Introduction to the Kinematics and Kinetics of the Top
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Screw and Lie Group Theory in Multibody Dynamics Recursive Algorithms and Equations of Motion of Tree-Topology Systems
Multibody Syst Dyn DOI 10.1007/s11044-017-9583-6 Screw and Lie group theory in multibody dynamics Recursive algorithms and equations of motion of tree-topology systems Andreas Müller1 Received: 12 November 2016 / Accepted: 16 June 2017 © The Author(s) 2017. This article is published with open access at Springerlink.com Abstract Screw and Lie group theory allows for user-friendly modeling of multibody sys- tems (MBS), and at the same they give rise to computationally efficient recursive algo- rithms. The inherent frame invariance of such formulations allows to use arbitrary reference frames within the kinematics modeling (rather than obeying modeling conventions such as the Denavit–Hartenberg convention) and to avoid introduction of joint frames. The com- putational efficiency is owed to a representation of twists, accelerations, and wrenches that minimizes the computational effort. This can be directly carried over to dynamics formula- tions. In this paper, recursive O(n) Newton–Euler algorithms are derived for the four most frequently used representations of twists, and their specific features are discussed. These for- mulations are related to the corresponding algorithms that were presented in the literature. Two forms of MBS motion equations are derived in closed form using the Lie group formu- lation: the so-called Euler–Jourdain or “projection” equations, of which Kane’s equations are a special case, and the Lagrange equations. The recursive kinematics formulations are readily extended to higher orders in order to compute derivatives of the motions equations. To this end, recursive formulations for the acceleration and jerk are derived. It is briefly discussed how this can be employed for derivation of the linearized motion equations and their time derivatives. -
Jean-Baptiste Charles Joseph Bélanger (1790-1874), the Backwater Equation and the Bélanger Equation
THE UNIVERSITY OF QUEENSLAND DIVISION OF CIVIL ENGINEERING REPORT CH69/08 JEAN-BAPTISTE CHARLES JOSEPH BÉLANGER (1790-1874), THE BACKWATER EQUATION AND THE BÉLANGER EQUATION AUTHOR: Hubert CHANSON HYDRAULIC MODEL REPORTS This report is published by the Division of Civil Engineering at the University of Queensland. Lists of recently-published titles of this series and of other publications are provided at the end of this report. Requests for copies of any of these documents should be addressed to the Civil Engineering Secretary. The interpretation and opinions expressed herein are solely those of the author(s). Considerable care has been taken to ensure accuracy of the material presented. Nevertheless, responsibility for the use of this material rests with the user. Division of Civil Engineering The University of Queensland Brisbane QLD 4072 AUSTRALIA Telephone: (61 7) 3365 3619 Fax: (61 7) 3365 4599 URL: http://www.eng.uq.edu.au/civil/ First published in 2008 by Division of Civil Engineering The University of Queensland, Brisbane QLD 4072, Australia © Chanson This book is copyright ISBN No. 9781864999211 The University of Queensland, St Lucia QLD JEAN-BAPTISTE CHARLES JOSEPH BÉLANGER (1790-1874), THE BACKWATER EQUATION AND THE BÉLANGER EQUATION by Hubert CHANSON Professor, Division of Civil Engineering, School of Engineering, The University of Queensland, Brisbane QLD 4072, Australia Ph.: (61 7) 3365 3619, Fax: (61 7) 3365 4599, Email: [email protected] Url: http://www.uq.edu.au/~e2hchans/ REPORT No. CH69/08 ISBN 9781864999211 Division of Civil Engineering, The University of Queensland August 2008 Jean-Baptiste BÉLANGER (1790-1874) (Courtesy of the Bibliothèque de l'Ecole Nationale Supérieure des Ponts et Chaussées) Abstract In an open channel, the transition from a high-velocity open channel flow to a fluvial motion is a flow singularity called a hydraulic jump. -
Nanocrystalline Nanowires: I. Structure
Nanocrystalline Nanowires: I. Structure Philip B. Allen Department of Physics and Astronomy, State University of New York, Stony Brook, NY 11794-3800∗ and Center for Functional Nanomaterials, Brookhaven National Laboratory, Upton, NY 11973-5000 (Dated: September 7, 2006) Geometric constructions of possible atomic arrangements are suggested for inorganic nanowires. These are fragments of bulk crystals, and can be called \nanocrystalline" nanowires (NCNW). To minimize surface polarity, nearly one-dimensional formula units, oriented along the growth axis, generate NCNW's by translation and rotation. PACS numbers: 61.46.-w, 68.65.La, 68.70.+w Introduction. Periodic one-dimensional (1D) motifs twinned16; \core-shell" (COHN)4,17; and longitudinally are common in nature. The study of single-walled car- heterogeneous (LOHN) NCNW's. bon nanotubes (SWNT)1,2 is maturing rapidly, but other Design principle. The remainder of this note is about 1D systems are at an earlier stage. Inorganic nanowires NCNW's. It offers a possible design principle, which as- are the topic of the present two papers. There is much sists visualization of candidate atomic structures, and optimism in this field3{6. Imaging gives insight into provides a template for arrangements that can be tested self-assembled nanostructures, and incentives to improve theoretically, for example by density functional theory growth protocols. Electron microscopy, diffraction, and (DFT). The basic idea is (1) choose a maximally linear, optical spectroscopy on individual wires7 provide detailed charge-neutral, and (if possible) dipole-free atomic clus- information. Device applications are expected. These ter containing a single formula unit, and (2) using if possi- systems offer great opportunities for atomistic modelling. -
GYRODYNAMICS Introduction to the Dynamics of Rigid Bodies
2 GYRODYNAMICS Introduction to the dynamics of rigid bodies Introduction. Though Newton wrote on many topics—and may well have given thought to the odd behavior of tops—I am not aware that he committed any of that thought to writing. But by Euler was active in the field, and it has continued to bedevil the thought of mathematical physicists. “Extended rigid bodies” are classical abstractions—alien both to relativity and to quantum mechanics—which are revealed to our dynamical imaginations not so much by commonplace Nature as by, in Maxwell’s phrase, the “toys of Youth.” That such toys behave “strangely” is evident to the most casual observer, but the detailed theory of their behavior has become notorious for being elusive, surprising and difficult at every turn. Its formulation has required and inspired work of wonderful genius: it has taught us much of great worth, and clearly has much to teach us still. Early in my own education as a physicist I discovered that I could not understand—or, when I could understand, remained unpersuaded by—the “elementary explanations” of the behavior of tops & gyros which are abundant in the literature. So I fell into the habit of avoiding the field, waiting for the day when I could give to it the time and attention it obviously required and deserved. I became aware that my experience was far from atypical: according to Goldstein it was in fact a similar experience that motivated Klein & Sommerfeld to write their 4-volume classic, Theorie des Kreisels (–). In November I had occasion to consult my Classical Mechanics II students concerning what topic we should take up to finish out the term. -
Symmetry Indicators and Anomalous Surface States of Topological Crystalline Insulators
PHYSICAL REVIEW X 8, 031070 (2018) Symmetry Indicators and Anomalous Surface States of Topological Crystalline Insulators Eslam Khalaf,1,2 Hoi Chun Po,2 Ashvin Vishwanath,2 and Haruki Watanabe3 1Max Planck Institute for Solid State Research, Heisenbergstraße 1, 70569 Stuttgart, Germany 2Department of Physics, Harvard University, Cambridge, Massachusetts 02138, USA 3Department of Applied Physics, University of Tokyo, Tokyo 113-8656, Japan (Received 15 February 2018; published 14 September 2018) The rich variety of crystalline symmetries in solids leads to a plethora of topological crystalline insulators (TCIs), featuring distinct physical properties, which are conventionally understood in terms of bulk invariants specialized to the symmetries at hand. While isolated examples of TCI have been identified and studied, the same variety demands a unified theoretical framework. In this work, we show how the surfaces of TCIs can be analyzed within a general surface theory with multiple flavors of Dirac fermions, whose mass terms transform in specific ways under crystalline symmetries. We identify global obstructions to achieving a fully gapped surface, which typically lead to gapless domain walls on suitably chosen surface geometries. We perform this analysis for all 32 point groups, and subsequently for all 230 space groups, for spin-orbit-coupled electrons. We recover all previously discussed TCIs in this symmetry class, including those with “hinge” surface states. Finally, we make connections to the bulk band topology as diagnosed through symmetry-based indicators. We show that spin-orbit-coupled band insulators with nontrivial symmetry indicators are always accompanied by surface states that must be gapless somewhere on suitably chosen surfaces. We provide an explicit mapping between symmetry indicators, which can be readily calculated, and the characteristic surface states of the resulting TCIs. -
Augustin-Louis Cauchy - Wikipedia, the Free Encyclopedia 1/6/14 3:35 PM Augustin-Louis Cauchy from Wikipedia, the Free Encyclopedia
Augustin-Louis Cauchy - Wikipedia, the free encyclopedia 1/6/14 3:35 PM Augustin-Louis Cauchy From Wikipedia, the free encyclopedia Baron Augustin-Louis Cauchy (French: [oɡystɛ̃ Augustin-Louis Cauchy lwi koʃi]; 21 August 1789 – 23 May 1857) was a French mathematician who was an early pioneer of analysis. He started the project of formulating and proving the theorems of infinitesimal calculus in a rigorous manner, rejecting the heuristic Cauchy around 1840. Lithography by Zéphirin principle of the Belliard after a painting by Jean Roller. generality of algebra exploited by earlier Born 21 August 1789 authors. He defined Paris, France continuity in terms of Died 23 May 1857 (aged 67) infinitesimals and gave Sceaux, France several important Nationality French theorems in complex Fields Mathematics analysis and initiated the Institutions École Centrale du Panthéon study of permutation École Nationale des Ponts et groups in abstract Chaussées algebra. A profound École polytechnique mathematician, Cauchy Alma mater École Nationale des Ponts et exercised a great Chaussées http://en.wikipedia.org/wiki/Augustin-Louis_Cauchy Page 1 of 24 Augustin-Louis Cauchy - Wikipedia, the free encyclopedia 1/6/14 3:35 PM influence over his Doctoral Francesco Faà di Bruno contemporaries and students Viktor Bunyakovsky successors. His writings Known for See list cover the entire range of mathematics and mathematical physics. "More concepts and theorems have been named for Cauchy than for any other mathematician (in elasticity alone there are sixteen concepts and theorems named for Cauchy)."[1] Cauchy was a prolific writer; he wrote approximately eight hundred research articles and five complete textbooks. He was a devout Roman Catholic, strict Bourbon royalist, and a close associate of the Jesuit order. -
Chapter 1 Rigid Body Kinematics
Chapter 1 Rigid Body Kinematics 1.1 Introduction This chapter builds up the basic language and tools to describe the motion of a rigid body – this is called rigid body kinematics. This material will be the foundation for describing general mech- anisms consisting of interconnected rigid bodies in various topologies that are the focus of this book. Only the geometric property of the body and its evolution in time will be studied; the re- sponse of the body to externally applied forces is covered in Chapter ?? under the topic of rigid body dynamics. Rigid body kinematics is not only useful in the analysis of robotic mechanisms, but also has many other applications, such as in the analysis of planetary motion, ground, air, and water vehicles, limbs and bodies of humans and animals, and computer graphics and virtual reality. Indeed, in 1765, motivated by the precession of the equinoxes, Leonhard Euler decomposed a rigid body motion to a translation and rotation, parameterized rotation by three principal-axis rotation (Euler angles), and proved the famous Euler’s rotation theorem [?]. A body is rigid if the distance between any two points fixed with respect to the body remains constant. If the body is free to move and rotate in space, it has 6 degree-of-freedom (DOF), 3 trans- lational and 3 rotational, if we consider both translation and rotation. If the body is constrained in a plane, then it is 3-DOF, 2 translational and 1 rotational. We will adopt a coordinate-free ap- proach as in [?, ?] and use geometric, rather than purely algebraic, arguments as much as possible. -
Script Unit 4.4 (Screw Axes in Crystal Structures).Docx
Script Unit 4.4 Welcome back! Slide 2 In the last unit, we introduced helical or screw symmetry in general; now, we want to investigate, what different kinds of screw axes, that is, what kind of different helical symmetries are present in crystal structures. Slide 3 Let’s look at a first example - here you see a unit cell of a crystal in two different views, a crystal, which should belong to the hexagonal crystal system; the right view is a projection along the c- direction. We see, that this crystal is composed of atoms, that build these helices running along all corners of the unit cell; if we look from above onto this plane, then these screws look like flat hexagons. Because this is a crystal we have translational symmetry, these helices are repeated again and again as a whole, here along the a- and b-direction. But there is - likewise as in glide planes - another symmetry element present, which has a translational component being smaller than a whole unit cell - and this is a screw axis. Slide 4 Along this axis the atoms are symmetry related to each other by applying a screw rotation: if we rotate first this atom by 60 degrees and then translate it parallel to the screw axis by one-sixth of the unit cell, then it will be mapped onto this atom. This can be done with all other atoms as well with this one, that one and so forth… This is an example of a six-fold screw axis, meaning the rotational part is 60 degrees - analogous to pure rotations. -
An Appreciation and Discussion of Paul Germain’S “The Method of Virtual Power in the Mechanics of Continuous Media I: Second-Gradient Theory”
NISSUNA UMANA INVESTIGAZIONE SI PUO DIMANDARE VERA SCIENZIA S’ESSA NON PASSA PER LE MATEMATICHE DIMOSTRAZIONI LEONARDO DA VINCI vol. 8 no. 2 2020 Mathematics and Mechanics of Complex Systems MARCELO EPSTEIN AND RONALD E. SMELSER AN APPRECIATION AND DISCUSSION OF PAUL GERMAIN’S “THE METHOD OF VIRTUAL POWER IN THE MECHANICS OF CONTINUOUS MEDIA I: SECOND-GRADIENT THEORY” msp MATHEMATICS AND MECHANICS OF COMPLEX SYSTEMS Vol. 8, No. 2, 2020 dx.doi.org/10.2140/memocs.2020.8.191 ∩ MM AN APPRECIATION AND DISCUSSION OF PAUL GERMAIN’S “THE METHOD OF VIRTUAL POWER IN THE MECHANICS OF CONTINUOUS MEDIA I: SECOND-GRADIENT THEORY” MARCELO EPSTEIN AND RONALD E. SMELSER Paul Germain’s 1973 article on the method of virtual power in continuum me- chanics has had an enormous impact on the modern development of the disci- pline. In this article we examine the historical context of the ideas it contains and discuss their continuing importance. Our English translation of the French original appears elsewhere in this volume (MEMOCS 8:2 (2020), 153–190). Introduction Among the many contributions of Paul Germain (1920–2009) to mechanics, this classical 1973 article[1973a] on the method of virtual power in continuum mechan- ics stands out for its enormous impact on the modern development of the discipline, as evidenced by hundreds of citations and by its direct or indirect influence in establishing a paradigm of thought for succeeding generations. In this article we examine the historical antecedents of the ideas contained in the article and discuss their continuing relevance. The article was published in French in the Journal de Mécanique. -
La Notion De Couple En Mécanique : Réhabiliter Poinsot
La notion de couple en mécanique : réhabiliter Poinsot par Ivor Grattan-Guinness Historien des mathématiques et philosophe des sciences Professeur émérite à l’université du Middlesex (UK) Figure 1: Louis Poinsot, gravure de Boilly. Jules Boilly (1796-1874) est un peintre et lithographe spécialisé dans la gravure de personnalités, dont les membres de l’Institut (P.S. Girard, J.D. Cassini, Alexis Bouvard). Il était le fils d’un peintre plus renommé, Léopold Boilly (1761-1845), auteur de peintures de genre et de portraits, notamment de Sadi Carnot. I - PRÉLIMINAIRES En 1803, Louis Poinsot publia un traité de statique, à caractère révolutionnaire puisqu’il posait clairement le sujet non seulement en termes de forces mais aussi en terme de « couples » (c’est son expression), c’est-à-dire des paires de forces non colinéaires égales en amplitude et en direction mais en sens opposés. Plus tard, il adapta cette notion pour induire en dynamique une relation 1 nouvelle entre mouvement linéaire et mouvement de rotation. Le présent article résume ces développements et examine leur réception, qui fut lente parmi ses contemporains mathématiciens et quasi inexistante parmi les « historiens » de la mécanique plus tard. 1. Les organisations Un beau jour, lors des années révolutionnaires II ou III, période à présent plus connue sous le nom d’année 1794, un adolescent orphelin, étudiant au collège Louis le Grand à Paris, tomba sur un prospectus annonçant la création d’une nouvelle institution d’enseignement supérieur. Intrigué, il se porta candidat et fut accepté, ce qui détermina la suite de sa longue carrière. Cette institution constituait un des deux projets du gouvernement français pour résoudre l’une des crises sociales causées par cinq années de révolution et de ruptures. -
A Computational Analysis of Line-Oriented Screw Transformations in Robotics
University of Pennsylvania ScholarlyCommons Technical Reports (CIS) Department of Computer & Information Science October 1988 A Computational Analysis of Line-Oriented Screw Transformations in Robotics Janez Funda University of Pennsylvania Follow this and additional works at: https://repository.upenn.edu/cis_reports Recommended Citation Janez Funda, "A Computational Analysis of Line-Oriented Screw Transformations in Robotics", . October 1988. University of Pennsylvania Department of Computer and Information Science Technical Report No. MS-CIS-88-83. This paper is posted at ScholarlyCommons. https://repository.upenn.edu/cis_reports/665 For more information, please contact [email protected]. A Computational Analysis of Line-Oriented Screw Transformations in Robotics Abstract This paper contains a computational analysis and comparison of various representations of a general rigid body spatial screw displacement. Point transformations and line transformations are treated separately. In the context of point transformations, only a brief summary of the known techniques (i.e., homogeneous transforms and quaternion/vector pairs) and their computational behavior is given. Among line transformations, which comprise the primary focus of this paper, four mathematical formalisms for effecting a general spatial screw displacement are presented and analyzed in terms of computational efficiency in performing (a) general screw displacements of lines, and (b) compositions of screw displacement operators. Both sequential and parallel algorithms are given for each operation. The four formalisms considered are: (1) dual orthogonal 3 x 3 matrix, (2) dual unit quaternion, (3) dual special unitary 2 x 2 matrix, and (4) dual Pauli spin matrices. The conclusion reached is that quaternion/vector pairs are the most economical of the point transformation operators, whereas dual unit quaternions represent the most compact and most efficient line ansformationtr formalism. -
La Notion De Couple En Mécanique : Réhabiliter Poinsot
Bibnum Textes fondateurs de la science Physique La notion de couple en mécanique : réhabiliter Poinsot Ivor Grattan-Guiness Traducteur : Alexandre Moatti Édition électronique URL : http://journals.openedition.org/bibnum/725 ISSN : 2554-4470 Éditeur FMSH - Fondation Maison des sciences de l'homme Référence électronique Ivor Grattan-Guiness, « La notion de couple en mécanique : réhabiliter Poinsot », Bibnum [En ligne], Physique, mis en ligne le 01 janvier 2013, consulté le 19 avril 2019. URL : http:// journals.openedition.org/bibnum/725 © BibNum La notion de couple en mécanique : réhabiliter Poinsot par Ivor Grattan-Guinness Historien des mathématiques et philosophe des sciences Professeur émérite à l’université du Middlesex (UK) Figure 1: Louis Poinsot, gravure de Boilly. Jules Boilly (1796-1874) est un peintre et lithographe spécialisé dans la gravure de personnalités, dont les membres de l’Institut (P.S. Girard, J.D. Cassini, Alexis Bouvard). Il était le fils d’un peintre plus renommé, Léopold Boilly (1761-1845), auteur de peintures de genre et de portraits, notamment de Sadi Carnot. I - PRÉLIMINAIRES En 1803, Louis Poinsot publia un traité de statique, à caractère révolutionnaire puisqu’il posait clairement le sujet non seulement en termes de forces mais aussi en terme de « couples » (c’est son expression), c’est-à-dire des paires de forces non colinéaires égales en amplitude et en direction mais en sens opposés. Plus tard, il adapta cette notion pour induire en dynamique une relation 1 nouvelle entre mouvement linéaire et mouvement de rotation. Le présent article résume ces développements et examine leur réception, qui fut lente parmi ses contemporains mathématiciens et quasi inexistante parmi les « historiens » de la mécanique plus tard.