Fatigue Crack Paths 2003
propagation rate was examined from the view points of the J-integral and the striation
spacing.
J - I N T E G REA SL T I M A T IFOONRM I X E D - M OCDREA C K
EnergyMethod
Considera circumferentially cracked cylindrical bar under an axial load, P, and torque,
T, as shown in Fig. 1(a). The J-integral value can be determined by the change of the
strain energy with crack extension under constant-displacement, u, or constant-twist
angle, 0 (Fig. 1(b)). The J-integral values of modeI under axial loading, J1, and of mode
111 under torsion, J11], were given by
J I : _” °L_P d u : _aUIL
(1)
27th 0 8a ,
2n'b 8a u
1 M 5 9;al d e b ;
(2)
27th 0 8a 9
27th 8a 9
where U1 and U111 are energy for modeI and III loadings, respectively.
In mixed-mode(I+III) loading, the J-integral value is determined by the change of
the total strain energy with crack extension. Since the total strain energy is the sum of
the mode I and III strain energies under constant-displacement and twist angle, the J
integral value of mixedmode, J1+1]1, was given by
1
8 U
J + I _
1+111
3
1 11
27th [ 8 a l fl
( )
Although J-integral values estimated from the energy method are exact, it is very
difficult to apply the energy methodto fatigue tests.
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Cracklength, a
(:1) Load vs. displacement or
(b) Strain energy vs. crack length
Torque vs. twist angle
Figure 1. J-integral estimation from the energy method.
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