Computational Mechanics of Composite Materials part 3 ppsx
Computational Mechanics of Composite Materials part 3 ppsx
...
0.0 232
18 0.985
0.0 236
0.9 93
0.0 234
0.994
0.0 231
1.0 03
0.0 230
27 0.895
0.0 239
0.897
0.0 235
0.908
0.0 234
0.910
0.0 231
36 0.7 83
0.0241
0.784
0.0 238
0.784
0.0 235
0.790
0.0 232 ... 53
-1.45E+02
+1 .37 E+02
+7.02E+02
+1.26E+ 03
+1.83E+ 03
+2 .39 E+ 03
+2.96E+ 03
+3. 24E+ 03
+3. 52E+ 03
Figure 2.20. The shear stresses for test no. 2
-8.25E+01
+1 .3...
Computational Mechanics of Composite Materials Part 1 ppsx
... then
M.M. Kamin
´
ski
Computational
Mechanics of
Composite Materials
Sensitivity, Randomness
and Multiscale Behaviour
viii Computational Mechanics of Composite Materials
and mechanics, numerical ... M.M.
Computational mechanics of composite materials :
Sensitivity, randomness and multiscale behaviour. —
(Engineering materials and processes)
1. Composite ma...
Computational Mechanics of Composite Materials part 2 ppsx
... analogous nth order partial
derivatives of external excitation, accelerations, velocities as well as displacements
of the system.
32 Computational Mechanics of Composite Materials
composite Y. In ... []
⎟
⎟
⎠
⎞
⎜
⎜
⎝
⎛
⋅−⋅=
⎥
⎥
⎦
⎤
⎢
⎢
⎣
⎡
⋅
−
=
ΩΩ
Ω
b
b
c
SE
S
eEe
S
SS
EeE
cc
c
22
2
1
1][
222
(2 .30 )
24 Computational Mechanics of Composite Materials
various mat...
Computational Mechanics of Composite Materials part 7 ppsx
... mm
Cross section of
the coil
Void
Figure 3. 1. Cross section of a superconducting coil
Figure 3. 2. 3D view of the superconducting coil part
Table 3. 1. Material characteristics of composite constituents ...
()
)()()2()1(
][
N
kl
N
klkl
kl
uBuBB
ζ
ζ
ζ
ζζ
ε
∆=∆+=∆ x
(3. 42)
()
)()( NN
klkl
uuB
ξζ
ζξ
ε
∆∆=∆ x
(3. 43)
172 Computational Mechanics of Composite Materi...
Computational Mechanics of Composite Materials part 14 ppsx
...
3 8 10.1/2.19 10.9/2.19 11.0/2 .31
4 16 14.1/2.62 14.9/2.62 17 .3/ 2.69
5 32 20.7 /3. 25 25.7 /3. 31 31 .8 /3. 44
6 64 53. 0/4.56 53. 7/4.56 70.5/4.94
7 128 131 .0/7.06 130 .7/7.06 185.4/7.75
8 256 39 5 .3/ 12.2 ... he
periodic composites. Comput. Mat. Sci. 22 (3- 4):221- 239 .
95.
of curved layered composites. Comput. & Struct. 81(18-19):1865-18 73.
37 6 Computational M...
Computational Mechanics of Composite Materials part 5 ppt
... -1.15e-7 -2.51e-7
γ(C)
3. 09 3. 06 3. 20 3. 02 3. 07 3. 17
Voigt-Reuss bounds
Deterministic values 171.49 130 .33 80.95 52. 63 45.27 38 .85
E[C] 171.88 129.97 81. 43 52.46 45. 23 38.76
α(C)
6.78e-2 4.72e-2 ...
)(
1111
eff
C
)(
1212
eff
C
)(
1122
eff
C
Deterministic values 102 .33 36 .47 33 .69
E[C] 102.50 36 .69 33 .49
α(C)
5.83e-2 5.90e-2 6 .38 e-2
β(C)
-1.86e-1 -1.92e...
Computational Mechanics of Composite Materials part 6 pdf
... coefficients of asymmetry of
)(eff
JKKJ
C bounds
2.900
3. 000
3. 100
3. 200
3. 300
3. 400
3. 500
3. 600
3. 700
3. 800
100 30 0 500 700 900 1500 2500 35 00 4500 6000 8000 10000
sup - VR
sup
inf
inf - VR
140 Computational ... 2. 132 and 2. 135 , for
)(eff
JKJK
C bounds in Figures
2. 130 , 2. 133 and 2. 136 and for
)(eff
JKKJ
C in Figures 2. 131 , 2. 134 and 2. 137 . On the...
Computational Mechanics of Composite Materials part 8 pps
... e
1
Figure 4. 23. Sensitivity of
)eff(
C
33 33
wrt
1
ν
Figure 4.24. Sensitivity of
)eff(
C
33 33
wrt e
2
Figure 4.25. Sensitivity of
)eff(
C
33 33
wrt
2
ν
Sensitivity Analysis for Some Composites ... parameter α
204 Computational Mechanics of Composite Materials
Figure 4 .32 . Sensitivity of
)eff(
C
1122
wrt e
2
Figure 4 .33 . Sensitivity of
)eff(
C
1122
wrt
2...
Computational Mechanics of Composite Materials part 9 ppt
... increase as follows: 3. 44E -3 m (6°), 7 .33 E-3m (10°), 8.93E -3 m (14°)
for Figure 5.21 and 3. 89E -3 m (6°), 5.04E-3m (10°), 8.93E -3 (14°) for Figure 6.22.
It is reasonable because of the greater non-uniform ... 5.25).
0.0E+00
2.5E+ 03
5.0E+ 03
7.5E+ 03
1.0E+04
1.3E+04
1.5E+04
0.00 0.20 0 .39 0.57 0.69 0.70
14°
10°
6°
0.0E+00
3. 0E+ 03
6.0E+ 03
9.0E+ 03
1.2E+04
1.5E+04
1...
Computational Mechanics of Composite Materials part 10 pps
...
adhesive bonding
X
X
〈τ〉
d
260 Computational Mechanics of Composite Materials
()()
[]
m
e
dN
da
m
σ
ln0. 235 910.12 132 0101
4
+−×
−
=
⎟
⎠
⎞
⎜
⎝
⎛
(5.82)
The usage of (5.82) makes it possible to ... equation:
ln (da/dN)
m
ln(σ
m
)
132 .12ln3591.2ln −=
⎟
⎠
⎞
⎜
⎝
⎛
m
m
dN
da
σ
258 Computational Mechanics of Composite Materials
Supposing that the shear mode of fa...