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NUI Galway – UL Alliance First Annual ENGINEERING AND - ARAN ...

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A multiaxial damage mechanics methodology for fretting fatigue prediction<br />

T. Zhang, P.E. McHugh, S.B. Leen<br />

Department of Mechanical and Biomedical Engineering, <strong>NUI</strong> <strong>Galway</strong>, Ireland<br />

t.zhang2@nuigalway.ie<br />

Abstract<br />

A multiaxial damage mechanics methodology is<br />

developed to predict fretting crack nucleation. Material<br />

degradation and wear behaviour are predicted<br />

incrementally during each fretting cycle using an<br />

energy-based wear simulation method. A combined<br />

wear-fatigue methodology is implemented in a finite<br />

element (FE) adaptive mesh framework. Predictions are<br />

validated against published data.<br />

1. Introduction<br />

Fretting occurs when two contacting bodies experience<br />

small amplitude oscillatory motion. Fretting in different<br />

layers of flexible marine risers is one application of the<br />

present work. The aim is to develop a continuum<br />

damage mechanics (CDM) methodology for fretting<br />

fatigue prediction. Two specific contact arrangements -round-on-flat<br />

(RF) and rounded punch-on-flat (RPF) are<br />

compared in terms of the prediction of evolution of<br />

wear, plasticity, fatigue damage and the contact<br />

geometry across a range of fretting variables. An<br />

incremental wear simulation method based on the<br />

energy approach of Fouvry et al [2] and previous work<br />

[1] is implemented within an adaptive mesh user<br />

subroutine. A non-linear kinematic hardening plasticity<br />

formulation is employed along with a critical-plane,<br />

Smith-Watson-Topper approach to predict multiaxial<br />

fretting crack nucleation. Wear evolution and crack<br />

nucleation predictions are validated against existing<br />

published data for Ti-6Al-4V [1]. CDM (user<br />

subroutine) implementations of the uniaxial Basquin<br />

equation and multiaxial Lemaitre and Chaboche [3]<br />

cumulative fatigue damage model are developed. To<br />

apply this fretting methodology to flexible riser<br />

pressure armour layer material, a tribology test<br />

programme is proposed.<br />

(a) (b)<br />

Figure 1. FE model in ABAQUS of (a) RF and (b) RPF<br />

2. Method<br />

Fig 1 shows FE models of the RF and RPF contact<br />

geometries for fretting wear simulation. Hertzian theory<br />

was used to validate the initial (no-wear) stress and<br />

contact pressure distributions. Non-linear kinematic<br />

183<br />

hardening plasticity is employed to capture a cyclic<br />

plasticity ratchetting phenomenon.<br />

For both the gross slip (no stick) and partial slip (central<br />

stick region) fretting regimes, a user subroutine<br />

UMESHMOTION was used to incrementally simulate<br />

wear damage, based on the energy wear approach<br />

proposed by Fouvy et al [2]. A multiaxial<br />

implementation of the Lemaitre and Chaboche nonlinear-continuous-damage<br />

(NLCD) model [3] is<br />

adopted to predict the evolution of fretting-induced<br />

fatigue damage via a UMAT user subroutine. The<br />

evolution of multiaxial damage is given by:<br />

β<br />

β α<br />

AII<br />

dD [ D ] dN<br />

M b σ H mean D ⎥ ⎡<br />

⎤<br />

+ 1<br />

= 1−<br />

( 1−<br />

) ⋅ ⎢<br />

⎣ 0 ( 1−<br />

3 2 , )( 1−<br />

) ⎦<br />

where AII is the amplitude of octahedral shear stress and<br />

σH,mean is the mean hydrostatic stress. The material is<br />

softened by the damage as follows:<br />

E = E ( 1−<br />

D)<br />

0<br />

3. Results and conclusion<br />

A validated fretting wear-fatigue methodology has been<br />

developed for Ti-6Al-4V. The key role of slip regime<br />

for crack nucleation is highlighted. Wear is predicted to<br />

have a significantly more profound effect on fatigue<br />

crack nucleation life for the RF case, reducing life in<br />

the partial slip regime and increasing it in the gross slip<br />

regime. The predicted (with wear) life for the RPF<br />

geometry under nominally identical load conditions, is<br />

significantly larger than for the RF case at low<br />

displacements but similar at high displacements. Fig 2<br />

shows the predicted evolution of fatigue damage.<br />

Fig. 2. Preicted evolution of fatigue damage.<br />

4. References<br />

1. Ding, J. et al., Trib Int, 42 (2009) 1651-1662<br />

2. Fouvry, S. et al., Wear, 255 (2003) 287-298.<br />

3. Lemaitre, J. and Chaboche, J.L. (1990) Mechanics of Solid<br />

Materials.: Cambridge University Press, Cambridge.

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