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Analysis of 2D Triaxial Braided Textile Composites & FEXL · 2012-03-08 · Slide 3 Introduction to...
Transcript of Analysis of 2D Triaxial Braided Textile Composites & FEXL · 2012-03-08 · Slide 3 Introduction to...
Analysis of 2D Triaxial Braided
Textile Composites & FEXL
Sung Kyu Ha, Kyu Kook Jin, Xu Lei
Structures and Composites Laboratory
Hanyang University
Slide 2Slide 2
Macro, Meso and Micro Mechanics
UNIT CELL
OF UNIDIRECTIONALTAPECOMPOSITE STRUCTURE
Thermal
Mechanical
Loads
(k) (k)M and ASTRESS AMPLIFICATION FACTORS
OF UNIDIRECTIONAL COMPOSITE
(i) (i)M and ASTRESS AMPLIFICATION FACTORS
OF MESO MODELS
(i,k) (k) (ki )( )σ σ=M + A ΔT
Cand EFFECTIVE MATERIAL PROPERTIES
OF UNIDIRECTIONAL COMPOSITE
Cand αEFFECTIVE MATERIAL PROPERTIES
OF MESO MODELS
MICRO-STRESSES
OF UNIDIRECTIONAL COMPOSITE
(i)i) (i)( σ=M +σ A ΔT
MESO-STRESSES
OF MESO MODELS
MACRO-STRESSES
σ
Micro-Mechanics Meso-Mechanics (fiber architecture) Macro-Mechanics
(k)(i)
FEM
Braided Composite
MESO MODELS MICRO MODELS
Unit Cell
Slide 3Slide 3
Introduction to Braided Textile Composites
Fig1. 2D Braided composite
Fig2. GEnx jet engine with
a braided composite fan
Advantages
1. Better out-of-plane stiffness, strength, and toughness
2. Lower fabrication costs, and easier handling in production
quality than tape laminates
Braid Patterns
Diamond Braid (1/1) Regular Braid (2/2) Hercules Braid (3/3)
Diamond Braid — 1 up, 1 down (1/1)
Regular Braid — 2 up, 2 down (2/2)
Hercules Braid —3 up, 3 down (3/3)
Slide 4Slide 4
Key parameters of (2/2) Triaxial Braided
Composite
θ — braiding angle
Wa — width of axial yarn
Wb — width of bias yarn
ta — thickness of axial yarn
tb — thickness of bias yarn
Introduction to Braided Textile Composites
Components of (2/2) Triaxial Braided Composite
1. Axial yarn
2. -θ Bias yarn
3. +θ Bias yarn
Green — -θ bias yarns Blue — axial yarns Red — θ bias yarns
θ
Wb
Wa θ
tb
ta
tb
Slide 5Slide 5
CAD Model
Unit Cell for Braided Composite
CAD Model for 2/2 Triaxial Braided Composite
Bias yarns
Axial yarns
Bias yarn cross section Axial yarn cross section
ab — width of bias yarn
bb — thickness of bias yarn
a — width of axial yarn
b— thickness of axial yarn
Undulation of bias yarn
z’= Asin(πx’/L)
Governing equation
Slide 6Slide 6
CAD Model of Repeating Unit Cell (RUC)
Unit Cell
Resin
Yarn
Red: +θ Bias Yarn
White: -θ Bias Yarn
Green: Axial Yarn
Unit Cell of Braided Composite
FEM Model of RUC
Mesh of Unit Cell Mesh of Fiber Mesh of Resin
Slide 7Slide 7
Analysis of Multi-Cell Model of Braided Composite
Unit Cell
Resin
Fiber
Geometry Information
Braiding angle: θ = 30°;
Width of axial yarn: Wa = 3.012mm
Width of bias yarn: Wb = 3.01mm
Thickness of axial yarn: ta = 0.503mm
Thickness of bias yarn: tb = 0.498mm
Multi Cell Model
Slide 8Slide 8
Assign material properties
Material Properties
E1(GPa) E2(GPa) E3(GPa) ν12 ν13 ν23 G12(GPa) G13(GPa) G23(GPa)
231 18 18 0.2 0.2 0.35 85 85 7Fiber
MatrixE(GPa) ν
4 0.38
Local Coordinate System (CSYS)
Cell_1 – Local CSYS_1
Cell_2 – Local CSYS_2
Cell_n – Local CSYS_n
CSYS_n
CSYS_1
CSYS_2
All Repeating Local CSYSs
Slide 9Slide 9
Load & Boundary Conditions
X: U(x) = 0
Y: U(y) = 0z
xy
x
x’
y
y’
P
X’: DOF_1(x’) = DOF_1(P)
Y’: DOF_2(y’) = DOF_2(P)
Boundary conditions
Loads
z
xy
Analysis 1
σ = 1
z
xy
Analysis 2
ε = 1
Slide 10Slide 10
Layers align configuration for NCF
Analysis results
Analysis 1 Analysis 2
Field Output: Stress, Mises
The two analysis under two different loads have the same stress distribution
ε = 1σ = 1
Slide 11Slide 11
Layers align configuration for NCF
Analysis results
Analysis 1 Analysis 2
Field Output: Strain, Max, Principal
The two analysis under two different loads have the same strain distribution
ε = 1σ = 1
Slide 12Slide 12
Summary of Braided Textile Composite
The unit cell of 2/2 braided composite has been defined;
The cad model and FEM model of 2/2 braided textile composite have
been developed;
The analysis of multi cell model has been finished.
A finite element program for Axisymmetric
Composite Structures : FEXL-AxiCom
13
Slide 14Slide 14 14
What are Axisymmetric Structures?
Water tanks Pipes
Pressure vess
els
……
Cap
Rotors
Slide 15Slide 15 15
FEXL-AxiCom
MS Excel based User-friendly finite element analysis program
for Axisymmetric Composite Structures
Axisymmetric Structure with
any cross section
Two loads (Internal pressure and
angular velocity) at any location
The FEXL-AxiCom is an accurate, yet easy-to-
use tool , greatly simplifying data input procedures
for cross-sections and layup sequences.
Slide 16Slide 16
Main Analysis
Modules
Step 1 : Geometry
Selection
Step 2 Material
Properties
Step 3 : Loads
Step 4 : Solve
•Decide the dimensions
for the selected model
• Number of nodes
• Internal Pressure
• Angular velocity
Input Output
• Displacement
• Global Strains
• Global Stresses
Program Flow : FEXL-AxiCom
3D Graphical Post Processor:
JAVA PostProcessor
Step 4 : Mesh Generation
Slide 17Slide 17
Introduction of FEXL-AxiCom
FEXL-AxiCom “Main” sheet
Pressure
Vessel
Cylinder Sphere
Material DB
Application of FEXL-AxiCom
18
Slide 19Slide 1919
Composite
Cylinders
Composite
Pressure Vessels
Samples
Composite
Spherical Cap
Slide 20Slide 20
Analysis of Composite Cylinder under Internal Pressure
Slide 21Slide 21
1. Material Properties
Ex [GPa] 132
Ey [GPa] 8.9
v_x 0.31
Es [GPa] 5.6
2. Load & Boundary conditions
P=100 Pa
Uy = 0
X
ZY Local CSYS
Y — Fiber direction
Z — Thickness direction
[± 90]m
Composite
Cylinders
Analysis of Composite Cylinder under Internal Pressure
ID=0.4 m
OD=0.7m
Height=0.6m
Slide 22Slide 22
FEXL
ABAQUS
Path for plot
Analysis of Composite Cylinder under internal Pressure
Radial disp. vs radius
0
2E-10
4E-10
6E-10
8E-10
1E-09
1.2E-09
1.4E-09
0.4 0.45 0.5 0.55 0.6 0.65 0.7 0.75
stre
ss
r
FEXL ABAQUS
P=100 Pa
[± 90]mID=0.4 m
OD=0.7m
Height=0.6m
Slide 23Slide 23
FEXL
ABAQUS
Path for plot
Analysis of Composite Cylinder under internal Pressure
σθθvs r
0
50
100
150
200
250
300
350
400
0.4 0.45 0.5 0.55 0.6 0.65 0.7 0.75
stre
ss
r
ABAQUS FEXL
P=100 Pa
[± 90]mID=0.4 m
OD=0.7m
Height=0.6m
Slide 24Slide 24
1. Material Properties
Ex [GPa] 132
Ey [GPa] 8.9
nu_x 0.31
Es [GPa] 5.6
2. Loads & Boundary conditions
Angular Velocity:
ω =100 rpm
ω
ID=0.4 m
OD=0.7m
Height=0.6m
Analysis of Composite Cylinder in Rotation (Flywheel Rotor)
Uy = 0X
ZY Local CSYS
Y — Fiber direction
Z — Thickness direction
[± 90]m
Composite
Cylinders
Slide 25Slide 25
FEXL
ABAQUS
Path for plot
1.70E-07
1.90E-07
2.10E-07
2.30E-07
2.50E-07
0.4 0.5 0.6 0.7
Dis
pla
cem
en
t
r
FEXL ABAQUS
ω =100 rpm
[± 90]m ID=0.4 m
OD=0.7m
Height=0.6m
Radial disp. vs radius
Analysis of Composite Cylinder in Rotation (Flywheel Rotor)
Slide 26Slide 26
σθθvs r
4.60E+04
4.80E+04
5.00E+04
5.20E+04
5.40E+04
5.60E+04
5.80E+04
6.00E+04
0.4 0.45 0.5 0.55 0.6 0.65 0.7
Str
ess
r
FEXL ABAQUSFEXL
ABAQUS
Path for plot
Analysis of Composite Cylinder in Rotation (Flywheel Rotor)
ω =100 rpm
[± 90]m ID=0.4 m
OD=0.7m
Height=0.6m
Slide 27Slide 27
Section
Cross section
Composite Spherical Cap
[+q/-q]m
FEA
FEM Model
Analysis of Composite Spherical Cap
Slide 28Slide 28
1. Material Properties
Ex [GPa] 132
Ey [GPa] 8.9
nu_x 0.31
Es [GPa] 5.6
2. Loads & Boundary conditions
Analysis of Composite Spherical Cap under internal Pressure
[± 90]m
ID=2 m
OD=2.15m
Angle_s=0
Angle_f=90
P = 100 Pa
Ux = 0
Uy = 0
Global CSYS X
ZY
Local CSYS-m
X
ZY
X
ZY
Local CSYS-1
Local CSYS-n
Y — Fiber direction
Z — Thickness direction
Slide 29Slide 29
Analysis of Composite Spherical Cap under internal Pressure
0.00E+00
5.00E-08
1.00E-07
1.50E-07
2.00E-07
2.50E-07
3.00E-07
3.50E-07
0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2
Dis
pla
ce
me
nt
r
FEXL ABAQUS
[± 90]m ID=2 m
OD=2.15m
Angle_s=0
Angle_f=90
P=100 Pa
Radial disp. vs radius
FEXL
ABAQU
S
Path for plot
Slide 30Slide 30
Analysis of Composite Spherical Cap under internal Pressure
-1500
-1000
-500
0
500
1000
0 0.5 1 1.5 2S
tre
ssr
ABAQUS FEXL
σθθvs r
[± 90]m ID=2 m
OD=2.15m
Angle_s=0
Angle_f=90
P=100 Pa
FEXL
ABAQUSPath for p
lot
Slide 31Slide 31
1. Material Properties
Ex [GPa] 132
Ey [GPa] 8.9
nu_x 0.31
Es [GPa] 5.6
2. Loads & Boundary conditions
Analysis of Composite Spherical Cap in Rotation
ID=2 m
OD=2.15m
Angle_s=0
Angle_f=90Ux = 0
Uy = 0
Global CSYS
ω
Angular Velocity:
ω=100 rpm
X
ZY
Local CSYS-m
X
ZY
X
ZY
Local CSYS-1
Local CSYS-n
Y — Fiber direction
Z — Thickness direction
Slide 32Slide 32
8.00E-06
9.00E-06
1.00E-05
1.10E-05
1.20E-05
1.30E-05
1.40E-05
0 0.2 0.4 0.6 0.8 1 1.2 1.4 1.6 1.8 2
Dis
pla
ce
me
nt
r
FEXL ABAQUS
32
Analysis of Composite Sphere in Rotation
ω =100 rpm
[± 90]m ID=0.4 m
OD=0.7m
Height=0.6m
Radial disp. vs radius
FEXL
ABAQUS
Path for p
lot
Slide 33Slide 33
Analysis of Composite Spherical Cap in Rotation
0.00E+00
1.00E+05
2.00E+05
3.00E+05
4.00E+05
5.00E+05
6.00E+05
7.00E+05
8.00E+05
0 0.5 1 1.5 2
Str
ess
r
FEXL ABAQUS
σθθvs r
ω =100 rpm
[± 90]m ID=0.4 m
OD=0.7m
Height=0.6m
FEXL
ABAQUS
Path for plot
Slide 34Slide 34
Analysis of Cylindrical Pressure Vessel for Various Angles
-2
0
2
4
6
8
10
12
0 10 20 30 40 50 60 70 80 90
sig_y (transverse direction)
analytic (thin)FEXL
0
2E-10
4E-10
6E-10
8E-10
1E-09
1.2E-09
1.4E-09
0 10 20 30 40 50 60 70 80 90
Disp_1(radial displacement)
FEXL
analytic (thin)
x
z
y
x
”
z”
y”
x’
y’
x”
y”
q
q
Fiber angle, q
Fiber angle, q
[q/-q]m
Slide 35Slide 35
Dimension input for pressure vessel
Analysis of Pressure Vessel
Radial disp. vs radius
Transverse stress vs radius
P = 100Pa