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XFEM Analysis of Cold
Hole Expansion
Daniel Stockton
2/24/2015
Table of Contents
• Successes:
– Repeat Past XFEM Studies
– Study Mesh Sensitivities
– Cold Expansion with Coarse Mesh
– SIF – Coarse Mesh w/ & w/o Residual Stress
– SIF – Fine Mesh w/o Residual Stress
– Putting Crack into Deformed Mesh
• Next Studies
• Issues
Success:
Repeat of past XFEM Studies
• XFEM Modeling of Mixed-
Mode Cracks in Thin Aluminum
Panels
• 30°, 60° and 90° crack, w.r.t. to
tensile direction, placed in
center
• Displacement until failure
• Abaqus version 6.9
Displacement
Clamped
90° crack 60° crack 30° crack
Success:
Repeat of past XFEM Studies
• XFEM Modeling of Mixed-
Mode Cracks in Thin Aluminum
Panels
Paper’s Results
My Results
Abaqus v6.12
90° crack 60° crack 30° crack
Success:
Repeat of past XFEM Studies
1500
1600
1700
1800
1900
2000
2100
2200
2 3 4 5 6 7
MaxReactionForce,N
Nominal Crack Length, mm
Reaction Force vs Nominal Crack Length
Experimental Results My Simulation Results Paper's Simulation Results
Crack Angle
Experimental
Force, N
My
Simulation
Force, N
My
Error
Paper's
Simulation
Force, N
Paper's
Error
30° 2162 2071 4.2% 2122 -1.9%
60° 1784 1694 5.0% 1864 4.4%
90° 1695 1601 5.5% 1686 -0.5%
Success:
Study Mesh Sensitivities
• Crack is placed and will jump to next element mesh line along the same
path as the crack.
• XFEM does not work when starting from a mesh line perpendicular to force
direction.
• Why? Because it needs to create two new phantom nodes along the same
direction as the force.
Success:
Study Mesh Sensitivities
• Mesh slightly modified.
• XFEM crack jumps to mesh line not perpendicular to the force.
• Crack propagates as expected.
XFEM Crack Placed XFEM Crack Jumps XFEM Crack Propagates
Success:
Study Mesh Sensitivities
• Basic concept for XFEM is that two new phantom mesh nodes are created
in place of the crack intersection.
• However, a crack along the mesh line will not separate in my experience.
New
phantom
nodes
Success:
Study Mesh Sensitivities
• XFEM crack “Short” jump vs “Long” jump, same crack angle.
• Results are impacted to a small degree.
Short vs Long
Crack Angle Experimental Short Jump Error Long Jump Error
Max Force Max Force Max Force
30° 2162 2071 4.21% 2030 6.11%
60° 1784 1694 5.04% 1640 8.07%
90° 1695 1601 5.55% 1543 8.97%
4.21%
5.04%
5.55%
6.11%
8.07%
8.97%
1500
1700
1900
2100
2300
30° Crack 60° Crack 90° Crack
MaxReactionForce,N
Experimental Reaction Force Short Jump Reaction Force Long Jump Reaction Force
% Error from Experimental Value
Success:
Cold Expansion with Coarse Mesh
• 4% hole expansion.
100 mm
100mm
6.35 mm
Ø 7.671 mm
(Initial)
Ø 7.978 mm
(max)
Ø 7.943 mm
(Final)
Success:
Cold Expansion with Coarse Mesh
Residual Stresses
after 4% Expansion
Success:
Cold Expansion with Coarse Mesh
• Residual Stresses after 4% expansion, Entry and Exit.
-700.00
-600.00
-500.00
-400.00
-300.00
-200.00
-100.00
0.00
100.00
200.00
0 0.01 0.02 0.03 0.04 0.05
Stress(MPa)
Distance from Hole (m)
3D - Residual Stresses
Entry Tangential
Exit Tangential
Entry Radial
Exit Radial
Success:
Cold Expansion with Coarse Mesh
• S22, Tangential Stress .
Success:
Stress Intensity Factor, SIF
• Contour integral method used to calculate stress intensity factor
• Each ring is a an individually calculated contour around the crack opening
• Ring is based off of mesh, user specifies # of rings.
• SIF value should converge as the number of rings increase
Converged Value
Ring 1 Ring 2 Ring 3 Ring 4
Ring 1
Ring 2
Ring 3 Ring 4 Ring 5 Ring 6 Ring 7
Success:
SIF – Fine Mesh w/ & w/o Residual Stress
• 1.0 mm crack at Mandrel Entry Edge, both sides
Crack Location
Entry Side Hole Surface
Entry Side Hole Surface
1.0 mm
0.6 mm
6.35 mm
Success:
SIF – With and Without Residual Stress
With Residual StressWithout Residual Stress
Success:
SIF – With and Without Residual Stress
• Crack Opening comparison
• 5x Deformation Scale
Without Residual Stress With Residual Stress
Crack Opening
Crack Opening
Success:
SIF – With and Without Residual Stress
• Stress intensity factor contour integrals.
Stress intensity factor = 26.2 𝑀𝑃𝑎 𝑚 Stress intensity factor = 8.1 𝑀𝑃𝑎 𝑚
Next Studies
• Low-Cycle fatigue in steps.
– Low-cycle fatigue maximum of 10,000 cycles
• Continue to high-cycle Fatigue correlation.
– XFEM only does low-cycle fatigue
• Al-Li fatigue testing
• Meshing
– Depends on crack size but always difficult with super fine mesh
• Cold Expansion with Fine Mesh
– Static: Large overpenetration except with Reduced Integration
– Implicit: Too slow and large penetration
– Explicit: Too slow
• Equilibrium of Residual Stresses
– If Equilibrium step used then residual stresses shift.
• Deformed Part
– Currently pulled from ODB but orphan mesh.
Issues:
THE END
Thank you

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Daniel Stockton - XFEM PRESENTATION

  • 1. XFEM Analysis of Cold Hole Expansion Daniel Stockton 2/24/2015
  • 2. Table of Contents • Successes: – Repeat Past XFEM Studies – Study Mesh Sensitivities – Cold Expansion with Coarse Mesh – SIF – Coarse Mesh w/ & w/o Residual Stress – SIF – Fine Mesh w/o Residual Stress – Putting Crack into Deformed Mesh • Next Studies • Issues
  • 3. Success: Repeat of past XFEM Studies • XFEM Modeling of Mixed- Mode Cracks in Thin Aluminum Panels • 30°, 60° and 90° crack, w.r.t. to tensile direction, placed in center • Displacement until failure • Abaqus version 6.9 Displacement Clamped 90° crack 60° crack 30° crack
  • 4. Success: Repeat of past XFEM Studies • XFEM Modeling of Mixed- Mode Cracks in Thin Aluminum Panels Paper’s Results My Results Abaqus v6.12 90° crack 60° crack 30° crack
  • 5. Success: Repeat of past XFEM Studies 1500 1600 1700 1800 1900 2000 2100 2200 2 3 4 5 6 7 MaxReactionForce,N Nominal Crack Length, mm Reaction Force vs Nominal Crack Length Experimental Results My Simulation Results Paper's Simulation Results Crack Angle Experimental Force, N My Simulation Force, N My Error Paper's Simulation Force, N Paper's Error 30° 2162 2071 4.2% 2122 -1.9% 60° 1784 1694 5.0% 1864 4.4% 90° 1695 1601 5.5% 1686 -0.5%
  • 6. Success: Study Mesh Sensitivities • Crack is placed and will jump to next element mesh line along the same path as the crack. • XFEM does not work when starting from a mesh line perpendicular to force direction. • Why? Because it needs to create two new phantom nodes along the same direction as the force.
  • 7. Success: Study Mesh Sensitivities • Mesh slightly modified. • XFEM crack jumps to mesh line not perpendicular to the force. • Crack propagates as expected. XFEM Crack Placed XFEM Crack Jumps XFEM Crack Propagates
  • 8. Success: Study Mesh Sensitivities • Basic concept for XFEM is that two new phantom mesh nodes are created in place of the crack intersection. • However, a crack along the mesh line will not separate in my experience. New phantom nodes
  • 9. Success: Study Mesh Sensitivities • XFEM crack “Short” jump vs “Long” jump, same crack angle. • Results are impacted to a small degree. Short vs Long Crack Angle Experimental Short Jump Error Long Jump Error Max Force Max Force Max Force 30° 2162 2071 4.21% 2030 6.11% 60° 1784 1694 5.04% 1640 8.07% 90° 1695 1601 5.55% 1543 8.97% 4.21% 5.04% 5.55% 6.11% 8.07% 8.97% 1500 1700 1900 2100 2300 30° Crack 60° Crack 90° Crack MaxReactionForce,N Experimental Reaction Force Short Jump Reaction Force Long Jump Reaction Force % Error from Experimental Value
  • 10. Success: Cold Expansion with Coarse Mesh • 4% hole expansion. 100 mm 100mm 6.35 mm Ø 7.671 mm (Initial) Ø 7.978 mm (max) Ø 7.943 mm (Final)
  • 11. Success: Cold Expansion with Coarse Mesh Residual Stresses after 4% Expansion
  • 12. Success: Cold Expansion with Coarse Mesh • Residual Stresses after 4% expansion, Entry and Exit. -700.00 -600.00 -500.00 -400.00 -300.00 -200.00 -100.00 0.00 100.00 200.00 0 0.01 0.02 0.03 0.04 0.05 Stress(MPa) Distance from Hole (m) 3D - Residual Stresses Entry Tangential Exit Tangential Entry Radial Exit Radial
  • 13. Success: Cold Expansion with Coarse Mesh • S22, Tangential Stress .
  • 14. Success: Stress Intensity Factor, SIF • Contour integral method used to calculate stress intensity factor • Each ring is a an individually calculated contour around the crack opening • Ring is based off of mesh, user specifies # of rings. • SIF value should converge as the number of rings increase Converged Value Ring 1 Ring 2 Ring 3 Ring 4 Ring 1 Ring 2 Ring 3 Ring 4 Ring 5 Ring 6 Ring 7
  • 15. Success: SIF – Fine Mesh w/ & w/o Residual Stress • 1.0 mm crack at Mandrel Entry Edge, both sides Crack Location Entry Side Hole Surface Entry Side Hole Surface 1.0 mm 0.6 mm 6.35 mm
  • 16. Success: SIF – With and Without Residual Stress With Residual StressWithout Residual Stress
  • 17. Success: SIF – With and Without Residual Stress • Crack Opening comparison • 5x Deformation Scale Without Residual Stress With Residual Stress Crack Opening Crack Opening
  • 18. Success: SIF – With and Without Residual Stress • Stress intensity factor contour integrals. Stress intensity factor = 26.2 𝑀𝑃𝑎 𝑚 Stress intensity factor = 8.1 𝑀𝑃𝑎 𝑚
  • 19. Next Studies • Low-Cycle fatigue in steps. – Low-cycle fatigue maximum of 10,000 cycles • Continue to high-cycle Fatigue correlation. – XFEM only does low-cycle fatigue • Al-Li fatigue testing
  • 20. • Meshing – Depends on crack size but always difficult with super fine mesh • Cold Expansion with Fine Mesh – Static: Large overpenetration except with Reduced Integration – Implicit: Too slow and large penetration – Explicit: Too slow • Equilibrium of Residual Stresses – If Equilibrium step used then residual stresses shift. • Deformed Part – Currently pulled from ODB but orphan mesh. Issues: