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15 pages, 3492 KiB  
Article
Real-Time Method and Implementation of Head-Wave Extraction for Ultrasonic Imaging While Drilling
by Liangchen Zhang, Junqiang Lu, Jinping Wu, Baiyong Men, Chao Xie, Yanbo Zong, Shubo Yang and Weining Ni
Appl. Sci. 2024, 14(12), 5292; https://doi.org/10.3390/app14125292 - 19 Jun 2024
Viewed by 874
Abstract
Extracting head waves and subsequently uploading their results from the downhole to the surface system in real time could improve the real-time guidance of ultrasonic imaging logging while drilling (UILWD) for drilling operations. To realize the downhole real-time extraction of head waves in [...] Read more.
Extracting head waves and subsequently uploading their results from the downhole to the surface system in real time could improve the real-time guidance of ultrasonic imaging logging while drilling (UILWD) for drilling operations. To realize the downhole real-time extraction of head waves in this logging, three aspects were explored in this study. First, an improved energy ratio head-wave arrival extraction algorithm based on the weighting coefficients and characteristic functions, along with an amplitude detection method relying on peak-to-peak values, was proposed. Second, an echo reception pre-processing analog circuit and a digital signal processing circuit based on FPGA were designed. A pipeline algorithm was developed in FPGA to extract the arrival time and amplitude of the head wave. Finally, software simulations, laboratory tests, and field experiments related to this method were conducted. Our results showed that the real-time head-wave extraction method demonstrated a strong anti-noise ability in real time. The maximum relative error of the arrival time was less than 5%. The relative error of the amplitude was acceptable, and 90% of this value was within 5%. Through the measurement, the time of processing a single-channel waveform by a downhole algorithm was less than 15 ms, thus meeting the requirements for the real-time processing of downholes. Full article
(This article belongs to the Topic Petroleum and Gas Engineering)
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<p>Effect comparison between the STA/LTA and improved STA/LTA methods.</p>
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<p>Diagram of the principal hardware used for head-wave real-time extraction.</p>
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<p>Structure diagram of the analog band-pass filter circuit.</p>
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<p>The calculated parameters of the band-pass filter circuit.</p>
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<p>Composition of the programmable gain amplification module.</p>
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<p>Structure of the front-end control program.</p>
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<p>Calculation flow of digital filtering.</p>
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<p>Program structure of head-wave extraction.</p>
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<p>Simulation results of head-wave extraction: (<b>a</b>) Head wave arrival detection; (<b>b</b>) Head wave amplitude detection; (<b>c</b>) Verification of simulation.</p>
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<p>Actual image and test result of the echo reception pre-processing module. (<b>a</b>) Actual image; (<b>b</b>) Gain at different temperatures.</p>
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<p>Test waveforms at 10 different depth points.</p>
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<p>Verification of the downhole arrival time extraction of the head wave. (<b>a</b>) Channel 1; (<b>b</b>) Channel 2; (<b>c</b>) Channel 3.</p>
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<p>Verification of downhole head-wave amplitude extraction. (<b>a</b>) Channel 1; (<b>b</b>) Channel 2; (<b>c</b>) Channel 3.</p>
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16 pages, 12958 KiB  
Article
Physical Simulation of Ultrasonic Imaging Logging Response
by Junqiang Lu, Jiyong Han, Jinping Wu, Xiaohua Che, Wenxiao Qiao, Jiale Wang and Xu Chen
Sensors 2022, 22(23), 9422; https://doi.org/10.3390/s22239422 - 2 Dec 2022
Cited by 3 | Viewed by 1740
Abstract
Ultrasonic imaging logging can visually identify the location, shape, dip angle and orientation of fractures and holes. The method has not been effectively applied in the field; one of the prime reasons is that the results of physical simulation experiments are insufficient. The [...] Read more.
Ultrasonic imaging logging can visually identify the location, shape, dip angle and orientation of fractures and holes. The method has not been effectively applied in the field; one of the prime reasons is that the results of physical simulation experiments are insufficient. The physical simulation of fracture and hole response in the laboratory can provide a reference for the identification and evaluation of the underground geological structure. In this work, ultrasonic scanning experiments are conducted on a grooved sandstone plate and a simulated borehole and the influence of different fractures and holes on ultrasonic pulse echo is studied. Experimental results show that the combination of ultrasonic echo amplitude imaging and arrival time imaging can be used to identify the fracture location, width, depth and orientation, along with accurately calculating the fracture dip angle. The evaluated fracture parameters are similar to those in the physical simulation model. The identification accuracy of the ultrasonic measurement is related to the diameter of the radiation beam of the ultrasonic transducer. A single fracture with width larger than or equal to the radiation beam diameter of the ultrasonic transducer and multiple fractures with spacing longer than or equal to the radiation beam diameter can be effectively identified. Full article
(This article belongs to the Topic Pipeline and Underground Space Technology)
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<p>Schematic of the experimental equipment.</p>
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<p>Time−domain waveform of the excitation signal.</p>
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<p>Photo of the ultrasonic transducer for physical simulation.</p>
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<p>Schematic of the spatial distribution in the radiated acoustic field experiment.</p>
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<p>Spatial distribution of the radiated acoustic field perpendicular to the radiation surface of the ultrasonic transducer.</p>
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<p>Diagram of distance d between the radiating surface of the ultrasonic transducer and the reflector plate.</p>
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<p>Reflector samples. (<b>a</b>) Grooved sandstone Plate 1 and (<b>b</b>) Grooved sandstone Plate 2.</p>
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<p>Fracture simulated borehole and its unfolded drawing. (<b>a</b>) Physical diagram of the simulated borehole and (<b>b</b>) Unfolded drawing of the borehole wall.</p>
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<p>Schematic of the measurement method of slotted sandstone plate.</p>
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<p>Schematic of the measurement method of the simulated borehole. (<b>a</b>) Schematic of the position of the transducer in the experimental measurement and (<b>b</b>) Schematic of the moving track of the ultrasonic transducer, unfolded drawing along the inner wall of the borehole.</p>
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<p>Measurement waveforms at the same height of grooved sandstone Plate 1.</p>
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<p>Measurement waveforms at the same height of grooved sandstone Plate 2.</p>
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<p>Schematic of the ultrasonic transducer scanning a fracture.</p>
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<p>Arriving point extraction of reflected echo waveforms.</p>
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<p>Echo amplitudes and arrival times for grooved sandstone Plate 1.</p>
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<p>Echo amplitudes and arrival times for grooved sandstone Plate 2.</p>
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<p>Echo amplitude imaging diagram for the grooved sandstone Plate 1.</p>
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<p>Echo amplitude imaging diagram for the grooved sandstone Plate 2.</p>
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<p>Echo arrival time imaging diagram for grooved sandstone Plate 1.</p>
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<p>Echo arrival time imaging diagram for grooved sandstone Plate 2.</p>
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<p>Circumferential echo waveforms for vertical fracture at the same height.</p>
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<p>Echo arrival time of vertical fracture.</p>
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<p>Echo amplitude of vertical fracture.</p>
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<p>Echo arrival time imaging for the simulated borehole.</p>
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<p>Echo amplitude imaging for the simulated borehole.</p>
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<p>Schematic for the calculation of dip angle of oblique fracture. (<b>a</b>) Side expanded view of oblique fracture. (<b>b</b>) Projection of oblique fracture on the horizontal plane.</p>
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<p>Echo amplitude imaging of oblique fractures and holes.</p>
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19 pages, 4456 KiB  
Article
Automated Real-Time Eddy Current Array Inspection of Nuclear Assets
by Euan Alexander Foster, Gary Bolton, Robert Bernard, Martin McInnes, Shaun McKnight, Ewan Nicolson, Charalampos Loukas, Momchil Vasilev, Dave Lines, Ehsan Mohseni, Anthony Gachagan, Gareth Pierce and Charles N. Macleod
Sensors 2022, 22(16), 6036; https://doi.org/10.3390/s22166036 - 12 Aug 2022
Cited by 13 | Viewed by 4040
Abstract
Inspection of components with surface discontinuities is an area that volumetric Non-Destructive Testing (NDT) methods, such as ultrasonic and radiographic, struggle in detection and characterisation. This coupled with the industrial desire to detect surface-breaking defects of components at the point of manufacture and/or [...] Read more.
Inspection of components with surface discontinuities is an area that volumetric Non-Destructive Testing (NDT) methods, such as ultrasonic and radiographic, struggle in detection and characterisation. This coupled with the industrial desire to detect surface-breaking defects of components at the point of manufacture and/or maintenance, to increase design lifetime and further embed sustainability in their business models, is driving the increased adoption of Eddy Current Testing (ECT). Moreover, as businesses move toward Industry 4.0, demand for robotic delivery of NDT has grown. In this work, the authors present the novel implementation and use of a flexible robotic cell to deliver an eddy current array to inspect stress corrosion cracking on a nuclear canister made from 1.4404 stainless steel. Three 180-degree scans at different heights on one side of the canister were performed, and the acquired impedance data were vertically stitched together to show the full extent of the cracking. Axial and transversal datasets, corresponding to the transmit/receive coil configurations of the array elements, were simultaneously acquired at transmission frequencies 250, 300, 400, and 450 kHz and allowed for the generation of several impedance C-scan images. The variation in the lift-off of the eddy current array was innovatively minimised through the use of a force–torque sensor, a padded flexible ECT array and a PI control system. Through the use of bespoke software, the impedance data were logged in real-time (7 ms), displayed to the user, saved to a binary file, and flexibly post-processed via phase-rotation and mixing of the impedance data of different frequency and coil configuration channels. Phase rotation alone demonstrated an average increase in Signal to Noise Ratio (SNR) of 4.53 decibels across all datasets acquired, while a selective sum and average mixing technique was shown to increase the SNR by an average of 1.19 decibels. The results show how robotic delivery of eddy current arrays, and innovative post-processing, can allow for repeatable and flexible surface inspection, suitable for the challenges faced in many quality-focused industries. Full article
(This article belongs to the Special Issue Robotic Non-destructive Testing)
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<p>Eddy current inspection hardware.</p>
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<p>Canisters with a matrix of 16 stress corrosion cracks. Depositions of 5 µL droplets of sea water, 3.03 g/L of MgCl2, 15.2 g/L of MgCl2 and 30.03 g/L of MgCl2 were used to induce the cracks in the top row, left, central and right columns, respectively.</p>
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<p>Eddy current array transmit and receive configurations. (<b>a</b>) Generic Eddy current array layout with two vertical columns of coils. (<b>b</b>) Axial transmit and receive configuration where <b><span style="color:#0070C0">x </span></b><span style="color:#0070C0">(<b>in blue</b>) </span>corresponds to the transmit/receive pair centres of the excited eddy current channels in the test part. (<b>c</b>) Transversal transmit and receive configuration where <b><span style="color:#00B050">x </span></b><span style="color:#00B050">(<b>in green</b>) </span>corresponds to the transmit/receive pair centres of the excited eddy currents in the test part resulting from the first/odd column of coils, and where <b><span style="color:#ED7D31">x </span></b><span style="color:#ED7D31">(<b>in orange</b>) </span>corresponds to the transmit/receive pair centres of the excited eddy currents in the test part resulting from the second/even column of coils.</p>
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<p>Illustration of complex impedance data positional compensation performed between axial and transversal configurations. (<b>a</b>) Axial complex array positional compensation. (<b>b</b>) Transversal complex array positional compensation.</p>
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<p>A flow chart showing the data transfer between different software and hardware elements.</p>
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<p>Illustration of the multi-threaded C and LabVIEW programs.</p>
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<p>Illustration of mixing datasets <math display="inline"><semantics> <mrow> <msub> <mi>Z</mi> <mn>1</mn> </msub> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mi>Z</mi> <mn>2</mn> </msub> </mrow> </semantics></math> impedance data to make <math display="inline"><semantics> <mrow> <msub> <mi>Z</mi> <mi>m</mi> </msub> </mrow> </semantics></math> mixed data.</p>
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<p>Axial vertical impedance component C−scan images at 250, 300, 400, and 450 kHz on a dB scale alongside impedance plane plots of the response from the highlighted defect.</p>
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<p>SNR vs. Angle of phase rotation for the axial dataset acquired at 250 kHz.</p>
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<p>Phase-rotated axial vertical impedance component C−scan images at 250,300,400 and 450 kHz on a dB scale alongside impedance plane plots of the response from the highlighted defect.</p>
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<p>Mixed vertical impedance component C−scan.</p>
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<p>Photo of crack matrix and micrograph (<b>a</b>) Photo of crack matrix with the defect of interest highlighted in a red circle. (<b>b</b>) Micrograph of the defect of interest at 96× zoom with desaturated background.</p>
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19 pages, 911 KiB  
Article
Automatic Estimation of Food Intake Amount Using Visual and Ultrasonic Signals
by Ki-Seung Lee
Electronics 2021, 10(17), 2153; https://doi.org/10.3390/electronics10172153 - 3 Sep 2021
Cited by 7 | Viewed by 2581
Abstract
The continuous monitoring and recording of food intake amount without user intervention is very useful in the prevention of obesity and metabolic diseases. I adopted a technique that automatically recognizes food intake amount by combining the identification of food types through image recognition [...] Read more.
The continuous monitoring and recording of food intake amount without user intervention is very useful in the prevention of obesity and metabolic diseases. I adopted a technique that automatically recognizes food intake amount by combining the identification of food types through image recognition and a technique that uses acoustic modality to recognize chewing events. The accuracy of using audio signal to detect eating activity is seriously degraded in a noisy environment. To alleviate this problem, contact sensing methods have conventionally been adopted, wherein sensors are attached to the face or neck region to reduce external noise. Such sensing methods, however, cause dermatological discomfort and a feeling of cosmetic unnaturalness for most users. In this study, a noise-robust and non-contact sensing method was employed, wherein ultrasonic Doppler shifts were used to detect chewing events. The experimental results showed that the mean absolute percentage errors (MAPEs) of an ultrasonic-based method were comparable with those of the audio-based method (15.3 vs. 14.6) when 30 food items were used for experiments. The food intake amounts were estimated for eight subjects in several noisy environments (cafeterias, restaurants, and home dining rooms). For all subjects, the estimation accuracy of the ultrasonic method was not degraded (the average MAPE was 15.02) even under noisy conditions. These results show that the proposed method has the potential to replace the manual logging method. Full article
(This article belongs to the Special Issue Ultrasonic Pattern Recognition by Machine Learning)
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<p>Developed sensor device.</p>
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<p>Block diagram of the developed sensor device.</p>
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<p>A photograph of a subject equipped with the developed sensor device.</p>
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<p>An example of signals received from the sensor device when cashew nuts were eaten. <b>Top</b>: The bandpass filtered signal. <b>Middle</b>: Demodulated signal. <b>Bottom</b>: Audio signal obtained by the low-pass filter.</p>
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<p>An example of signals received from the sensor device when pizza was eaten. <b>Top</b>: The bandpass filtered signal. <b>Middle</b>: Demodulated signal. <b>Bottom</b>: Audio signal obtained by the low-pass filter.</p>
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<p>A block diagram of the proposed dual-modality food intake estimation method.</p>
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<p>Architecture of the proposed CNN for the classification of food type.</p>
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<p>The MAPEs for each modality and each food item.</p>
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19 pages, 3962 KiB  
Article
Estimation of Tissue Attenuation from Ultrasonic B-Mode Images—Spectral-Log-Difference and Method-of-Moments Algorithms Compared
by Dinah Maria Brandner, Xiran Cai, Josquin Foiret, Katherine W. Ferrara and Bernhard G. Zagar
Sensors 2021, 21(7), 2548; https://doi.org/10.3390/s21072548 - 5 Apr 2021
Cited by 15 | Viewed by 4574
Abstract
We report on results from the comparison of two algorithms designed to estimate the attenuation coefficient from ultrasonic B-mode scans obtained from a numerical phantom simulating an ultrasound breast scan. It is well documented that this parameter significantly diverges between normal tissue and [...] Read more.
We report on results from the comparison of two algorithms designed to estimate the attenuation coefficient from ultrasonic B-mode scans obtained from a numerical phantom simulating an ultrasound breast scan. It is well documented that this parameter significantly diverges between normal tissue and malignant lesions. To improve the diagnostic accuracy it is of great importance to devise and test algorithms that facilitate the accurate, low variance and spatially resolved estimation of the tissue’s attenuation properties. A numerical phantom is realized using k-Wave, which is an open source Matlab toolbox for the time-domain simulation of acoustic wave fields that facilitates both linear and nonlinear wave propagation in homogeneous and heterogeneous tissue, as compared to strictly linear ultrasound simulation tools like Field II. k-Wave allows to simulate arbitrary distributions, resolved down to single voxel sizes, of parameters including the speed of sound, mass density, scattering strength and to include power law acoustic absorption necessary for simulation tasks in medical diagnostic ultrasound. We analyze the properties and the attainable accuracy of both the spectral-log-difference technique, and a statistical moments based approach and compare the results to known reference values from the sound field simulation. Full article
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<p>Setup used for the measurement of tissue-mimicking phantoms. (<b>a</b>) Piston-type US transducer (ROHE-5604), (<b>b</b>) phantom, (<b>c</b>) needle hydrophone (HNA-0400, ONDA, Sunnyvale, CA, USA) with amplifier (AH-1100, ONDA, Sunnyvale, CA, USA). The thickness of the phantom is 2 cm.</p>
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<p>Attenuation coefficient vs. concentration of aluminum oxide (grain size 0.3 μm) for homogeneously prepared tissue mimicking phantoms (as shown in <a href="#sensors-21-02548-f001" class="html-fig">Figure 1</a>b). Reprinted from ref. [<a href="#B15-sensors-21-02548" class="html-bibr">15</a>].</p>
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<p>Ultrasonic wave’s envelope propagating downwards, focused at 35 mm and being scattered off discretely placed scatterers (indicated as red circles in exaggerated size). The chosen colormap for the log-compressed display extends from 100 kPa (orange) to 1 Pa (in blue).</p>
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<p>Left diagram: decrease of sound pressure amplitude vs. depth along the center line within the volume in blue and the expected decrease in sound pressure for the assumed attenuation coefficient of 2.3 dB/(MHz cm) in red. Right diagram decrease of sound pressure level vs. depth estimated from a B-mode line (in dB ref. 100 kPa). Indicated in red is the expected decrease in amplitude vs. depth for the chosen attenuation of 2.3 dB/(MHz cm).</p>
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<p>(<b>Left</b>): To define locations and indices within a sector scan used in the estimation algorithms. At the top the US transducer is assumed operating as a phased array. (<b>Right</b>): Simulated US B-mode image, exhibiting typical US speckles and shadowing behind a strongly absorbing region (a simulated lesion). Distal (bottom, subscript (...)<math display="inline"><semantics> <msub> <mrow/> <mi>d</mi> </msub> </semantics></math>) and proximal (top, subscript (...)<math display="inline"><semantics> <msub> <mrow/> <mi>p</mi> </msub> </semantics></math>) windows are indicated.</p>
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<p>The blue graph represents the power spectral density for the ultrasound propagation in pure water, the red line is the measured spectrum obtained over the thickness of 2 cm of the tissue mimicking phantom depicted in <a href="#sensors-21-02548-f001" class="html-fig">Figure 1</a> which was designed to result in an <math display="inline"><semantics> <msub> <mi>α</mi> <mn>0</mn> </msub> </semantics></math> of 0.6 dB/(MHz cm), and the green line is the spectral-log-difference. The two estimators used, led to an estimated attenuation of: <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>α</mi> <mo stretchy="false">^</mo> </mover> <mn>0</mn> </msub> <msub> <mrow> <mo>|</mo> </mrow> <mrow> <mi>S</mi> <mi>L</mi> <mi>D</mi> </mrow> </msub> </mrow> </semantics></math> = 0.5663 dB/(MHz cm) and <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>α</mi> <mo stretchy="false">^</mo> </mover> <mn>0</mn> </msub> <msub> <mrow> <mo>|</mo> </mrow> <mrow> <mi>M</mi> <mi>o</mi> <mi>M</mi> </mrow> </msub> </mrow> </semantics></math> = 0.5759 dB/(MHz cm).</p>
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<p>Comparison of the performance of both estimators. (<b>a</b>) The imaging geometry and the spectral density analysis windows. As a steering angle of <math display="inline"><semantics> <mrow> <mo>±</mo> <msup> <mn>15</mn> <mo>∘</mo> </msup> </mrow> </semantics></math> would appear very slim, the image was stretched to square, leading to speckles that appear wider than those seen in real ultrasound images. Furthermore, the distal and proximal windows are displayed larger than they actually are, to give an idea of what is done here, meaning there is not as much averaging done than could be assumed by inspecting the graphic. (<b>b</b>) Shows the simulated B-mode image rendered with correct time-gain-compensation. This raw data is analyzed by both attenuation estimating algorithms. (<b>c</b>) The color-coded overlaid estimation result for the spectral-log-difference algorithm. (<b>d</b>) Estimation result for the method-of-moments. (<b>e</b>) Probability density function for the spectral-log-difference algorithm. (<b>f</b>) Probability density function for the method-of-moments.</p>
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<p>Result of estimating <math display="inline"><semantics> <msub> <mover accent="true"> <mi>a</mi> <mo stretchy="false">^</mo> </mover> <mn>2</mn> </msub> </semantics></math> from simulations of the homogeneous phantom (<b>left</b>). The true value is <math display="inline"><semantics> <mrow> <msub> <mi>a</mi> <mn>2</mn> </msub> <mo>=</mo> <mn>0.2</mn> </mrow> </semantics></math>, and the histogram for <math display="inline"><semantics> <msub> <mover accent="true"> <mi>a</mi> <mo stretchy="false">^</mo> </mover> <mn>2</mn> </msub> </semantics></math> (<b>right</b>). One can observe a rather large spread thus rendering the estimate to be of limited use in diagnosis.</p>
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<p>(<b>a</b>) B-mode images of an inclusion with a radius of 7.5 mm positioned centered at a depth of 20 mm, left, the inclusion is mimicking a cyst (<math display="inline"><semantics> <mrow> <msub> <mi>α</mi> <mn>0</mn> </msub> <mo>=</mo> <mn>0.2</mn> </mrow> </semantics></math> dB/(MHz cm)). (<b>b</b>) B-mode images of an inclusion with a radius of 7.5 mm positioned centered at a depth of 20 mm, the inclusion is mimicking a malignant lesion (<math display="inline"><semantics> <mrow> <msub> <mi>α</mi> <mn>0</mn> </msub> <mo>=</mo> <mn>2.5</mn> </mrow> </semantics></math> dB/(MHz cm)). (<b>c</b>,<b>d</b>) Estimation results obtained from the application of the spectral-log-difference algorithm. (<b>e</b>,<b>f</b>) Estimation results obtained from the method-of-moments.</p>
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24 pages, 13387 KiB  
Article
Research on a Measurement Method for Downhole Drill String Eccentricity Based on a Multi-Sensor Layout
by Hongqiang Li and Ruihe Wang
Sensors 2021, 21(4), 1258; https://doi.org/10.3390/s21041258 - 10 Feb 2021
Cited by 2 | Viewed by 5799
Abstract
The drill string used in drilling is in a complex motion state downhole for several kilometers. The operating attitude and eccentricity of the downhole drill string play important roles in avoiding downhole risks and correcting the output of the imaging measurement sensor while [...] Read more.
The drill string used in drilling is in a complex motion state downhole for several kilometers. The operating attitude and eccentricity of the downhole drill string play important roles in avoiding downhole risks and correcting the output of the imaging measurement sensor while drilling (IMWD). This paper proposes a method for measuring eccentricity while drilling using two sets of caliper sensors coupled with a fiber-optic gyroscope for continuous attitude measurement, which is used to solve the problem of the quantitative measurement of complex eccentricity that changes in real-time downhole. According to the measurement and calculation methods involved in this article, we performed simulations of the attitude of the drill string near where the IMWD tool is located in the wellbore under a variety of complex downhole conditions, such as centering, eccentricity, tilt, buckling, rotation, revolution, etc. The simulation and field test results prove that the distance between the imaging while drilling sensor and the borehole wall is greatly affected by the downhole attitude and revolution. The multi-sensor layout measurement scheme and the data processing based on the above-mentioned measurement involved can push the drill collar movement and eccentricity matrix specifically studied downhole from only qualitative estimation to real-time measurement and quantitative calculation. The above measurement and data processing methods can accurately measure and identify the local operating posture of the drill string where the IMWD sensor is located, and quantitatively give the eccentric distance matrix from the measuring point to the borehole wall required for environmental correction of the IMWD sensor. Full article
(This article belongs to the Special Issue Advanced Fiber-Optic Sensors in Civil Engineering)
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<p>(<b>a</b>) Position and force of drill collars while drilling in the wellbore; (<b>b</b>) Schematic diagram of drill collar force.</p>
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<p>Profile of the drill collar and wellbore relative to each other.</p>
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<p>(<b>a</b>) Gamma mud gravity correction; (<b>b</b>) Gamma correction pattern of potassium-based mud.</p>
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<p>(<b>a</b>) Schematic diagram of the multi-sensor layout of the drill string eccentricity measurement system; (<b>b</b>) Diagram of upper sensor set eccentricity; (<b>c</b>) Diagram of down sensor set eccentricity.</p>
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<p>Schematic diagram of the multi-sensor layout of the drill string eccentricity measurement data processing.</p>
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<p>Ultrasonic caliper measurement echo.</p>
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<p>(<b>a</b>) Drill string eccentricity diagram section; (<b>b</b>) The drill string is eccentric in the wellbore.</p>
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<p>The eccentric distance of the drill collars running in the center of the wellbore.</p>
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<p>Eccentricity distance distribution along the surface of the drill collar during eccentric rotation.</p>
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<p>Eccentricity distance in order of recorded data.</p>
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<p>(<b>a</b>) Display the eccentricity in the order of recording according to 1.5 RPM revolution; (<b>b</b>) Display the eccentricity in the order of recording according to 3 RPM revolution.</p>
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<p>Eccentricity distribution of drill collars as they tilt in the wellbore.</p>
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<p>Eccentricity distribution of drill collars in the wellbore. with oblique rotation and additional revolution at a speed of 1.5 RPM.</p>
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<p>Eccentricity distribution of drill collars in the wellbore, with oblique rotation and additional revolution at a speed of 3 RPM.</p>
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<p>Eccentricity distribution of drill collars during buckling rotation (no revolution) in wellbore.</p>
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<p>Comparison of the eccentricity distribution of drill collars recorded in the order of buckling rotation and additional revolution in the wellbore.</p>
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<p>The phase change after additional revolution compared with that without additional revolution.</p>
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<p>Eccentricity distribution along the drill collar surface after drill collar buckling with a revolution of 1.5 RPM.</p>
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<p>(<b>a</b>) Ground north-finding for fiber-optic gyro (FOG) while drilling; (<b>b</b>) Go down well with LWD tools.</p>
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<p>(<b>a</b>) The original caliper data of the fused gyro attitude extracted from memory; (<b>b</b>) Eccentric data set.</p>
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<p>Eccentricity distribution of each tool surface along the drill collar axis.</p>
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19 pages, 7385 KiB  
Article
Design of 2D Sparse Array Transducers for Anomaly Detection in Medical Phantoms
by Xiaotong Li, Anthony Gachagan and Paul Murray
Sensors 2020, 20(18), 5370; https://doi.org/10.3390/s20185370 - 19 Sep 2020
Cited by 9 | Viewed by 3422
Abstract
Aperiodic sparse 2D ultrasonic array configurations, including random array, log spiral array, and sunflower array, have been considered for their potential as conformable transducers able to image within a focal range of 30–80 mm, at an operating frequency of 2 MHz. Optimisation of [...] Read more.
Aperiodic sparse 2D ultrasonic array configurations, including random array, log spiral array, and sunflower array, have been considered for their potential as conformable transducers able to image within a focal range of 30–80 mm, at an operating frequency of 2 MHz. Optimisation of the imaging performance of potential array patterns has been undertaken based on their simulated far field directivity functions. Two evaluation criteria, peak sidelobe level (PSL) and integrated sidelobe ratio (ISLR), are used to access the performance of each array configuration. Subsequently, a log spiral array pattern with −19.33 dB PSL and 2.71 dB ISLR has been selected as the overall optimal design. Two prototype transducers with the selected log spiral array pattern have been fabricated and characterised, one using a fibre composite element composite array transducer (CECAT) structure, the other using a conventional 1–3 composite (C1–3) structure. The CECAT device demonstrates improved coupling coefficient (0.64 to 0.59), reduced mechanical cross-talk between neighbouring array elements (by 10 dB) and improved operational bandwidth (by 16.5%), while the C1–3 device performs better in terms of sensitivity (~50%). Image processing algorithms, such as Hough transform and morphological opening, have been implemented to automatically detect and dimension particles located within a fluid-filled tube structure, in a variety of experimental scenarios, including bespoke phantoms using tissue mimicking material. Experiments using the fabricated CECAT log spiral 2D array transducer demonstrated that this algorithmic approach was able to detect the walls of the tube structure and stationary anomalies within the tube with a precision of ~0.1 mm. Full article
(This article belongs to the Section Physical Sensors)
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<p>Three sparse array configurations which have been simulated in this work: (<b>a</b>) random array; (<b>b</b>) sunflower spiral array; (<b>c</b>) log spiral array.</p>
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<p>PSL and ISLR performance of (<b>a</b>) random array configuration and (<b>b</b>) sunflower array. configuration with respect to number of elements within the array.</p>
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<p>(<b>a</b>,<b>d</b>,<b>g</b>) illustrate the layout of the optimised random array, sunflower array and log spiral array separately. The corresponding unsteered directivity functions are illustrated in (<b>b</b>,<b>e</b>,<b>h</b>). (<b>c</b>,<b>f</b>,<b>i</b>) show the steered beam profile (10°) for each array configuration.</p>
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<p>Illustration of prototype transducer structure.</p>
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<p>Illustration of the manufacturing process for (<b>a</b>) the CECAT active layer and (<b>b</b>) the C1–3 active layer.</p>
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<p>Impedance response of all array elements for (<b>a</b>) the CECAT and (<b>b</b>) the C1–3.</p>
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<p>(<b>a</b>) Illustration of the experimental setup for mechanical cross-talk measurement. (<b>b</b>) Illustration of how the LDV scanning was processed. The black circle represents the fired array element. The blue block represents the area that was scanned.</p>
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<p>Cross-talk contours for (<b>a</b>) the CECAT and (<b>b</b>) the C1–3 when firing the first element in the 3rd arm individually. The red circles represent the theoretical position of the neighbouring elements.</p>
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<p>Pulse-echo response of the centre element for (<b>a</b>) the CECAT and (<b>b</b>) the C1–3.</p>
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<p>Block diagram to illustrate the particle detecting algorithm.</p>
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<p>The current frame with the particles detected. The dashed yellow lines indicate the regions in which a particle was detected. The solid red lines represent the distance from the particles (red dots) to the top and bottom inner walls of the tube (solid green lines).</p>
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<p>An example current frame from the CECAT with the particles detected: (<b>a</b>) is the TFM image and (<b>b</b>) presents the particle detection algorithm image result. The dashed yellow lines indicate the regions in which a particle was detected. The solid red lines represent the distance from the particles (red dots) to the top and bottom inner walls of the tube (solid green lines).</p>
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<p>Illustrations of the basic structures of the lab phantoms. From (<b>a</b>–<b>e</b>), the phantoms are named the 55 mm phantom, the 65 mm phantom, the 75 mm phantom, the Angle V phantom and the Angle H phantom, respectively.</p>
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<p>Illustration of the experimental setup for imaging the lab phantom using the CECAT.</p>
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<p>Illustration of the size and shape of the TMM particle. A 2 mm ball bearing is used as a reference.</p>
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<p>TFM image of (<b>a</b>) the 55 mm phantom, (<b>b</b>) the 65 mm phantom, (<b>c</b>) the 75 mm phantom, (<b>d</b>) the Angle V phantom and (<b>e</b>) the Angle H phantom with the TMM particle placed inside the tube from the CECAT.</p>
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<p>The results after applying the particle detection algorithm to the frames which were converted from the example TFM images of (<b>a</b>) the 55 mm phantom, (<b>b</b>) the 65 mm phantom, (<b>c</b>) the 75 mm phantom, (<b>d</b>) the Angle V phantom and (<b>e</b>) the Angle H phantom with the TMM particle placed inside the tube from the CECAT. The dashed yellow lines indicate the regions in which a particle was detected. The solid red lines represent the distance from the particles (red dots) to the top and bottom inner walls of the tube (solid green lines).</p>
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17 pages, 7762 KiB  
Article
Damage Detection of CFRP Stiffened Panels by Using Cross-Correlated Spatially Shifted Distributed Strain Sensors
by Monica Ciminello, Natalino Daniele Boffa, Antonio Concilio, Bernardino Galasso, Fulvio Romano and Ernesto Monaco
Appl. Sci. 2020, 10(8), 2662; https://doi.org/10.3390/app10082662 - 12 Apr 2020
Cited by 6 | Viewed by 2621
Abstract
This paper presents a cross-correlation function-based method applied to a spatially shifted differential strain readout vectors using distributed sensors under backscattering random noise and impact excitations. Structural damage is generated by low/medium energy impact on two aeronautical 24-ply CFRP (carbon fiber reinforced plastic) [...] Read more.
This paper presents a cross-correlation function-based method applied to a spatially shifted differential strain readout vectors using distributed sensors under backscattering random noise and impact excitations. Structural damage is generated by low/medium energy impact on two aeronautical 24-ply CFRP (carbon fiber reinforced plastic) stiffened panels. Two different drop impact locations, two different sensor layouts and two different post-impact solicitations are provided for a skin-stringer debonding detection and length estimation. The differential signal with respect to an arbitrarily selected grounding is used. Then the effects of noise filtering are evaluated post-processing the differential signal by cross-correlating two strain vectors having one sensor gauge position lag. A Rayleigh backscattering sensing technology, with 5 mm of spatial resolution, is used to log the strain map. The results show a good coherence with respect to the NDI (nondestructive inspection) performed by ultrasonic C-scan (an ultrasonic imaging system) flaw detector. Full article
(This article belongs to the Special Issue NondestructiveTesting in Composite Materials Ⅱ)
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<p>Methodology flowchart.</p>
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<p>Carbon fiber reinforced plastic (CFRP) geometry: front view (<b>a</b>); dymetric view with thickness detail (<b>b</b>).</p>
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<p>Test rig: drop-weight machine (<b>a</b>); aluminum fixture for the panel (<b>b</b>).</p>
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<p>Impact position indicated by a star: PNL1 panel in the center of the skin (<b>a</b>); PNL2 panel under a stringer (<b>b</b>).</p>
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<p>Fiber optic sensor interrogation unit.</p>
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<p>Scan pattern section view (upper) and scan setup (lower).</p>
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<p>Sensor layout dotted line: on PNL1 all along the stringer perimeter (<b>a</b>); on PNL2 along the inner line of left stringer and on the skin (<b>b</b>). The red arrow indicates the light insertion origin.</p>
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<p>Differential strain after impact for PNL1.</p>
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<p>Damage index and threshold level (red line) estimated from the Damage Index (DI).</p>
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<p>Graphical user interface of the panel geometry and fiber optic layout (yellow dotted line). The red dots are the sensors with higher DI value.</p>
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<p>Panel PNL1: left stringers C-scan (<b>upper</b>) and B–B longitudinal section with B-scan view (<b>bottom</b>)—scan length 200 mm.</p>
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<p>Panel PNL1: left stringers C-scan (<b>upper</b>) and B–B longitudinal section with B-scan view (<b>bottom</b>)—scan length 200 mm.</p>
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<p>Panel PNL1: right stringers C-scan (<b>upper</b>) and B–B longitudinal section B scan view (<b>bottom</b>)—scan length 200 mm.</p>
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<p>Dynamic differential strain acquisition after impact for PNL2.</p>
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<p>Damage index and threshold level (red line) estimated from the DI.</p>
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<p>Graphical user interface of the panel geometry and fiber optic layout (yellow dotted line). The red and blue dots are the sensors with higher DI value.</p>
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<p>Panel PNL2: left (<b>upper</b>) and right (<b>bottom</b>) stringers C-scan amplitude views—scan length 200 mm.</p>
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<p>Panel PNL2: left (<b>upper</b>) and right (<b>bottom</b>) stringers C-scan amplitude views—scan length 200 mm.</p>
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24 pages, 4194 KiB  
Article
A POSHE-Based Optimum Clip-Limit Contrast Enhancement Method for Ultrasonic Logging Images
by Qingqing Fu, Zhengbing Zhang, Mehmet Celenk and Aiping Wu
Sensors 2018, 18(11), 3954; https://doi.org/10.3390/s18113954 - 15 Nov 2018
Cited by 6 | Viewed by 3592
Abstract
Enabled by piezoceramic transducers, ultrasonic logging images often suffer from low contrast and indistinct local details, which makes it difficult to analyze and interpret geologic features in the images. In this work, we propose a novel partially overlapped sub-block histogram-equalization (POSHE)-based optimum clip-limit [...] Read more.
Enabled by piezoceramic transducers, ultrasonic logging images often suffer from low contrast and indistinct local details, which makes it difficult to analyze and interpret geologic features in the images. In this work, we propose a novel partially overlapped sub-block histogram-equalization (POSHE)-based optimum clip-limit contrast enhancement (POSHEOC) method to highlight the local details hidden in ultrasonic well logging images obtained through piezoceramic transducers. The proposed algorithm introduces the idea of contrast-limited enhancement to modify the cumulative distribution functions of the POSHE and build a new quality evaluation index considering the effects of the mean gradient and mean structural similarity. The new index is designed to obtain the optimal clip-limit value for histogram equalization of the sub-block. It makes the choice of the optimal clip-limit automatically according to the input image. Experimental results based on visual perceptual evaluation and quantitative measures demonstrate that the proposed method yields better quality in terms of enhancing the contrast, emphasizing the local details while preserving the brightness and restricting the excessive enhancement compared with the other seven histogram equalization-based techniques from the literature. This study provides a feasible and effective method to enhance ultrasonic logging images obtained through piezoceramic transducers and is significant for the interpretation of actual ultrasonic logging data. Full article
(This article belongs to the Special Issue Recent Advances of Piezoelectric Transducers and Applications)
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<p>Diagram of the operating principle.</p>
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<p>Example of POSHE.</p>
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<p>The example of enhanced results by the HE and the clipped HE method. (<b>a</b>) Original input image; (<b>b</b>) Image enhanced by HE; (<b>c</b>) Image enhanced by clipped HE with <span class="html-italic">β</span> = 2.5 <span class="html-italic">N<sub>av</sub></span>; (<b>d</b>) Image enhanced by clipped HE with <span class="html-italic">β</span> = 1.5 <span class="html-italic">N<sub>av</sub></span>.</p>
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<p>Clipping and redistribution of clipped histogram equalization. (<b>a</b>) Histogram of the original input image; (<b>b</b>) Histogram of the original input image and the modified histogram after redistribution; (<b>c</b>) The cumulative density function of original and modified histograms with <span class="html-italic">β</span> = 2.5 <span class="html-italic">N<sub>av</sub></span>; (<b>d</b>) The cumulative density function of original and modified histograms with <span class="html-italic">β</span> = 1.5 <span class="html-italic">N<sub>av</sub></span>.</p>
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<p>Clipping and redistribution of clipped histogram equalization. (<b>a</b>) Histogram of the original input image; (<b>b</b>) Histogram of the original input image and the modified histogram after redistribution; (<b>c</b>) The cumulative density function of original and modified histograms with <span class="html-italic">β</span> = 2.5 <span class="html-italic">N<sub>av</sub></span>; (<b>d</b>) The cumulative density function of original and modified histograms with <span class="html-italic">β</span> = 1.5 <span class="html-italic">N<sub>av</sub></span>.</p>
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<p>The relationships between the two measures and <span class="html-italic">n</span>. (<b>a</b>) MG of the enhanced image with different <span class="html-italic">n</span> values; (<b>b</b>) MMSIM of the enhanced image with different <span class="html-italic">n</span> values.</p>
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<p>Examples of the proposed POSHEOC with different <span class="html-italic">n</span> values. (<b>a</b>) The original ultrasonic logging image; (<b>b</b>) PMGSIM of the enhanced image with different <span class="html-italic">n</span> values; (<b>c</b>) The enhanced result of the proposed POSHEOC with <span class="html-italic">n</span> = 1.5; (<b>d</b>) The enhanced result of the proposed POSHEOC with <span class="html-italic">n</span> = 3; (<b>e</b>) The enhanced result of the proposed POSHEOC with <span class="html-italic">n</span> = 6.</p>
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<p>Comparison of enhancement results with corresponding statistical histogram using various techniques for ultrasonic logging image of the model well. (<b>a</b>) Original image; (<b>b</b>) HE; (<b>c</b>) BOHE; (<b>d</b>) POSHE; (<b>e</b>) MLBOHE; (<b>f</b>) BBHE; (<b>g</b>) RMSHE; (<b>h</b>) CLAHE-PL; (<b>i</b>) Proposed POSHEOC.</p>
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<p>Comparison of enhancement results with corresponding statistical histogram using various techniques for ultrasonic logging image of the model well. (<b>a</b>) Original image; (<b>b</b>) HE; (<b>c</b>) BOHE; (<b>d</b>) POSHE; (<b>e</b>) MLBOHE; (<b>f</b>) BBHE; (<b>g</b>) RMSHE; (<b>h</b>) CLAHE-PL; (<b>i</b>) Proposed POSHEOC.</p>
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<p>Comparison of enhancement results with corresponding statistical histogram using various techniques for ultrasonic logging image of Changqingyi well. (<b>a</b>) Original image; (<b>b</b>) HE; (<b>c</b>) BOHE; (<b>d</b>) POSHE; (<b>e</b>) MLBOHE; (<b>f</b>) BBHE; (<b>g</b>) RMSHE; (<b>h</b>) CLAHE-PL; (<b>i</b>) Proposed POSHEOC.</p>
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<p>Comparison of enhancement results with corresponding statistical histogram using various techniques for ultrasonic logging image of Changqingyi well. (<b>a</b>) Original image; (<b>b</b>) HE; (<b>c</b>) BOHE; (<b>d</b>) POSHE; (<b>e</b>) MLBOHE; (<b>f</b>) BBHE; (<b>g</b>) RMSHE; (<b>h</b>) CLAHE-PL; (<b>i</b>) Proposed POSHEOC.</p>
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<p>Comparison of enhancement results with corresponding statistical histogram using various techniques for ultrasonic logging image of Changqingli well. (<b>a</b>) Original image; (<b>b</b>) HE; (<b>c</b>) BOHE; (<b>d</b>) POSHE; (<b>e</b>) MLBOHE; (<b>f</b>) BBHE; (<b>g</b>) RMSHE; (<b>h</b>) CLAHE-PL; (<b>i</b>) Proposed POSHEOC.</p>
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<p>Comparison of enhancement results with corresponding statistical histogram using various techniques for ultrasonic logging image of Changqingli well. (<b>a</b>) Original image; (<b>b</b>) HE; (<b>c</b>) BOHE; (<b>d</b>) POSHE; (<b>e</b>) MLBOHE; (<b>f</b>) BBHE; (<b>g</b>) RMSHE; (<b>h</b>) CLAHE-PL; (<b>i</b>) Proposed POSHEOC.</p>
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18080 KiB  
Review
Fiber Bragg Grating Sensors for the Oil Industry
by Xueguang Qiao, Zhihua Shao, Weijia Bao and Qiangzhou Rong
Sensors 2017, 17(3), 429; https://doi.org/10.3390/s17030429 - 23 Feb 2017
Cited by 174 | Viewed by 15037
Abstract
With the oil and gas industry growing rapidly, increasing the yield and profit require advances in technology for cost-effective production in key areas of reservoir exploration and in oil-well production-management. In this paper we review our group’s research into fiber Bragg gratings (FBGs) [...] Read more.
With the oil and gas industry growing rapidly, increasing the yield and profit require advances in technology for cost-effective production in key areas of reservoir exploration and in oil-well production-management. In this paper we review our group’s research into fiber Bragg gratings (FBGs) and their applications in the oil industry, especially in the well-logging field. FBG sensors used for seismic exploration in the oil and gas industry need to be capable of measuring multiple physical parameters such as temperature, pressure, and acoustic waves in a hostile environment. This application requires that the FBG sensors display high sensitivity over the broad vibration frequency range of 5 Hz to 2.5 kHz, which contains the important geological information. We report the incorporation of mechanical transducers in the FBG sensors to enable enhance the sensors’ amplitude and frequency response. Whenever the FBG sensors are working within a well, they must withstand high temperatures and high pressures, up to 175 °C and 40 Mpa or more. We use femtosecond laser side-illumination to ensure that the FBGs themselves have the high temperature resistance up to 1100 °C. Using FBG sensors combined with suitable metal transducers, we have experimentally realized high- temperature and pressure measurements up to 400 °C and 100 Mpa. We introduce a novel technology of ultrasonic imaging of seismic physical models using FBG sensors, which is superior to conventional seismic exploration methods. Compared with piezoelectric transducers, FBG ultrasonic sensors demonstrate superior sensitivity, more compact structure, improved spatial resolution, high stability and immunity to electromagnetic interference (EMI). In the last section, we present a case study of a well-logging field to demonstrate the utility of FBG sensors in the oil and gas industry. Full article
(This article belongs to the Special Issue Recent Advances in Fiber Bragg Grating Sensing)
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<p>Frequency band range and longitudinal resolution of multi scale geophysical data [<a href="#B100-sensors-17-00429" class="html-bibr">100</a>,<a href="#B101-sensors-17-00429" class="html-bibr">101</a>,<a href="#B102-sensors-17-00429" class="html-bibr">102</a>].</p>
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<p>Mechanical model of a FBG accelerometer.</p>
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<p>(<b>a</b>) Scheme structure of the proposedaccelerometer; (<b>b</b>) Photograph of the accelerometer and testing exciter; (<b>c</b>) Amplitude-frequency response of accelerometer; (<b>d</b>) Transverse direction dependence of resonance wavelength difference of FBGsunder the acceleration excitation of 1.5 G.</p>
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<p>(<b>a</b>) Schematic diagram of FBG accelerometer based on double diaphragms; (<b>b</b>) Simulated sensitivity and resonant frequency as a function of mass diameter; (<b>c</b>) Frequency response of accelerometer (insets show the time-domain variation of resonant wavelength for vibration frequencies 100, 200, 600 and 800 Hz); (<b>d</b>) Stabilities of the accelerometer under the vibrations with the different frequencies.</p>
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<p>(<b>a</b>) Schematic diagram of TCF-FBG directional accelerometer; (<b>b</b>) Image of TCF-FBG, insets show the zoomed images of gratings in fiber cladding (up) and fiber core (bottom); (<b>c</b>) The transmission spectrum of TCF-FBG with two well-defined resonances; (<b>d</b>) Real-time power output of cladding mode and core mode (blue curve) under the same vibration condition; (<b>e</b>) Angular dependence of acceleration responsivity of sensor.</p>
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<p>(<b>a</b>) Cross-sectional photomicrograph of the MCF-FBG; (<b>b</b>) Refractive index profile of the MCF-cross section; (<b>c</b>) Longitudinal photomicrograph of gratings inside MFC; (<b>d</b>) Schematic of the vector grating; (<b>e</b>) Spectra of the vector-FBG; (<b>f</b>) Angular dependence of acceleration responsivity of this sensor.</p>
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<p>Reflection and transmission spectra of seed gratings (black curve) and regenerated fiber Bragg gratings (red curve).</p>
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<p>(<b>a</b>) Reflection and transmission spectrum of FBG written in a SMF (inset is imaging photo of FBG); (<b>b</b>) FBG wavelength versus temperature up to 1100 °C.</p>
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<p>Schematic diagram of FBG pressure sensor.</p>
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<p>Schematic diagram of FBG sensor for simultaneous temperature and pressure measurements simultaneously.</p>
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<p>FBG sensor peak wavelength versus (<b>a</b>) Temperature; (<b>b</b>) Pressure.</p>
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<p>(<b>a</b>) Experimental setup for vector pressure measurement; (<b>b</b>) Reflection spectrum of PM-FBG with two polarized mode resonances; (<b>c</b>) Orthogonal responses of two polarized mode versus transverse stress.</p>
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<p>Simulation results: (<b>a</b>) FBG length versus response sensitivity; (<b>b</b>) Detection direction versus response sensitivity.</p>
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<p>(<b>a</b>) Scheme diagram of π-FBG sensor structure; (<b>b</b>) π-FBG probe’s responses versus ultrasonic directions (this figure is concluded by recording the peak power of ultrasonic signals in the different detection directions).</p>
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<p>(<b>a</b>) Scheme diagram of directional FBG-FP sensor structure; (<b>b</b>) Photo image of the sensing probe; (<b>c</b>) FBG-FP spectrum with several interference dips overlapping on the top of the FBG resonance spectrum.</p>
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<p>(<b>a</b>) Spectral side-band filtering mechanism; (<b>b</b>) FBG spectral response to ultrasonic; sensor’s responses to the pulse ultrasonic under the different distances and with different frequencies: (<b>c</b>) 300 kHz and (<b>d</b>) 1 MHz.</p>
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<p>(<b>a</b>) Photograph of the step-type Plexiglas model; (<b>b</b>) UW image of the physical model; (<b>c</b>) Photograph of the sunken plexiglas model; (<b>d</b>) UW image of the physical model.</p>
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<p>Testing result of the glue, the sample with the particles of 4% nanometer SiO<sub>2</sub> is the optimized one.</p>
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<p>Series of FBG sensors, including strain sensors, high temperature sensors, high pressure sensors, and accelerometers.</p>
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<p>(<b>a</b>) Cross-section structure of downhole cable; (<b>b</b>) Photo of the 10 km-long downhole cable.</p>
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<p>Schematic diagram of the downhole testing.</p>
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<p>Photos of well-logging field: (<b>a</b>) Downhole cable; (<b>b</b>) Tied to the downhole tube; (<b>c</b>) Sensor down well process.</p>
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<p>Temperature distribution down to 1100 m depth of well hole, measured by FBG sensors.</p>
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<p>Photo of Oilfield test in Jinbian.</p>
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<p>Downwell temperature, pressure and liquid level distribution.</p>
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