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- 2010 (24) (entfernen)
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- Phased array (3)
- Ultrasonic testing (3)
- Sound field (2)
- Visualization (2)
- Airborne ultrasonics (1)
- Anisotropic weld (1)
- Anisotropy (1)
- Austenitic weld material (1)
- Critical angle (1)
- D-nozzle (1)
Eingeladener Vortrag
- nein (3)
When dealing in ultrasonic testing with inhomogeneous and anisotropic material structure such as
diverse types of components made from austenitic or nickel based cast, which are currently used
for modern power plant concepts, data interpretation is quite difficult. For better understanding of
the complex interaction between the sound field and the component under test, the mathematical
modeling of sound propagation in solids is a substantial task to increase the probability of
detection of relevant defects.
First we present a mathematical approach for modeling the three dimensional transient
particle displacement as a function of time in each point in a half space excited by an impulsive
point load at the surface. The transient ultrasonic field of a rectangular array element is calculated
with this approach by a point source synthesis. Based on this solution we model the wave
propagation of a phased array transducer by time delayed superposition of the wave field of the
transducer elements.
Next we use an electrodynamic technique to visualize the grazing sound field at the surface
of a test block radiated by a phased array probe. By detecting the grazing beam at the samples
surface with a small electrodynamic probe, we measured the particle displacement as a function of
time. It allows for measuring the displacement in all three spatial directions. This comprises the
detection of the horizontal and vertical particle displacement with respect to the surface and thus
also the detection of longitudinal and shear waves is possible.
The calculated and measured wave fields will be compared for different delay laws in
isotropic and transversely isotropic media. The results support the theoretical activities to model
the wave propagation and to find optimal testing parameters for different components and
configurations.
In this contribution a simulation tool is developed to compute the energy skewing angles and energy coefficients
for the reflected and refracted plane waves in following general cases: (1) reflection and refraction
of plane elastic waves at an interface between isotropic and transversely isotropic solid, (2) reflection
and refraction of plane elastic waves at an interface between transversely isotropic and isotropic solid, (3)
reflection and refraction of plane elastic waves at an interface between two general transversely isotropic
solid and (4) reflection of plane elastic waves from a stress free boundary of a transversely isotropic solid.
Computational results for analytically evaluated acoustic wave energy skewing angles and energy reflection
and transmission coefficients in acoustically anisotropic materials such as austenitic steel materials
exhibiting columnar grain orientation are presented. The obtained results show that the acoustic energy
skewing angles and coefficients in austenitic steel materials strongly depend upon the columnar grain
orientation and are less influenced by the grain orientations which are parallel and perpendicular to the
interface.
The ultrasonic transmission between two air-coupled polypropylene (PP) ferroelectret (FE) transducers in dependence on the amplitude of the high-voltage exciting pulse revealed a strongly nonlinear electromechanical response of the FE transmitter. This phenomenon is described by a linear increase of the inverse electromechanical transducer constant t33(1) of the PP FE film with an increase of the exciting electrical pulse amplitude. Enlargement of t33(1) by a factor of 4 was achieved by application of 3500 V exciting pulses. The electrostriction contribution to t33(1) can be attributed to the electrostatic force between electrodes and the Maxwell stress effect. The nonlinear electromechanical properties of the PP FE result in a strong increase of its air-coupled ultrasonic (ACUS) figure of merit (FOM) under the high-voltage excitation, which exceeds results of the PP FE technological optimization. The FOM increase can be related to the increase of PP FE coupling factor and/or to the decrease of its acoustic impedance. A significant enhancement of the ACUS system transmission (12 dB) and signal-to-noise ratio (32 dB) was demonstrated by the increase of excitation voltage up to 3500 V. The nonlinear electromechanical properties of the PP FEs seem to be very important for their future applications.
The determination of magnetic distortion fields caused by inclusions hidden in a
conductive matrix using homogeneous current flow needs to be addressed in multiple tasks of
electromagnetic non-destructive testing and materials science. This includes a series of testing
problems such as the detection of tantalum inclusions hidden in niobium plates, metal inclusion in
a nonmetallic base material or porosity in aluminum laser welds. Unfortunately, straightforward
tools for an estimation of the defect response fields above the sample using pertinent detection
concepts are still missing. In this study the Finite Element Method (FEM) was used for modeling
spherically shaped defects and an analytical expression developed for the strength of the response
field including the conductivity of the defect and matrix, the sensor-to-inclusion separation and the
defect size. Finally, the results also can be useful for Eddy Current Testing problems, by taking the
skin effect into consideration.
The spatial resolution in ultrasonic testing as a wave phenomenon in nature is limited to a
certain fraction of the wavelength, usually defined to be close to the Rayleigh criterion. In case of
complicated reflector surfaces – such as stress corrosion cracking - this limitation prevents an exact
visualization of the defect shape. There exist a few approaches to improve the spatial resolution, whose
reconstruction quality all in common also depend on the achieved signal-to-noise ratio of the raw data. In this
work we present a specific SAFT analysis, in which a high number of different angles of incidence produce a
sufficiently high number of different reflections at the crack edges resulting in an improved SNR. In doing
so, we reconstruct a coherent crack structure. First investigations were made at artificially simulated crack
configurations with different contours and curvatures in flat and cylindrical test blocks. The measurements
results visualized by representative scans – show details of crack design and crack orientation. We also will
present a comparison of the SAFT analysis between modelling and phased array measurements.
Within a know-how transfer project funded by the government conventional ultrasonic
technique was replaced by phased array technique for automated round-bar testing. Instead of
applying a great number of conventional probes to achieve acceptable volume coverage we used
curved linear arrays. The benefits of phased array technique such as programmable skew angles,
beamforming and beam positions, led not only to a significant decrease in inspection time, but also the
number of probes could be substantially reduced . Finally, the testing parameters for a large range of
bar-diameters could be adapted by software control instead of time-consuming mechanical
replacement. The probe-design was carried out by a proprietary modelling program. Both the
theoretical calculations as well as the latter experimental verifications revealed significant advantages
of curved arrays versus the planar types. A radial oriented probe offers perfect adaption to the
cylindrical shape of the specimen allowing wide variations of the sound field. Thus beam direction,
beam size and beam position could be optimized with respect to a minimum of inspection cycles, as
inspections have to be executed in-line during the production. A number of laboratory tests were
carried out on special test components. In order to achieve an optimal performance of the reference
rod we implemented three different types of reference reflectors: (i) flat-bottom-holes with diameters
of 0.8 mm and 1.2 mm, (ii) side-drilled-holes with a diameter of 0.7 mm for the detection of
volumetric flaws, and (iii) notches with a depth of 0.2 mm and 0.5 mm for the detection of surfaceoriented
defects. All laboratory tests were carried out with the COMPAS-XXL inspection system, a
proprietary development of BAM.
In diesem Beitrag wird eine Methode zur Charakterisierung von
offenen Oberflächenrissen mittels aktiver Thermografie präsentiert. Hierzu wird die
Probe ortsfest lokal mit einem Laser erwärmt und die resultierende
Oberflächentemperatur mittels Infrarotkamera aufgenommen. Bei einer ungestörten
Probe ergibt sich ein rotationssymmetrisches Temperaturprofil. Betrachtet man
hingegen einen Bereich mit einem Oberflächenriss, so kommt es durch die Störung
des lateralen Wärmetransports zu einer unsymmetrischen Temperaturverteilung.
Durch die quantitative Analyse diese Unsymmetrie lassen sich Aussagen über
geometrische Parameter des Risses treffen.
Dispersions of very small non-magnetic metal particles or inclusions in a non-magnetic semiconductor matrix are well known to produce unusually large and linear magnetoresistance effects. So far these materials were limited to the binary silver-rich chalcogenides Ag2Se and Ag2Te. In this contribution Ag3AuTe2 was selected as a first candidate for a ternary matrix material, thus offering enhanced capabilities for the generation of heterogeneous microstructure and spatially varying composition on the nanoscale. In gold-rich Ag3Au1.1Te2 two kinds of inhomogeneities are present, namely Au deposits with a size on the micron scale and an inhomogeneous distribution of Au and Ag within the matrix. The matrix consists of micron-sized grains with the structure type of Ag3AuTe2 as studied by electron microscopy. Like the binary silver chalcogenide phases, the material also shows a large and linear magnetoresistance effect. The transversal magnetoresistance effect was measured between 20 K and 270 K in magnetic fields up to B = 5 T. The results are discussed on the basis of existing models for a large and linear positive MR effect.