings of the Twenty-first (2011) International Offshore and Polar Engineering Conference Maui, Hawaii, USA, June 19-24, 2011 Copyright 2011 by the International Society of Offshore and Polar Engineers
Solution: Angular velocity in consistent units (Table 8.1): 753.8. Velocity of a point on the disk: Rate at which bits pass by the read/write head:
Problem P8: The disk in a computer hard drive spins at 7200 rpm At the radius of 0 mm, a stream of data is magnetically written on the disk, and the spacing between data bits is 25 μm Determine the number
Mounting instructions. Acceleration Transducer B12. B 26.B12.10 en
Mounting instructions Acceleration Transducer B12 B 26.B12.10 en B12 3 Contents Page Safety instructions.............................................. 4 1 Scope of supply..............................................
INSTRUMENTATION AND CONTROL TUTORIAL 3 SIGNAL PROCESSORS AND RECEIVERS
INSTRUMENTATION AND CONTROL TUTORIAL 3 SIGNAL PROCESSORS AND RECEIVERS This tutorial provides an overview of signal processing and conditioning for use in instrumentation and automatic control systems.
Useful Motor/Torque Equations for EML2322L
Useful Motor/Torque Equations for EML2322L Force (Newtons) F = m x a m = mass (kg) a = acceleration (m/s 2 ) Motor Torque (Newton-meters) T = F x d F = force (Newtons) d = moment arm (meters) Power (Watts)
An Industrial Case Study - Control of BeoSound 9000 Sledge System
An Industrial Case Study - Control of BeoSound 9000 Sledge System Zhenyu Yang Department of Computer Science and Engineering, Aalborg University Esbjerg, Niels Bohrs Vej 8, DK-6700 Esbjerg, Denmark. yangcs.aaue.dk
SERVO CONTROL SYSTEMS 1: DC Servomechanisms
Servo Control Sstems : DC Servomechanisms SERVO CONTROL SYSTEMS : DC Servomechanisms Elke Laubwald: Visiting Consultant, control sstems principles.co.uk ABSTRACT: This is one of a series of white papers
