Shallow flaws under biaxial loading conditions - Part I: The effect of specimen size on fracture toughness values obtained from large-scale cruciformspecimens

A technology to determine shallow-flaw fracture toughness of reactor pressu re vessel (RPV) steels is being developed This technology is for applicatio n to the safety assessment of RPVs containing postulated shallow-surface pm vs. It has been shown that relaxation of crack-tip constraint causes shall ow-flaw fracture toughness of RPV material to have a higher mean value than that for deep flaws in the lower transition temperature, region. Cruciform beam specimens developed at Oak Ridge National Laboratory (ORNL) introduce far-field, out-of-plane biaxial stress components in the test section that approximates the nonlinear stresses resulting from pressurized-thermal-sho ck (PTS) loading of an RPV. The biaxial stress component has been shown to increase stress triaxiality (constraint) at the crack tip, and thereby redu ce the shallow-flaw fracture toughness enhancement. The cruciform specimen pe,mits controlled application of biaxial loading ratios, resulting in cont rolled variation of crack-tip constraint. An extensive matrix of intermedia te-scale cruciform specimens with a uniform depth surface flaw, was previou sly tested and demonstrated a continued decrease in shallow-flaw fracture t oughness with increasing biaxial loading. This paper describes the test res ults for. a series of large-scale cruciform specimens with a uniform depth surface flaw. These specimens weve all of the same size with the same depth flaw and were tested at the same temperature and biaxial load ratio (1:1). The configuration is the same as the previous set of intermediate-scale te sts, brit has been scaled upward in size by 150 percent. These tests demons trated the effect of biaxial lending and specimen size on shallow-flaw frac ture toughness in the lower transition temperature region for RPV materials . For specimens tested under frill biaxial (I:1) loading at test temperatur es in the range of 23 degreesF (-5 degreesC) to 34 degreesF (1 degreesC), t oughness was reduced by approximately 15 percent for a 150-percent increase in specimen size. This decrease was slightly greater than the predicted re duction for this increase in specimen size. The size corrections for 1/2T C (T) specimens did not predict the experimentally determined mean toughness values for larger size shallow-flaw specimens tested under biaxial (1:I) lo ading in the lower transition temperature region.