APPLIED DYNAMICS, with Applications to Multibody and Mechatronic Systems
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A Collision Avoidance Method Using Assur Virtual Chains
ABCM Symposium Series in Mechatronics - Vol. 3 - pp.316-325 Copyright °c 2008 by ABCM A COLLISION AVOIDANCE METHOD USING ASSUR VIRTUAL CHAINS Henrique Simas, [email protected] Universidade do Vale do Itajaí - Centro de Ensino São José Curso de Engenharia de Computação Rodovia SC 407, km 4 - Sertão do Imaruim 88122 000 - São José, SC. Brasil Daniel Fontan Maia da Cruz, [email protected] Raul Guenther, [email protected] Daniel Martins, [email protected] Universidade Federal de Santa Catarina Departamento de Engenharia Mecânica Laboratório de Robótica Campus Universitário - Trindade 88040-900 – Florianópolis, SC. Brasil Abstract. In hydroelectric power plants, the rotor blades are eroded by the cavitation process. The erosion results in craters that are usually recovered by a manual welding process. The ROBOTURB project developed an automatized system, where a robot is used for recovery the rotor blade surfaces by welding process. The robot workspace is constrained by freeform surfaces and the collision imminency is constant. For this reason, the robot is redundant, making possible the collisions avoidance, keeping the end- effector trajectory tracking. In recent years, the collision avoidance problem has been dealt with algorithms based on artificial intelligence. This article considers a methodology for implementation a deterministic collision avoidance algorithm. The Solution of this proposal is based on the method of kinematic constraint and on the use of Assur virtual chains. The method consists in the obstacle identification and in the definition of a free collison workspace area. Thus, it is used a Assur virtual chain to detect and avoid the collision by evaluating the distance between a point at the robot and the obstacle. -
Dynamic Analysis of Planar Rigid Multibody Systems Modeled Using Natural Absolute Coordinates C
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by DSpace at University of West Bohemia ARTICLE IN PRESS Applied and Computational Mechanics 12 (2018) XXX–YYY Dynamic analysis of planar rigid multibody systems modeled using Natural Absolute Coordinates C. M. Pappalardoa,∗,D.Guidaa a Department of Industrial Engineering, University of Salerno, Via Giovanni Paolo II, 132, 84084 Fisciano, Salerno, Italy Received 5 July 2017; accepted 1 February 2018 Abstract This paper deals with the dynamic simulation of rigid multibody systems described with the use of two-dimensional natural absolute coordinates. The computational methodology discussed in this investigation is referred to as planar Natural Absolute Coordinate Formulation (NACF). The kinematic representation used in the planar NACF is based on a vector of generalized coordinates that includes two translational coordinates and four rotational parameters. In particular, the set of natural absolute coordinates is employed for describing the global location and the geometric orientation relative to the general configuration of a planar rigid body. The kinematic description utilized in the planar NACF is based on the separation of variable principle. Therefore, a constant symmetric positive-definite mass matrix and a zero inertia quadratic velocity vector associated with the centrifugal and Coriolis inertia effects enter in the formulation of the equations of motion. However, since a redundant set of rotational parameters is used in the kinematic description of the planar NACF for defining the geometric orientation of a rigid body, the introduction of a set of intrinsic normalization conditions is necessary for the mathematical formulation of the algebraic constraint equations. -
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NOTE TO USERS This reproduction is the best copy available. UMJ Algebraic Screw Pairs by James D. Robinson A Dissertation submitted to the Faculty of Graduate and Postdoctoral Affairs in partial fulfilment of the requirements for the degree of Doctor of Philosophy in Mechanical Engineering Ottawa-Carleton Institute for Mechanical and Aerospace Engineering Department of Mechanical and Aerospace Engineering Carleton University Ottawa, Ontario, Canada May 2012 Copyright © 2012 - James D. Robinson Library and Archives Bibliotheque et Canada Archives Canada Published Heritage Direction du 1+1 Branch Patrimoine de I'edition 395 Wellington Street 395, rue Wellington Ottawa ON K1A0N4 Ottawa ON K1A 0N4 Canada Canada Your file Votre reference ISBN: 978-0-494-93679-5 Our file Notre reference ISBN: 978-0-494-93679-5 NOTICE: AVIS: The author has granted a non L'auteur a accorde une licence non exclusive exclusive license allowing Library and permettant a la Bibliotheque et Archives Archives Canada to reproduce, Canada de reproduire, publier, archiver, publish, archive, preserve, conserve, sauvegarder, conserver, transmettre au public communicate to the public by par telecommunication ou par I'lnternet, preter, telecommunication or on the Internet, distribuer et vendre des theses partout dans le loan, distrbute and sell theses monde, a des fins commerciales ou autres, sur worldwide, for commercial or non support microforme, papier, electronique et/ou commercial purposes, in microform, autres formats. paper, electronic and/or any other formats. The author retains copyright L'auteur conserve la propriete du droit d'auteur ownership and moral rights in this et des droits moraux qui protege cette these. Ni thesis. -
1 Portraits Leonhard Euler Daniel Bernoulli Johann-Heinrich Lambert
Portraits Leonhard Euler Daniel Bernoulli Johann-Heinrich Lambert Compiled and translated by Oscar Sheynin Berlin, 2010 Copyright Sheynin 2010 www.sheynin.de ISBN 3-938417-01-3 1 Contents Foreword I. Nicolaus Fuss, Eulogy on Leonhard Euler, 1786. Translated from German II. M. J. A. N. Condorcet, Eulogy on Euler, 1786. Translated from French III. Daniel Bernoulli, Autobiography. Translated from Russian; Latin original received in Petersburg in 1776 IV. M. J. A. N. Condorcet, Eulogy on [Daniel] Bernoulli, 1785. In French. Translated by Daniel II Bernoulli in German, 1787. This translation considers both versions V. R. Wolf, Daniel Bernoulli from Basel, 1700 – 1782, 1860. Translated from German VI. Gleb K. Michajlov, The Life and Work of Daniel Bernoullli, 2005. Translated from German VII. Daniel Bernoulli, List of Contributions, 2002 VIII. J. H. S. Formey, Eulogy on Lambert, 1780. Translated from French IX. R. Wolf, Joh. Heinrich Lambert from Mühlhausen, 1728 – 1777, 1860. Translated from German X. J.-H. Lambert, List of Publications, 1970 XI. Oscar Sheynin, Supplement: Daniel Bernoulli’s Instructions for Meteorological Stations 2 Foreword Along with the main eulogies and biographies [i, ii, iv, v, viii, ix], I have included a recent biography of Daniel Bernoulli [vi], his autobiography [iii], for the first time translated from the Russian translation of the Latin original but regrettably incomplete, and lists of published works by Daniel Bernoulli [vii] and Lambert [x]. The first of these lists is readily available, but there are so many references to the works of these scientists in the main texts, that I had no other reasonable alternative. -
Design for Additive Manufacturing of Kinematic Pairs
DESIGN FOR ADDITIVE MANUFACTURING OF KINEMATIC PAIRS Shrey Pareek*, Vaibhav Sharma*, and Rahul Rai* *Design Analytics Research and Technology (DART) Lab, Department of Mechanical and Aerospace Engineering, University at Buffalo-SUNY, Buffalo-NY, 14260 Abstract While additive manufacturing processes are better suited for fabrication of parts with complex geometries, they face serious challenges whilst fabricating parts that require relative motion with respect to each other. The primary challenge in additive manufacturing of mechanisms is preventing the mating parts from bonding with each other during the fabrication process. In this paper the authors investigate design and additive fabrication of kinematic pairs that can move relative to each other. The paper outlines fabrication of kinematic pairs based on optimal clearance value for three basic lower order kinematic pairs, viz. revolute pair, prismatic pair, and cylindrical pair. Using empirical testing functional relationships between extractive force and clearance, and between moment and clearance have been developed. These functional relationships can be used by users to fabricate kinematic pairs using FDM based 3D printing processes. The efficacy of the proposed approach is demonstrated on 3D printed kinematic pairs and experimental validation studies. Introduction Additive manufacturing holds the unquestioned advantage over conventional manufacturing techniques when it comes to fabrication of parts with complex geometries. However, additive manufacturing (Fused Deposition Modeling in particular) encounters serious challenges whilst fabricating parts that require relative motion with respect to each other. Generally such models require that each part be produced separately and then assembled together. However, due to inherent inaccuracies of 3D printing these assemblies seldom function correctly. For instance, inaccurate circularity of a 3D printed shaft may prevent its smooth movement inside the hub. -
New General Principle of Mechanics and Its Application to General Nonideal Nonholonomic Systems
New General Principle of Mechanics and Its Application to General Nonideal Nonholonomic Systems Firdaus E. Udwadia1 Abstract: In this paper we develop a general minimum principle of analytical dynamics that is applicable to nonideal constraints. The new principle encompasses Gauss’s Principle of Least Constraint. We use this principle to obtain the general, explicit, equations of motion for holonomically and/or nonholonomically constrained systems with non-ideal constraints. Examples of a nonholonomically constrained system where the constraints are nonideal, and of a system with sliding friction, are presented. DOI: 10.1061/͑ASCE͒0733-9399͑2005͒131:4͑444͒ CE Database subject headings: Constraints; Equations of motion; Mechanical systems; Friction. Introduction ments. Such systems have, to date, been left outside the perview of the Lagrangian framework. As stated by Goldstein ͑1981, p. The motion of complex mechanical systems is often mathemati- 14͒ “This ͓total work done by forces of constraint equal to zero͔ cally modeled by what we call their equations of motion. Several is no longer true if sliding friction is present, and we must exclude formalisms ͓Lagrange’s equations ͑Lagrange 1787͒, Gibbs– such systems from our ͓Lagrangian͔ formulation.” And Pars Appell equations ͑Gibbs 1879, Appell 1899͒, generalized inverse ͑1979͒ in his treatise on analytical dynamics writes, “There are in equations ͑Udwadia and Kalaba 1992͔͒ have been developed for fact systems for which the principle enunciated ͓D’Alembert’s obtaining the equations of motion for such structural and me- principle͔… does not hold. But such systems will not be consid- chanical systems. Though these formalisms do not all afford the ered in this book.” Newtonian approaches are usually used to deal same ease of use in any given practical situation, they are equiva- with the problem of sliding friction ͑Goldstein 1981͒. -
On Stability Problem of a Top Rendiconti Del Seminario Matematico Della Università Di Padova, Tome 68 (1982), P
RENDICONTI del SEMINARIO MATEMATICO della UNIVERSITÀ DI PADOVA V. V. RUMJANTSEV On stability problem of a top Rendiconti del Seminario Matematico della Università di Padova, tome 68 (1982), p. 119-128 <http://www.numdam.org/item?id=RSMUP_1982__68__119_0> © Rendiconti del Seminario Matematico della Università di Padova, 1982, tous droits réservés. L’accès aux archives de la revue « Rendiconti del Seminario Matematico della Università di Padova » (http://rendiconti.math.unipd.it/) implique l’accord avec les conditions générales d’utilisation (http://www.numdam.org/conditions). Toute utilisation commerciale ou impression systématique est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit conte- nir la présente mention de copyright. Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques http://www.numdam.org/ On Stability Problem of a Top. V. V. RUMJANTSEV (*) This paper deals with the stability of a heavy gyrostate [1] on a horizontal plane. The gyrostate is considered as a rigid body with a rotor rotating freely (without friction) about an axis invariably con- nected with the body leaning on a plane by a convex surface, i.e. the top in a broad sence of this word. For mechanician the top is a symple and principal object of study [2] attracting investigators’ attention. 1. Let $ql be the fixed coordinate system with the origin in some point of a horizontal plane and vertically up directed axis I with unit vector y; OXIX2Xa is the coordinate system rigidly connected with the body with the origin in centre of mass of gyrostate and axis ~3 coincided with one of its principal central axes of inertia. -
On the Foundations of Analytical Dynamics F.E
International Journal of Non-Linear Mechanics 37 (2002) 1079–1090 On the foundations of analytical dynamics F.E. Udwadiaa; ∗, R.E. Kalabab aAerospace and Mechanical Engineering, Civil Engineering, Mathematics, and Information and Operations Management, 430K Olin Hall, University of Southern California, Los Angeles, CA 90089-1453, USA bBiomedical Engineering and Economics, University of Southern California, Los Angeles, CA 90089, USA Abstract In this paper, we present the general structure for the explicit equations of motion for general mechanical systems subjected to holonomic and non-holonomic equality constraints. The constraints considered here need not satisfy D’Alembert’s principle, and our derivation is not based on the principle of virtual work. Therefore, the equations obtained here have general applicability. They show that in the presence of such constraints, the constraint force acting on the systemcan always be viewed as madeup of the sumof two components.The explicit formfor each of the two components is provided. The ÿrst of these components is the constraint force that would have existed, were all the constraints ideal; the second is caused by the non-ideal nature of the constraints, and though it needs speciÿcation by the mechanician and depends on the particular situation at hand, this component nonetheless has a speciÿc form. The paper also provides a generalized formof D’Alembert’sprinciple which is then used to obtain the explicit equations of motion for constrained mechanical systems where the constraints may be non-ideal. We show an example where the new general, explicit equations of motion obtained in this paper are used to directly write the equations of motion for describing a non-holonomically constrained system with non-ideal constraints. -
Recent Advances in Multi-Body Dynamics and Nonlinear Control
Recent Advances in Multi-body Dynamics and Nonlinear Control Recent Advances in Multi-body Firdaus E. Udwadia Dynamics and Nonlinear Control Aerospace and Mechanical Engineering This paper presents some recent advances in the dynamics and control of constrained Civil Engineering,, Mathematics multi-body systems. The constraints considered need not satisfy D’Alembert’s principle Systems Architecture Engineering and therefore the results are of general applicability. They show that in the presence of and Information and Operations Management constraints, the constraint force acting on the multi-body system can always be viewed as University of Southern California, Los Angeles made up of the sum of two components whose explicit form is provided. The first of these CA 90089-1453 components consists of the constraint force that would have existed were all the [email protected] constraints ideal; the second is caused by the non-ideal nature of the constraints, and though it needs specification by the mechanician who is modeling the specific system at hand, it nonetheless has a specific form. The general equations of motion obtained herein provide new insights into the simplicity with which Nature seems to operate. They are shown to provide new and exact methods for the tracking control of highly nonlinear mechanical and structural systems without recourse to the usual and approximate methods of linearization that are commonly in use. Keywords : Constrained motion, multi-body dynamics, explicit equations of motion, exact tracking control of nonlinear systems In this paper we extend these results along two directions. First, Introduction we extend D’Alembert’s Principle to include constraints that may be, in general, non-ideal so that the forces of constraint may The general problem of obtaining the equations of motion of a therefore do positive, negative, or zero work under virtual constrained discrete mechanical system is one of the central issues displacements at any given instant of time during the motion of the in multi-body dynamics. -
Explicit Equations of Motion for Constrained
Explicit equations of motion for constrained mechanical systems with singular mass matrices and applications to multi-body dynamics Firdaus Udwadia, Phailaung Phohomsiri To cite this version: Firdaus Udwadia, Phailaung Phohomsiri. Explicit equations of motion for constrained mechanical systems with singular mass matrices and applications to multi-body dynamics. Proceedings of the Royal Society A: Mathematical, Physical and Engineering Sciences, Royal Society, The, 2006, 462 (2071), pp.2097 - 2117. 10.1098/rspa.2006.1662. hal-01395968 HAL Id: hal-01395968 https://hal.archives-ouvertes.fr/hal-01395968 Submitted on 13 Nov 2016 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. Distributed under a Creative Commons Attribution| 4.0 International License Explicit equations of motion for constrained mechanical systems with singular mass matrices and applications to multi-body dynamics 1 2 FIRDAUS E. UDWADIA AND PHAILAUNG PHOHOMSIRI 1Civil Engineering, Aerospace and Mechanical Engineering, Mathematics, and Information and Operations Management, and 2Aerospace and Mechanical Engineering, University of Southern California, Los Angeles, CA 90089, USA We present the new, general, explicit form of the equations of motion for constrained mechanical systems applicable to systems with singular mass matrices. The systems may have holonomic and/or non holonomic constraints, which may or may not satisfy D’Alembert’s principle at each instant of time. -
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. -
Theory of Machine(Tom)
BITT POLYTECHNIC GETLATU, RANCHI SUBJECT : THEORY OF MACHINE ( MEC405) SEMESTER : 4TH OBJECTIVE QUESTION 1. Turning moment diagram is a graph between a. Torque and Crank angle b. Torque and crank radius c. Force and crank radius d. none of the above ANS – a 2. In reciprocating engine, which of the following restraining body does not exist? a. Connecting rod b. Crank c. Slider d. Lever ANS – d 3. A kinematic pair consists of a. Two links b. Three links c. Four links d. Any number of links ANS - a 4. A kinematic pair cannot be classified according to a. Nature of contact between the links b. Type of relative motion between the links c. Nature of mechanical constraints between the links d. Number of links connected ANS - d 5. A lower pair has a. Surface contact b. Line contact c. Point contact d. All of the above ANS - a 6. In four bar kinematic chain, the relation between the number of pairs (p) and number of links (L) is given by a. L=2p-4 b. L=4p-2 c. L=3p-2 d. L=2p-3 ANS - a 7. Which of the following is not a type of constrained motions? a. Completely b. Incompletely c. Successfully d. Unsuccessfully ANS - d 8. Mechanism is a kinematic chain in which a. None of the link is fixed b. One link is fixed c. Two links are fixed d. None of the above ANS - b 9. A four bar kinematic chain has ____ turning pairs a. One b. Two c. Three d.