Issue 35

A. Vshivkov et alii, Frattura ed Integrità Strutturale, 35 (2016) 57-63; DOI: 10.3221/IGF-ESIS.35.07 61 T HE STUDY OF THE THERMOELASTIC EFFECT he sensitivity of the sensors was illustrated by the study of thermoelastic effects in metals under investigation. The amplitude of applied stress did not exceed 40% of the limit of proportionality, which provided the absence of sample heating caused by plastic deformation. In the goal of the experiments was the investigation of the accuracy of the proposed method and the influence of the conditions of heat exchange with the environment. The experimental data was compared with the analytical solution of the Kelvin equation. Additionally, the influence of the conditions of contact between the sensor and the sample on the measured parameters was checked. The amplitude of the stress was 5 kN, the frequency of 1 Hz, the stress ratio R = -1. The experimental results for various conditions of sensor contact with the sample are shown in Fig. 6. Figure 6 : Power of heat flux during the thermoelastic test (1 – the analytical solution of the Kelvin equation; 2 – the experimental data from the sensor pressed by the spring to the sample; 3 – the experimental data from the sensor corrected by the consideration of whole free surface of the sample; 4 – the experimental data from the sensor located with a gap of 0.5 mm. from the sample; 5 – the experimental data from the sensor located with a gap of 0.1 mm. from the sample.) Fig. 6 shows three variants of mounting the sensor to the sample: a tripod with a gap of 0.5 mm (4) and 0.1 (5), and the pressing of sensor to the sample by the spring (3). Analysis of the results presented in Fig. 6, allows us to conclude that there is no influence of friction on the measured heat flow. The measured value with a tripod is substantially less than the theoretically calculated (graphs (4) and (5) in Fig. 6). In this case, it is assumed that the sensor does not change the conditions of heat exchange of the sample and the environment (heat dissipation is the same in all directions). To correct the heat measured data from the pressed sensor (2) we assumed that the sensor with cooling system does not change the heat transfer conditions and multiply the data by a factor taking into account the whole free surface of the sample. Taking these hypothesis into account we can obtain a complete coincidence of measured and theoretical values (graphs (1) and (3) in Fig. 6). T HE STUDY OF FATIGUE CRACK PROPAGATION he developed sensor was used to study the heat dissipation caused by growth of fatigue cracks. Typical result of measurements of the heat flux during the experiment is presented in Fig. 7. The plots can be divided into three parts. Short initial increasing part corresponds to starting of crack propagation (part 1). The second part with constant heat flux corresponds to the regime of short crack propagation (part 2). The last part of the plot (part 3) is characterized by sharp increasing of heat dissipation. During this part we observe the long crack propagation process. The last part is finished by specimen failure. Fig. 8 presents the experimental data to illustrate general regularities in the dynamics of fatigue crack growth. The tests presented in the figure were carried out on the samples made from steel. The geometry of the samples is presented in Fig. 4a. The stress amplitude was constant during the test. The unfilled point corresponds to the results of the heat measurement with the developed sensors. There are three different stress amplitudes in Fig. 8 with corresponds to following applied forces: 13 kN (unfilled squares), 15 kN (unfilled circles) and 17 kN (unfilled diamonds). The filled marks T T