1996
DOI: 10.1016/s0022-3115(96)00330-3
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Fracture behavior of surface cracked panels of HT-9 at low temperatures

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Cited by 4 publications
(6 citation statements)
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“…For certain well-defined conditions, 4 known as SSY, the fields are self-similar in non-dimensional distance, r=d % r= ½K 2 J =ð2E 0 r y Þ, and are uniquely determined by K J , E 0 and rðeÞ [1]. As discussed below, the high r n fields must reach a critical level ðr n ¼ r Ã Þ that encompasses a sufficient volume of trigger particle microstructure in front of the crack tip to cause cleavage [1,[4][5][6][7][16][17][18][19][20][21][22][23][24][25][26][27][28][29][30][31][32].…”
Section: And 5)mentioning
confidence: 99%
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“…For certain well-defined conditions, 4 known as SSY, the fields are self-similar in non-dimensional distance, r=d % r= ½K 2 J =ð2E 0 r y Þ, and are uniquely determined by K J , E 0 and rðeÞ [1]. As discussed below, the high r n fields must reach a critical level ðr n ¼ r Ã Þ that encompasses a sufficient volume of trigger particle microstructure in front of the crack tip to cause cleavage [1,[4][5][6][7][16][17][18][19][20][21][22][23][24][25][26][27][28][29][30][31][32].…”
Section: And 5)mentioning
confidence: 99%
“…In almost all-practical situations, the amplitude of the fields at a given K J is reduced from the SSY limit, due to the loss of constraint, which increases with increasing D (Fig. 4(b)) [1,4,6,[23][24][25][26][27][28][29][30]. 5 CL increases the K Jm and K Je at cleavage.…”
Section: And 5)mentioning
confidence: 99%
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