Issue 41

S. K. Kourkoulis et alii, Frattura ed Integrità Strutturale, 41 (2017) 536-551; DOI: 10.3221/IGF-ESIS.41.64 545 0.00 0.50 1.00 1.50 2.00 2.50 3.00 0.0E+00 3.0E+08 6.0E+08 9.0E+08 1.2E+09 1.5E+09 1.8E+09 0 100 200 300 400 δ [mm] Cumulative energy [aJ] Load [kN] cumEnergy δ 0.0 0.5 1.0 1.5 2.0 0.0E+00 4.0E+08 8.0E+08 1.2E+09 1.6E+09 0 100 200 300 400 PSC [nA] Cumulative Energy AE [aJ] Load [kN] cumEnergy PSC 0.18 0.57 1.04 3.07 2.25 0.0 1.0 2.0 3.0 4.0 5.0 0 10000 20000 30000 40000 50000 0 300 600 900 1200 1500 δ, ζ [mm] Cumulative hits/s Time [s] cumulative hits/s COD- y=0.07 LVDT (central) ζ δ 2.25 Figure 8 : The time dependence of the cumulative hits per second in conjunction to that of the deflection and the opening of the fault. An alternative approach of quantifying the acoustic activity within the restored epistyle is attempted in Fig. 9a: The cumu- lative energy of the acoustic emissions is plotted against the level of the mechanical load imposed to the structure in juxta- position to that of the deflection, δ, of the epistyle’s central section. The two plots exhibit the same qualitative character- istics: A stage of more or less smooth increase followed by a “plateau”, a sudden change at the instant of the first load drop and again a stage of increase. The correlation of the cumulative energy of the acoustic emissions with the PSC is shown in Fig.9b, in which the dependence of both quantities on the load level is plotted. Besides partial differences it is evident that the overall behaviour of the two plots is quite similar to each other. (a) (b) Figure 9: (a) The variation of the cumulative energy of the AE and δ versus the load applied; (b) The variation of the cumulative energy of the AE and PSC recordings versus the load applied. Further exploitation of the experimental data provided by the acoustic sensors is achieved by calculating the respective Ib - value. In Fig.10 the time variation of the Ib -value is plotted in juxtaposition to the respective one of the load imposed. It is very interesting to observe that the Ib -value remains almost constant, equal to about Ib =1.5 for over 90% of the experiment’s overall duration. At t=1150 s a decrease of the Ib -value is observed almost simultaneously with the abrupt