Conventionally, the transition fracture toughness and upper-shelf fracture toughness of ferritic steels are viewed as separate properties: they are measured by tests conducted according to different standards, and neither toughness property can be estimated (except in very qualitative terms) based on knowledge of the other. Information presented in this paper demonstrates that quite the opposite is true: transition fracture toughness and upper-shelf fracture toughness are directly related because the microstructural features responsible for both the temperature dependence of fracture toughness and for the magnitude of fracture toughness at any given temperature are the same in both transition and on the upper shelf (the lattice structure controls the temperature dependence, while the size and distribution of second-phase particles control crack initiation and thus the magnitude of fracture toughness). These features bind the transition fracture tough. ness and upper-shelf fracture toughness together in a way that is extremely consistent for all ferritic steels. We present empirical evidence of this relationship based on fracture toughness data from a variety of ferritic steels: various heats of nuclear grade pressure vessel steels and welds (both before and after irradiation), copper precipitation hardened steels used in naval ship construction and mild steels used in ship construction. In total, these data span a broad range of To: from -180 °C to +140 °C. The combination of this theoretically motivated, empirically calibrated relationship between transition and upper-shelf toughness with Wallin's Master Curve (for toughness in fracture mode transition), and EricksonKirk's proposed Master Curve for toughness on the upper shelf, produces a model that predicts the temperature dependence of, and scatter in, fracture toughness of ferritic steels throughout the transition and upper-shelf temperature regimes. As input information, this model needs only the value of To, which can be estimated by performing fracture toughness tests according to the protocols of ASTM test standard E1921-05.
[1]
R.K. Nanstad,et al.
Irradiation effects on fracture toughness of two high-copper submerged-arc welds, HSSI Series 5. Volume 1, Main report and Appendices A, B, C, and D
,
1992
.
[2]
J. Knott,et al.
Effects of microstructure on cleavage fracture in pressure vessel steel
,
1986
.
[3]
Influence of fluence rate on radiation-induced mechanical property changes in reactor pressure vessel steels
,
1990
.
[4]
S. Ishino,et al.
The effect of chemical composition on irradiation embrittlement
,
1990
.
[5]
B. R. Bass,et al.
Pressurized-thermal-shock test of 6-in. -thick pressure vessels: PTSE-2 (pressurized-thermal-shock experiment): Investigation of low tearing resistance and warm prestressing
,
1987
.
[6]
R. Armstrong,et al.
Dislocation-mechanics-based constitutive relations for material dynamics calculations
,
1987
.
[7]
M. Sokolov,et al.
Comparison of Irradiation-Induced Shifts of K Jc and Charpy Impact Toughness for Reactor Pressure Vessel Steels
,
1999
.
[8]
Kim Wallin,et al.
The scatter in KIC-results
,
1984
.
[9]
K. Wallin,et al.
Irradiation damage effects on the fracture toughness transition curve shape for reactor pressure vessel steels
,
1993
.
[10]
A. L. Hiser,et al.
J-R curve characterization of irradiated low upper shelf welds
,
1984
.