Nonlinear dynamics in a cam- follower impacting system Ricardo Alzate Ph.D. Student University of Naples FEDERICO II (SINCRO GROUP)

Slides:



Advertisements
Similar presentations
Piecewise-smooth dynamical systems: Bouncing, slipping and switching: 1. Introduction Chris Budd.
Advertisements

Bifurcations in piecewise-smooth systems Chris Budd.
Understanding the complex dynamics of a cam-follower impacting system
2. Piecewise-smooth maps Chris Budd. Maps Key idea … The functions or one of their nth derivatives, differ when Discontinuity set Interesting discontinuity.
III: Hybrid systems and the grazing bifurcation Chris Budd.
Dominic Hudson, Simon Lewis, Stephen Turnock
Nonlinear dynamics of a rotor contacting an elastically suspended stator 1 st International Conference on Vibro-Impact Systems Loughborough, UK, July 20-22,
IFAC AIRTC, Budapest, October 2000 On the Dynamic Instability of a Class of Switching System Robert Noel Shorten Department of Computer Science National.
Presentation outline Product development process: =>Design for Six Sigma =>Advanced modelling tools Practical examples => SKF quiet running bearing.
Overarching Goal: Understand that computer models require the merging of mathematics and science. 1.Understand how computational reasoning can be infused.
Critical Transitions in Nature and Society Marten Scheffer.
Chattering: a novel route to chaos in cam-follower impacting systems Ricardo Alzate Ph.D. Student University of Naples FEDERICO II, ITALY Prof. Mario di.
Fuzzy immune PID neural network control method based on boiler steam pressure system Third pacific-asia conference on circuits,communications and system,
Cam-follower systems: experiments and simulations by Ricardo Alzate University of Naples – Federico II WP6: Applications.
Trajectory Planning.  Goal: to generate the reference inputs to the motion control system which ensures that the manipulator executes the planned trajectory.
Mechanical Design II Spring 2013.
HMM-BASED PATTERN DETECTION. Outline  Markov Process  Hidden Markov Models Elements Basic Problems Evaluation Optimization Training Implementation 2-D.
Introduction to chaotic dynamics
Ch4: FLOWS ON THE CIRCLE Presented by Dayi Zhou 2/1/2006.
A Study on Object Grasp with Multifingered Robot Hand Ying LI, Ph.D. Department of Mechanical Engineering Kagoshima University, Japan.
UNC Chapel Hill S. Redon - M. C. Lin Rigid body dynamics II Solving the dynamics problems.
Interactive Manipulation of Rigid Body Simulations Presenter : Chia-yuan Hsiung Proceedings of SIGGRAPH 2000 Jovan Popovi´c, Steven M. Seitz, Michael.
The Islamic University of Gaza Faculty of Engineering Numerical Analysis ECIV 3306 Introduction.
Generic Simulation Approach for Multi-Axis Machining, Part 2: Model Calibration and Feed Rate Scheduling Journal of Manufacturing Science and Engineering.
1 شبيه سازی Simulation. 2 مقايسه! Experimental –Provide useful quantitative information –Are common as they use real system –Considerable Time and cost.
The Islamic University of Gaza Faculty of Engineering Civil Engineering Department Numerical Analysis ECIV 3306 Chapter 1 Mathematical Modeling.
Nonlinear Physics Textbook: –R.C.Hilborn, “Chaos & Nonlinear Dynamics”, 2 nd ed., Oxford Univ Press (94,00) References: –R.H.Enns, G.C.McGuire, “Nonlinear.
Davide Fiore Tutor: Mario di Bernardo XXIX Cycle - I year presentation Incremental stability of Filippov systems.
Aeronautics & Astronautics Autonomous Flight Systems Laboratory All slides and material copyright of University of Washington Autonomous Flight Systems.
On the Accuracy of Modal Parameters Identified from Exponentially Windowed, Noise Contaminated Impulse Responses for a System with a Large Range of Decay.
Mechatronic group at UiA 15 full time employed in teaching and labs. Mechatronic profile at UiA characterized by: High power / Power Mechatronics Dynamic.
Concluding Remarks about Phys 410 In this course, we have … The physics of small oscillations about stable equilibrium points Driven damped oscillations,
Towards Appropriate Selection of Analysis Tools and Methods.
Concluding Remarks about Phys 410 In this course, we have … The physics of small oscillations about stable equilibrium points Re-visited Newtonian mechanics.
1 Final Conference, 19th – 23rd January 2015 Geneva, Switzerland RP 15 Force estimation based on proprioceptive sensors for teleoperation in radioactive.
1 Enviromatics Environmental simulation models Environmental simulation models Вонр. проф. д-р Александар Маркоски Технички факултет – Битола 2008.
Introduction to Quantum Chaos
MA354 Mathematical Modeling T H 2:45 pm– 4:00 pm Dr. Audi Byrne.
ADAMS Assignment 5 ME451:Kinematics and Dynamics of Machine Systems.
Chaos, Communication and Consciousness Module PH19510 Lecture 16 Chaos.
Mathematical Modeling and Engineering Problem Solving
Can nonlinear dynamics contribute to chatter suppression? Gábor Stépán
ADAMS Assignment 5 ME451:Kinematics and Dynamics of Machine Systems (Spring 09)
A METHODOLOGY FOR QUALITATIVE MODELLING OF ECONOMIC, FINANCIAL SYSTEMS WITH EMPHASIS TO CHAOS THEORY Tomas Vicha, Mirko Dohnal Faculty of Business and.
LATTICE BOLTZMANN SIMULATIONS OF COMPLEX FLUIDS Julia Yeomans Rudolph Peierls Centre for Theoretical Physics University of Oxford.
Synchronization in complex network topologies
Manas Bajaj (ME) Qingguo Zhang (AE) Sripathi Mohan (AE) Thao Tran (AE)
Coupled maps for electron and ion clouds Ubaldo Iriso and Steve Peggs Many thanks to: M. Blaskiewicz, A. Drees, W. Fischer, H. Hseuh, G. Rumolo, R. Tomás,
Nonlinear Dynamics and Stability of Power Amplifiers
MA354 An Introduction to Math Models (more or less corresponding to 1.0 in your book)
Bypass transition in thermoacoustics (Triggering) IIIT Pune & Idea Research, 3 rd Jan 2011 Matthew Juniper Engineering Department,
Control and Synchronization of Chaos Li-Qun Chen Department of Mechanics, Shanghai University Shanghai Institute of Applied Mathematics and Mechanics Shanghai.
2D Henon Map The 2D Henon Map is similar to a real model of the forced nonlinear oscillator. The Purpose is The Investigation of The Period Doubling Transition.
Transition to Tubulence in the Hartmann Layer A. Thess 1, D.Krasnov 1, E. Zienicke 1, O. Zikanov 2, T. Boeck 3 1-Ilmenau University of Technology 2-University.
Controlling Chaos Journal presentation by Vaibhav Madhok.
MA354 Math Modeling Introduction. Outline A. Three Course Objectives 1. Model literacy: understanding a typical model description 2. Model Analysis 3.
MECHANICS Ms. Peace Introduction. Sequence 1.1 What is Mechanics? 1.1 What is Mechanics? 1.2 Fundamental Concepts and Principles 1.2 Fundamental Concepts.
Integrated Hands-On Mechanical System Laboratories Arif Sirinterlikci, Ph.D., Professor of Engineering Tony Kerzmann, Ph.D., Assistant Professor of Mechanical.
Aerodynamic Damping (WP2)
Global Analysis of Impacting Systems Petri T Piiroinen¹, Joanna Mason², Neil Humphries¹ ¹ National University of Ireland, Galway - Ireland ²University.
Traffic Simulation L2 – Introduction to simulation Ing. Ondřej Přibyl, Ph.D.
TOM Lab Project Anshul Padyal Anmol Mukati –
The Cournot duopoly Kopel Model
Date of download: 10/21/2017 Copyright © ASME. All rights reserved.
OSE801 Engineering System Identification Spring 2010
Introduction to chaotic dynamics
Introduction to chaotic dynamics
Large Time Scale Molecular Paths Using Least Action.
Chattering and grazing in impact oscillators
Key Ideas How do scientists explore the world?
Presentation transcript:

Nonlinear dynamics in a cam- follower impacting system Ricardo Alzate Ph.D. Student University of Naples FEDERICO II (SINCRO GROUP)

R. Alzate - Barcelona, 2007 NLD in a cam-follower impacting system2/22 Outline Background Results Conjectures and open problems

R. Alzate - Barcelona, 2007 NLD in a cam-follower impacting system3/22 Background

R. Alzate - Barcelona, 2007 NLD in a cam-follower impacting system4/22 Application problem Valve floating phenomena in cam-shaft based engines (performance reduction, piece-wearing and damage)

R. Alzate - Barcelona, 2007 NLD in a cam-follower impacting system5/22 Theoretical context Cam-follower systems are particular cases of: Hybrid automata (constrained and unconstrained modes + reset) Impact oscillator with surface forcing (nonsmooth dynamics and complex behaviour) Broad application (mechanical tools)

R. Alzate - Barcelona, 2007 NLD in a cam-follower impacting system6/22 The system: features Experimental rig to validate theoretical approaches: Flat-faced sliding follower driven by a rotating, shape selectable, eccentric cam (circular and discontinuous) with spring preload High performance sensors (encoders and gyroscope) and actuator Flexible storage and programming tools

R. Alzate - Barcelona, 2007 NLD in a cam-follower impacting system7/22 The experimental rig

R. Alzate - Barcelona, 2007 NLD in a cam-follower impacting system8/22 Results (circular shape case)

R. Alzate - Barcelona, 2007 NLD in a cam-follower impacting system9/22 Dynamics overview Low velocity region - contact condition Which phenomenon is behind this abrupt transition? Detachment and periodic regime A-periodic behaviour and chaos

R. Alzate - Barcelona, 2007 NLD in a cam-follower impacting system10/22 Modeling Mathematical representation of main events (see [1] for details): Development of expression for unconstrained state vector evolution using Lagrangian approach Transition rule between modes: impact law based on a single Newton’s restitution model Numeric evaluation with event-driven algorithm (G. Osorio) [1]. R. Alzate, M. Di Bernardo, U. Montanaro and S. Santini. “Experimental and numerical verification of bifurcations and chaos in a cam-follower impacting system”, Nonlinear dynamics, Springer

R. Alzate - Barcelona, 2007 NLD in a cam-follower impacting system11/22 Equations unconstrainedconstrained

R. Alzate - Barcelona, 2007 NLD in a cam-follower impacting system12/22 Identification Assignment of quantitative values for model parameters searching agreement with experimental data: Geometric parameters Physical parameters Restitution coefficient

R. Alzate - Barcelona, 2007 NLD in a cam-follower impacting system13/22 Validation experimentalnumerical 110 rpm 150 rpm

R. Alzate - Barcelona, 2007 NLD in a cam-follower impacting system14/22 Dynamics: simulation

R. Alzate - Barcelona, 2007 NLD in a cam-follower impacting system15/22 Conjectures and open problems

R. Alzate - Barcelona, 2007 NLD in a cam-follower impacting system16/22 Conjectures: bif. cascade 1 ω  [150,155] rpm Is particular transition to chaos on scenario 1 consequence of interrupted chattering sequences? Is such interruption of chattering due to grazing? Is scenario 1 the particular transition observed in bifurcation map obtained experimentally?

R. Alzate - Barcelona, 2007 NLD in a cam-follower impacting system17/22 Conjectures: bif. cascade 1 ω  [150,155] rpm (2) Fingered patterns

R. Alzate - Barcelona, 2007 NLD in a cam-follower impacting system18/22 Conjectures bif. cascade 2 ω  [135,160] rpm How to predict analytically conditions for existence of the period doubling cascade? [Note that vector field under study is highly nonlinear] Is scenario 2 detectable experimentally?

R. Alzate - Barcelona, 2007 NLD in a cam-follower impacting system19/22 Open problems Development of a more accurate simulation algorithm and of an appropriated continuation algorithm

R. Alzate - Barcelona, 2007 NLD in a cam-follower impacting system20/22 Open problems (2) Continuation of stable and unstable solutions and detection of smooth and DIB Analysis for coexistence of attractors and computation for related basins of attraction Experimental evidence of solutions Analysis of discontinuous-cam case

R. Alzate - Barcelona, 2007 NLD in a cam-follower impacting system21/22 Conclusion We have studied a cam follower system with continuous cam profile, involving highly nonlinearities in associated model We have detected two main bifurcation scenarios Scenario 1 involves sudden transition to chaos with chattering solutions Scenario 2 involves a period doubling route to chaos The open problem regards numerical and experimental study of coexistence between such dynamics

R. Alzate - Barcelona, 2007 NLD in a cam-follower impacting system22/22 Thanks !!!