Forced Response Prediction of Constrained and Unconstrained Structures Coupled Through Frictional Contacts

In this paper, a forced response prediction method for the analysis of constrained and unconstrained structures coupled through frictional contacts is presented. This type of frictional contact problem arises in vibration damping of turbine blades, in which dampers and blades constitute the unconstrained and constrained structures, respectively. The model of the unconstrained/free structure includes six rigid body modes and several elastic modes, the number of which depends on the excitation frequency. In other words, the motion of the free structure is not artificially constrained. When modeling the contact surfaces between the constrained and free structure, discrete contact points along with contact stiffnesses are distributed on the friction interfaces. At each contact point, contact stiffness is determined and employed in order to take into account the effects of higher frequency modes that are omitted in the dynamic analysis. Depending on the normal force acting on the contact interfaces, quasistatic contact analysis is initially employed to determine the contact area as well as the initial preload or gap at each contact point due to the normal load. A friction model is employed to determine the three-dimensional nonlinear contact forces, and the relationship between the contact forces and the relative motion is utilized by the harmonic balance method. As the relative motion is expressed as a modal superposition, the unknown variables, and thus the resulting nonlinear algebraic equations in the harmonic balance method, are in proportion to the number of modes employed. Therefore the number of contact points used is irrelevant. The developed method is applied to a bladed-disk system with wedge dampers where the dampers constitute the unconstrained structure, and the effects of normal load on the rigid body motion of the damper are investigated. It is shown that the effect of rotational motion is significant, particularly for the in-phase vibration modes. Moreover, the effect of partial slip in the forced response analysis and the effect of the number of harmonics employed by the harmonic balance method are examined. Finally, the prediction for a test case is compared with the test data to verify the developed method. DOI: 10.1115/1.2940356

[1]  C. Menq,et al.  Characterization of 3D contact kinematics and prediction of resonant response of structures having 3D frictional constraint , 1998 .

[2]  M. Hajek,et al.  Stick-slip motion of turbine blade dampers , 1992, Philosophical Transactions of the Royal Society of London. Series A: Physical and Engineering Sciences.

[3]  Chandramouli Padmanabhan,et al.  Analysis of periodically excited systems with clearances , 1994 .

[4]  Aldo A. Ferri,et al.  Friction Damping and Isolation Systems , 1995 .

[5]  Chia-Hsiang Menq,et al.  Periodic Response of Blades Having Three-Dimensional Nonlinear Shroud Constraints , 2001 .

[6]  Chengwu Duan,et al.  Transient responses of a 2-dof torsional system with nonlinear dry friction under a harmonically varying normal load , 2005 .

[7]  D. Dane Quinn,et al.  Using Series-Series Iwan-Type Models for Understanding Joint Dynamics , 2005 .

[8]  Chia-Hsiang Menq,et al.  Characterization of Contact Kinematics and Application to the Design of Wedge Dampers in Turbomachinery Blading: Part 2—Prediction of Forced Response and Experimental Verification , 1998 .

[9]  John E. Mottershead,et al.  Experimental and theoretical studies of a bolted joint excited by a torsional dynamic load , 2006 .

[10]  David J. Ewins,et al.  Underplatform Dampers for Turbine Blades: Theoretical Modeling, Analysis, and Comparison With Experimental Data , 2001 .

[11]  Chia-Hsiang Menq,et al.  One-dimensional dynamic microslip friction model , 2006 .

[12]  Chia-Hsiang Menq,et al.  The forced response of shrouded fan stages , 1986 .

[13]  D. Ewins,et al.  Analytical Formulation of Friction Interface Elements for Analysis of Nonlinear Multi-Harmonic Vibrations of Bladed Discs , 2002 .

[14]  Chia-Hsiang Menq,et al.  Characterization of Contact Kinematics and Application to the Design of Wedge Dampers in Turbomachinery Blading: Part 1—Stick-Slip Contact Kinematics , 1998 .

[15]  Walter Sextro,et al.  Spatial Dynamics of Tuned and Mistuned Bladed Disks with Cylindrical and Wedge-Shaped Friction Dampers , 2003 .

[16]  Jean-François Ferrero,et al.  Analysis of a dry friction problem under small displacements: application to a bolted joint , 2004 .

[17]  Walter Sextro,et al.  Improved Reliability of Bladed Disks due to Friction Dampers , 1997 .

[18]  Chia-Hsiang Menq,et al.  NON-LINEAR SPRING RESISTANCE AND FRICTION DAMPING OF FRICTIONAL CONSTRAINT HAVING TWO-DIMENSIONAL MOTION , 1998 .

[19]  C. Menq,et al.  STICK–SLIP–SEPARATION ANALYSIS AND NON-LINEAR STIFFNESS AND DAMPING CHARACTERIZATION OF FRICTION CONTACTS HAVING VARIABLE NORMAL LOAD , 1998 .

[20]  Chengwu Duan,et al.  Dynamics of a 3dof torsional system with a dry friction controlled path , 2006 .

[21]  Earl H. Dowell,et al.  Forced response of a cantilever beam with a dry friction damper attached, part I: Theory , 1983 .

[22]  Robert E. Kielb,et al.  An Integrated Approach for Friction Damper Design , 1990 .

[23]  D. J. Ewins,et al.  Analytical Formulation of Friction Interface Elements for Analysis of Nonlinear Multi-Harmonic Vibrations of Bladed Disks , 2003 .

[24]  David J. Ewins,et al.  MODELLING TWO-DIMENSIONAL FRICTION CONTACT AND ITS APPLICATION USING HARMONIC BALANCE METHOD , 1996 .

[25]  Ning An,et al.  A microslip friction model with normal load variation induced by normal motion , 2007 .

[26]  J. Griffin Friction Damping of Resonant Stresses in Gas Turbine Engine Airfoils , 1980 .