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Influence of abradable coating wear mechanical properties on rotor stator interaction A. Batailly, M. Legrand, C. Pierre Structural Dynamics and Vibration Laboratory McGill University Introduction Structural model Contact dynamics


  1. Influence of abradable coating wear mechanical properties on rotor stator interaction A. Batailly, M. Legrand, C. Pierre Structural Dynamics and Vibration Laboratory – McGill University

  2. Introduction Structural model Contact dynamics Abradable coating modeling Results Conclusion and perspectives Outline 1 Introduction 2 Structural model 3 Contact dynamics 4 Abradable coating modeling 5 Results 6 Conclusion and perspectives A. Batailly, M. Legrand, C. Pierre Turbo Expo 2011 June 9 2011 2 / 19

  3. Introduction Structural model Contact dynamics Abradable coating modeling Results Conclusion and perspectives Industrial context combustion chamber compressor booster fan • Modern turbomachines • Optimization of power efficiency • ⇒ new designs (higher casing conicity, clearance closure...) A. Batailly, M. Legrand, C. Pierre Turbo Expo 2011 June 9 2011 3 / 19

  4. Introduction Structural model Contact dynamics Abradable coating modeling Results Conclusion and perspectives Industrial context • Compressor stage • Possible parasitic leakage • ⇒ significant loss of power A. Batailly, M. Legrand, C. Pierre Turbo Expo 2011 June 9 2011 3 / 19

  5. Introduction Structural model Contact dynamics Abradable coating modeling Results Conclusion and perspectives Industrial context CASING BLADE • Compressor stage • Possible parasitic leakage • ⇒ significant loss of power A. Batailly, M. Legrand, C. Pierre Turbo Expo 2011 June 9 2011 3 / 19

  6. Introduction Structural model Contact dynamics Abradable coating modeling Results Conclusion and perspectives Industrial context • Modeling of abradable coating ◮ Mono-dimensional plastic law ◮ Plastic finite-elements around the casing • Blade / abradable coating contact simulations ◮ Variation of the material parameters of the abradable coating ◮ Consequences over the blade’s amplitude of vibration ◮ Consequences in terms of wear level A. Batailly, M. Legrand, C. Pierre Turbo Expo 2011 June 9 2011 3 / 19

  7. Introduction Structural model Contact dynamics Abradable coating modeling Results Conclusion and perspectives Outline 1 Introduction 2 Structural model 3 Contact dynamics 4 Abradable coating modeling 5 Results 6 Conclusion and perspectives A. Batailly, M. Legrand, C. Pierre Turbo Expo 2011 June 9 2011 4 / 19

  8. Introduction Structural model Contact dynamics Abradable coating modeling Results Conclusion and perspectives Blade • Industrial finite element model ( ≃ 65 , 000 dof) • 8 nodes used for contact management between the contact nodes leading edge and the trailing edge f Ω • clamped boundary conditions between the blade and the disk • use of the Craig-Bampton CMS (ROM contains 85 dof) e r e z f Ω clamped e θ boundaries Both centrifugal stiffening and � Blade with eight interface nodes clearance closure are taken into account A. Batailly, M. Legrand, C. Pierre Turbo Expo 2011 June 9 2011 5 / 19

  9. Introduction Structural model Contact dynamics Abradable coating modeling Results Conclusion and perspectives Blade 35 • ROM of 85 dof • Good approximation of the 8 28 first eigenfrequencies over the frequency 21 rotational frequency range 14 7 0 0 0.1 0.2 0.3 0.4 rotational frequency � Campbell diagram of the ROM A. Batailly, M. Legrand, C. Pierre Turbo Expo 2011 June 9 2011 5 / 19

  10. Introduction Structural model Contact dynamics Abradable coating modeling Results Conclusion and perspectives Outline 1 Introduction 2 Structural model 3 Contact dynamics 4 Abradable coating modeling 5 Results 6 Conclusion and perspectives A. Batailly, M. Legrand, C. Pierre Turbo Expo 2011 June 9 2011 6 / 19

  11. Introduction Structural model Contact dynamics Abradable coating modeling Results Conclusion and perspectives Contact dynamics • Master/slave approach (abradable/blade), • Contact forces computed from plastic deformation of the abradable element, • Kuhn and Tucker contact conditions: ∀ x ∈ Γ m c (master surface) t N � 0 , g ( x ) � 0 , t N g ( x ) = 0 ◮ t N discretized contact pressure ◮ g gap function A. Batailly, M. Legrand, C. Pierre Turbo Expo 2011 June 9 2011 7 / 19

  12. Introduction Structural model Contact dynamics Abradable coating modeling Results Conclusion and perspectives Contact dynamics Algorithm: • Master/slave approach 1. prediction of the displacements (abradable/blade), without considering abradable coating, • Contact forces computed from plastic deformation of the 2. determination of the gap abradable element, function g , • Kuhn and Tucker contact 3. abradable internal forces conditions: ∀ x ∈ Γ m c (master computation through a surface) deformation increment ∆ ε t N � 0 , g ( x ) � 0 , t N g ( x ) = 0 introduced by predicted displacements, ◮ t N discretized contact pressure 4. displacements correction compatible with the calculated ◮ g gap function contact forces. A. Batailly, M. Legrand, C. Pierre Turbo Expo 2011 June 9 2011 7 / 19

  13. Introduction Structural model Contact dynamics Abradable coating modeling Results Conclusion and perspectives Outline 1 Introduction 2 Structural model 3 Contact dynamics 4 Abradable coating modeling 5 Results 6 Conclusion and perspectives A. Batailly, M. Legrand, C. Pierre Turbo Expo 2011 June 9 2011 8 / 19

  14. Introduction Structural model Contact dynamics Abradable coating modeling Results Conclusion and perspectives Theoretical description • one-dimensional two-node bar elements casing • nonlinear plastic constitutive law abradable e r profile θ • numerical profile in order to represent blade width e θ rotation blade tip bar element • casing is assumed perfectly � Blade interface node numerical profile rigid A. Batailly, M. Legrand, C. Pierre Turbo Expo 2011 June 9 2011 9 / 19

  15. Introduction Structural model Contact dynamics Abradable coating modeling Results Conclusion and perspectives Theoretical description • one-dimensional two-node bar elements casing • nonlinear plastic constitutive law abradable F c e r θ profile θ • numerical profile in order to F c F c represent blade width e θ r rotation blade tip bar element • casing is assumed perfectly � Blade interface node numerical profile rigid One layer of abradable elements per contact node on the blade tip ⇒ ≃ 16.000 abradable elements on the casing A. Batailly, M. Legrand, C. Pierre Turbo Expo 2011 June 9 2011 9 / 19

  16. Introduction Structural model Contact dynamics Abradable coating modeling Results Conclusion and perspectives Theoretical description Plastic constitutive law σ • Young’s modulus E K σ Y • Plastic modulus K • Yield limit σ Y E ε ε p � Plastic law for abradable modeling A. Batailly, M. Legrand, C. Pierre Turbo Expo 2011 June 9 2011 9 / 19

  17. Introduction Structural model Contact dynamics Abradable coating modeling Results Conclusion and perspectives Case study • Blade-tip/casing abradable interaction, • One blade (disk dynamics is neglected in this example), • Imperfections of the casing: deformed casing deformation along 2 and disk 5-nodal diameter free vibration modes, f Ω • Simulation parameters abradable coating (normalized) ◮ E = 11 ◮ K = 0 . 5 � Casing shapes for case study ◮ σ Y = 1 . 5 · 10 − 8 ◮ f Ω ∈ [0; 0 . 4] ◮ θ = 0 A. Batailly, M. Legrand, C. Pierre Turbo Expo 2011 June 9 2011 10 / 19

  18. Introduction Structural model Contact dynamics Abradable coating modeling Results Conclusion and perspectives Case study f Ω dependent wear level map 2 π • Abradable profiles at the end of each simulation pictured 3 angular position (rad) with colour code, 2 wear • Distinct wear profiles with π both odd and even number of lobes, 1 • Two critical velocities 0 0 appear. 0 . 24 0 . 32 0 . 4 0 . 08 0 . 16 f Ω � Abradable coating wear patterns A. Batailly, M. Legrand, C. Pierre Turbo Expo 2011 June 9 2011 10 / 19

  19. Introduction Structural model Contact dynamics Abradable coating modeling Results Conclusion and perspectives Case study s e s s s e b e e f Ω dependent wear level map b o b b l o o o 0 l l l 1 5 6 4 2 π • Abradable profiles at the end 1 of each simulation pictured 3 angular position (rad) with colour code, 2 2 wear • Distinct wear profiles with 3 π both odd and even number 4 of lobes, 1 5 • Two critical velocities 0 0 appear. 0 . 24 0 . 32 0 . 4 0 . 08 0 . 16 f Ω � Abradable coating wear patterns Complementary results: blade response spectrum for f Ω ∈ [0; 0 . 4] A. Batailly, M. Legrand, C. Pierre Turbo Expo 2011 June 9 2011 10 / 19

  20. Introduction Structural model Contact dynamics Abradable coating modeling Results Conclusion and perspectives Case study eo ( k = 5) eo ( k = 4) C 1 � Spectrum of the blade response A. Batailly, M. Legrand, C. Pierre Turbo Expo 2011 June 9 2011 11 / 19

  21. Introduction Structural model Contact dynamics Abradable coating modeling Results Conclusion and perspectives Case study eo (6) eo (4) � Spectrum of the blade response A. Batailly, M. Legrand, C. Pierre Turbo Expo 2011 June 9 2011 11 / 19

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