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Ph. D. Defense Computational Mechanics Laboratory
Numerical Analysis and Optimal Design of
Composite Thermoforming Process
by
Shih-Wei Hsiao
Department of Mechanical Engineering
and Applied Mechanics
The University of Michigan
March 25, 1997
Ph. D. Defense Computational Mechanics Laboratory
Outline
• Introduction
• FEM Analysis of Composite Thermoforming Process
– Rheological Characterization of Continuous fiber Composites
– Global FEM Analysis of Thermoforming Process
– Residual Stress Analysis
• Optimal Design of Composite Thermoforming Process
• Conclusions and Future Work
Ph. D. Defense Computational Mechanics Laboratory
Schematic of Thermoforming Process
Microstructure
Die
Blankholder
Before forming After forming
Laminate
Ph. D. Defense Computational Mechanics Laboratory
Motivations of this research
Deep drawing (stamping) of woven-fabric thermoplastic composites is a
mass production and precision shaping technology to produce composite
components.
Objectives of this research
• Develop a FEM model to analyze this thermoforming process.
• Develop an optimization algorithm based on this FEM model to
optimize this forming process.
Ph. D. Defense Computational Mechanics Laboratory
Why Thermoplastic Composites?
From the manufacturing viewpoints
• Thermosetting Resins
– Hand layed up into structural fiber preform and impregnation
after shaping
– Need chemical additives to cure after shaping and very long
cure cycle time
– Labor intense
• Thermoplastic Resins
– Shaping only depends on heat transfer and force without chemistry
– In a preimpregnated continuous tape form
– High processing rate
– Drawback: higher processing viscosity and forming
temperature (320~400 C), and higher equipment cost
Ph. D. Defense Computational Mechanics Laboratory
Advantages of the composite stamping process
u Deep drawing (stamping) of woven-fabric thermoplastic composites
is a mass production technology to produce composite components.
u This stamping process is also a precision shaping process.
u Woven-fabric composites possess a balanced drawability, and can
avoid the excessive thinning caused by the transverse intraply
shearing.
Ph. D. Defense Computational Mechanics Laboratory
Related work
• Under the kinematic consideration, the draping behavior of woven
fabrics over 3-D spherical, conical or arbitrary surfaces was
simulated by solving the intersection equations numerically.
• This approach provides a preliminary prediction of fiber buckling
and final fiber orientation.
• This approach can be used as a design tool fot selecting suitable
draped configurations for specific surfaces.
• Kinematic approach
Potter (1979)
Robertson et al. (1981)
Van West et al. (1990)
Ph. D. Defense Computational Mechanics Laboratory
• Diaphragm and blowing forming processes.
• Newtonian viscous flow formulation with the fiber inextensibility
constraint
• Inplane prediction of macroscopic stress and strain.
• Isothermal forming processes.
• Unidirectional composite sheets.
• FEM Analysis
O’Bradaigh and Pipes (1991)
O’Bradaigh et al. (1993)
Ph. D. Defense Computational Mechanics Laboratory
Goals of this FEM Analysis
A 3-D numerical modeling of thermoforming process on woven-fabric
thermoplastic composite laminates:
• Characterization of the processing rheology of woven-fabric
thermoplastic composite materials by the homogenization method.
• Coupled viscous flow and heat transfer FEM analyses for forming.
– Predictions of global and local stress, temperature and fiber
orientation distribution.
• Residual stress FEM analysis for cooling.
– Predictions of macroscopic and microscopic residual stress
and warpage after cooling.
Ph. D. Defense Computational Mechanics Laboratory
Governing equations for thermoforming process
Momentum and
continuity equations Thermal equation
Viscosity equation
Coupled
• Impossible to solve these equations at each microcell to obtain
obtain the global response.
• Homogenization method is used to overcome this difficulty.
Ph. D. Defense Computational Mechanics Laboratory
Homogenization Method for Composite Materials
X
Y
Γ
Ω
b
t
Γt
Γg
Unit cell
Unit cell
Review
• Under the assumption of periodic microstructures which can be
represented by unit cells.
• Using the asymptotic expansion of all variables and the average
technique to determine the homogenized material properties and
constitutive relations of composite materials.
• Capable of predicting microscopic fields of deformation mechanics
through the localization process.
Ph. D. Defense Computational Mechanics Laboratory
Digitized woven-fabric unit cell
Woven fabric laminate
Unit cell
Ph. D. Defense Computational Mechanics Laboratory
Thermal conductivity prediction for unidirectional
composites vs volume fraction
0
1
2
3
4
5
6
0 10 20 30 40 50 60 70 80
Thermal
conductivity
(W/m-K)
Fiber volume fraction (%)
Axial conductivity
Transverse conductivity
Experimental (axial)
Experimental (transverse)
Ph. D. Defense Computational Mechanics Laboratory
Implementation of Global FEA
• 3-D sheet forming FE analysis coupled with heat transferFE analysis
using ‘Viscous shell with thermal analysis’.
vz
vy
vx
ωx
ωy
ωz
x
y
z
Membrane element
+
Bending element
Shell element
X
Y
Z
Ph. D. Defense Computational Mechanics Laboratory
Viscous shell with thermal analysis
• Plane stress asumption-- the incompressibility constraint can be
achieved by adjusting the thickness of each shell element.
• Large deformation process divided into a series of small time step.
• Complicated geometry, friction and contact considerations.
v
(i)
→ Ý
ε
(i)
⇔ µ
(i)
⇔ T
(i)
At i-th time step
Coupled thermal analysis
Viscous shell
• Transient heat transfer FEM to solve temperature at each node.
are solved.
• At each step, solve nodal temperature and velocity iteratively
until convergence.
Ph. D. Defense Computational Mechanics Laboratory
Fiber Orientation Model
Purposes:
• Update the fiber intersection angle of each global finite element
by the global strain increment at every time step.
• Change material properties according to updated fiber orientation.
Assumptions:
• The fiber orientation of all the microstructures in one global finite
element is identical.
• The warp yarn and weft yarn of woven-fabric composites can be
represented by two unit fiber vectors.
Ph. D. Defense Computational Mechanics Laboratory
Schematic of lamina coordinate
X
Y Z
X
Y
X
Y
Layer A
Layer B
Fiber
Matrix
Lamina
Warp yarn
Weft yarn
1
2
1
2
a
b
Ph. D. Defense Computational Mechanics Laboratory
Updating Scheme
.
FEM mesh
Weft vector
Warp vector
X
Y
Z
∆t
∆ε
a
n
an+1
b
n+1
bn
φn
θ
n
θ
n+1
φn+1
x x
y y
Ph. D. Defense Computational Mechanics Laboratory
Global-local solution scheme
Global finite
element analysis
Fiber orientation
model
Obtain homogenized
material properties
Construct unit cells
Check if forming
is done
End
No
Yes
Local finite element
analysis (PREMAT)
Localization
(POSTAMT)
Begin
Ph. D. Defense Computational Mechanics Laboratory
Comparison with experiments
(cylindrical cup)
55
60
65
70
75
80
85
90
0 5 10 15 20 25
Simulation (Diagonal)
Simulation (Median)
Experiment (Diagonal)
Experiment (Median)
Fiber
intersection
angle
(deg)
Distance from the origin (mm)
Punch zone Free zone
Diagonal
Median
Median
Ph. D. Defense Computational Mechanics Laboratory
P
Laminate Unit Cell
Effective stress of laminate and unit cell at P.
Effective stress prediction
(square box)
Ph. D. Defense Computational Mechanics Laboratory
Temperature distribution
Ph. D. Defense Computational Mechanics Laboratory
Stamped body panel
Ph. D. Defense Computational Mechanics Laboratory
Residual Stress Analysis
• Three levels of residual stresses are generated during cooling
–Microscopic stress: Due to CTE mismatch between matrix and fiber
–Macroscopic stress: Due to stacking sequence of laminates
–Global stress: Due to thermal history along laminate thickness
• Warpage due to the release of residual stresses after demoulding.
• In this study, homogenization method based on incremental elastic
analysis with thermal history is adopted.
• Thermoelastic properties are dependent on temperature and crystallinity
from the thermal history.
Ph. D. Defense Computational Mechanics Laboratory
Thermal history along thickness
100
150
200
250
300
350
400
0 0.1 0.2 0.3 0.4 0.5 0.6
Temperature
(
C)
Location (mm)
10 sec
20 sec
40 sec
60 sec
90 sec
0
0.1
0.2
0.3
0.4
0 0.1 0.2 0.3 0.4 0.5 0.6
Location (mm)
10 sec
20 sec
30 sec
40 sec
50 sec
60 sec
65.1 sec
Volume
fraction
crystallinity
Z
o
Sym.
Laminate
Ph. D. Defense Computational Mechanics Laboratory
Curvature prediction compared with experimental data
[0/90] asymmetric laminate Compared with experimental data
Ph. D. Defense Computational Mechanics Laboratory
Stress prediction compared with experimental data
0
20
40
60
80
100
0 50 100 150 200 250 300
Residual
stress
(MPa)
Temperature ( C)
-40
-30
-20
-10
0.0
10
20
-1 -0.5 0 0.5 1
5 C/s
15 C/s
25 C/s
Global
residual
stress
(MPa)
Location (mm)
Macroscopic stress prediction for cross-ply laminate
compared with experimental data.
Global stress prediction for unidirectional
laminates with various cooling rates.
Macroscopic stress Global stress
Ph. D. Defense Computational Mechanics Laboratory
Warped shapes of square box and cylindrical cup
Deformed
Undeformed
Square box Cylindrical cup
Ph. D. Defense Computational Mechanics Laboratory
Warped body panel with its microscopic residual stress
Unit cell
Fiber part
Laminate
Deformed
Undeformed
Ph. D. Defense Computational Mechanics Laboratory
Conclusions
• The thermoforming process of woven-fabric thermoplastic
composite laminates was analyzed by the 3-D thermo-viscous flow
FEM.
• The constitutive and energy equations of the composites forming
were formulated by the Homogenization Method.
• The global-local analysis of the Homogenization Method enables
us to examine the macro and microscopic deformation mechanics.
• An optimization algorithm is developed to obtain uniform
distribution by adjusting preheating temperature field.

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thermoforming.PDF

  • 1. Ph. D. Defense Computational Mechanics Laboratory Numerical Analysis and Optimal Design of Composite Thermoforming Process by Shih-Wei Hsiao Department of Mechanical Engineering and Applied Mechanics The University of Michigan March 25, 1997
  • 2. Ph. D. Defense Computational Mechanics Laboratory Outline • Introduction • FEM Analysis of Composite Thermoforming Process – Rheological Characterization of Continuous fiber Composites – Global FEM Analysis of Thermoforming Process – Residual Stress Analysis • Optimal Design of Composite Thermoforming Process • Conclusions and Future Work
  • 3. Ph. D. Defense Computational Mechanics Laboratory Schematic of Thermoforming Process Microstructure Die Blankholder Before forming After forming Laminate
  • 4. Ph. D. Defense Computational Mechanics Laboratory Motivations of this research Deep drawing (stamping) of woven-fabric thermoplastic composites is a mass production and precision shaping technology to produce composite components. Objectives of this research • Develop a FEM model to analyze this thermoforming process. • Develop an optimization algorithm based on this FEM model to optimize this forming process.
  • 5. Ph. D. Defense Computational Mechanics Laboratory Why Thermoplastic Composites? From the manufacturing viewpoints • Thermosetting Resins – Hand layed up into structural fiber preform and impregnation after shaping – Need chemical additives to cure after shaping and very long cure cycle time – Labor intense • Thermoplastic Resins – Shaping only depends on heat transfer and force without chemistry – In a preimpregnated continuous tape form – High processing rate – Drawback: higher processing viscosity and forming temperature (320~400 C), and higher equipment cost
  • 6. Ph. D. Defense Computational Mechanics Laboratory Advantages of the composite stamping process u Deep drawing (stamping) of woven-fabric thermoplastic composites is a mass production technology to produce composite components. u This stamping process is also a precision shaping process. u Woven-fabric composites possess a balanced drawability, and can avoid the excessive thinning caused by the transverse intraply shearing.
  • 7. Ph. D. Defense Computational Mechanics Laboratory Related work • Under the kinematic consideration, the draping behavior of woven fabrics over 3-D spherical, conical or arbitrary surfaces was simulated by solving the intersection equations numerically. • This approach provides a preliminary prediction of fiber buckling and final fiber orientation. • This approach can be used as a design tool fot selecting suitable draped configurations for specific surfaces. • Kinematic approach Potter (1979) Robertson et al. (1981) Van West et al. (1990)
  • 8. Ph. D. Defense Computational Mechanics Laboratory • Diaphragm and blowing forming processes. • Newtonian viscous flow formulation with the fiber inextensibility constraint • Inplane prediction of macroscopic stress and strain. • Isothermal forming processes. • Unidirectional composite sheets. • FEM Analysis O’Bradaigh and Pipes (1991) O’Bradaigh et al. (1993)
  • 9. Ph. D. Defense Computational Mechanics Laboratory Goals of this FEM Analysis A 3-D numerical modeling of thermoforming process on woven-fabric thermoplastic composite laminates: • Characterization of the processing rheology of woven-fabric thermoplastic composite materials by the homogenization method. • Coupled viscous flow and heat transfer FEM analyses for forming. – Predictions of global and local stress, temperature and fiber orientation distribution. • Residual stress FEM analysis for cooling. – Predictions of macroscopic and microscopic residual stress and warpage after cooling.
  • 10. Ph. D. Defense Computational Mechanics Laboratory Governing equations for thermoforming process Momentum and continuity equations Thermal equation Viscosity equation Coupled • Impossible to solve these equations at each microcell to obtain obtain the global response. • Homogenization method is used to overcome this difficulty.
  • 11. Ph. D. Defense Computational Mechanics Laboratory Homogenization Method for Composite Materials X Y Γ Ω b t Γt Γg Unit cell Unit cell Review • Under the assumption of periodic microstructures which can be represented by unit cells. • Using the asymptotic expansion of all variables and the average technique to determine the homogenized material properties and constitutive relations of composite materials. • Capable of predicting microscopic fields of deformation mechanics through the localization process.
  • 12. Ph. D. Defense Computational Mechanics Laboratory Digitized woven-fabric unit cell Woven fabric laminate Unit cell
  • 13. Ph. D. Defense Computational Mechanics Laboratory Thermal conductivity prediction for unidirectional composites vs volume fraction 0 1 2 3 4 5 6 0 10 20 30 40 50 60 70 80 Thermal conductivity (W/m-K) Fiber volume fraction (%) Axial conductivity Transverse conductivity Experimental (axial) Experimental (transverse)
  • 14. Ph. D. Defense Computational Mechanics Laboratory Implementation of Global FEA • 3-D sheet forming FE analysis coupled with heat transferFE analysis using ‘Viscous shell with thermal analysis’. vz vy vx ωx ωy ωz x y z Membrane element + Bending element Shell element X Y Z
  • 15. Ph. D. Defense Computational Mechanics Laboratory Viscous shell with thermal analysis • Plane stress asumption-- the incompressibility constraint can be achieved by adjusting the thickness of each shell element. • Large deformation process divided into a series of small time step. • Complicated geometry, friction and contact considerations. v (i) → Ý ε (i) ⇔ µ (i) ⇔ T (i) At i-th time step Coupled thermal analysis Viscous shell • Transient heat transfer FEM to solve temperature at each node. are solved. • At each step, solve nodal temperature and velocity iteratively until convergence.
  • 16. Ph. D. Defense Computational Mechanics Laboratory Fiber Orientation Model Purposes: • Update the fiber intersection angle of each global finite element by the global strain increment at every time step. • Change material properties according to updated fiber orientation. Assumptions: • The fiber orientation of all the microstructures in one global finite element is identical. • The warp yarn and weft yarn of woven-fabric composites can be represented by two unit fiber vectors.
  • 17. Ph. D. Defense Computational Mechanics Laboratory Schematic of lamina coordinate X Y Z X Y X Y Layer A Layer B Fiber Matrix Lamina Warp yarn Weft yarn 1 2 1 2 a b
  • 18. Ph. D. Defense Computational Mechanics Laboratory Updating Scheme . FEM mesh Weft vector Warp vector X Y Z ∆t ∆ε a n an+1 b n+1 bn φn θ n θ n+1 φn+1 x x y y
  • 19. Ph. D. Defense Computational Mechanics Laboratory Global-local solution scheme Global finite element analysis Fiber orientation model Obtain homogenized material properties Construct unit cells Check if forming is done End No Yes Local finite element analysis (PREMAT) Localization (POSTAMT) Begin
  • 20. Ph. D. Defense Computational Mechanics Laboratory Comparison with experiments (cylindrical cup) 55 60 65 70 75 80 85 90 0 5 10 15 20 25 Simulation (Diagonal) Simulation (Median) Experiment (Diagonal) Experiment (Median) Fiber intersection angle (deg) Distance from the origin (mm) Punch zone Free zone Diagonal Median Median
  • 21. Ph. D. Defense Computational Mechanics Laboratory P Laminate Unit Cell Effective stress of laminate and unit cell at P. Effective stress prediction (square box)
  • 22. Ph. D. Defense Computational Mechanics Laboratory Temperature distribution
  • 23. Ph. D. Defense Computational Mechanics Laboratory Stamped body panel
  • 24. Ph. D. Defense Computational Mechanics Laboratory Residual Stress Analysis • Three levels of residual stresses are generated during cooling –Microscopic stress: Due to CTE mismatch between matrix and fiber –Macroscopic stress: Due to stacking sequence of laminates –Global stress: Due to thermal history along laminate thickness • Warpage due to the release of residual stresses after demoulding. • In this study, homogenization method based on incremental elastic analysis with thermal history is adopted. • Thermoelastic properties are dependent on temperature and crystallinity from the thermal history.
  • 25. Ph. D. Defense Computational Mechanics Laboratory Thermal history along thickness 100 150 200 250 300 350 400 0 0.1 0.2 0.3 0.4 0.5 0.6 Temperature ( C) Location (mm) 10 sec 20 sec 40 sec 60 sec 90 sec 0 0.1 0.2 0.3 0.4 0 0.1 0.2 0.3 0.4 0.5 0.6 Location (mm) 10 sec 20 sec 30 sec 40 sec 50 sec 60 sec 65.1 sec Volume fraction crystallinity Z o Sym. Laminate
  • 26. Ph. D. Defense Computational Mechanics Laboratory Curvature prediction compared with experimental data [0/90] asymmetric laminate Compared with experimental data
  • 27. Ph. D. Defense Computational Mechanics Laboratory Stress prediction compared with experimental data 0 20 40 60 80 100 0 50 100 150 200 250 300 Residual stress (MPa) Temperature ( C) -40 -30 -20 -10 0.0 10 20 -1 -0.5 0 0.5 1 5 C/s 15 C/s 25 C/s Global residual stress (MPa) Location (mm) Macroscopic stress prediction for cross-ply laminate compared with experimental data. Global stress prediction for unidirectional laminates with various cooling rates. Macroscopic stress Global stress
  • 28. Ph. D. Defense Computational Mechanics Laboratory Warped shapes of square box and cylindrical cup Deformed Undeformed Square box Cylindrical cup
  • 29. Ph. D. Defense Computational Mechanics Laboratory Warped body panel with its microscopic residual stress Unit cell Fiber part Laminate Deformed Undeformed
  • 30. Ph. D. Defense Computational Mechanics Laboratory Conclusions • The thermoforming process of woven-fabric thermoplastic composite laminates was analyzed by the 3-D thermo-viscous flow FEM. • The constitutive and energy equations of the composites forming were formulated by the Homogenization Method. • The global-local analysis of the Homogenization Method enables us to examine the macro and microscopic deformation mechanics. • An optimization algorithm is developed to obtain uniform distribution by adjusting preheating temperature field.