Waveguide for a bulk-type medium, vibrator using same to transmit shear waves to a bulk-type medium, and method using the vibrator to transmit shear waves to a bulk-type medium
US-9527111-B2 · Dec 27, 2016 · US
US9903840B2 · US · B2
| Field | Value |
|---|---|
| Publication number | US-9903840-B2 |
| Application number | US-201414771162-A |
| Country | US |
| Kind code | B2 |
| Filing date | Feb 20, 2014 |
| Priority date | Feb 28, 2013 |
| Publication date | Feb 27, 2018 |
| Grant date | Feb 27, 2018 |
A practical reading order for non-experts. Skip the full description unless you need deep technical detail.
What the patent document calls the invention.
A short plain-language summary of the technical disclosure.
Who owns or filed the patent and who is credited as inventor.
Filing, priority, publication, and grant dates set the timeline.
The legal scope of protection — read this for what is actually claimed.
Technology tags used to group this patent with similar filings.
Prior art links and similar publications in this corpus.
Official abstract text for this publication.
The present invention relates to a method for detecting temporally varying thermomechanical stresses and/or stress gradients over the wall thickness of metal bodies, in particular pipelines. In the method, the temperature on the outer surface of the body is measured in order to determine a temperature progression and stress progression therefrom. In addition, electromagnetic ultrasonic transducers are used at at least one measuring point on the outer surface in order to determine the progression of the stresses and/or stress gradients over time over the wall thickness of the body in conjunction with the result of the temperature measurement. The method allows the fatigue monitoring of pipelines even in the event of rapid stress changes.
Opening claim text (preview).
The invention claimed is: 1. A method for detecting temporally varying thermomechanical stresses and stress gradients over a wall thickness of metal bodies, in particular pipelines, in which a temperature is measured at at least one measurement point on an outer surface of a body and additional measurements are carried out using electromagnetic ultrasound transducers in a region of the measurement point to determine the one or more of stresses or stress gradients over the wall thickness of the body via the measured temperature from the additional measurements, wherein a temperature curve between an inner surface and the outer surface is ascertained from the measured temperature and is used for the determination of the one or more of stresses or stress gradients over the wall thickness of the body from the additional measurements; characterized in that one or more of ultrasound runtime, amplitude, or eddy current impedance measurements are carried out using the electromagnetic ultrasound transducers, wherein the one or more of stresses or stress gradients are determined by analyzing the one or more of ultrasound runtime, amplitude, or eddy current impedance measurements in conjunction with the measured temperature or the ascertained temperature curve; and characterized in that the determination of the one or more stresses or stress gradients is performed on the basis of a layer model of a wall of the body, which uses the ascertained temperature curve and a stress curve derived therefrom as well as measured and temperature-corrected ultrasound runtimes, amplitudes, and eddy current impedances as input variables and supplies layer-related ultrasound runtimes, amplitudes, eddy current impedances, and stress curves as output variables, wherein the layer-related stress curves are determined by iterative optimization of the layer model from the layer-related ultrasound runtimes, amplitudes, and eddy current impedances. 2. The method as claimed in claim 1 , characterized in that two linearly polarized transverse waves, which are perpendicular to one another, are emitted perpendicularly into a wall of the body in each case using the electromagnetic ultrasound transducers, to measure ultrasound runtimes and amplitudes in pulse echo operation. 3. The method as claimed in claim 2 , characterized in that, during the measurement on a pipe as the body, one of the transverse waves is linearly polarized in an axial direction of the pipe and the other is linearly polarized in a circumferential direction of the pipe. 4. The method as claimed in claim 2 , characterized in that two pairs of electromagnetic ultrasound transducers in separate transmission-reception arrangement are additionally used, which generate Rayleigh waves or horizontally polarized transverse waves, wherein the two pairs are arranged at an angle of 90° in relation to one another at the measurement point. 5. The method as claimed in claim 1 , characterized in that the electromagnetic ultrasound transducers are used at multiple measurement points distributed over an external surface.
using the magnetostrictive properties of the material to be examined, e.g. electromagnetic acoustic transducers [EMAT]; (investigating the presence of flaws using eddy currents G01N27/90, magnetostrictive transducers B06B1/08, measuring magnetostrictive properties G01R33/18) · CPC title
by measuring propagation velocity or propagation time of acoustic waves · CPC title
Fatigue, creep, strain-stress relations or elastic constants · CPC title
Elastic parameters, strength or force · CPC title
of elongated objects, e.g. pipes, masts, towers or railways (G01M5/0058 takes precedence) · CPC title
Related publications grouped by family.
Answers are generated from the same data shown on this page.