I. INTRODUCTIONCURRENT models for characterizing arrest toughness of dynamic ductile fracture in gas-transmission pipelines have used upper shelf energy (USE) of Charpy V-notch (CVN) impact test and USE of drop-weight tear test (DWTT) as fracture resistance values. [1] In general, the arrest toughness of pipeline steels is predicted by a simplified semiempirical formula obtained from the correlation of fracture speed of pipelines with crack propagation speed, which depends on gas decompression behavior. According to the API RP 5L3 specification, [2] the CVN USE shows a linear relation with the USE of the pressed-notch (PN) DWTT or the chevron-notch (CN) DWTT. In the case of the currently produced high-toughness pipeline steels, however, the correlation of the CVN USE with fundamental fracture process or crack speed is less obvious. This is because a considerable amount of initiation energy is involved, which is unrelated to actual material resistance to fracture propagation as plastic deformation significantly increases at the crack tip. [3,4,5] Also, the impact testing methods are limited by specimen geometries, and the reliability of the correlation between CVN USE and DWTT USE decreases. The evaluation of the absorbed energy has provided reliable standards for low-toughness pipeline steels (CVN USE Յ 100 J), but it is more or less inconsistent with full-scale fracture behavior in currently produced high-toughness pipeline steels.Correlation between Charpy V-notch (CVN) impact properties, drop-weight tear test (DWTT) properties, and crack-tip opening angles for stable crack propagation (CTOA sc ) in high-toughness API X70 pipeline steels was investigated in this study. Two-specimen CTOA test (TSCT) was conducted on the rolled steel materials to measure the CTOA sc , and the test results were compared to the CVN and DWTT data to find correlations between them. The CVN total energy density showed an almost 1:1 linear correlation with the DWTT initiation energy density. The TSCT results indicated that the materials rolled in the single-phase region had the larger CTOA sc as well as the higher CVN and DWTT energy density than those rolled in the two-phase region because their microstructures were composed of acicular ferrites and fine polygonal ferrites. The CTOA sc had a better correlation with the DWTT propagation energy density or the CVN total energy density than the DWTT total energy density. In particular, the value of sin (2CTOA sc ) reliably represented a linear proportional relation to the DWTT propagation energy density.