Issue 42

A. Strafella et alii, Frattura ed Integrità Strutturale, 42 (2017) 352-365; DOI: 10.3221/IGF-ESIS.42.36 360 Figure 10 : Creep curves of specimens tested in lead. 0 200 400 600 800 1000 1200 0,0 0,2 0,4 0,6 0,8 1,0 1,2 1,4 1,6 1,8 2,0 2,2 2,4 15-15 Ti (Si) T= 550°C Creep Strain [%] Time [h] Creep Strain % - [575MPa]- Pb Creep Strain % - [560 MPa]- Pb Creep Strain - [560 MPa] Figure 11 : Comparison of 15-15Ti(Si) creep curves in air at 560MPa and in lead at 560 and 575Mpa. Therefore, up to 800h, the behaviour of 15-15Ti(Si) in lead and in air at 560 MPa is almost similar. For these reasons the test in lead was stopped. An increase of steel deformation in lead took place, but it isn’t relevant and it can be said that creep mechanisms seem to be predominant than lead corrosion. It could be ascribable to the stress value near yield stress 1 and it can be hypothesized that lead corrosion appears after a long time of steel/lead contact. To better understand the effect of lead corrosion, it is necessary to discuss the test in lead at higher stress level, 575MPa, and its comparison with curves at 560MPa because it can provide important information on creep corrosion. 1 theoretical 620 MPa ≤ R p0.002 ≤ 840 MPa, after 20% CW 0 100 200 300 400 500 600 0,0 0,1 0,2 0,3 0,4 0,5 T= 550°C in Pb creep strain % Creep Strain % - [575MPa]- Pb Creep Strain % - [560 MPa]- Pb Creep Strain % - [500 MPa]- Pb Time [h]