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R-curve behaviour of a structural steel

✍ Scribed by P.M.S.T. De Castro


Publisher
Elsevier Science
Year
1984
Tongue
English
Weight
886 KB
Volume
19
Category
Article
ISSN
0013-7944

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✦ Synopsis


The ductile tearing behaviour.of BS4360 50D structural steel has been studied using two bending specimen geometries: square (W = B) cross section three point bend specimens with different initial fatigue crack length, ranging from a/W = 0.20 to about 0.75, and rectangular cross section (W = 2B) specimens with initial fatigue crack length a/W = 0.3. With the first set of specimens it was intended to investigate the possible dependence of the tearing behaviour on initial crack length. It was concluded that specimens with shorter values of initial crack length present higher Tesistance to ductile tearing. Two different methods of calculating the J-resistance curve. one based on the approximate equation J = ZA/( W -a)B and a more elaborate calculation procedure introduced by Garwood were used. The curves determined following the more accurate procedure were used to determine the value of the tearing modulus T, which is related to the occurrence of tearing instabilities in structures. It was found that T decreases slightly with increasing value of initial crack length.

The tests using the wider specimen geometry were intended to examine the tearing behaviour over a larger amount of crack growth allowed by the wider geometry used. It was found that the resistance curves, using the COD concept, present a maximum after which the resistance begins to drop. This maximum value of the CODresis@ce curve is higher than the conventional 8 mpx measured at max load. These tests were performed using the compliance technique of evaluating the crack length. Tests performed with 10% unloading presented slightly lower values of resistance than tests performed with complete unloading.

It was found that the relationship J = tnu~,~~S presents increasing values of m with crack growth. This is attributed to an increasing local yield stress. caused by the through thickness deformation.


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