PSI - Issue 80
Akihide Saimoto et al. / Procedia Structural Integrity 80 (2026) 352–367 A. Saimoto et al. / Structural Integrity Procedia 00 (2023) 000–000
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The above six equations are combined to yield the following relationship. ℑ 3 j = 1 b 2 j µ j = ℑ 3 j = 1 µ j b 2 j = ℑ 3 j = 1 µ 3 j b 2 j = 0 ℑ 3 j = 1 b 2 j = − ϵ 11 d 12 + ϵ 22 d 61 ϵ 11 ( ϵ 11 d 12 + ϵ 22 d 61 − ϵ 22 d 22 ) i ∆ 2 , ℑ 3 j = 1 µ 2 j b 2 j =
d 22 ϵ 11 d 12 + ϵ 22 d 61 − ϵ 22 d 22
i ∆ 2
(A.6)
ℑ 3 j = 1
j b 2 j
b 2 j −
j b 2 j
ℑ 3
ℑ 3 j = 1
ϵ 11 s 12 ϵ 22 s 11 − d 2 12
ϵ 22 s 12 + ϵ 11 s 11 + d 12 ( d 61 − d 22 ) ϵ 22 s 11 − d 2 12
µ 4
µ 2
j = 1
= −
Finally, multiplication of left matrix and the 3rd column of the right matrix in Eq.(A.3) gives following relations. ℑ 3 j = 1 µ j γ j b 3 j = ϵ 11 ℑ 3 j = 1 µ j b 3 j + ϵ 22 ℑ 3 j = 1 µ 3 j b 3 j = 0 ℑ 3 j = 1 γ j b 3 j = ϵ 11 ℑ 3 j = 1 b 3 j + ϵ 22 ℑ 3 j = 1 µ 2 j b 3 j = 0 ℑ 3 j = 1 r j b 3 j = − ϵ 11 d 22 ℑ 3 j = 1 b 3 j − ( ϵ 12 d 12 + ϵ 22 d 61 ) ℑ 3 j = 1 µ 2 j b 3 j = − i ∆ 2 ℑ 3 j = 1 p j b 3 j = ϵ 11 s 12 ℑ 3 j = 1 b 3 j + { ϵ 22 s 12 + ϵ 11 s 11 + d 12 ( d 61 − d 22 ) }ℑ 3 j = 1 µ 2 j b 3 j + ( ϵ 22 s 11 − d 2 12 ) ℑ 3 j = 1 µ 4 j b 3 j = 0 ℑ 3 j = 1 q j b 3 j = ϵ 11 s 22 ℑ 3 j = 1 b 3 j /µ j + { ϵ 11 s 12 + ϵ 22 s 22 + d 22 ( d 61 − d 22 ) }ℑ 3 j = 1 µ j b 3 j + ( ϵ 22 s 12 − d 12 d 22 ) ℑ 3 j = 1 µ 3 j b 3 j = 0 ℑ 3 j = 1 λ j b 3 j = ( d 61 − d 22 ) ℑ 3 j = 1 µ j b 3 j − d 12 ℑ 3 j = 1 µ 3 j b 3 j = 0
The above six equations are combined to yield the following relationship. ℑ 3 j = 1 b 3 j µ j = ℑ 3 j = 1 µ j b 3 j = ℑ 3 j = 1 µ 3 j b 3 j = 0 ℑ 3 j = 1 b 3 j = ϵ 22 /ϵ 11 ϵ 11 d 12 + ϵ 22 d 61 − ϵ 22 d 22 i ∆ 2 , ℑ 3 j = 1 µ 2 j b 3 j = − 1
i ∆ 2
(A.7)
ϵ 11 d 12 + ϵ 22 d 61 − ϵ 22 d 22
j b 3 j
ℑ 3 j = 1
b 3 j −
j b 3 j
ℑ 3
ℑ 3 j = 1
ϵ 11 s 12 ϵ 22 s 11 − d 2 12
ϵ 22 s 12 + ϵ 11 s 11 + d 12 ( d 61 − d 22 ) ϵ 22 s 11 − d 2 12
µ 4
µ 2
j = 1
= −
Accordingly, the following 6 sums are real number not complex. 3 j = 1 b 2 j µ j , 3 j = 1 µ j b 2 j , 3 j = 1 µ 3 j b 2 j , 3 j = 1 b 3 j µ j , 3 j = 1 µ j b 3 j , 3 j = 1 µ 3 j b 3 j Appendix B. Constants A i j in Eq.(38) and B i j inEq.(47)
(A.8)
Constants A i j defined in Eq.(38) are as follows.
γ j
b 1 j
b 1 j
2 j ϵ 22 )
3 j = 1 3 j = 1 3 j = 1
3 j = 1
ϵ 22 s 12 − d 12 d 22 ϵ 22 s 11 − d 2
ϵ 22 s 12 − d 12 d 22 ϵ 22 s 11 − d 2
µ j b 2 j −
12
µ j b 2 j −
12
= 2
(B.1)
( ϵ 11 + µ
A 11 = 2
3 j = 1
2 j ϵ 22 )( µ j b 1 j + b 2 j + d 61 b 3 j )
γ j ( µ j b 1 j + b 2 j + d 61 b 3 j ) = 2
A 12 = 2
( ϵ 11 + µ
(B.2)
γ j
b 1 j
b 1 j
2 j ϵ 22 )
3 j = 1
d 12 ϵ 22 d 11 − d 2
d 12 ϵ 22 d 11 − d 2
µ j b 3 j −
12
µ j b 3 j −
12
A 13 = 2
= 2
(B.3)
( ϵ 11 + µ
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