CleanSky2 LPA - Platform 1 l Efficient simulation of ...Element type: S8R (quadrilateral shell with...

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This document is the property of one or more Parties to the Clean Sky 2 LPA IADP consortium and shall not be distributed or reproduced without their formal approval CleanSky2 LPA - Platform 1 Efficient simulation of multiple impacts on double-curved composite structures presented by Marc Garbade (German Aerospace Center) Paris, 7 th of September 2017

Transcript of CleanSky2 LPA - Platform 1 l Efficient simulation of ...Element type: S8R (quadrilateral shell with...

Page 1: CleanSky2 LPA - Platform 1 l Efficient simulation of ...Element type: S8R (quadrilateral shell with eight nodes) ... Implementation of subsequent analysis steps to assess the residual

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CleanSky2 LPA - Platform 1 Efficient simulation of multiple impacts on double-curved composite structures presented by

Marc Garbade (German Aerospace Center)

Paris, 7th of September 2017

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The Big Picture

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Composite aircraft structures are vulnerable to impacts by foreign objects, e.g.

in-flight & ground hail ice-shedding tool-drop (production & maintenance)

… leading to barely visible impact damage (BVID), potentially

remaining undetected in the structure accumulating up to the next maintenance

date

adapted from [1]

Single-curved panel Double-curved panel

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Project objectives

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un

dam

age

d

sin

gle

d

amag

e

mu

ltip

le

dam

age

Project objectives: Assessment of multiple impact damage in

composite aircraft components Simulation methodology to evaluate the

impact response and the residual properties of the structure

[2][3]

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πœ‰

πœ‚

𝜌

Fiber breakage

Matrix cracking

Delamination

No damage

Low-fidelity simulation methodology…

… in a nutshell

Structural modeling Contact modeling by using contact laws Discretization with a single layer of

shell elements

Material modeling Three-dimensional stress state recovery Use of modern three-dimensional failure

criteria (Puck, Cuntze, LaRC04) Material degradation with a lookup table

Exp. Sim. Application in a multiple impact simulation

Experimental vs. virtual

testing

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II. Eye candy

Fiber breakage

Matrix cracking

Delamination

No damage

Example:

5 unique impactors with isotropic material behavior (stainless steel & aluminium alloy)

Kinetic energies 25 𝐽 – 60 𝐽

Application in a multiple impact simulation

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Outline

I. Introduction

The Big Picture

Project objectives

Low-fidelity simulation methodology in a nutshell

II. Eye candy

III. Numerical experiments

Modeling strategy

Verification by means of literature results

Validation by means of single-drop tests

IV. Conclusion

V. Acknowledgements

VI. Contact

VII. References

VIII. Appendix

Verification of the material degradation lookup table

Verification of the extended 2D method

6

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III. Numerical experiments

Modeling strategy

Fiber breakage

Matrix cracking

Delamination

No damage

Three-dimensional stress state recovery: Transverse shear stresses Transverse normal stress Damage initiation: Fiber breakage = Maximum Stress criterion Matrix cracking = Cuntze [5] Delamination = Choi & Chang [6] Damage evolution:

Elastic constants in Pa 𝑒𝐹𝐡 β‰₯ 1 𝑒𝑀𝐢 β‰₯ 1 𝑒𝐷𝐸𝐿 β‰₯ 1

𝐸11 𝐸22 𝐸33 𝜈12 𝜈13 𝜈23 𝐺12 𝐺13 𝐺23 - - -

1. 𝐸22 𝐸33 0. 0. 0. 1. 𝐺13 𝐺23 X - -

𝐸11 1. 1. 0. 0. 0. 𝐺12 𝐺13 𝐺23 - X -

𝐸11 𝐸22 𝐸33 𝜈12 𝜈13 𝜈23 1. 1. 1. - - X

1. 1. 1. 0. 0. 0. 1. 1. 1. X X -

𝐸11 1. 1. 0. 0. 0. 1. 1. 1. - X X

1. 𝐸22 𝐸33 0. 0. 0. 1. 1. 1. X - X

1. 1. 1. 0. 0. 0. 1. 1. 1. X X X

Rolfes & Rohwer [4]

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III. Numerical experiments

Modeling strategy

𝑦

π‘₯ 𝑧

100 π‘šπ‘š

100 π‘šπ‘š

Contact modeling: Loading phase = Hertz Unloading phase = Crook Reloading phase = Tan & Sun [7]

Element type: S8R (quadrilateral shell with eight nodes) Boundary conditions (π’–π’Š, π’—π’Š = 0): 𝑒π‘₯, 𝑒𝑦, 𝑒𝑧, 𝑣π‘₯, 𝑣𝑦, 𝑣𝑧 at edges T & R (clamped) or

𝑒π‘₯, 𝑒𝑦, 𝑒𝑧 at edges T & R (simple supported)

𝑒π‘₯, 𝑣𝑦, 𝑣𝑧 at edge L (symmetry in x-direction)

𝑒𝑦, 𝑣π‘₯, 𝑣𝑧 at edge B (symmetry in y-direction)

T

R

B

L

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III. Numerical experiments

Modeling strategy

𝑦

π‘₯ 𝑧

100 π‘šπ‘š

75 π‘šπ‘š

150 π‘šπ‘š

125 π‘šπ‘š

Contact modeling: Loading phase = Hertz Unloading phase = Crook Reloading phase = Tan & Sun [7]

Element type: S8R (quadrilateral shell with eight nodes) Boundary conditions (π’–π’Š, π’—π’Š = 0): 𝑒π‘₯, 𝑒𝑦, 𝑒𝑧, 𝑣π‘₯, 𝑣𝑦, 𝑣𝑧 at edges T & B (clamped)

𝑒π‘₯, 𝑒𝑦, 𝑒𝑧 at edges L & R (simple supported)

𝑒𝑦 in the red-shaded area

T

R

B

L

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Verification by means of literature values

III. Numerical experiments

[8][9][10]

Impactor: stainless steel 32.67 𝑔 𝑣 = 1 π‘š 𝑠 Ø 20 π‘šπ‘š Target: 8 π‘šπ‘š thickness stainless steel clamped

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Verification by means of literature values

III. Numerical experiments

Impactor: stainless steel 8.84 𝑔 𝑣 = 3 π‘š 𝑠 Ø 12.7 π‘šπ‘š Target: 2.69 π‘šπ‘š thickness [(0,90)2, 0]𝑠 simple supported

[11][12][13]

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III. Numerical experiments

Validation by means of single-drop tests

10 𝐽 15 𝐽

35 𝐽 25 𝐽 Impactor: stainless steel 3.95 π‘˜π‘” Ø 16 π‘šπ‘š Target: 4 π‘šπ‘š thickness [ Β±45 5, 45]s

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III. Numerical experiments

Validation by means of single-drop tests

35 𝐽

15 𝐽

25 𝐽

Projected delamination areas: LHS C-scan result RHS Simulation

10 𝐽

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III. Numerical experiments

Validation by means of single-drop tests

10 𝐽 15 𝐽

30 𝐽 25 𝐽 Impactor: stainless steel 3.95 π‘˜π‘” Ø 16 π‘šπ‘š Target: 4 π‘šπ‘š thickness [ Β±45, 0,90 2, Β±45,0]s

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III. Numerical experiments

Validation by means of single-drop tests

30 𝐽

15 𝐽

25 𝐽

Projected delamination areas: LHS C-scan result RHS Simulation

10 𝐽

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IV. Conclusion

Verification by means of literature results: All results are in line with literature results Validation by means of single-drop tests: Very satisfying results w.r.t. the projected delamination areas Good agreement between the measured & simulated contact force history

Points to optimize: Simulated contact stiffness is slightly too soft in all cases explains the right-shift The effect of material degradation on the contact force history is slightly too small results in

overestimated contact force maxima

Next challenges: Validation of simulation methodology for multiple impact problems Implementation of an expression for brittle impact behavior (hail, ice-shedding) Implementation of subsequent analysis steps to assess the residual strength or fatigue behavior of the

damaged structure

conservative deviations

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This project has received funding from the Clean

Sky 2 Joint Undertaking under the European

Union's Horizon 2020 research and innovation

programme under H2020-CS2-CPW01-2014-01

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V. Acknowledgements

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VI. Contact

Thank you for your attention!

Marc Garbade, M.Sc.

Email: [email protected]

Phone: +49(0)5312953666

German Aerospace Center e.V. (DLR)

Composite Structures and Adaptive Systems | Lilienthalplatz 7 | 38108

Brunswick, Germany

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VII. References

[1] http://testcs.openimpact.be/green-regional-aircraft-gra (saved on 26.08.2017) [2] Wolff, C. & Wilckens, D. (2015) Testing and simulation of impact damaged stiffened CFRP-panels. 3rd Int. Conference on Buckling and Postbuckling Behaviour of Composite Laminated Shell Structures, 25.03.2015-27.03.2015, Brunswick.

[3] Wilckens, D. (2015) Buckling and Post Buckling of Stiffened CFRP Panels under Compression and Shear Loading. 3rd Int. Conference on Buckling and Postbuckling Behaviour of Composite Laminated Shell Structures, 25.03.2015-27.03.2015, Brunswick. [4] Rolfes R., & Rohwer K. (1997). Improved transverse shear stresses in composite finite elements based on first order shear deformation theory. Int J Numer Methods Eng, 40, 51–60. [5] Cuntze RG, & Freund A. (2004). The predictive capability of failure mode concept-based strength criteria for multidirectional laminates. Compos Sci Technol, 64(3-4), 343–77. [6] Choi HY, Chang FK (1992). A model for predicting damage in graphite/ epoxy laminated composites resulting from low-velocity point impact. J Compos Mater, 26, 2134–69. [7] Tan TM, & Sun CT (1985). Use of statical indentation laws in the impact analysis of laminated composite plates. Journal of Applied Mechanics, 52, 6– 12.

[8] Karas, K. (1939). Platten unter seitlichem Stoss. Ingenieur-Archiv, 10(1883), 237–50.

[9] Mahajan, P., & Dutta, a. (1999). Adaptive computation of impact force under low velocity impact. Computers & Structures, 70(2),

229–241.

[10] Lin, J., Naceur, H., Coutellier, D., & Abrate, S. (2015). Numerical modeling of the low-velocity impact of composite plates using a shell-based SPH method. Meccanica.

[11] Krishnamurthy, K. S., Mahajan, P., & Mittal, R. K. (2001). A parametric study of the impact response and damage of laminated

cylindrical composite shells. Composites Science and Technology, 61(12), 1655–1669.

[12] Chandrashekhara, K., & Schroeder, T. (1995). Nonlinear impact analysis of laminated cylindrical and doubly curved shells.

Journal of Composite Materials, 29(16), 2160-2178.

[13] Sun, C. T., & Chen, J. K. (1985). On the Impact of Initially Stressed Composite Laminates. Journal of Composite Materials, 19(6), 490–504.

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impact side

VIII. Appendix

Verification of the material degradation lookup table

Damage evolution: Degradation model

causes stress redistribution in cases of damage

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VIII. Appendix

Verification of the extended 2D method

Double-cosine load: Amplitude of +1 Rectangular plate: 1 π‘šπ‘š thickness 0.128 mm layer thickness [ 0,90 2]s