Theory of Machines. Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering

Similar documents
How To Understand The Relationship Between A Body And A Joint

Chapter. 4 Mechanism Design and Analysis

Robot coined by Karel Capek in a 1921 science-fiction Czech play

ME Week 11 Introduction to Dynamic Simulation

Figure Cartesian coordinate robot

SYLLABUS MAE342 Dynamics of Machines (CRN: 12551) Term: Spring 2015

SOLID MECHANICS TUTORIAL MECHANISMS KINEMATICS - VELOCITY AND ACCELERATION DIAGRAMS

Fric-3. force F k and the equation (4.2) may be used. The sense of F k is opposite

Mechanics lecture 7 Moment of a force, torque, equilibrium of a body

Use Of Hoeken s And Pantograph Mechanisms For Carpet Scrapping Operations

Rules of Actuator and Guide Alignment in Linear Motion Systems

Chapter 10 Rotational Motion. Copyright 2009 Pearson Education, Inc.

MECHANICAL PRINCIPLES OUTCOME 4 MECHANICAL POWER TRANSMISSION TUTORIAL 1 SIMPLE MACHINES

Synthesis of Four Bar Mechanism for Polynomial Function Generation by Complex Algebra

Physics 2A, Sec B00: Mechanics -- Winter 2011 Instructor: B. Grinstein Final Exam

Unit 4 Practice Test: Rotational Motion

Center of Gravity. We touched on this briefly in chapter 7! x 2

Chapter 2 Lead Screws

KINEMATICS OF PARTICLES RELATIVE MOTION WITH RESPECT TO TRANSLATING AXES

Practice Exam Three Solutions

UNIT II Robots Drive Systems and End Effectors Part-A Questions

Equivalent Spring Stiffness

Modeling Mechanical Systems

Fig 1 Power Transmission system of Tractor

Design of a Universal Robot End-effector for Straight-line Pick-up Motion

Problem Set 1. Ans: a = 1.74 m/s 2, t = 4.80 s

CATIA V5 Tutorials. Mechanism Design & Animation. Release 18. Nader G. Zamani. University of Windsor. Jonathan M. Weaver. University of Detroit Mercy

Belt Drives and Chain Drives. Power Train. Power Train

Rotation: Moment of Inertia and Torque

C B A T 3 T 2 T What is the magnitude of the force T 1? A) 37.5 N B) 75.0 N C) 113 N D) 157 N E) 192 N

Linear Motion vs. Rotational Motion

Figure 1 - Delta Theta Input Selection

There are four types of friction, they are 1).Static friction 2) Dynamic friction 3) Sliding friction 4) Rolling friction

Using Design Accelerators in Autodesk Inventor

FUNdaMENTALS of Design Topic 4 Linkages Alexander Slocum 4-0

Animations in Creo 3.0

Module 5 Couplings. Version 2 ME, IIT Kharagpur

Sample Questions for the AP Physics 1 Exam

3 Work, Power and Energy

Design and Modeling of Fluid Power Systems ME 597/ABE 591 Lecture 5

freedom 3 Constraints on motion: degrees ot 3.1 Constraint in kinematic chains

11. Rotation Translational Motion: Rotational Motion:

Stirling Paatz of robot integrators Barr & Paatz describes the anatomy of an industrial robot.

Topics. Introduction Gear schematics Types of gears Measuring gears

Lecture 17. Last time we saw that the rotational analog of Newton s 2nd Law is

CAD/ CAM Prof. P. V. Madhusudhan Rao Department of Mechanical Engineering Indian Institute of Technology, Delhi Lecture No. # 03 What is CAD/ CAM

Gear Trains. Introduction:

Physics 1A Lecture 10C

ACTUATOR DESIGN FOR ARC WELDING ROBOT

Lecture L6 - Intrinsic Coordinates

Salem Community College Course Syllabus. Course Title: Physics I. Course Code: PHY 101. Lecture Hours: 2 Laboratory Hours: 4 Credits: 4

HW Set VI page 1 of 9 PHYSICS 1401 (1) homework solutions

Thermodynamic efficiency of an actuator that provides the mechanical movement for the driven equipments:

Scooter, 3 wheeled cobot North Western University. PERCRO Exoskeleton

Section. Tolerances. Aluminum Extrusion Manual. 4th Edition

Physics 160 Biomechanics. Angular Kinematics

PHY121 #8 Midterm I

Learning Autodesk. Modeling, Analysis and Animation SDC. Randy H. Shih. Better Textbooks. Lower Prices. PUBLICATIONS

Computer Aided Design (CAD), ME , JHU Professor Dan Stoianovici,

Midterm Solutions. mvr = ω f (I wheel + I bullet ) = ω f 2 MR2 + mr 2 ) ω f = v R. 1 + M 2m

Mechanical Reasoning Review

CHAPTER 6 WORK AND ENERGY

F N A) 330 N 0.31 B) 310 N 0.33 C) 250 N 0.27 D) 290 N 0.30 E) 370 N 0.26

7 TH GRADE SCIENCE REVIEW

Torque Analyses of a Sliding Ladder

Chapter 3.8 & 6 Solutions

Lecture 07: Work and Kinetic Energy. Physics 2210 Fall Semester 2014

Chapter 11 Equilibrium

Valve Train Design and Calculation for High-Performance Engines

Rolling cylinder on a horizontal plane

PHYS 211 FINAL FALL 2004 Form A

MACHINE TOOL DRIVES. Learning Objectives:

TOP VIEW. FBD s TOP VIEW. Examination No. 2 PROBLEM NO. 1. Given:

Autodesk Fusion 360: Assemblies. Overview

Pre-requisites

Working Drawing and Assemblies. Chapter 10

APPLIED MATHEMATICS ADVANCED LEVEL

Lecture L25-3D Rigid Body Kinematics

MET 306. Activity 8a. Mechanism Design Creo 2.0 Level 7 POINT A GROUND LINK LINK 1 LINK 2 LINK 3 POINT B 10/15/2010 1

AP Physics Circular Motion Practice Test B,B,B,A,D,D,C,B,D,B,E,E,E, m/s, 0.4 N, 1.5 m, 6.3m/s, m/s, 22.9 m/s

PHYSICS 111 HOMEWORK SOLUTION #9. April 5, 2013

Lecture L2 - Degrees of Freedom and Constraints, Rectilinear Motion

3600 s 1 h. 24 h 1 day. 1 day

CIS009-2, Mechatronics Robotic Arms & Hands

Increase the efficiency of your rotating machines by optimizing your bearing lubrication

Chapter 6 Work and Energy

Lecture L22-2D Rigid Body Dynamics: Work and Energy

Slide Basic system Models

Physics 201 Homework 8

Structural Analysis - II Prof. P. Banerjee Department of Civil Engineering Indian Institute of Technology, Bombay. Lecture - 02

Torque and Rotary Motion

Common Mechanical Engineering Terms

Highly flexible couplings

Chapter 4. Forces and Newton s Laws of Motion. continued

BLR s Safety Training Presentations

Simulation of Trajectories and Comparison of Joint Variables for Robotic Manipulator Using Multibody Dynamics (MBD)

THEORETICAL MECHANICS

How To Design A Bevel And Hypoid Gear Drive

Lecture L3 - Vectors, Matrices and Coordinate Transformations

Welcome back to Physics 211. Physics 211 Spring 2014 Lecture ask a physicist

Transcription:

Theory of Machines Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 1

Syllabus and Course Outline Faculty of Engineering Department of Mechanical Engineering EMEC 3302, Theory of Machines Instructor: Dr. Anwar Abu-Zarifa Office: IT Building, Room: I413 Tel: 2821 email: aabuzarifa@iugaza.edu.ps Website: http://site.iugaza.edu.ps/abuzarifa Office Hrs: see my website SAT 09:30 11:00 Q412 MON 09:30 11:00 Q412 Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 2

Text Book: R. L. Norton, Design of Machinery An Introduction to the Synthesis and Analysis of Mechanisms and Machines, McGraw Hill Higher Education; 3rd edition Reference Books: John J. Uicker, Gordon R. Pennock, Joseph E. Shigley, Theory of Machines and Mechanisms R.S. Khurmi, J.K. Gupta,Theory of Machines Thomas Bevan, The Theory of Machines The Theory of Machines by Robert Ferrier McKay Engineering Drawing And Design, Jensen ect., McGraw-Hill Science, 7th Edition, 2007 Mechanical Design of Machine Elements and Machines, Collins ect., Wiley, 2 Edition, 2009 Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 3

Grading: Attendance 5% Design Project 25% Midterm 30% Final exam 40% Course Description: The course provides students with instruction in the fundamentals of theory of machines. The Theory of Machines and Mechanisms provides the foundation for the study of displacements, velocities, accelerations, and static and dynamic forces required for the proper design of mechanical linkages, cams, and geared systems. Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 4

Course Objectives: Students combine theory, graphical and analytical skills to understand the Engineering Design. Upon successful completion of the course, the student will be able: To develop the ability to analyze and understand the dynamic (position, velocity, acceleration, force and torque) characteristics of mechanisms such as linkages and cams. To develop the ability to systematically design and optimize mechanisms to perform a specified task. To increase the ability of students to effectively present written, oral, and graphical solutions to design problems. To increase the ability of students to work cooperatively on teams in the development of mechanism designs. Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 5

Chapter 1 Introduction Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 6

Definitions The subject Theory of Machines may be defined as that branch of Engineering-science, which deals with the study of relative motion between the various parts of a machine, and forces which act on them. The knowledge of this subject is very essential for an engineer in designing the various parts of a machine. Kinematics: The study of motion without regard to forces More particularly, kinematics is the study of position, displacement, rotation, speed, velocity, and acceleration. Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 7

Kinetics: The study of forces on systems in motion A mechanism: is a device that transforms motion to some desirable pattern and typically develops very low forces and transmits little power. A machine: typically contains mechanisms that are designed to provide significant forces and transmit significant power. Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 8

Application of Kinematics Any machine or device that moves contains one or more kinematic elements such As linkages, gears. belts and chains. Bicycle is a simple example of a kinematic system that contains a chain drive to provide Torque. Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 9

An Automobile contains many more examples of kin-systems the transmission is full of gears. Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 10

Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 11

Chapter 2 DEGREES OF FREEDOM (MOBILITY) Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 12

Degrees of Freedom (DOF) or Mobility DOF: Number of independent parameters (measurements) needed to uniquely define position of a system in space at any instant of time. A mechanical system s mobility (M) can be classified according to the number of degrees of freedom (DOF). DOF is defined with respect to a selected frame of reference (ground). Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 13

Rigid body in a plane has 3 DOF: x,y,z Rigid body in 3D-space has 6 DOF, 3 translations & 3 rotations three lengths (x, y, z), plus three angles (θ, φ, ρ). The pencil in these examples represents a rigid body, or link. Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 14

Types of Motion Pure rotation: the body possesses one point (center of rotation) that has no motion with respect to the stationary frame of reference. All other points move in circular arcs. Pure translation: all points on the body describe parallel (curvilinear or rectilinear) paths. Complex motion: a simultaneous combination of rotation and translation. Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 15

Excavator Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 16

Slider-Crank Mechanism Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 17

Links, joints, and kinematic chains Linkage design: Linkages are the basic building blocks of all mechanisms All common forms of mechanisms (cams, gears, belts, chains) are in fact variations on a common theme of linkages. Linkages are made up of links and joints. Links: rigid member having nodes Node: attachment points Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 18

1. Binary link: 2 nodes 2. Ternary link: 3 nodes 3. Quaternary link: 4 nodes Joint: connection between two or more links (at their nodes) which allows motion; (Joints also called kinematic pairs) Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 19

Joint Classification Joints can be classified in several ways: 1.By the type of contact between the elements, line, point, or surface. 2.By the number of degrees of freedom allowed at the joint. 3.By the type of physical closure of the joint: either force or form closed. 4.By the number of links joined (order of the joint). A more useful means to classify joints (pairs) is by the number of degrees of freedom that they allow between the two elements joined. Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 20

A joint with more than one freedom may also be a higher pair Type of contact: line, point, surface Number of DOF: full joint=1dof, half joint=2dof Form closed (closed by geometry) or Force closed (needs an external force to keep it closed) Joint order Joint order = number of links-1 Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 21

lower pair to describe joints with surface contact The six lower pairs Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 22

The half joint is also called a roll-slide joint because it allows both rolling and sliding Form closed (closed by geometry) or Force closed Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 23

Terminology of Joints A joint (also called kinematic pair) is a connection between two or more links at their nodes, which may allow motion between the links. A lower pair is a joint with surface contact; ahigher pair is a joint with point or line contact. A full joint has one degree of freedom; a half joint has two degrees of freedom. Full joints are lower pairs; half-joints are higher pairs and allow both rotation and translation (roll-slide). A form-closed joint is one in which the links are kept together form by its geometry; a force-closed joint requires some external force to keep the links together. Joint order is the number of links joined minus one (e.g. 1 st order means two links). Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 24

Kinematic chains, mechanisms, machines, link classification Kinematic chain: links joined together for motion Mechanism: grounded kinematic chain Machine: mechanism designed to do work Link classification: Ground: any link or links that are fixed, nonmoving with respect to the reference frame Crank: pivoted to ground, makes complete revolutions Rocker: pivoted to ground, has oscillatory motion Coupler: link has complex motion, not attached to ground Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 25

crank mechanism Elements: 0: Ground (Casing, Frame) 1: Rocker 2: Coupler 3: Crank Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 26

The Ground Link When studying mechanisms it is very helpful to establish a fixed reference frame by assigning one of the links as ground. The motion of all other links are described with respect to the ground link. For example, a fourbar mechanism often looks like a 3-bar mechanism, where the first bar is simply the ground link. Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 27

Drawing kinematic Diagrams Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 28

Determining Degrees of Freedom Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 29

Determining Degrees of Freedom Two unconnected links: 6 DOF (each link has 3 DOF) When connected by a full joint: 4 DOF (each full joint eliminates 2 DOF) Gruebler s equation for planar mechanisms: DOF = 3L-2J-3G Where: L: number of links J: number of full joints G: number of grounded links Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 30

Determining DOF s Gruebler s equation for planar mechanisms M= 3L-2J-3G Where M = degree of freedom or mobility L = number of links J = number of full joints (half joints count as 0.5) G = number of grounded links =1 M 3 L 1 2J Kutzbach s modification of Gruebler s equation Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 31

The Cylindrical (cylindric) joint - two degrees of freedom It permits both angular rotation and an independent sliding motion (C joint) Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 32

The Spherical (spheric) - Three degree of freedom It permits rotational motion about all three axes, a ball-and-socket joint (S joint) Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 33

Example Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 34

Example Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 35

Gruebler s Equation Gruebler s equation can be used to determine the mobility of planar mechanisms. Gruebler s Equation Link 1 3 DOF L = 2 J = 1 G = 1 DOF = 1 DOF L J G = mobility = number of links = number of revolute joints or prismatic joints = number of grounded links 1 DOF DOF (M) = 3*L 2* J 3 *G = 3 (L-1) 2 * J Link 2 3 DOF Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012

Mobility of Vise Grip Pliers This example applies Gruebler s equation to the determine the mobility of a vise grip plier. 4 4 3 3 1 2 1 2 5 Each revolute joint removes two DOF. The screw joint removes two DOF. L = 5 J = 4 (revolute) J = 1 (screw) G = 1 (your hand) DOF = 3*5-2*5-1*3 = 2 The mobility of the plier is two. Link 3 can be moved relative link1 when you squeeze your hand and the jaw opening is controlled by rotating link 5. Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012

Punch Press Slider-Crank Mechanism As designated in the figure, there are four links link 1, link 2, link 3 and link 4. Link 1 acts as a crank. Link 2 acts as connecting link, link 3 is the slider and link 4 is ground. Joint Number Formed between links 1 Link 4 and Link 1 2 Link 1 and Link 2 3 Link 2 and Link 3 4 Link 3 and Link 4 Joint type Revolute (or Pin) Revolute (or Pin) Revolute (or Pin) Translatio nal or (Slider) Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 38

Mechanisms and Structures If DOF > 0, the assembly of links is a mechanism and will exhibit relative motion If DOF = 0, the assembly of links is a structure and no motion is possible. If DOF < 0,then the assembly is a preloaded structure, no motion is possible, and in general stresses are present. Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 39

Paradoxes Greubler criterion does not include geometry, so it can give wrong prediction We must use inspection L=5 J=6 G=1 M=3*5-2*6-3*1=0 E-quintet Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 40

Rolling cylinders even without slip (The joint between the two wheels can be postulated to allow no slip, provided that sufficient friction is available) is an example in which the ground link is exactly the same length as the sum of two other links. If no slip occurs, then this is a one-freedom, or full, joint that allows only relative angular motion (Δθ) between the wheels. With that assumption, there are 3 links and 3 full joints, The equation predicts DOF =0(L=3, J1=3), but the mechanism has DOF =1. Others paradoxes exist, so the designer must not apply the equation blindly. Dr. Anwar Abu-Zarifa. Islamic University of Gaza. Department of Mechanical Engineering. 2012 41