346
S. Zacek et al.
∂ n t gp
∂δ ci
=
∂ n t
∂δ ci
1
n δ
[β
2 n
δ + (1 − β
2 )(
n
δ · n)n].
(20)
From Equation (3), the partial derivatives of the scalar effective traction are
∂t
∂η i
=
⎧
⎨
⎩
−2σ c
1 −
δ e
δ c1
δ e
δ 2
c1
0 ≤ δ e < δ c1
0
e l s e
for η i = δ c1
6σ c
δ e −δ c2
δ c3 −δ c2
− 1
δ e −δ c2
δ c3 −δ c2
δ e −δ c3
(δ c3 −δ c2 ) 2
δ c2 ≤ δ e < δ c3
0
e l s e
for η i = δ c2
−6σ c
δ e −δ c2
δ c3 −δ c2
− 1
δ e −δ c2
δ c3 −δ c2
δ e −δ c2
(δ c3 −δ c2 ) 2
δ c2 ≤ δ e < δ c3
0
e l s e .
for η i = δ c3
(21)
Acknowledgements This work has been supported through a grant No. FA9550-12-1-0445 to the
Center of Excellence on Integrated Materials Modeling (CEIMM) at Johns Hopkins University
(partners JHU, UIUC, UCSB), awarded by the AFOSR/RSL (Computational Mathematics Program, Manager Dr. A. Sayir) and AFRL/RX (Monitors Dr. C. Woodward and C. Przybyla).
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