| Ultrasonic Testing of Austenitic and Dissimilar Metal Welds << ..... < ..... > |
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4.3 ..... Test Effects and Test Techniques 4.3.1 .. Geometry Reflection 4.3.2 .. Corner Effect 4.3.3 .. Mode Conversion with Neighbor Echo 2 method 4.3.4 .. Tandem- and Equivalent Tandem Test Technique 4.3.4.1 The classical Tandem Technique with Vertical Polarized Shear Waves 4.3.4.2 The LLT-Technique 4.3.4.3 Normal Probe - Mode Conversion Technique (Neighbor Echo 1) |
![]() Fig 4.6: Corner effect and wave modes [104] |
Fig. 4.6 makes those different qualities clear. It shows that the corner effect for longitudinal waves exists only faintly at app. 45°. The vertical polarized shear wave is fully present between 35° to 55°, and the horizontal polarized shear wave (SH- Wave) is present in the full range of incidence angle between 0° to 90°. The reason is that SH- wave exists in isotropy materials, but also in transversal isotropy materials, like austenitic welds; no wave conversion applies, if columnar grains are present in the beam orientation (longitudinal flaw testing).
![]() Fig 4.7: "counterbore" and test effect ![]() Corner Effect ---- Mode Conversion Fig 4.8: Neighbor Echo 2- Method and Corner Effect. ![]() Fig 4.9: Tandem- and equivalent tandem test technique |
Assuming the presence of all necessary conditions for the Neighbor Echo 2 method, this test method offers the highest detection sensibility. This is confirmed in Fig. 4.8 shows this, using a fatigue crack as an example.
Each of these three methods provides a specific detection capability, as described in item 5. The principles of these three techniques are outlined as follows:
4.3.4.1 The classical Tandem Technique with vertical polarized Shear Waves
It uses two 45°-Shear Wave Probes, which work on the transmitter/receiver principle. The depth of sensitivity is adjusted via the distance between transmitter and receiver. Fig. 4.9 displays the Tandem principle.
A longitudinal wave with small angle of incidence is reflected at the probe's far surface (1. crystal). This reflected wave is received from a 2. crystal and undergoes mode conversion at the point of circular shaped defects. [77] - [79], [196, 197]. The basic principle is displayed in Fig 4.9. The LLT-Technique can be built very compactly into one probe incorporating two test functions, thus a large thickness range is covered. The sound beam in Fig. 4.10 characterizes the working principle of a LLT- compact probe.
Fig 4.10:
LLT-compact test technique, test frequency 2 MHz, shown are the real
crystals with their true propagation, M 1:2
4.3.4.3 Normal Probe - Mode Conversion Technique (Neighbor Echo 1)
SEL- Probes are used as the basic element of the Neighbor Echo 1 method. Depending on the angle of incidence, different sensitivities and projection distances are provided at the reflector. The schema in Fig. 4.9 confirms this, using a 55°- and a 70°- SEL-Probe as examples.
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