Reconstruction of Lamb Wave Dispersion Curves in Different Objects Using Signals Measured at Two Different Distances

The possibilities of an effective method of two adjacent signals are investigated for the evaluation of Lamb waves phase velocity dispersion in objects of different types, namely polyvinyl chloride (PVC) film and wind turbine blade (WTB). A new algorithm based on peaks of spectrum magnitude is prese...

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Autores principales: Lina Draudvilienė, Olgirdas Tumšys, Renaldas Raišutis
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Publicado: MDPI AG 2021
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spelling oai:doaj.org-article:85b9225f0d6541459afd3248234c7b3b2021-11-25T18:15:30ZReconstruction of Lamb Wave Dispersion Curves in Different Objects Using Signals Measured at Two Different Distances10.3390/ma142269901996-1944https://doaj.org/article/85b9225f0d6541459afd3248234c7b3b2021-11-01T00:00:00Zhttps://www.mdpi.com/1996-1944/14/22/6990https://doaj.org/toc/1996-1944The possibilities of an effective method of two adjacent signals are investigated for the evaluation of Lamb waves phase velocity dispersion in objects of different types, namely polyvinyl chloride (PVC) film and wind turbine blade (WTB). A new algorithm based on peaks of spectrum magnitude is presented and used for the comparison of the results. To use the presented method, the wavelength-dependent parameter is proposed to determine the optimal distance range, which is necessary in selecting two signals for analysis. It is determined that, in the range of 0.17–0.5 wavelength where <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>δ</mi><mrow><msub><mi>c</mi><mrow><mi>p</mi><mi>h</mi></mrow></msub></mrow></msub></mrow></semantics></math></inline-formula> is not higher than 5%, it is appropriate to use in the case of an A<sub>0</sub> mode in PVC film sample. The smallest error of 1.2%, in the distance greater than 1.5 wavelengths, is obtained in the case of the S<sub>0</sub> mode. Using the method of two signals analysis for PVC sample, the phase velocity dispersion curve of the A<sub>0</sub> mode is reconstructed using selected distances <i>x</i><sub>1</sub> = 70 mm and <i>x</i><sub>2</sub> = 70.5 mm between two spatial positions of a receiving transducer with a mean relative error <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>δ</mi><mrow><msub><mi>c</mi><mrow><mi>p</mi><mi>h</mi></mrow></msub></mrow></msub><mo>=</mo><mn>2.8</mn><mo>%</mo></mrow></semantics></math></inline-formula>, and for S<sub>0</sub> mode, <i>x</i><sub>1</sub> = 61 mm and <i>x</i><sub>2</sub> = 79.7 mm with <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>δ</mi><mrow><msub><mi>c</mi><mrow><mi>p</mi><mi>h</mi></mrow></msub></mrow></msub><mo>=</mo><mn>0.99</mn><mo>%</mo></mrow></semantics></math></inline-formula>. In the case of the WTB sample, the range of 0.1–0.39 wavelength, where <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>δ</mi><mrow><msub><mi>c</mi><mrow><mi>p</mi><mi>h</mi></mrow></msub></mrow></msub></mrow></semantics></math></inline-formula> is not higher than 3%, is determined as the optimal distance range between two adjacent signals. The phase velocity dispersion curve of the A<sub>0</sub> mode is reconstructed in two frequency ranges: first, using selected distances <i>x</i><sub>1</sub> = 225 mm and <i>x</i><sub>2</sub> = 231 mm with mean relative error <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>δ</mi><mrow><msub><mi>c</mi><mrow><mi>p</mi><mi>h</mi></mrow></msub></mrow></msub><mo>=</mo><mn>0.3</mn><mo>%</mo></mrow></semantics></math></inline-formula>; and second, <i>x</i><sub>1</sub> = 225 mm and <i>x</i><sub>2</sub> = 237 mm with <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>δ</mi><mrow><msub><mi>c</mi><mrow><mi>p</mi><mi>h</mi></mrow></msub></mrow></msub><mo>=</mo><mn>1.3</mn><mo>%</mo></mrow></semantics></math></inline-formula>.Lina DraudvilienėOlgirdas TumšysRenaldas RaišutisMDPI AGarticleultrasonic Lamb wavenon-destructive testingnon-homogeneous materialsignal processingLamb wave phase velocitydispersion curve reconstructionTechnologyTElectrical engineering. Electronics. Nuclear engineeringTK1-9971Engineering (General). Civil engineering (General)TA1-2040MicroscopyQH201-278.5Descriptive and experimental mechanicsQC120-168.85ENMaterials, Vol 14, Iss 6990, p 6990 (2021)
institution DOAJ
collection DOAJ
language EN
topic ultrasonic Lamb wave
non-destructive testing
non-homogeneous material
signal processing
Lamb wave phase velocity
dispersion curve reconstruction
Technology
T
Electrical engineering. Electronics. Nuclear engineering
TK1-9971
Engineering (General). Civil engineering (General)
TA1-2040
Microscopy
QH201-278.5
Descriptive and experimental mechanics
QC120-168.85
spellingShingle ultrasonic Lamb wave
non-destructive testing
non-homogeneous material
signal processing
Lamb wave phase velocity
dispersion curve reconstruction
Technology
T
Electrical engineering. Electronics. Nuclear engineering
TK1-9971
Engineering (General). Civil engineering (General)
TA1-2040
Microscopy
QH201-278.5
Descriptive and experimental mechanics
QC120-168.85
Lina Draudvilienė
Olgirdas Tumšys
Renaldas Raišutis
Reconstruction of Lamb Wave Dispersion Curves in Different Objects Using Signals Measured at Two Different Distances
description The possibilities of an effective method of two adjacent signals are investigated for the evaluation of Lamb waves phase velocity dispersion in objects of different types, namely polyvinyl chloride (PVC) film and wind turbine blade (WTB). A new algorithm based on peaks of spectrum magnitude is presented and used for the comparison of the results. To use the presented method, the wavelength-dependent parameter is proposed to determine the optimal distance range, which is necessary in selecting two signals for analysis. It is determined that, in the range of 0.17–0.5 wavelength where <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>δ</mi><mrow><msub><mi>c</mi><mrow><mi>p</mi><mi>h</mi></mrow></msub></mrow></msub></mrow></semantics></math></inline-formula> is not higher than 5%, it is appropriate to use in the case of an A<sub>0</sub> mode in PVC film sample. The smallest error of 1.2%, in the distance greater than 1.5 wavelengths, is obtained in the case of the S<sub>0</sub> mode. Using the method of two signals analysis for PVC sample, the phase velocity dispersion curve of the A<sub>0</sub> mode is reconstructed using selected distances <i>x</i><sub>1</sub> = 70 mm and <i>x</i><sub>2</sub> = 70.5 mm between two spatial positions of a receiving transducer with a mean relative error <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>δ</mi><mrow><msub><mi>c</mi><mrow><mi>p</mi><mi>h</mi></mrow></msub></mrow></msub><mo>=</mo><mn>2.8</mn><mo>%</mo></mrow></semantics></math></inline-formula>, and for S<sub>0</sub> mode, <i>x</i><sub>1</sub> = 61 mm and <i>x</i><sub>2</sub> = 79.7 mm with <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>δ</mi><mrow><msub><mi>c</mi><mrow><mi>p</mi><mi>h</mi></mrow></msub></mrow></msub><mo>=</mo><mn>0.99</mn><mo>%</mo></mrow></semantics></math></inline-formula>. In the case of the WTB sample, the range of 0.1–0.39 wavelength, where <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>δ</mi><mrow><msub><mi>c</mi><mrow><mi>p</mi><mi>h</mi></mrow></msub></mrow></msub></mrow></semantics></math></inline-formula> is not higher than 3%, is determined as the optimal distance range between two adjacent signals. The phase velocity dispersion curve of the A<sub>0</sub> mode is reconstructed in two frequency ranges: first, using selected distances <i>x</i><sub>1</sub> = 225 mm and <i>x</i><sub>2</sub> = 231 mm with mean relative error <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>δ</mi><mrow><msub><mi>c</mi><mrow><mi>p</mi><mi>h</mi></mrow></msub></mrow></msub><mo>=</mo><mn>0.3</mn><mo>%</mo></mrow></semantics></math></inline-formula>; and second, <i>x</i><sub>1</sub> = 225 mm and <i>x</i><sub>2</sub> = 237 mm with <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><msub><mi>δ</mi><mrow><msub><mi>c</mi><mrow><mi>p</mi><mi>h</mi></mrow></msub></mrow></msub><mo>=</mo><mn>1.3</mn><mo>%</mo></mrow></semantics></math></inline-formula>.
format article
author Lina Draudvilienė
Olgirdas Tumšys
Renaldas Raišutis
author_facet Lina Draudvilienė
Olgirdas Tumšys
Renaldas Raišutis
author_sort Lina Draudvilienė
title Reconstruction of Lamb Wave Dispersion Curves in Different Objects Using Signals Measured at Two Different Distances
title_short Reconstruction of Lamb Wave Dispersion Curves in Different Objects Using Signals Measured at Two Different Distances
title_full Reconstruction of Lamb Wave Dispersion Curves in Different Objects Using Signals Measured at Two Different Distances
title_fullStr Reconstruction of Lamb Wave Dispersion Curves in Different Objects Using Signals Measured at Two Different Distances
title_full_unstemmed Reconstruction of Lamb Wave Dispersion Curves in Different Objects Using Signals Measured at Two Different Distances
title_sort reconstruction of lamb wave dispersion curves in different objects using signals measured at two different distances
publisher MDPI AG
publishDate 2021
url https://doaj.org/article/85b9225f0d6541459afd3248234c7b3b
work_keys_str_mv AT linadraudviliene reconstructionoflambwavedispersioncurvesindifferentobjectsusingsignalsmeasuredattwodifferentdistances
AT olgirdastumsys reconstructionoflambwavedispersioncurvesindifferentobjectsusingsignalsmeasuredattwodifferentdistances
AT renaldasraisutis reconstructionoflambwavedispersioncurvesindifferentobjectsusingsignalsmeasuredattwodifferentdistances
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