![]() ·Table of Contents ·Computer Processing and Simulation | An Interactive CAD Environment for Ultrasonic Evaluation of Welded JointsFairouz Bettayeb, Amar BenchaalaScientific Research Center on Welding And Non Destructive Testing, C.S.C, Route de Dely Brahim, BP: 64, Chéraga, Algiers. Tel/fax: (213-2) 361850.Email: bettayeb@excite.com, f_bettayeb@email.com Mohammed Kassel, Karim Hamzi University of Science and Technology USTHB, BP:32, El Alia, Algiers. Contact |
| (1) |
The ultrasonic beams are reflected from surfaces, refracted when they cross a boundary between two materials that have different acoustic impedance, and diffracted at edges or around obstacles [4].
In Ultrasonic inspection, sound beams of high frequency are introduced into materials for the detection of surface and subsurface flaws. The sound waves travel through the material with some loss of energy and are reflected at interfaces. The reflected beam is displayed and then analyzed to define presence and location of discontinuities. The reflection depends largely on the physical state of the interface and physical properties of the material. The relation between the reflected wave amplitude and the incident wave amplitude on a perpendicular surface is defined by the following reflection coefficient:
| (2) |
The literature has proposed several physical formulas and numerical data dealing with the acoustic wave propagation, and numerous authors have presented many of the fundamental aspect of elastic wave distribution. Some of these data are implemented in USNDT2000, and will be reported in a future contribution because of the page limitation.
| (3) |
| (4) |
[F] : applied load vector
[M] : global mass matrix determined by the density distribution of the medium
[K] : global rigidity matrix determined by the elastic properties of the medium.
[¶u/¶t] : velocity vector
[D] : displacements vector
5.1 Signal acquisition
Once the condition of testing are defined, and the probe which characteristics have been taken from a krautkramer database[6] is truly positioned on the tested piece, the system performs an acquisition and a numerical representation of the received signal thanks to the simulation of a virtual oscilloscope.
Pulse echo waveforms are obtained from the weld area. This area includes the weld shape, surface and the weld root. The ultrasonic pulse is directed into the weld section at a specific angle, and a software is used to monitor and control the transducer pulsing, digitization of acquired signals and data storage.
Then the program generates from digitized A-scan data an image with high resolution. A computation of the path of the central beam is performed, and the expected response in amplitude is given. The limits of the area to be scanned by the probe, are computed and designed by A and B in fig.1. The path tracing is estimated considering the geometric reflections of the component as well as of the defects. And a 2D visualization of the beam travel inside the component is displayed. If a defect is detected, the system displays its depth P and its position by computing the distance S, displayed in fig.1.
Signal analysis
The implementation of the philosophy of the ultrasonic inspection requires: to register, during the transducer scanning, all signals reflected from the defects, to determine linear co-ordinates of the beginning of each defect and its extension and to have parameters of the inspected joint into the memory [7].
Fundamental and applied aspects of the mathematical background of ultrasonic modeling, computer technologies and analytical methods developed for non-destructive evaluations have produced new advanced techniques for flaw identification. The simulation models of ultrasonic wave propagation, in solid media contribute to reduce the number of laboratory testing and to learn more about inspection results [8]. These models can be classified into 3 categories: exacts solutions, approximate solutions and numerical solutions .
USNDT2000 performs a computerized model of the signal propagation, a qualitative agreement between theory and experiment ultrasonic interpretation methods. So, in addition of the numerical modeling formulated in (3) & (4) of the general algorithm below, experimental methods[9] such as the triangulation, the DGS diagram, -6dB, have been implemented and drawn in fig.1 and fig.2.
Fig 1: "USNDT2000 software package"
|
Fig 2: "DGS diagram calculation |
The oscillations are scattered from defect in the direction of the transducer, the echo signal obtained is selected in time and the transfer function of the defect is analyzed. Once the A-scan traces are selected by USNDT2000 system, the parameterization is automatically performed and displayed in fig.1, both in time and frequency domain (pulse width, run time, echo, and energy...). The combination of detected signal data, with all informations on the welded joint, component geometry, material properties and the welding process, allows extracting relevant data for better defect characterization.
5.2 Displaying results
When the flaw has been sized, a pattern recognition software [10] introduced in USNDT2000 performs its identification by the use of a set of normalized databases about planar and volumetric defects. Then the reference, the severity and the kind of the defect are displayed. And a short definition and comments on the site and orientation of the flaw are given. At last, USNDT2000 performs a graphical representation of the discontinuity.
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