Crack Paths 2009
140
250
Experimental
120
Homogenou(sparent
100
200
material strength) Heterogneous(localwelds ength)
.5 )
a*m0
0
K e ff ( M P
24680
Experimental Homogenou(sparent material strength), [10] Heterogeneous(local w ld str ngth)
105 0
50
0 10 20 30 40 50 60 70
Δa (mm) 6
Δa
(mm)
0
2
4
8 10 12
eff
Fig. 5: comparison FEM-experiment, M(T) Fig. 6: comparison FEM-experiment,
specimen, 2W=160mm.
M(T)specimen, 2W=750mm.
PLASTIDC E F O R M A T IA ONNDC R A CPKA T H
The experiments [7, 8] recorded generally an instability of the crack path of the kind
shown in Fig. 7. After a few millimeters of propagation the crack jumps suddenly in the
TMAZ,characterized by a lower strength and fracture toughness [7].
Fig. 7: experimental crack path, [7].
From the optical strain measurements done with the A R A M I sSystem [7] the instant
of fracture instability corresponds to point 5 in Fig. 8, where te plastic zone has spread
910
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