Described below are a method and a device for induction thermography for nondestructive material examination.
During an examination by induction thermography, a test head, which is also denoted as an inductor, is positioned over a test object or over a test specimen. The magnetic field resulting from the current flowing in the test head generates an electric induction current in the test specimen to be examined. The induction current leads to a heating of the test specimen by ohmic losses. The heat distribution resulting in the test specimen can, in turn, be detected by an infrared camera. If the test specimen includes defects, such as cracks, for example, the induced current must flow around them or via existing contact points. The process leads to an increase in a local current density and, following therefrom, a heating at the points. Cracks can therefore be detected in the infrared image. The method and device described below for induction thermography of a test specimen by which material defects are detected with a maximum defect detection probability in the case of nonautomated measuring processes. The aim is to be able to find all material defects of a specific type, starting from a defined and specific size, reproducibly in the entire test specimen or in a specific region of the test specimen.
The aim is to ensure that the defect detection probability is maximized. The aim is to use an examination of a test specimen to be able to find all defects of a specific type, such as cracks, for example, starting from a defined and specific size, reproducibly in the entire test specimen or in a specific region of the test specimen.
Here, defect detection probability is defined as a statement represented as a probability curve used to describe probabilities of the acquisition of material defects as a function of the size of the material defect, and of all relevant measurement parameters. The measurement parameters can be known and/or be set directly or indirectly. Measurement parameters are, in particular, the distance between inductor and test specimen, size of the induction region in the test specimen, and direction of the induction current flow.
Use is made of so-called defect detection probability curves (probability of detection/POD curves) which represent the probability of detection as a function of the defect size and taking account of all the important measurement parameters. The measurement parameters are either known or can be influenced directly or indirectly. It is therefore possible to make a statement concerning the minimum size a defect must have in order to be detected with sufficient accuracy. However, the statement is only correct when all the restrictions of a measurement are taken into account. If, for example, the inductor is held too far away from the test specimen by the testing technician, the measurement parameters are changed and the statement loses its validity.
In accordance with a first aspect, a method for scanning induction thermography is proposed for nondestructive material examination of a test specimen, the test specimen and an inductor which has an infrared camera, which records infrared images, and generates an electric induction current in the test specimen being positioned relative to one another by a testing technician during a manual measurement. An evaluation, carried out by a computer device, of at least one of the recorded infrared images, and a projection, performed by a projector device onto the surface of the test specimen, of in each case one indication for the testing technician which corresponds to a result of the evaluation are performed.
In accordance with a second aspect, a device for scanning induction thermography for nondestructive material examination of a test specimen is proposed, the test specimen and an inductor which has an infrared camera, which records infrared images, and generates an electric induction current in the test specimen being positioned relative to one another by a testing technician during a manual measurement, an evaluation, carried out by a computer device, of at least one of the recorded infrared images, and a projection, performed by a projector device onto the surface of the test specimen, of in each case one indication for the testing technician which corresponds to a result of the evaluation being carried out.
Thus, a system is proposed which supports the testing technician during or after a measurement by virtue of the fact that important indications are projected directly onto the test specimen. The aim is to provide the testing condition during or directly after the measurement with feedback which is projected onto the test specimen and indicates to the testing technician whether the measurement is or has been carried out correctly with respect, in particular, to the defect detection probability. It has been recognized that the measurement result of a manual, nonautomated induction thermography depends very strongly on the testing technician with regard to the acquisition of material defects and likewise with regard to the defect detection probability (so-called human aspect). According to the invention, information from infrared images is used to evaluate material defects and to estimate the defect detection probability, in order to support the testing technician during or after the measurement and to reduce as far as possible the influence of the so-called human aspect.
In accordance with an advantageous refinement, an indication during or after the measurement can indicate whether the measurement is or has been carried out correctly in respect of a required defect detection probability, taking account of measurement parameters. It has been recognized that the following effect, specifically the distance between the inductor and the test specimen, can influence the defect detection probability. A further measurement parameter results from the fact that the induced current typically flows in the vicinity of the inductor or of the test head such that defects can be detected only in a specific region around the inductor. The region can be designated as measurement region. Should the entire test specimen or a relatively large region be examined, the measurement must be repeated several times with appropriate displacement of the test head. A further important finding is that because of the direction of the current flow it is defects which are situated perpendicular to the current flow or to the inductor which can best be detected. According to the invention, it has been recognized that given nonautomated measurement processes the measurement parameters can lead to limitations such that the measurement becomes defective and the defect detection probability is too low. By projection of the respective defect detection probability onto the testing technician, the defect detection probability can be kept constant during measurement over the entire test specimen or a plurality of test specimens. This is a great advantage in the case of measurements for which it would either be impossible or not profitable to automate.
In accordance with a further advantageous refinement, the computer device can determine the maximum possible defect detection probability of the measurement by defect detection probability curves depending on the magnitude, which is to be acquired, of a material defect while taking account of the measurement parameters, that is to say the characteristics under which the measurement is performed.
In accordance with a further advantageous refinement, the computer device can carry out the evaluation of at least one of the recorded infrared images in order to calculate the measurement parameters of the measurement.
In accordance with a further advantageous refinement, the evaluation of the infrared image of the test specimen can be carried out without an inductor in order to calculate measurement parameters.
In accordance with a further advantageous refinement, in order to calculate measurement parameters the evaluation of an infrared image, recorded before the induction of the induction current, of the positioned inductor and of the test specimen can be carried out.
In accordance with a further advantageous refinement, in order to calculate measurement parameters the evaluation of an amplitude image generated by pulse-phase analysis of the infrared images recorded during the measurement can be carried out.
In accordance with a further advantageous refinement, in order to calculate measurement parameters the evaluation of a phase image generated by pulse-phase analysis of the infrared images recorded during the measurement can be carried out.
In accordance with a further advantageous refinement, the measurement parameters can be the distance between inductor and test specimen, the measurement range of the inductor and/or the orientation of the inductor with respect to the test specimen.
In accordance with a further advantageous refinement, as an indication lines running perpendicular to the orientation of the inductor can be projected onto the test specimen during or after the measurement in order to indicate that material defects extending along the lines are or have been acquired with a maximum possible defect detection probability.
In accordance with a further advantageous refinement, as an indication color-coded areas can be projected onto the test specimen during or after the measurement in order to indicate that material defects extending in specific directions in the respective colored areas are or have been acquired with a maximum defect detection probability.
In accordance with a further advantageous refinement, the orientation of the inductor can be changed after the measurement and a further measurement can be carried out, further lines running perpendicular to the changed orientation of the inductor and further color-coded areas additionally being able to be projected onto the test specimen.
In accordance with a further advantageous refinement, an indication during or after the measurement can be indicated whether the measurement parameters of the measurement are or have been correctly set, given that the geometry of the inductor, the position of the latter with respect to the test specimen, and all the measurement parameters are known.
In accordance with a further advantageous refinement, an indication can indicate the measurement range of the inductor as a colored area on the test specimen as a function of the position of the inductor relative to the test specimen.
In accordance with a further advantageous refinement, an indication can indicate the correctness of the distance between inductor and test specimen during or after the measurement by a specific color of the colored area.
In accordance with a further advantageous refinement, identical measurement ranges of measurements with different orientations of the inductor can be indicated in an overlapping fashion.
In accordance with a further advantageous refinement, an indication can indicate an information item relating to the quality of the positioning of the inductor.
These and other aspects and advantages will become more apparent and more readily appreciated from the following description of exemplary embodiments, taken in conjunction with the accompanying drawings of which:
Reference will now be made in detail to the preferred embodiments, examples of which are illustrated in the accompanying drawings, wherein like reference numerals refer to like elements throughout.
The indication 11 in accordance with
Ix′=(I−O).
Ax′=A*T′;
It can be judged subsequently whether the defect detection probability in the region under examination is in agreement with the requirement, and the information is projected onto the test specimen 7. It is to be taken into account in this case that the detectability and the defect detection probability depend strongly on the orientation of the test head or of the inductor 1 with respect to potential defects. This must be expressed in the projection. In accordance with
Information is represented cumulatively for all further measurements. If the testing technician changes the orientation of the inductor 1 for further measurements, for example by 90 degrees, the lines are projected for all measurements. They give an indication as to which crack directions of measurements already carried out have been covered by the assumed defect detection probability. Alternatively or cumulatively, new regions of the test specimen 7 can be covered by the inductor 1 for further measurements. Information and indications 11 can, for example, be projected onto the object as numbers, letters, colored fields, lines or any desired symbols.
The invention proposes a method and a device for scanning induction thermography for nondestructive material examination of a test specimen 7 which can be used by a testing technician to effectively improve the quality of a manual measurement. In order to achieve this, the testing technician is provided with an evaluation of recorded infrared images and the projection onto the test specimen 7 of indications 11 corresponding to the evaluation.
A description has been provided with particular reference to preferred embodiments thereof and examples, but it will be understood that variations and modifications can be effected within the spirit and scope of the claims which may include the phrase “at least one of A, B and C” as an alternative expression that means one or more of A, B and C may be used, contrary to the holding in Superguide v. DIRECTV, 358 F3d 870, 69 USPQ2d 1865 (Fed. Cir. 2004).
Number | Date | Country | Kind |
---|---|---|---|
10 2012 212 434.9 | Jul 2012 | DE | national |
This application is the U.S. national stage of International Application No. PCT/EP2013/062098, filed Jun. 12, 2013 and claims the benefit thereof. The International Application claims the benefit of German Application No. 102012212434.9 filed on Jul. 16, 2012, both applications are incorporated by reference herein in their entirety.
Filing Document | Filing Date | Country | Kind |
---|---|---|---|
PCT/EP2013/062098 | 6/12/2013 | WO | 00 |