Me6401 Kinematics of Machinery
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On the Configurations of Closed Kinematic Chains in Three
On the Configurations of Closed Kinematic Chains in three-dimensional Space Gerhard Zangerl Department of Mathematics, University of Innsbruck Technikestraße 13, 6020 Innsbruck, Austria E-mail: [email protected] Alexander Steinicke Department of Applied Mathematics and Information Technology, Montanuniversitaet Leoben Peter Tunner-Straße 25/I, 8700 Leoben, Austria E-mail: [email protected] Abstract A kinematic chain in three-dimensional Euclidean space consists of n links that are connected by spherical joints. Such a chain is said to be within a closed configuration when its link lengths form a closed polygonal chain in three dimensions. We investigate the space of configurations, described in terms of joint angles of its spherical joints, that satisfy the the loop closure constraint, meaning that the kinematic chain is closed. In special cases, we can find a new set of parameters that describe the diagonal lengths (the distance of the joints from the origin) of the configuration space by a simple domain, namely a cube of dimension n − 3. We expect that the new findings can be applied to various problems such as motion planning for closed kinematic chains or singularity analysis of their configuration spaces. To demonstrate the practical feasibility of the new method, we present numerical examples. 1 Introduction This study is the natural further development of [32] in which closed configurations of a two-dimensional kine- matic chain (KC) in terms of its joint angles were considered. As a generalization, we study the configuration spaces of a three-dimensional closed kinematic chain (CKC) with n links in terms of the joint angles of its spherical joints. -
Department of Mechanical Engineering ME 8492 – Kinematics of Machinery Unit I – Introduction to Mechanism - MCQ Bank 1
ChettinadTech Dept. of MECH Department of Mechanical Engineering ME 8492 – Kinematics of Machinery Unit I – Introduction to Mechanism - MCQ Bank 1. In a reciprocating steam engine, which of the following forms a kinematic link ? (a) cylinder and piston (b) piston rod and connecting rod (c) crank shaft and flywheel (d) flywheel and engine frame Answer: (c) 2. The motion of a piston in the cylinder of a steam engine is an example of (a) completely constrained motion (b) incompletely constrained motion (c) successfully constrained motion (d) none of these Answer: (a) 3. The motion transmitted between the teeth of gears in mesh is (a) sliding (b) rolling (c) may be rolling or sliding depending upon the shape of teeth (d) partly sliding and partly rolling Answer: (d) 4. The cam and follower without a spring forms a (a) lower pair (b) higher pair (c) self closed pair (d) force closed pair Answer: (c) 5. A ball and a socket joint forms a (a) turning pair (b) rolling pair (c) sliding pair (d) spherical pair Answer: (d) 6. The lead screw of a lathe with nut forms a (a) sliding pair (b) rolling pair (c) screw pair (d) turning pair ME 8692 – Finite Element Analysis Page 1 ChettinadTech Dept. of MECH Answer: (c) 7. When the elements of the pair are kept in contact by the action of external forces, the pair is said to be a (a) lower pair (b) higher pair (c) self closed pair (d) force closed pair Answer: (d) 8. Which of the following is a turning pair ? (a) Piston and cylinder of a reciprocating steam engine (b) Shaft with collars at both ends fitted in a circular hole (c) Lead screw of a lathe with nut (d) Ball and socket joint Answer: (b) 9. -
TEE Final Report
Project Number: AHH – 1171 Pseudo‐Fluid Control Extension System A Major Qualifying Project Submitted to the Faculty of the WORCESTER POLYTECHNIC INSTITUTE in partial fulfillment of the requirements for the Degree of Bachelor of Science In Mechanical Engineering by John Dunbar ______________________________ Christopher Farren ______________________________ Mari Freitas ______________________________ Date: April 26, 2012 Approved: Keywords ______________________________ Professor Allen H. Hoffman, Major Advisor 1. Transducer 2. TEE 3. Pseudo‐fluid ______________________________ Professor Holly K. Ault, Co‐Advisor Abstract An interventional cardiologist (IC) performs procedures using a transesophageal echocardiogram transducer (TEE). The TEE is positioned by an echo cardiologist who is present for the entirety of the procedures. The purpose of this project was to redesign the user interface of the TEE in order to minimize the role of the echo cardiologist and give more control to the IC. This was accomplished by creating an extension of the TEE control system that can remotely control the TEE from a distance of five feet. Preliminary designs were created using cable and fluid hydraulic systems; however, both types of systems were problematic. A pseudo‐fluid system consisting of tubes filled with steel balls was developed to capture the positive aspects of the cable and fluid systems. The user interface of the new system consisted of two rotatable knobs that actuate rack and pinion gear sets, which push the pseudo‐ fluid balls through tubes. At the distal ends of the tubes, the balls move the racks of rack and pinion gear sets that in turn rotate shafts in the current TEE. The resulting user interface has similar ergonomic and mechanical properties as the original TEE. -
Kinematic Singularities of Mechanisms Revisited
IMA Conference on Mathematics of Robotics 9 – 11 September 2015, St Anne’s College, University of Oxford 1 Kinematic Singularities of Mechanisms Revisited By Andreas M¨uller1, Dimiter Zlatanov2 1Johannes Kepler University, Linz, Austria; 2University of Genoa, Genoa, Italy Abstract The paper revisits the definition and the identification of the singularities of kinematic chains and mechanisms. The degeneracy of the kinematics of an articulated system of rigid bodies cannot always be identified with the singularities of the configuration space. Local analysis can help identify kinematic chain singularities and better understand the way the motion characteristics change at such configurations. An example is shown that exhibits a kinematic singularity although its configuration space is a smooth manifold. 1. Introduction Kinematic singularities of a mechanism are critical configurations that can lead to a loss of structural stability or controllability. This has been a central topic in mechanism theory and still is a field of active research. A systematic approach to the study of singular configurations involves a mathematical model for the kinematic chain and its interaction with the environment via inputs and outputs. Thereupon critical configurations can be identified for the kinematic chain itself and for the input and output relations. A kinematic chain is a system of rigid bodies (links), some pairs of which are connected with joints. It is defined by specifying exactly which links are jointed (by a connectiv- ity graph [Wittenburg (1994)]), the type of each joint, and the joint's locations in the adjacent links. Mathematically, a kinematic chain is modeled by specifying its possible motions as a subset of the smooth curves on an ambient manifold, usually assumed to have a global parametrization, Vn. -
Novel Mechanical Mechanisms for the Development of Undergraduate Knowledge
Novel Mechanical Mechanisms for the Development of Undergraduate Knowledge by Michael L. Stern Submitted to the Department of Mechanical Engineering in Partial Fulfillment of the Requirements for the degree of Bachelor of Science in Mechanical Engineering at the Massachusetts Institute of Technology June 2009 2009 Michael Stern All rights reserved The Author hereby grants to MIT permission to reproduce and to distribute publicly paper and electronic copies of this thesis document in whole or in part in any medium now known or hereafter created. Signature of Author ……………………………………………………………………………… Department of Mechanical Engineering May 19, 2009 Certified by ...……………………………………………………………………………………… Barbara Hughey, PhD Thesis Supervisor Instructor Accepted by ……..………………………………………………………………………………… Professor J. Lienhard V Collins Professor of Mechanical Engineering Chairman, Undergraduate Thesis Committee Acknowledgements I would like to give special thanks to Dr. Barbara Hughey for the enormous amount of help she provided both in developing the idea for this thesis and the execution of the thesis itself. She helped me take the idea from a neat project and turn it into an academic thesis, enduring my daily bothering throughout the semester, for advice, troubleshooting and writing recommendations. I would also like to thank Michael Tarkanian for allowing me to use his laser cutter. The ease of access made a world of difference in completing my thesis and doing so in a timely manner. Finally, I would like to thank my mom for helping me proofread the drafts, catching my grammatical foolishness. 2 Novel Mechanical Mechanisms for the Development of Undergraduate Knowledge by Michael L. Stern Submitted to the Department of Mechanical Engineering on May 19th, 2009 in Partial Fulfillment of the Requirements for the degree of Bachelor of Science in Mechanical Engineering Abstract: Although MIT Students have been taught an enormous amount of theory and design, they are not exposed to simple machine elements and designs from the past. -
1700 Animated Linkages
Nguyen Duc Thang 1700 ANIMATED MECHANICAL MECHANISMS With Images, Brief explanations and Youtube links. Part 1 Transmission of continuous rotation Renewed on 31 December 2014 1 This document is divided into 3 parts. Part 1: Transmission of continuous rotation Part 2: Other kinds of motion transmission Part 3: Mechanisms of specific purposes Autodesk Inventor is used to create all videos in this document. They are available on Youtube channel “thang010146”. To bring as many as possible existing mechanical mechanisms into this document is author’s desire. However it is obstructed by author’s ability and Inventor’s capacity. Therefore from this document may be absent such mechanisms that are of complicated structure or include flexible and fluid links. This document is periodically renewed because the video building is continuous as long as possible. The renewed time is shown on the first page. This document may be helpful for people, who - have to deal with mechanical mechanisms everyday - see mechanical mechanisms as a hobby Any criticism or suggestion is highly appreciated with the author’s hope to make this document more useful. Author’s information: Name: Nguyen Duc Thang Birth year: 1946 Birth place: Hue city, Vietnam Residence place: Hanoi, Vietnam Education: - Mechanical engineer, 1969, Hanoi University of Technology, Vietnam - Doctor of Engineering, 1984, Kosice University of Technology, Slovakia Job history: - Designer of small mechanical engineering enterprises in Hanoi. - Retirement in 2002. Contact Email: [email protected] 2 Table of Contents 1. Continuous rotation transmission .................................................................................4 1.1. Couplings ....................................................................................................................4 1.2. Clutches ....................................................................................................................13 1.2.1. Two way clutches...............................................................................................13 1.2.1. -
Planar Kinematics
Introduction to Robotics, H. Harry Asada 1 Chapter 4 Planar Kinematics Kinematics is Geometry of Motion. It is one of the most fundamental disciplines in robotics, providing tools for describing the structure and behavior of robot mechanisms. In this chapter, we will discuss how the motion of a robot mechanism is described, how it responds to actuator movements, and how the individual actuators should be coordinated to obtain desired motion at the robot end-effecter. These are questions central to the design and control of robot mechanisms. To begin with, we will restrict ourselves to a class of robot mechanisms that work within a plane, i.e. Planar Kinematics. Planar kinematics is much more tractable mathematically, compared to general three-dimensional kinematics. Nonetheless, most of the robot mechanisms of practical importance can be treated as planar mechanisms, or can be reduced to planar problems. General three-dimensional kinematics, on the other hand, needs special mathematical tools, which will be discussed in later chapters. 4.1 Planar Kinematics of Serial Link Mechanisms Example 4.1 Consider the three degree-of-freedom planar robot arm shown in Figure 4.1.1. The arm consists of one fixed link and three movable links that move within the plane. All the links are connected by revolute joints whose joint axes are all perpendicular to the plane of the links. There is no closed-loop kinematic chain; hence, it is a serial link mechanism. y A 3 E End Effecter ⎛ xe ⎞ Link 3 ⎜ ⎟ ⎝ ye ⎠ A 2 θ3 φ B e A1 Link 2 Joint 3 θ 2 Link 1 A Joint 2 Joint 1 θ O 1 x Link 0 Figure 4.1.1 Three dof planar robot with three revolute joints To describe this robot arm, a few geometric parameters are needed. -
Engineering Information Spur Gears Gear Nomenclature
Engineering Information Spur Gears Gear Nomenclature ADDENDUM (a) is the height by which a tooth projects GEAR is a machine part with gear teeth. When two gears beyond the pitch circle or pitch line. run together, the one with the larger number of teeth is called the gear. BASE DIAMETER (Db) is the diameter of the base cylinder from which the involute portion of a tooth profile is generated. HUB DIAMETER is outside diameter of a gear, sprocket or coupling hub. BACKLASH (B) is the amount by which the width of a tooth space exceeds the thickness of the engaging tooth on the HUB PROJECTION is the distance the hub extends beyond pitch circles. As actually indicated by measuring devices, the gear face. backlash may be determined variously in the transverse, normal, or axial-planes, and either in the direction of the pitch INVOLUTE TEETH of spur gears, helical gears and worms circles or on the line of action. Such measurements should be are those in which the active portion of the profile in the corrected to corresponding values on transverse pitch circles transverse plane is the involute of a circle. for general comparisons. LONG- AND SHORT-ADDENDUM TEETH are those of BORE LENGTH is the total length through a gear, sprocket, engaging gears (on a standard designed center distance) or coupling bore. one of which has a long addendum and the other has a short addendum. CIRCULAR PITCH (p) is the distance along the pitch circle or pitch line between corresponding profiles of adjacent teeth. KEYWAY is the machined groove running the length of the bore. -
1.0 Simple Mechanism 1.1 Link ,Kinematic Chain
SYLLABUS 1.0 Simple mechanism 1.1 Link ,kinematic chain, mechanism, machine 1.2 Inversion, four bar link mechanism and its inversion 1.3 Lower pair and higher pair 1.4 Cam and followers 2.0 Friction 2.1 Friction between nut and screw for square thread, screw jack 2.2 Bearing and its classification, Description of roller, needle roller& ball bearings. 2.3 Torque transmission in flat pivot& conical pivot bearings. 2.4 Flat collar bearing of single and multiple types. 2.5 Torque transmission for single and multiple clutches 2.6 Working of simple frictional brakes.2.7 Working of Absorption type of dynamometer 3.0 Power Transmission 3.1 Concept of power transmission 3.2 Type of drives, belt, gear and chain drive. 3.3 Computation of velocity ratio, length of belts (open and cross)with and without slip. 3.4 Ratio of belt tensions, centrifugal tension and initial tension. 3.5 Power transmitted by the belt. 3.6 Determine belt thickness and width for given permissible stress for open and crossed belt considering centrifugal tension. 3.7 V-belts and V-belts pulleys. 3.8 Concept of crowning of pulleys. 3.9 Gear drives and its terminology. 3.10 Gear trains, working principle of simple, compound, reverted and epicyclic gear trains. 4.0 Governors and Flywheel 4.1 Function of governor 4.2 Classification of governor 4.3 Working of Watt, Porter, Proel and Hartnell governors. 4.4 Conceptual explanation of sensitivity, stability and isochronisms. 4.5 Function of flywheel. 4.6 Comparison between flywheel &governor. -
Motion Planning Algorithms for General Closed-Chain Mechanisms Juan Cortés
Motion planning algorithms for general closed-chain mechanisms Juan Cortés To cite this version: Juan Cortés. Motion planning algorithms for general closed-chain mechanisms. Automatique / Robo- tique. Institut National Polytechnique de Toulouse - INPT, 2003. Français. tel-00011002 HAL Id: tel-00011002 https://tel.archives-ouvertes.fr/tel-00011002 Submitted on 16 Nov 2005 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. These` pr´esent´eeau Laboratoire d'Analyse et d'Architecture des Syst`emes en vue de l'obtention du Doctorat de l'Institut National Polytechnique de Toulouse Ecole Doctorale Syst`emes Sp´ecialit´e: Syst`emesAutomatiques / Robotique par Juan Cort´es Algorithmes pour la Planification de Mouvements de Mecanismes´ Articules´ avec Cha^ınes Cinematiques´ Fermees´ Motion Planning Algorithms for General Closed-Chain Mechanisms Soutenue le 16 D´ecember 2003 devant le Jury compos´ede : Lydia E. Kavraki Rice University, Houston Rapporteurs Steven M. LaValle University of Illinois, Urbana Raja Chatila LAAS-CNRS, Toulouse Examinateurs Jean-Paul Laumond LAAS-CNRS, Toulouse Jean-Pierre Merlet INRIA, Sophia Antipolis Pierre Monsan INSA, Toulouse Membre invit´e Thierry Sim´eon LAAS-CNRS, Toulouse Directeur de th`ese Ojal´aque esta tesis pueda aportar a la Ciencia al menos una peque~na parte de lo que su realizaci´onme ha aportado a mi. -
Hand-Eye Calibration of Robonaut
Source of Acqui ition ASA Johnson Space Center Hand-Eye Calibration of Robonaut Kevin Nickels Eric Huber Engineering Science Metrica, Inc. Trinity University Dexterous Robotics Laboratory San Antonio, TX 78212-7200 NASA Jolmson Space Center Email: [email protected] Houston, TX 77058 Email: [email protected] Abstract-NASA's Human Space Flight program depends heavily on Extra-Vehicular Activities (EVA's) performed by human astronauts. EVA is a high risk environment tbat requires extensive training and ground support III coDaboration with the Defense Advanced Research Projects Agency (DARPA), NASA is conducting a ground development project to produce a robotic astronaut's assistant, caUed Robonaut, that could help reduce human EVA time and workload. The project described in this paper designed and implemented a hand-eye calibration scheme for Robonaut, Unit A. The intent of this calibration scheme is to improve hand-eye coordination of the robot. The basic approach is to use kinematic and stereo vision measurements, namely the joint angles self-reported by the right arm and 3-D positions of a calibration fixture as measured by vision, to estimate the transformation from Robonaut's base coordinate system to its hand coordinate system and to its vision coordinate system. Two methods of gathering data sets bave been developed, along with software to support each. III the first, the system observes the robotic arm and neck angles as the robot is operated under e,,:ternal control, and measures the 3-D position of a calibration fixture using Robonaut's stereo cameras, and logs these data. In the second, the system drives tile arm and neck through a set of prerecorded configurations, and data are again logged. -
Robotics & Automation Lecture 23 Closed Kinematic Chain And
Robotics & Automation Lecture 23 Closed Kinematic Chain and Parallel Mechanisms John T. Wen November 10, 2008 JTW-RA23 RPI ECSE/CSCI 4480 Robotics I Examples of closed kinematic chains ² Constrained robot, e.g., robot in contact with environment (polishing, assembly, etc.). ² Multiple interacting robots, e.g., multi-finger grasp, multiple cooperative robots. ² Parallel mechanism, e.g., 4-bar linkage, slider-crank, Stewart-Gough Platform, Delta robot. qq 2 qq 1 qq 3 November 10, 2008Copyrighted by John T. Wen Page 1 JTW-RA23 RPI ECSE/CSCI 4480 Robotics I Kinematics Forward kinematics and inverse kinematics are the same as before: given joint positions, find the task frame, and vice versa – subject to the closed chain constraints. Usually: Serial mechanism has complicated geometry, inverse kinematics is more dif- ficult than the forward kinematics. Parallel mechanisms usually are based on imposing kinematic constraints to simple serial mechanisms. Therefore, inverse kinematics is usu- ally easy. The forward kinematics needs to take into account of constraints, and is more difficult to solve. November 10, 2008Copyrighted by John T. Wen Page 2 JTW-RA23 RPI ECSE/CSCI 4480 Robotics I Constrained mechanisms Consider a serial kinematic chain with n joints (q 2 Rn). Suppose the chain is constrained: f(q) = 0; f : Rn ! Rk: Then the mechanism has n ¡ k (unconstrained) DOF. Example: ² 3-DOF Planar arm with tip constrained to move along a line (2 dof) ² 4-bar linkage (1 dof) November 10, 2008Copyrighted by John T. Wen Page 3 JTW-RA23 RPI ECSE/CSCI 4480 Robotics I Greubler’s Formula Consider a planar mechanism.