Literature DB >> 30533468

Dataset on reflection and transmission coefficients of ultrasonic shear horizontal guided waves in plates with wall thinning.

Alan C Kubrusly1, Miguel A Freitas1, Jean Pierre von der Weid1, Steve Dixon2.   

Abstract

This data article reports the data for reflection and transmission coefficients of the SH0 and SH1 ultrasonic guided waves modes due to their interaction with tapered wall thinning in aluminium plates. Several thinning depths and edge taper angles were machined, at the total of 35 different samples. Periodic permanent magnet array electromagnet acoustic transducers were used to generate and receive the waves. Both modes were individually generated and separated in the received signal by means of effective post-processing technique. Reflection and transmission coefficients were calculated at both the leading and trailing edges of the thinning region for mode-converted and non-mode converted signals; therefore, eight coefficients were calculated for each generated mode, at the total of sixteen coefficients for each sample. Additional finite-element model was used in order to obtain numerical values for the coefficients. These data were used in order to analyze the interaction of the SH0 and SH1 modes with wall thinning and the capabilities of using them in non-destructive evaluation of corrosion-like defects in the research paper entitled "Interaction of SH guided waves with wall thinning" (Kubrusly et al., 2019).

Entities:  

Year:  2018        PMID: 30533468      PMCID: PMC6265498          DOI: 10.1016/j.dib.2018.11.053

Source DB:  PubMed          Journal:  Data Brief        ISSN: 2352-3409


Specifications table Value of the data The data allow investigation on the interaction of the SH0 and SH1 guided wave modes with thinning regions that simulate wall loss due to corrosion in metallic plates, which is important for non-destructive tests of plates and pipes. Up to now, detailed experimental data on the reflection and transmission coefficients for mode-converted and non-mode converted waves of the SH0 and SH1 guided wave modes were not reported. The data allow one to address the capabilities and limitation on the use of ultrasonic SH guided wave to estimate and detect wall thinning. The data can be used for developing and evaluating novel techniques in order to assess the amount and severity of wall loss by means of reflected and transmitted SH guided waves.

Data

The dataset within this data article provides the reflection and transmission coefficients of shear horizontal (SH) guided wave modes at both the leading and trailing edges of linearly tapered thinning regions. Each experimental sample had a different thinning depth and taper angle, 35 different samples were machined and experimentally analyzed. Coefficients for reflection at the leading edge, transmission to the thinning region, reflection at the trailing edge, and transmission out of the thinning region, were calculated. Either the SH0 or SH1 modes were individually generated; both modes were received in each generation case for each coefficient in order to obtain data on mode-converted and non-mode converted waves, therefore giving rise to a total of 16 different coefficients for each sample. Additional numerical data were obtained by means of a finite-element model for a wider collection of thinning geometry. The coefficient data are reported in Table 1, Table 2, Table 3, Table 4, Table 5, Table 6, Table 7, Table 8 and in Table 9, Table 10, Table 11, Table 12, Table 13, Table 14, Table 15, Table 16, for generation of the SH0 and SH1 mode, respectively.
Table 1

R00 coefficient.

Taper angle (degree)
9065554535302510
Relative depth (%)0FEM0.00540.00540.00540.00540.00540.00540.00540.0054
Exp.0.03420.03420.03420.03420.03420.03420.03420.0342
12.5FEM0.09380.08500.07940.07830.07280.06480.06190.0122
Exp.0.08320.07830.08180.0280
25FEM0.22660.18950.17350.15110.11220.08110.04170.0243
Exp.0.20540.17280.13730.0269
37FEM0.37890.32870.29410.24690.19220.17360.16840.0165
Exp.0.32590.28050.22650.0354
50FEM0.51040.46090.39800.31520.19410.14780.12030.0379
Exp.0.46600.34630.30010.0585
62.5FEM0.62100.53550.40580.25580.13780.14390.15870.0447
Exp.0.55670.32110.24100.0648
75FEM0.72430.56150.33730.19520.23580.19040.07450.0320
Exp.0.67020.24700.20030.18360.16280.08880.0794
87.5FEM0.84500.45150.26280.39550.23810.05420.23580.0557
Exp.0.75240.40220.31360.28930.09470.19370.0843
Table 2

R01 coefficient.

Taper angle (degree)
9065554535302510
Relative depth (%)0FEM0.00000.00000.00000.00000.00000.00000.00000.0000
Exp.0.02230.02230.02230.02230.02230.02230.02230.0223
12.5FEM0.13110.11940.11260.11220.10410.09500.09250.0083
Exp.0.10190.09360.09830.0215
25FEM0.29930.25510.23790.21360.17150.13570.08600.0324
Exp.0.25520.21650.17210.0294
37FEM0.45950.41870.39200.35590.29470.26690.26800.0883
Exp.0.37470.35630.28030.0773
50FEM0.49990.47190.45890.45670.41240.36720.35100.1246
Exp.0.43310.42070.36990.1143
62.5FEM0.46930.47120.49610.48960.38850.31640.28360.1211
Exp.0.39020.44950.40820.1213
75FEM0.39170.50670.56600.49890.32340.28760.30880.1255
Exp.0.34040.49280.41430.27510.23030.23740.1211
87.5FEM0.25530.64350.62160.38040.37100.35360.26130.1320
Exp.0.24080.59040.46540.34940.31170.20370.1219
Table 3

T00 coefficient.

Taper angle (degree)
9065554535302510
Relative depth (%)0FEM0.99970.99970.99970.99970.99970.99970.99970.9997
Exp.0.99180.99180.99180.99180.99180.99180.99180.9918
12.5FEM0.98170.98390.98550.98540.98680.98810.98930.9945
Exp.0.96270.98510.98070.9871
25FEM0.90990.93260.93950.94720.95790.96380.96950.9796
Exp.0.90920.90880.92050.9670
37FEM0.79570.83280.85210.87270.89540.90510.91240.9867
Exp.0.79770.82690.87090.9667
50FEM0.69920.74670.78690.83260.89150.91620.93310.9918
Exp.0.70470.76920.81050.9574
62.5FEM0.62760.69690.76070.83040.91090.93840.95050.9912
Exp.0.63060.74370.79990.9575
75FEM0.56770.65010.74380.83950.91930.93740.95330.9917
Exp.0.54200.71550.76990.86490.82100.82920.9459
87.5FEM0.47330.60990.72770.83710.89640.93270.94040.9900
Exp.0.40660.54500.65790.72880.76400.77870.8235
Table 4

T01 coefficient.

Taper angle (degree)
9065554535302510
Relative depth (%)0FEM0.00000.00000.00000.00000.00000.00000.00000.0000
Exp.0.04860.04860.04860.04860.04860.04860.04860.0486
12.5FEM0.06570.06240.05960.06160.06010.06010.05960.0630
Exp.0.11860.08570.10970.0922
25FEM0.07130.06940.07060.07340.07760.08160.08620.0748
Exp.0.09060.08550.09610.0812
37FEM0.03330.03610.04440.05730.06430.06450.06110.0368
Exp.0.04240.04540.03770.0522
50FEM0.00450.00400.00340.00270.00210.00200.00170.0007
Exp.0.02590.02070.03050.0445
62.5FEM0.00000.00010.00010.00000.00000.00000.00000.0000
Exp.0.03330.04230.04710.0442
75FEM0.00010.00000.00000.00000.00000.00000.00000.0000
Exp.0.03060.05520.05860.10270.06440.06970.0672
87.5FEM0.00000.00000.00000.00000.00000.00000.00000.0000
Exp.0.04620.04370.10010.08130.05550.07150.1109
Table 5

TR00 coefficient.

Taper angle (degree)
9065554535302510
Relative depth (%)0FEM0.00280.00280.00280.00280.00280.00280.00280.0028
Exp.0.01900.01900.01900.01900.01900.01900.01900.0190
12.5FEM0.06220.05390.05330.05060.04710.04520.03990.0116
Exp.0.05790.04970.05330.0221
25FEM0.08540.07550.06740.05390.03230.02370.01060.0188
Exp.0.08880.05140.05170.0234
37FEM0.04510.03050.02010.02020.02750.03660.04190.0216
Exp.0.04830.04240.03670.0374
50FEM0.02530.02070.03240.04810.06300.05580.02230.0264
Exp.0.04240.05490.04800.0439
62.5FEM0.04620.07490.09170.09870.05410.03250.07090.0225
Exp.0.06160.09610.09280.0484
75FEM0.12140.14950.16610.12630.07870.13010.06340.0279
Exp.0.12290.14100.09580.06840.08970.06940.0552
87.5FEM0.23180.25570.20800.18390.21180.15910.17600.0709
Exp.0.17650.18340.13850.08650.08630.13270.0462
Table 6

TR01 coefficient.

Taper angle (degree)
9065554535302510
Relative depth (%)0FEM0.00000.00000.00000.00000.00000.00000.00000.0000
Exp.0.04090.04090.04090.04090.04090.04090.04090.0409
12.5FEM0.06880.06030.05900.05680.05390.05140.04680.0080
Exp.0.06880.08190.06550.0150
25FEM0.08550.07750.07020.05840.04280.03350.02080.0141
Exp.0.08440.05490.06020.0346
37FEM
Exp.
50FEM
Exp.
62.5FEM
Exp.
75FEM
Exp.
87.5FEM
Exp.
Table 7

TT00 coefficient.

Taper angle (degree)
9065554535302510
Relative depth (%)0FEM0.99990.99990.99990.99990.99990.99990.99990.9999
Exp.1.02181.02181.02181.02181.02181.02181.02181.0218
12.5FEM0.96360.97040.97140.97290.97500.97690.97900.9903
Exp.0.98401.00851.01001.0062
25FEM0.82800.86460.87960.89800.91790.92820.93900.9575
Exp.0.85230.88320.91680.9768
37FEM0.63270.69560.72890.76320.80210.82020.83260.9729
Exp.0.65460.73300.79780.9656
50FEM0.48850.56380.62050.70170.79470.83970.87410.9822
Exp.0.51710.65070.73240.9780
62.5FEM0.39420.48190.57480.69860.82970.88120.90550.9835
Exp.0.40970.61960.70130.9888
75FEM0.32230.42590.55240.71200.84420.87710.91020.9824
Exp.0.32320.61930.71440.84460.86460.90940.9745
87.5FEM0.22430.36990.53310.70490.80350.86880.88490.9778
Exp.0.24490.38370.62990.72670.90130.89580.9882
Table 8

TT01 coefficient.

Taper angle (degree)
9065554535302510
Relative depth (%)0FEM0.00000.00000.00000.00000.00000.00000.00000.0000
Exp.0.04580.04580.04580.04580.04580.04580.04580.0458
12.5FEM0.13070.12760.13050.12580.12530.12630.12210.1115
Exp.0.10000.19200.14320.0968
25FEM0.31520.29120.27840.25980.25190.24730.24160.2248
Exp.0.34290.25990.27390.2321
37FEM0.46220.44110.42780.41300.39210.37790.37170.1643
Exp.0.44690.40820.41670.2004
50FEM0.49320.48400.47800.44300.39880.36320.32970.1288
Exp.0.50960.43290.43920.1642
62.5FEM0.47960.49040.48260.43440.37230.32380.28190.1272
Exp.0.50140.42480.43100.1753
75FEM0.44150.45920.46390.42420.35480.30360.27770.1273
Exp.0.45770.41930.42560.33870.32030.26190.1652
87.5FEM0.33960.40540.44330.41360.33540.30130.27030.1269
Exp.0.35950.39750.40220.40610.26470.27490.1585
Table 9

R11 coefficient.

Taper angle (degree)
9065554535302510
Relative depth (%)0FEM0.00930.00930.00930.00930.00930.00930.00930.0093
Exp.0.01870.01870.01870.01870.01870.01870.01870.0187
12.5FEM0.21040.17910.17600.16750.15200.13840.12240.0192
Exp.0.17160.15720.15210.0263
25FEM0.44840.35230.30710.25390.17690.12180.06280.0277
Exp.0.39640.26700.22880.0222
37FEM0.52540.40550.33250.22950.09180.11640.17790.1222
Exp.0.47620.30540.23010.0762
50FEM0.52610.52350.50040.52610.58270.61940.69490.9014
Exp.0.49270.50670.40840.6858
62.5FEM0.48010.49680.51790.50950.61670.70790.84740.9786
Exp.0.44440.50720.44490.7662
75FEM0.55120.43690.46860.52750.69270.77620.85620.9794
Exp.0.53410.48420.47780.60590.64620.73370.7579
87.5FEM0.71930.27090.48390.65660.70450.72410.87700.9772
Exp.0.63380.25660.56520.56450.64320.72610.7516
Table 10

R10 coefficient.

Taper angle (degree)
9065554535302510
Relative depth (%)0FEM0.00000.00000.00000.00000.00000.00000.00000.0000
Exp.0.00800.00800.00800.00800.00800.00800.00800.0080
12.5FEM0.06810.05770.05680.05370.04830.04330.03750.0091
Exp.0.03920.03990.03810.0072
25FEM0.15980.12350.10710.08580.05530.03290.01360.0160
Exp.0.09750.06790.05700.0132
37FEM0.20870.15380.12210.07880.04100.06460.07960.0218
Exp.0.13260.08750.05930.0178
50FEM0.22980.20230.19000.20070.20760.21300.19960.0435
Exp.0.15300.13420.10690.0717
62.5FEM0.21460.20660.20760.20600.22160.21630.17570.0713
Exp.0.13280.15820.13230.0994
75FEM0.17400.22460.23800.22000.19720.18450.17770.0702
Exp.0.10520.18130.14370.14690.13320.13990.0869
87.5FEM0.10890.28120.24560.16930.19580.22840.15450.0767
Exp.0.05820.20690.15600.11820.15550.11640.0886
Table 11

T11 coefficient.

Taper angle (degree)
9065554535302510
Relative depth (%)0FEM1.01231.01231.01231.01231.01231.01231.01231.0123
Exp.0.96170.96170.96170.96170.96170.96170.96170.9617
12.5FEM0.94260.95880.95960.96250.96840.97220.97610.9894
Exp.0.91530.94100.91920.9463
25FEM0.51910.62740.66140.69030.71950.73210.73790.7449
Exp.0.49530.56320.62680.6685
37FEM0.08250.14470.16320.17810.18550.18580.18630.2092
Exp.0.10000.17340.17850.2182
50FEM0.00600.01570.01830.02020.02150.02290.02640.0354
Exp.0.01490.01050.02330.0221
62.5FEM0.00000.00000.00000.00000.00000.00000.00000.0000
Exp.0.02110.01450.01930.0059
75FEM0.00000.00000.00000.00000.00000.00000.00000.0000
Exp.0.02060.01960.02170.02230.01300.01140.0077
87.5FEM0.00000.00000.00000.00000.00000.00000.00000.0000
Exp.0.02720.02270.02590.02350.00980.01030.0106
Table 12

T10 coefficient.

Taper angle (degree)
9065554535302510
Relative depth (%)0FEM0.00180.00180.00180.00180.00180.00180.00180.0018
Exp.0.05630.05630.05630.05630.05630.05630.05630.0563
12.5FEM0.07270.06340.06280.06150.05790.05650.05490.0494
Exp.0.09890.07920.09100.0717
25FEM0.18500.15160.13960.13060.11870.11510.11190.0979
Exp.0.14950.09950.11220.0790
37FEM0.26730.22710.21350.20630.19630.19580.19090.1133
Exp.0.22670.16890.18110.1023
50FEM0.31830.30270.29030.28630.27560.26350.23180.0510
Exp.0.29360.21860.24760.0811
62.5FEM0.34260.33790.31790.30000.26270.23540.18530.0722
Exp.0.30330.21770.24380.0730
75FEM0.33950.34500.31630.28730.24080.21820.17600.0715
Exp.0.29080.20210.22320.17090.14050.11220.0695
87.5FEM0.30010.33710.30860.27160.23760.21470.17610.0717
Exp.0.21260.21260.16070.18390.12450.10230.0562
Table 13

TR11 coefficient.

Taper angle (degree)
9065554535302510
Relative depth (%)0FEM0.01210.01210.01210.01210.01210.01210.01210.0121
Exp.0.03160.03160.03160.03160.03160.03160.03160.0316
12.5FEM0.22300.20230.20230.18700.17130.15260.14430.0328
Exp.0.18740.16880.16920.0232
25FEM0.28710.27020.23870.21030.13740.08850.04120.0403
Exp.0.25420.20070.17010.0409
37FEM0.05220.05880.05620.06190.07440.07090.05910.0549
Exp.0.05320.08480.05660.0612
50FEM
Exp.
62.5FEM
Exp.
75FEM
Exp.
87.5FEM
Exp.
Table 14

TR10 coefficient.

Taper angle (degree)
9065554535302510
Relative depth (%)0FEM0.00000.00000.00000.00000.00000.00000.00000.0000
Exp.0.01280.01280.01280.01280.01280.01280.01280.0128
12.5FEM0.05890.05310.05270.04780.04390.03880.03610.0108
Exp.0.05390.04020.04620.0135
25FEM0.08750.07760.06670.05610.03300.01760.00960.0149
Exp.0.07790.05760.04220.0124
37FEM0.03950.04320.03170.01600.02500.03130.03020.0148
Exp.0.03180.02780.01850.0179
50FEM0.01370.01580.01620.01790.01270.00920.01080.0090
Exp.0.02670.02450.02520.0153
62.5FEM0.04130.04620.03980.02490.01250.01730.01140.0062
Exp.0.03230.02350.02030.0105
75FEM0.11670.08410.04940.02400.02920.01960.01310.0072
Exp.0.08550.02360.01730.02400.01700.01070.0108
87.5FEM0.17910.08490.06630.06480.04390.03500.02540.0102
Exp.0.10250.06090.02400.03530.01760.02160.0088
Table 15

TT10 coefficient.

Taper angle (degree)
9065554535302510
Relative depth (%)0FEM0.00180.00180.00180.00180.00180.00180.00180.0018
Exp.0.01930.01930.01930.01930.01930.01930.01930.0193
12.5FEM0.09210.08450.08460.08310.08020.07950.07950.0825
Exp.0.07700.05190.07550.0585
25FEM0.15940.13750.12910.12200.11180.11540.11790.0996
Exp.0.13830.09890.11630.0810
37FEM0.20700.19260.18600.18310.17550.17500.17140.1094
Exp.0.17550.14900.16490.0956
50FEM0.23070.22860.22440.22020.21870.21610.20120.0510
Exp.0.20970.17490.20090.0827
62.5FEM0.22320.22380.21920.21460.21160.20160.17070.0716
Exp.0.19420.16960.18930.0715
75FEM0.18840.20100.21200.21020.20030.19190.16340.0710
Exp.0.16280.17020.18560.16250.15130.12900.0679
87.5FEM0.13160.19440.20970.19420.19750.18660.16320.0710
Exp.0.11940.14950.15430.16090.14000.12180.0674
Table 16

TT11 coefficient.

Taper angle (degree)
9065554535302510
Relative depth (%)0FEM1.01981.01981.01981.01981.01981.01981.01981.0198
Exp.0.98680.98680.98680.98680.98680.98680.98680.9868
12.5FEM0.92070.94540.94430.94980.96170.97030.97520.9985
Exp.0.92270.94600.93610.9790
25FEM0.50010.68310.75450.80510.87510.90210.91740.9411
Exp.0.51630.72940.78820.9366
37FEM0.33380.39370.48880.56590.59830.59050.58340.7127
Exp.0.30720.42940.53540.6460
50FEM0.48680.44300.41740.41370.38480.34120.26150.0106
Exp.0.49390.37600.39480.0234
62.5FEM0.56260.55820.51030.46750.36230.27670.16570.0242
Exp.0.56750.41870.44100.0421
75FEM0.54290.58310.50840.42960.30950.23870.14830.0238
Exp.0.54020.40870.43160.28970.22420.13790.0381
87.5FEM0.41540.57170.48200.37880.30090.23020.14930.0238
Exp.0.45700.53750.39920.38860.18460.13090.0369
R00 coefficient. R01 coefficient. T00 coefficient. T01 coefficient. TR00 coefficient. TR01 coefficient. TT00 coefficient. TT01 coefficient. R11 coefficient. R10 coefficient. T11 coefficient. T10 coefficient. TR11 coefficient. TR10 coefficient. TT10 coefficient. TT11 coefficient.

Experimental design, materials and methods

Aluminium plates were used as test samples with dimension of 8 mm thick, 800 mm long and 250 mm wide. A tapered thinner section was machined in each sample starting at position  = 182 mm with a total length of  = 150 mm, several different depths, d, and edge angles, α, of the thinned region were machined in order to analyze the coefficients as a function of d and α. Specimens were prepared at edge angles of 10°, 45°, 55°, and 90°; for each of these angles, depths from 1 mm down to 7 mm were machined in 1 mm step. Additional specimens were prepared with 6 mm and 7 mm depth at edge angles of 25°, 30° and 35° and 25°, 30° and 65°, respectively. Therefore, a total of 34 samples were machined plus one non-machined reference sample, all of which were experimentally evaluated. Fig. 1 shows the sample and machined thinning region drawing with dimension and Fig. 2 shows one machined test sample.
Fig. 1

Plate dimension with a machined section. Marked positions denote the origin O, where transmitter is positioned, and receiver positions before the thinning region (1), in the middle of the region (2) and after the region (3).

Fig. 2

Machined plate at 45° edges and 4 mm depth.

Plate dimension with a machined section. Marked positions denote the origin O, where transmitter is positioned, and receiver positions before the thinning region (1), in the middle of the region (2) and after the region (3). Machined plate at 45° edges and 4 mm depth. The machined samples were experimentally evaluated using a RITEC ® RPR-4000 Pulser/Receiver and periodic permanent magnet array electromagnet acoustic transducers (PPM EMATs) from Sonemat Ltd. (3cycle, 10 mm nominal wavelength) as transmitter and receiver. PPM EMATs are able to generate shear horizontal guided waves in metallic plates [2]. In order to generate either the SH0 or the SH1 mode an 8 cycle tone burst at 311 kHz or 367 kHz, respectively, were applied to the transmitter PPM EMAT according to dispersion curve of each mode [1]. Dual excitation and reception on both plate׳s surfaces was adopted in order to ensure that a single mode was generated and then to separate the two possible received modes due to mode conversion. Details on the dual transduction procedure and experimental setup are described in Refs. [3] and [1], respectively. Transmitters were placed at position O whereas receiver was positioned at positions (1), (2) or (3), see Fig. 1, in order to receive signals before, at and after the thinning region, respectively. Signals acquired by the oscilloscope were averaged in order to diminish the noise level, also a digital low-pass filter at 400 kHz 3 dB cut-off frequency was applied to the raw signals. Signals acquired at both surfaces were combined following [3] in order to separate mode-converted and non-mode converted signals for each generation. Four coefficients were calculated, namely R, T, TR, TT, which denote the reflection at the thinning region leading edge, transmission to the region, reflection at the thinning region trailing edge, and transmission out of the far end of the region, respectively. The first subscript, i, denotes the generated mode, whereas the second one, j, denotes the received mode. Either i or j can be 0 or 1, here, corresponding to the SH0 or SH1 modes, respectively. These coefficients are defined by:where A is the peak-to-peak of the received signal inside a time gate in which the mode is expected to arrive, the superscripts + and – mean the forward and backward propagating waves, and (1), (2) and (3) indicate the reading positions according to Fig. 1. All coefficients are related to the incident wave, . Since the wave amplitude is increased when it is transmitted to a thinner region, due to the energy distribution across the thickness, it is necessary to include the square root in Eq. (1b) and (1c) in order to compensate it, where is the plate׳s original thickness, and therefore is the remaining thickness in the thinner region. The time gate to select the amplitude of the incident mode before the thinning region, starts and ends, respectively at:where is the longitudinal coordinate of position (1), is the group velocity of the generated mode, , at its working frequency, , is the number of cycles used in the exciting signal and is a time margin which ensures that the whole signal is included in the time gate, empirically . The group velocities for the SH0 and SH1 modes in an 8 mm aluminium plate are 3111 m/s and 2428 m/s, respectively at 311 kHz and 367 kHz. The time gates to select the other amplitudes, namely, , , and due to the incident mode , start and end instants are, respectively:where is the group velocity of the received mode, , is the group velocity within the thinning region. It is necessary to consider velocity change at the thinning region because the SH1 mode is dispersive and its velocity is a function of the plate׳s thickness [4]. The minimum and maximum of the two possible modes within the thinner region length, in Eqs. (5a), (5b), (6a), (6b), is considered because, at first, both modes can propagate in the thinning region due to mode conversion of any incident mode at the leading edge, and the coefficients TR and TT consider the two possible modes, SH0 or SH1, propagating inside the thinning region. This, however, only holds when the region remaining thickness is above the SH1 mode cut-off thickness. Otherwise, its group velocity is not defined and this mode cannot propagate inside the thinning. Thus, either or should read in this case, since the group velocity for the non-dispersive SH0 mode is constant for any thickness. Also, in this case, a time gate for T or TR cannot be defined, therefore no time gate restriction was applied and the whole SH1 signal on the region is considered to calculate the T coefficient, whereas TR is not calculated in this case. Prior to calculating the experimental reflection and transmission coefficients, it is necessary to compensate for attenuation. The experimental attenuation of the guided wave modes was calculated by receiving the SH0 and SH1 signals in several positions in a non-machined sample and fitting the peak-to-peak of the signals versus the position with an exponential decay curve. The exponential coefficient was then used to compensate the values of the amplitudes, , , and of the received signals considering the forward and backward propagating path at each position. Finally, the sixteen coefficients were calculated for each thinning depth and taper angle. In addition to experiments, finite-element analysis was also performed using a commercial, time-domain, Finite-Element Method (FEM) solver, PZFlex©, which allows simulation of SH waves in two-dimensional models. The numerical model was executed for thinning depth from 0.5 to 7.5 mm in 0.5 mm step with the following taper angles, 90°, 65°, 55°, 45°, 35°, 30°, 25° and 10°, therefore including all the experimental thinning geometries. Numerical simulation mimicked the PPM EMATs generation by applying forces in surface nodes along the transducer length according to the transducer spatial profile following the procedure used and validated previously [3], [5], whereas reception was done by numerically convolving the wave field on the surface of the model with the probe spatial profile. Then, likewise in the experiments, the dual excitation and reception procedure, filtering and time gating were applied. Therefore numerical and experimental data can be straightforwardly compared. The only procedure which was not included in the numerical data was attenuation compensation since damping was not included in the model. Figs. 3 and 4 show the experimental and numerical coefficients for generation of the SH0 and SH1 mode, respectively. This data not only helps on understanding the interaction of the SH0 and SH1 modes with wall thinning sections but also allows one to address the capabilities and limitation on the use of ultrasonic SH guided wave to estimate and detect wall thinning when both modes are allowed to propagate (see Ref. [1]).
Fig. 3

Coefficients for SH0 generation, obtained experimentally (symbols) and numerically (lines) at 90° edge (a) and (b), 55° (c) and (d), 45° (e) and (f) and 10° (g) and (h).

Fig. 4

Coefficients for SH1 generation, obtained experimentally (symbols) and numerically (lines) at 90° edge (a) and (b), 55° (c) and (d), 45° (e) and (f) and 10° (g) and (h).

Coefficients for SH0 generation, obtained experimentally (symbols) and numerically (lines) at 90° edge (a) and (b), 55° (c) and (d), 45° (e) and (f) and 10° (g) and (h). Coefficients for SH1 generation, obtained experimentally (symbols) and numerically (lines) at 90° edge (a) and (b), 55° (c) and (d), 45° (e) and (f) and 10° (g) and (h).
Subject areaPhysics
More specific subject areaNon-destructive testing, ultrasonic wave propagation
Type of dataTables, Figures
How data were acquiredUltrasonic SH guided wave signals on machined aluminium plates. Ultrasound equipment: RITEC ® RPR-4000 Pulser/Receiver with ultrasound transducers: 10 mm pitch PPM EMATs from Sonemat Ltd.
Additional finite element simulations performed with PZFlex©solver.
Data formatFiltered.
Experimental factorsAluminium plates, 8 mm thick, 800 mm long, 250 mm wide, with machined thinning sections, 150 mm long all width wide, several depths and taper angles.
Experimental featuresUltrasound transducer positioned at the sample surface in specific positions in order to measure reflected and transmitted waves due to interaction with thinning region in the samples.
Data source locationUltrasonics Group, Department of Physics, University of Warwick, Coventry CV4 7AL, United Kingdom.
Data accessibilityData are with this article
Related research articleA. C. Kubrusly, M. A. Freitas, J. P. von der Weid, and S. Dixon, "Interaction of SH guided waves with wall thinning," NDT &E International, 101 (2019), pp. 94–103[1]
  1 in total

1.  Mode Selectivity of SH Guided Waves by Dual Excitation and Reception Applied to Mode Conversion Analysis.

Authors:  Alan C Kubrusly; Miguel A Freitas; Jean Pierre von der Weid; Steve Dixon
Journal:  IEEE Trans Ultrason Ferroelectr Freq Control       Date:  2018-07       Impact factor: 2.725

  1 in total

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