inherent carbon fibre stiffening as seen in textile reinforced composites
DESCRIPTION
Inherent carbon fibre stiffening as seen in textile reinforced composites Stepan V. Lomov 1 , Alexander E. Bogdanovich 2 , Ichiro Taketa 1,3 , Jian Xu 1 , Ignaas Verpoest 1 1 Depertment MTM, Katholieke Universiteit Leuven, Belgium 2 3Tex Inc, Cary, NC, USA 3 Toray Industries, Japan. - PowerPoint PPT PresentationTRANSCRIPT
S.V. Lomov CompTest-2011 Lausanne 1
Inherent carbon fibre stiffening
as seen
in textile reinforced composites
Stepan V. Lomov1, Alexander E. Bogdanovich2,
Ichiro Taketa1,3, Jian Xu1, Ignaas Verpoest1
1Depertment MTM, Katholieke Universiteit Leuven, Belgium
23Tex Inc, Cary, NC, USA
3Toray Industries, Japan
S.V. Lomov CompTest-2011 Lausanne 2
Contents
1. Introduction: The carbon fibre stiffening phenomenon and previously observed stiffening effects in carbon fibre textile composites
2. Strain measurements during tensile test
3. Stiffening in 3D woven non-crimp carbon/epoxy composites
4. Conclusions
S.V. Lomov CompTest-2011 Lausanne 3
1. Introduction: • The carbon fibre stiffening phenomenon
• Previously observed stiffening effects in carbon fibre textile composites
2. Strain measurements during tensile test
3. Stiffening in 3D woven non-crimp carbon/epoxy composites
4. Conclusions
S.V. Lomov CompTest-2011 Lausanne 4
Inherent stiffening of carbon fibres
First observed:
Curtis, G. J., J. M. Milne and W. N. Reynolds (1968). "Non-Hookean Behaviour of Strong Carbon Fibres." Nature 220(5171): 1024-1025
strain 1%
20% increase E
figure from:
Shioya, M., E. Hayakawa and A. Takaku (1996). "Non-hookean stress-strain response and changes in crystallite orientation of carbon fibres." Journal of Materials Science 31(17): 4521-4532
S.V. Lomov CompTest-2011 Lausanne 5
Literature on carbon fibre stiffening
1. Curtis, G.J., J.M. Milne and W.N. Reynolds, Non-Hookean behaviour of strong carbon fibres, Nature, 1968, 220(5171): 1024-1025.
2. van Dreumel, W.H.M. and J.L.M. Kamp, Non Hookean behaviour in fibre direction of carbon-fibre composites and the influence of fibre waviness on the tensile properties, Journal of Composite Materials, 1977, 11(Oct): 461-469.
3. Morley, H., A simple strand test for routine fibre strength and modulus evaluation, Composites, 1982, 13(1): 21-23.
4. Beetz, C.P., Jr., Strain-induced stiffening of carbon fibres, Fibre Science and Technology, 1982, 16: 219-229.
5. Beetz, C.P., Jr. and G.W. Budd, Strain modulation measurements of stiffening effects in carbon fibers, Review of Scientific Instruments, 1983, 54(9): 1222-1226.
6. Vangerko, H. and A.J. Barker, The stiffness of unidirectionally reinforced CFRP as a function of strain rate, strain magnitude and temperature, Composites, 1985, 16(1): 19-22.
7. Ishikawa, T., M. Matsushima and Y. Hayashi, Hardening non-linear behaviour in longitudinal tension of unidirectional carbon composites, Journal of Materials Science, 1985, 20: 4075-4083.
8. Hughes, J.D.H., Strength and modulus of current carbon fibres, Carbon, 1986, 24(5): 551-556.
9. Stecenko, T.B. and M.M. Stevanovic, Variation of elastic moduli with strain in carbon/epoxy laminates, Journal of Composite Materials, 1990, 24: 1152-1158.
10. Northolt, M.G., L.H. Veldhuizen and H. Jansen, Tensile deformation of carbon fibers and the relationship with the modulus for shear between the basal planes, Carbon, 1991, 29(8): 1267-1279.
11. Shioya, M and A. Takaku, Rotation and extension of crystallites in carbon fibers by tensile stress, Carbon, 1994, 32(4): 615-619.
12. Shioya, M., E. Hayakawa and A. Takaku, Non-hookean stress-strain response and changes in crystallite orientation of carbon fibres, Journal of Materials Science, 1996, 31(17): 4521-4532.
13. Toyama, N. and J. Takatsubo, An investigation of non-linear elastic behavior of CFRP laminates and strain measurement using Lamb waves, Composites Science and Technology, 2004, 64: 2509–2516
1 1
5
4
1
1960s 1970s 1980s 1990s 2000s
S.V. Lomov CompTest-2011 Lausanne 6
Cross-ply carbon laminates: stiffening vs damage softening
Toyama, N. and J. Takatsubo (2004). "An investigation of non-linear elastic behavior of CFRP laminates and strain measurement using Lamb waves." Composites Science and Technology 64: 2509–2516.
S.V. Lomov CompTest-2011 Lausanne 7
Textile composites
Ishikawa, T., M. Matsushima and Y. Hayashi, Hardening non-linear behaviour in longitudinal tension of unidirectional carbon composites, Journal of Materials Science, 1985, 20: 4075-4083
Stiffening effect is noted for 8-harness satin – more pronounced effect for straight fibres
Truong, T. C. . The mechanical performance and damage of multi-axial milti-ply carbon fabric reinforced composites. PhD thesis, Department MTM. Leuven, Katholieke Universiteit Leuven, 2005
S.V. Lomov CompTest-2011 Lausanne 8
Carbon/PP woven composites
+20%
spectacular increase of stiffness …
… may be caused by decrimping as well …
S.V. Lomov CompTest-2011 Lausanne 9
Carbon/epoxy twill woven composite
stress, MPa
E, GPa
strain, %
0.4 0.6
60
700.2
0.2 0.4 0.6
S.V. Lomov CompTest-2011 Lausanne 10
1. Introduction: The carbon fibre stiffening phenomenon and previously observed stiffening effects in carbon fibre textile composites
2. Strain measurements during tensile test
3. Stiffening in 3D woven non-crimp carbon/epoxy composites
4. Conclusions
S.V. Lomov CompTest-2011 Lausanne 11
Optical extensometry
y = -4.9477x2 + 0.6852x
R2 = 0.9996
y = 0.1848x + 0.0059
R2 = 0.9994
0.000
0.002
0.004
0.006
0.008
0.010
0.012
0.014
0.000 0.010 0.020 0.030 0.040
eps grips
eps_
X
0
200
400
600
800
1000
0 0.01 0.02 0.03 0.04 0.05 0.06
strain
sig,
MP
a
grips
true: LIMESS
Instron
LIMESS
1. Precise position of zero of LIMESS curves
2. Two regions on the curves
3. Choice of the fitting
S.V. Lomov CompTest-2011 Lausanne 12
1. Introduction: The carbon fibre stiffening phenomenon and previously observed stiffening effects in carbon fibre textile composites
2. Strain measurements during tensile test
3. Stiffening in 3D woven non-crimp carbon/epoxy composites
4. Conclusions
S.V. Lomov CompTest-2011 Lausanne 13
The 3D woven non-crimp carbon/epoxy composite
Warp/fill yarnsToho Tenax 12K, 800
texAreal density, g/m2 2499
Z yarns Toho Tenax 1K, 66 tex Ends/picks, per inch in layer 12 / 10
Fiber diameter, µm 7* Fibre Young modulus, GPa 238*
Fibre strength,MPa 3950* Fibre ultimate elongation 1.7%*
Composite thickness, mm
2.760.028Fiber volume fraction in the
composite51.1%0.5%
Waviness, warp 0.03%Fibre volume fraction, fibres in
warp:fill:vertical directions24.2%:26.2%:0.7%
Waviness, fill, outer/inner layer
0.08% / 0.02%Fibre volume fraction inside
warp and fill yarns61…73%
* datasheet of Toho Tenax
S.V. Lomov CompTest-2011 Lausanne 14
Expected values of Young’s modulus
Fibre Young modulus, GPa 238*
Fiber volume fraction in the composite 51.1%0.5%
Fibre volume fraction, fibres in warp:fill:vertical directions
24.2%:26.2%:0.7%
Waviness, warp 0.03%
Waviness, fill, outer/inner layer 0.08% / 0.02%
GPaGPaE
GPaGPaE
fill
warp
65 4.62262.0*238
60 7.57242.0*238
* datasheet of Toho Tenax
S.V. Lomov CompTest-2011 Lausanne 15
Change of Young’s modulus
0
100
200
300
400
500
600
700
800
900
1000
0 0.005 0.01 0.015
strain
stre
ss,
MP
a
0
10
20
30
40
50
60
70
80
90
100
E,
GP
a
warp
fillexpected
GPaGPaE
GPaGPaE
fill
warp
65 4.62262.0*238
60 7.57242.0*238
expected:
S.V. Lomov CompTest-2011 Lausanne 16
0
100
200
300
400
500
600
700
800
900
1000
0 0.002 0.004 0.006 0.008 0.01 0.012 0.014 0.016
1.E+00
1.E+01
1.E+02
1.E+03
1.E+04
1.E+05
1.E+06
1.E+07
1.E+08
Change of Young modulus and damage
0
100
200
300
400
500
600
700
800
900
1000
0 0.002 0.004 0.006 0.008 0.01 0.012 0.014 0.016
1.E+00
1.E+01
1.E+02
1.E+03
1.E+04
1.E+05
1.E+06
1.E+07
1.E+08
strain
AE
AE
stress, MPa
E*10, GPa
20% increase of E
S.V. Lomov CompTest-2011 Lausanne 17
Impregnated carbon yarns: 6K and 12K
stress – strain:
mixed data for 3K and 12 K
6K
12K
fabric, warp and fill
Young’s modulus, normalised
VF = 70%
S.V. Lomov CompTest-2011 Lausanne 18
Stiffening and fatigue: S-N curve
0
100
200
300
400
500
600
700
800
900
1000
1.E+00 1.E+01 1.E+02 1.E+03 1.E+04 1.E+05 1.E+06 1.E+07
fatigue cycles
max
imum
fat
igue
str
ess,
MP
a
WARP staticWARPWARP no breakFILL staticFILLFILL no breakLog. (FILL)Log. (WARP)
I
II
III
warp
fill
tim e
stre
ss
m ax
m in
S.V. Lomov CompTest-2011 Lausanne 19
Post-fatigue tensile test: Fatigue @ 450 MPa, 1,000,000 cycles
0
100
200
300
400
500
600
700
800
0 0.002 0.004 0.006 0.008 0.01 0.012 0.014 0.016 0.018 0.02
0
10
20
30
40
50
60
70
80
0
100
200
300
400
500
600
700
800
0 0.002 0.004 0.006 0.008 0.01 0.012 0.014 0.016
0
10
20
30
40
50
60
70
80
warp fill
static @450 MPastatic @450 MPa
50
55
60
65
70
0 200 400 600 800 1000
stress, MPa
E, G
Pa
quasi-static evolution of Young’s modulus
stress E
strain strain
tim e
stre
ss
m ax
m in
initial static
S.V. Lomov CompTest-2011 Lausanne 20
1. Introduction: The carbon fibre stiffening phenomenon and previously observed stiffening effects in carbon fibre textile composites
2. Strain measurements during tensile test
3. Stiffening in 3D woven non-crimp carbon/epoxy composites
4. Conclusions
S.V. Lomov CompTest-2011 Lausanne 21
Conclusions: Evolution of Young’s modulus of carbon/epoxy textile composites
Quasi-static tension:
• inherent stiffening of carbon fibres
• softening of the composite due to damage
Fatigue and post-fatigue:
• change of Young modulus in the first cycles: possible high modulus
• softening due to damageE, warp
55
60
65
0 200 400 600 800 1000
stress, MPa
E, G
Pa
tim e
stre
ssm ax
m in