Coupled Principles for Computational Frictional Contact Mechanics
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Dynamics of Multibody Systems in Research and Education
Editorial Dynamics of Multibody Systems in Research and Education prof. Ing. Štefan Segľa, CSc. Technical University of Košice, Faculty of Mechanical Engineering, Department of Applied Mechanics and Mechanical Engineering Štefan Segľa, prof., Ing., CSc., (born in 1954) is a professor at the Technical University of Košice, Faculty of Mechanical Engineering, Institute of Design and Process Engineering. He graduated from the Faculty of Mechanical Engineering, Czech Technical University in Prague in 1978. His research areas are kinematic and dynamic analysis and optimization of mechanical and mechatronical systems. He is an author of three monographs, twelve textbooks and more than one hundred scientific publications in journals and conference proceedings in Slovakia and abroad. Forteen papers are registered in Web of Science and SCOPUS. He is a member of IFToMM (International Federation for the Promotion of Mechanism and Machine Science), its Permanent Commission for the Standardization of Terminology and Multibody Dynamics, a vice-chairman of the Slovak National Committee of IFToMM, a member of the Czech Society of Mechanics, Slovak Society of Mechanics and Central European Association for Computational Mechanics. Many common mechanisms and machines such as vehicle and aircraft subsystems, robotic systems, biomechanical and mechatronic systems consist of rigid and deformable bodies that undergo large rigid body motion. The bodies are interconnected with kinematical constraints and coupling elements. The dynamics of these large-scale and nonlinear systems under dynamic loading in most cases can only be solved with methods of computational mechanics. For these systems the concept of the multibody dynamics can be successfuly utilized. Their mechanical models should be as complex as necessary but also as simple as possible. -
Contact Mechanics in Gears a Computer-Aided Approach for Analyzing Contacts in Spur and Helical Gears Master’S Thesis in Product Development
Two Contact Mechanics in Gears A Computer-Aided Approach for Analyzing Contacts in Spur and Helical Gears Master’s Thesis in Product Development MARCUS SLOGÉN Department of Product and Production Development Division of Product Development CHALMERS UNIVERSITY OF TECHNOLOGY Gothenburg, Sweden, 2013 MASTER’S THESIS IN PRODUCT DEVELOPMENT Contact Mechanics in Gears A Computer-Aided Approach for Analyzing Contacts in Spur and Helical Gears Marcus Slogén Department of Product and Production Development Division of Product Development CHALMERS UNIVERSITY OF TECHNOLOGY Göteborg, Sweden 2013 Contact Mechanics in Gear A Computer-Aided Approach for Analyzing Contacts in Spur and Helical Gears MARCUS SLOGÉN © MARCUS SLOGÉN 2013 Department of Product and Production Development Division of Product Development Chalmers University of Technology SE-412 96 Göteborg Sweden Telephone: + 46 (0)31-772 1000 Cover: The picture on the cover page shows the contact stress distribution over a crowned spur gear tooth. Department of Product and Production Development Göteborg, Sweden 2013 Contact Mechanics in Gears A Computer-Aided Approach for Analyzing Contacts in Spur and Helical Gears Master’s Thesis in Product Development MARCUS SLOGÉN Department of Product and Production Development Division of Product Development Chalmers University of Technology ABSTRACT Computer Aided Engineering, CAE, is becoming more and more vital in today's product development. By using reliable and efficient computer based tools it is possible to replace initial physical testing. This will result in cost savings, but it will also reduce the development time and material waste, since the demand of physical prototypes decreases. This thesis shows how a computer program for analyzing contact mechanics in spur and helical gears has been developed at the request of Vicura AB. -
AC Fischer-Cripps
A.C. Fischer-Cripps Introduction to Contact Mechanics Series: Mechanical Engineering Series ▶ Includes a detailed description of indentation stress fields for both elastic and elastic-plastic contact ▶ Discusses practical methods of indentation testing ▶ Supported by the results of indentation experiments under controlled conditions Introduction to Contact Mechanics, Second Edition is a gentle introduction to the mechanics of solid bodies in contact for graduate students, post doctoral individuals, and the beginning researcher. This second edition maintains the introductory character of the first with a focus on materials science as distinct from straight solid mechanics theory. Every chapter has been 2nd ed. 2007, XXII, 226 p. updated to make the book easier to read and more informative. A new chapter on depth sensing indentation has been added, and the contents of the other chapters have been completely overhauled with added figures, formulae and explanations. Printed book Hardcover ▶ 159,99 € | £139.99 | $199.99 The author begins with an introduction to the mechanical properties of materials, ▶ *171,19 € (D) | 175,99 € (A) | CHF 189.00 general fracture mechanics and the fracture of brittle solids. This is followed by a detailed description of indentation stress fields for both elastic and elastic-plastic contact. The discussion then turns to the formation of Hertzian cone cracks in brittle materials, eBook subsurface damage in ductile materials, and the meaning of hardness. The author Available from your bookstore or concludes with an overview of practical methods of indentation. ▶ springer.com/shop MyCopy Printed eBook for just ▶ € | $ 24.99 ▶ springer.com/mycopy Order online at springer.com ▶ or for the Americas call (toll free) 1-800-SPRINGER ▶ or email us at: [email protected]. -
Modeling of Flexible Multibody Systems Excited by Moving Loads with Application to a Robotic Portal System
CORE Metadata, citation and similar papers at core.ac.uk Provided by Institute of Transport Research:Publications The 2nd Joint International Conference on Multibody System Dynamics May 29–June 1, 2012, Stuttgart, Germany Modeling of Flexible Multibody Systems Excited by Moving Loads with Application to a Robotic Portal System Stefan Hartweg and Andreas Heckmann Department of System Dynamics and Control Robotics and Mechatronics Center (RMC) German Aerospace Center (DLR) Muenchner Strasse 20, D-82234 Wessling, Germany [Stefan.Hartweg, Andreas.Heckmann]@DLR.de ABSTRACT In this paper, an approach to solve mechanical problems with moving loads and flexible bodies is presented. Therefore, the multi-disciplinary modeling language Modelica together with the DLR FlexibleBodies Li- brary is utilized. Rather than solving the equations of motion analytically, this approach solves them numer- ically. While large overall motions of the flexible parts are described using the Floating Frame of Reference (FFR) method, the deformation is represented by appropriate shape functions. It is shown how a subsystem with masses and spring-damper elements can be connected to the flexible body and how the occurring forces of this moving load affect it. The equations of motion are derived in a general way, yielding a formulation compatible to e. g. a finite element models which are reduced to global shape functions. The usage of this formulation is shown for the simulation of a robotic portal system. 1 INTRODUCTION A variety of structures in the field of engineering is subject to moving loads. These loads can result from external forces, masses or whole subsystems moving with constant or varying velocity along the structure. -
1 Classical Theory and Atomistics
1 1 Classical Theory and Atomistics Many research workers have pursued the friction law. Behind the fruitful achievements, we found enormous amounts of efforts by workers in every kind of research field. Friction research has crossed more than 500 years from its beginning to establish the law of friction, and the long story of the scientific historyoffrictionresearchisintroducedhere. 1.1 Law of Friction Coulomb’s friction law1 was established at the end of the eighteenth century [1]. Before that, from the end of the seventeenth century to the middle of the eigh- teenth century, the basis or groundwork for research had already been done by Guillaume Amontons2 [2]. The very first results in the science of friction were found in the notes and experimental sketches of Leonardo da Vinci.3 In his exper- imental notes in 1508 [3], da Vinci evaluated the effects of surface roughness on the friction force for stone and wood, and, for the first time, presented the concept of a coefficient of friction. Coulomb’s friction law is simple and sensible, and we can readily obtain it through modern experimentation. This law is easily verified with current exper- imental techniques, but during the Renaissance era in Italy, it was not easy to carry out experiments with sufficient accuracy to clearly demonstrate the uni- versality of the friction law. For that reason, 300 years of history passed after the beginning of the Italian Renaissance in the fifteenth century before the friction law was established as Coulomb’s law. The progress of industrialization in England between 1750 and 1850, which was later called the Industrial Revolution, brought about a major change in the production activities of human beings in Western society and later on a global scale. -
Newton Euler Equations of Motion Examples
Newton Euler Equations Of Motion Examples Alto and onymous Antonino often interloping some obligations excursively or outstrikes sunward. Pasteboard and Sarmatia Kincaid never flits his redwood! Potatory and larboard Leighton never roller-skating otherwhile when Trip notarizes his counterproofs. Velocity thus resulting in the tumbling motion of rigid bodies. Equations of motion Euler-Lagrange Newton-Euler Equations of motion. Motion of examples of experiments that a random walker uses cookies. Forces by each other two examples of example are second kind, we will refer to specify any parameter in. 213 Translational and Rotational Equations of Motion. Robotics Lecture Dynamics. Independence from a thorough description and angular velocity as expected or tofollowa userdefined behaviour does it only be loaded geometry in an appropriate cuts in. An interface to derive a particular instance: divide and author provides a positive moment is to express to output side can be run at all previous step. The analysis of rotational motions which make necessary to decide whether rotations are. For xddot and whatnot in which a very much easier in which together or arena where to use them in two backwards operation complies with respect to rotations. Which influence of examples are true, is due to independent coordinates. On sameor adjacent joints at each moment equation is also be more specific white ellipses represent rotations are unconditionally stable, for motion break down direction. Unit quaternions or Euler parameters are known to be well suited for the. The angular momentum and time and runnable python code. The example will be run physics examples are models can be symbolic generator runs faster rotation kinetic energy. -
A Review on Application of Multibody Dynamics in the Field of Robotics
© 2019 JETIR January 2019, Volume 6, Issue 1 www.jetir.org (ISSN-2349-5162) A Review on Application of Multibody Dynamics in the Field of Robotics Nitin Chauhan1, Dr. Manjeet Singh Sekhon2 1, 2 – Assistant Professor, School of Mechanical Engineering, Lovely Professional University ABSTRACT With advancements in technology, robots have become very common. As robots consists of multiple connected links and moving parts, their design involves multibody dynamic analysis. This paper reviews how multibody dynamics have been explored as a design tool in the field of robotics. INTRODUCTION Most of the machines and systems including automobiles consists of a number of solid bodies that are interconnected to each other and motion of one component results in constrained motion of other. Such systems are called multibody systems[1]. Suspension systems in automobiles, landing gear of an aircraft, robotic manipulators, wind turbines all are examples of multibody systems. As different components are interacting together in a multibody system, for designing the system it becomes important to analyze how motion and forces are transmitted in the body. The study of motion of multibody system under the influence of force is commonly termed as multibody dynamics. Figure 1 Example of Multi-body Systems [1] A multibody dynamic analysis involves study of the movement of, impact of multiple bodies. As a robot manipulator consists of multiple links connected together and is used for applications that require control over path and forces involved in movement, multibody dynamics is used in robotics for manipulator design and motion analysis. This paper discusses the research trends in the application areas of multibody dynamics and major applications of MBD in the field of robotics. -
C: Contact Mechanics, in "Principles and Techniques for Desiging Precision Machines." MIT Phd Thesis, 1999
C Contact MechanicsI The theory developed by Hertz in 1880 remains the foundation for most contact problems encountered in engineering. It applies to normal contact between two elastic solids that are smooth and can be described locally with orthogonal radii of curvature such as a toroid. Further, the size of the actual contact area must be small compared to the dimensions of each body and to the radii of curvature. Hertz made the assumption based on observations that the contact area is elliptical in shape for such three-dimensional bodies. The equations simplify when the contact area is circular such as with spheres in contact. At extremely elliptical contact, the contact area is assumed to have constant width over the length of contact such as between parallel cylinders. The first three sections present the Hertz equations for these distinct cases. In addition, Section C.4 presents the equations for a sphere contacting a conical socket. Hertz theory does not account for tangential forces that may develop in applications where the surfaces slide or carry traction. Extensions to Hertz theory approximate this behavior to reasonable accuracy. Section C.5 presents the more useful equations. The final section C.6 contains MathcadÔ documents that implement these equations for computer analysis. The Hertz equations are important in the engineering of kinematic couplings particularly if the loads carried are relatively high. For a particular choice of material and contact geometry, the pertinent calculations reduce to families of curves that are convenient for sizing purposes. The typical material used is hardened bearing steel, for example, 52100 steel or 440C stainless steel heat treated to 58-62 Rockwell C. -
Contact Mechanics and Friction
Contact Mechanics and Friction Valentin L. Popov Contact Mechanics and Friction Physical Principles and Applications 1 3 Professor Dr. Valentin L. Popov Berlin University of Technology Institute of Mechanics Strasse des 17.Juni 135 10623 Berlin Germany [email protected] ISBN 978-3-642-10802-0 e-ISBN 978-3-642-10803-7 DOI 10.1007/978-3-642-10803-7 Springer Heidelberg Dordrecht London New York Library of Congress Control Number: 2010921669 c Springer-Verlag Berlin Heidelberg 2010 This work is subject to copyright. All rights are reserved, whether the whole or part of the material is concerned, specifically the rights of translation, reprinting, reuse of illustrations, recitation, broadcasting, reproduction on microfilm or in any other way, and storage in data banks. Duplication of this publication or parts thereof is permitted only under the provisions of the German Copyright Law of September 9, 1965, in its current version, and permission for use must always be obtained from Springer. Violations are liable to prosecution under the German Copyright Law. The use of general descriptive names, registered names, trademarks, etc. in this publication does not imply, even in the absence of a specific statement, that such names are exempt from the relevant protective laws and regulations and therefore free for general use. Cover design: WMXDesign GmbH Printed on acid-free paper Springer is part of Springer Science+Business Media (www.springer.com) Dr. Valentin L. Popov studied physics and obtained his doctorate from the Moscow State Lomonosow University. He worked at the Institute of Strength Physics and Materials Science of the Russian Academy of Sciences. -
Multibody System Dynamics (IMSD) Was Held at the Institute of Engineering and Computational Mechanics at the University of Stuttgart, Germany in May 29 - June 1, 2012
Final Report of the IMSD 2012 Stuttgart, Germany For more information www.itm.uni-stuttgart.de/imsd2012 1. Summary The Joint International Conference on Multibody System Dynamics (IMSD) was held at the Institute of Engineering and Computational Mechanics at the University of Stuttgart, Germany in May 29 - June 1, 2012. The IMSD conference is a biannual series that serves as a meeting point for the international Multibody community and as an opportunity to exchange high-level, current information on the theory and applications of Multibody systems. As a rapidly growing branch of mechanical dynamics, Multibody System Dynamics is seeing more and more use, and is becoming increasingly important in the development of complex engineered systems. The continual new challenges faced by the IMSD community demand productive conference forums where ideas are freely exchanged and a spirit of cooperation is encouraged. Overview of the Conference Besides seven distinguished keynote lectures, 56 technical sessions were held, offering 192 technical presentations authored by more than 450 authors. In total, 299 participants from 29 different countries participated in the IMSD 2012. The conference website can be found at: http://www.itm.uni-stuttgart.de/imsd2012 We would like to thank the following institutional sponsors for their highly appreciated support. ASME (American Society of Mechanical Engineers) IFToMM (International Federation for the Promotion of Mechanism and Machine Science) IUTAM (International Union of Theoretical and Applied Mechanics) JSME (Japan Society of Mechanical Engineers) KSME (Korean Society of Mechanical Engineers) We would like to thank the following industrial sponsors for their highly appreciated support. Alcatel-Lucent Carl Zeiss SMT ESTA Apparatebau FunctionBay GmbH Maplesoft Europe Robert Bosch GmbH SIMPACK The organization of the IMSD 2012 was supervised by an International Steering Committee consisting of the following distinguished academics. -
Introduction the Failure Process
Introduction The subject of this thesis is the surface damage due to rolling contact fatigue. Surfaces that are repeatedly loaded by rolling and sliding motion may be exposed to contact fatigue. Typical mechanical applications where such contact arises are: gears; cams; bearings; rail/wheel contacts. These components are in general exposed to high contact stresses. Despite the different purposes, they will according to Tallian [1] sooner or later suffer to contact fatigue damage if other failure modes are avoided. Even if the contact stresses may be of the same magnitude for different applications the resulting fatigue damage may vary. This is due to the fact that the contact conditions differ between the applications. The objective with the work was to verify the asperity point load mechanism for surface initiated rolling contact fatigue damage. The main focus has been on surface fatigue damage in spur gears. However, similar surface damage has been found in the other applications as well. The hypothesis was that local surface contacts can be of importance for surface initiated contact damage. The hypothesis can be visualized as local contact between asperities. When two surfaces are brought into contact the real contact area will be smaller than the apparent, this due too the fact that the contact surface is not perfectly smooth. Thus, the asperities will support the contact; see for instance Johnson [2]. The local asperity contacts will introduce stress concentrations, which will change the nominal stress field. A single asperity contact can be viewed as a Boussinesq point contact [2]. For non-conformal mechanical contacts that are susceptible for rolling contact fatigue the nominal stress fields are of Hertzian type. -
Contact Mechanics and Tribology Match
FEATURE ARTICLE Jeanna Van Rensselar / Contributing Editor Beneath the Why contact mechanics and tribology are a natural match KEY CONCEPTCONCEPTSS • CoContacntact mechanics iiss a sometimes oveoverlookedrlooked bbutut ccriticalritical asaspectpect of ttribology.ribology. • FriFrictionction rereductionduction iiss maximizmaximizeded by lleveragingeveraging the dydynaminamic bbetweenetween ssurfaceurface mmaterialaterial gengineeringg aandnd lublubricationrication genengineering. gineering. g. ••A Atetexturedxtured bbearinbearingg susurfacrface acts ass a lublubricantricant ,reservoirreservoir,, sstoringtoring daandnd ddispens-ispens- ing ththee llubricantubricant directly taatt ththee ppotinintt of ccontactontact wherwheree iitt makes mmostost ssense.ense. 52 • JULY 2015 TRIBOLOGY & LUBRICATION TECHNOLOGY WWW.STLE.ORG surface: Leveraging both disciplines together can yield results neither can achieve alone. WHEN THE THEORY OF CONTACT MECHANICS WAS FIRST DEVELOPED IN 1882, lubricants were not factored into the equation at all. Experts say that may be due to the lack of powerful ana- lytical and numerical tools that necessitated simplicity.1 The omission of lubrication from contact mechanics theory was resolved four years later when Osborne Reynolds developed what is now known as the Reynolds Equation. It describes the pressure distribution in nearly any type of fluid film bearing. WWW.STLE.ORG TRIBOLOGY & LUBRICATION TECHNOLOGY JULY 2015 • 53 Even with that breakthrough, how- WHY IS IT THE STRIBECK CURVE?4 ever, it was decades later before