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function X2(m,t) integer m double precision X2,t,tt1(),tt2() common /crack/...

function X2(m,t) integer m double precision X2,t,tt1(),tt2() common /crack/tt1,tt2 X2=dO*(tt2(m+1)+tt2(m)) & +dO*t*(tt2(m+1)—tt2(m)) return end.

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() where a stands for the crack face displacement w(x, y, 0), R(M, N) is th...

() where a stands for the crack face displacement w(x, y, 0), R(M, N) is the distance between the points M(p, q}, z) and N(r, p, 0), and the “TT2+(n-T).

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1 — Geometry and coordinate system for analysis of steady-state crack ab^e2...

1 — Geometry and coordinate system for analysis of steady-state crack ab^e2 - tt2/4)(1 + H/R)/2Rr (1) (2) (3) This displacement field was constructed by.

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For the low crack growth rate, an effect of microstructure has been found o...

For the low crack growth rate, an effect of microstructure has been found on the 60CV2 55SC7 35 55SC7-TT2

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k=0, x2=, y2=95, a2=0, b2=0; int hin1=0, hb,2=0, h 1=, h2=, m1=, m2=; int t...

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The tractions can be decomposed into normal and tangential contributions by...

The tractions can be decomposed into normal and tangential contributions by projections on the unit normal vectors tn = t ⋅ nn, tt1 = t⋅ nt1 and tt2 = t⋅ nt2.

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Fracture Mechanical Analysis of the Thermal Shock STAGES OF CRACK 5 that a ...

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