PSI - Issue 2_A
Jürgen Bär / Procedia Structural Integrity 2 (2016) 2105–2112 Author name / Structural Integrity Procedia 00 (2016) 000–000
2109
5
0.58
0.08
a
b
0.56
0.06
0.54
0.04
0.52
E-Amplitude [°C]
D-Amplitude [°C]
0.02
0.50
0.48
0.00
0
50000
100000
150000
200000
250000
0
50000
100000
150000
200000
250000
cycle number
cycle number
1.8
1.2
44
c
d
1.6
42
1.0
1.4
40
1.2
38
0.8
1.0
36
0.8
0.6
34
0.6 Heat-Flow [W]
Potential [mV]
32
0.4
0.4
specimen temperature [°C]
30
0.2
0.0
0.2
28
0
50000
100000
150000
200000
250000
0
50000
100000
150000
200000
250000
cycle number
cycle number
Fig. 5. Results of thermographic measurements (a-c) and heat flow measurement (d) of an experiment with a constant force of F=8 kN.
3.2. Experiments with constant stress intensity The experiments were started with a constant force of 8 to 8.5 kN. When the stress intensity reached the desired value the force was reduced with increasing crack length so that the maximum stress intensity K max as well as the stress intensity factor K was kept constant. The curve progression of the stress intensity is given in figure 6(a). The experiments were undertaken with stress intensities of 12.5, 15, 17.5, 20 and 22.5 MPa m, respectively. The corresponding crack propagation rates are shown in figure 6(b). For stress intensities up to 17.5 MPa m the crack propagation rate is constant within the scatter over the complete crack length. For the experiments with stress intensities of 20 and 22.5 MPa m the crack propagation rates decreases with the crack length.
10 -6
24
a
b
K max = 12.5 MPa m K max = 15 MPa m K max = 17.5 MPa m K max = 20 MPa m K max = 22.5 MPa m
22
20
K max [MPa m]
10 -7
18
16
14
crack propagation rate [m/cycle]
10 -8
12
2
3
4
5
6
7
8
2
3
4
5
6
7
8
crack length a [mm]
crack length a [mm]
Fig. 6. Measured stress intensities (a) and crack propagation rates (b) for the experiments with constant stress intensity.
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