Method for monitoring the integrity of an eddy current inspection channel
AssigneeOlympus NDT
InventorBenoit LePage
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AssigneeOlympus NDT
InventorBenoit LePage
Estimating the term…
An eddy current object testing system includes an EC probe and an acquisition channel which is configured to receive an EC signal from the EC probe and to generate a visual output, namely an impedance plane representation, of the output. A display is coupled to the acquisition channel to display the visual output. The at least one probe is provided with a test loop substantially surrounding it and has a series switch which can be selectively closed or opened to thereby cause the image plane to assume a state that is indicative of a fault, if any, in the EC probe.
An eddy current object testing system, comprising:
A method of detecting a faulty eddy current testing channel in an eddy current probe having at least two drive-sense channels, the probe is electronically coupled with an acquisition unit, which is subsequently electronically coupled with a data processing and display unit, and the acquisition unit receiving an EC signal from the at least one channel and to generate an EC output representative of characteristics of the EC signal,
Dependencies are inferred from the claim text.
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For investigating the presence of flaws: using eddy currents
Using eddy currents: details, e.g. in the structure or functioning of sensors
Investigating or analysing materials by determining their chemical or physical properties
About 7 years 8 months of term left · ends 22 Jun 2034 (estimated)
The present invention relates to non-destructive testing and inspection systems (NDT/NDI) and, more particularly, to Eddy Current (EC) or Eddy Current Array technology (ECA), employing eddy current probes with a test loop linked to it, which allows checking the integrity of the testing system.
Eddy current inspection is commonly used as a non-destructive method to detect flaws in surfaces of manufactured components fabricated from a conductive material, such as bars, tubes, and special parts for automotive, aeronautic or energy industries.
Typical eddy current sensor configurations are impedance bridge, pitch-catch (alternatively called reflection or transmit-receive) and differential, but can also include more complex combinations such as pitch-catch with differential receivers, multi-differential, etc.
FIG. 1 shows the test loop for a simple configuration of one channel composed of one coil.
FIG. 2 illustrates the impedance plane signal associated with the activation of the test loop. This figure shows the reference test loop signal (operation point shift vector) as well as the signal associated with the current probe check evaluation.
FIG. 3A shows the test loop for a pitch-catch coil configuration. Each transmitter or receiver is composed of a channel. Each channel can be composed of a different coil number and configuration.
The test loop of the present invention is based on eddy current basics. Thus, when a shielding loop is positioned around an eddy current test coil, a signal will be induced in the loop and this signal will change the magnitude and phase of current flowing in the coil. The detection of these changes enables checking the ECA inspection system functionality.
FIG. 1 is a simple configuration of the test loop in one channel, which is composed of a single coil 1, which is being used for both the generation and reception of the eddy current signals. The test loop 3 in this case consists of a conductive circuit, which turns around the inspection coil 1. The switch 5 is utilized to activate test loop 3. Once the switch 5 is closed, an eddy current is induced in the test loop 3. Consequently, the coil 1 impedance is changed. However, when the coil 1 is broken, it does not induce current in test loop 3 and consequently, shows no changes in coil's 1 impedance associated with the switch 5 position.
The electrical impedance (Z) is the total resistance that a circuit presents to an alternating current. In Eddy current circuits, impedance includes the possible resistance (R) and the inductive reactance (XL) components. The resistance component and the reactance component are not in phase, so vector addition must be used to relate them to the overall impedance. For an eddy current circuit with resistance and inductive reactance components, the total impedance is calculated using Z=√{square root over (R2+XL2)}.