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Sensors, Volume 16, Issue 4 (April 2016) – 171 articles

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1983 KiB  
Article
Electromyographic Patterns during Golf Swing: Activation Sequence Profiling and Prediction of Shot Effectiveness
by Antanas Verikas, Evaldas Vaiciukynas, Adas Gelzinis, James Parker and M. Charlotte Olsson
Sensors 2016, 16(4), 592; https://doi.org/10.3390/s16040592 - 23 Apr 2016
Cited by 25 | Viewed by 10624
Abstract
This study analyzes muscle activity, recorded in an eight-channel electromyographic (EMG) signal stream, during the golf swing using a 7-iron club and exploits information extracted from EMG dynamics to predict the success of the resulting shot. Muscles of the arm and shoulder on [...] Read more.
This study analyzes muscle activity, recorded in an eight-channel electromyographic (EMG) signal stream, during the golf swing using a 7-iron club and exploits information extracted from EMG dynamics to predict the success of the resulting shot. Muscles of the arm and shoulder on both the left and right sides, namely flexor carpi radialis, extensor digitorum communis, rhomboideus and trapezius, are considered for 15 golf players (∼5 shots each). The method using Gaussian filtering is outlined for EMG onset time estimation in each channel and activation sequence profiling. Shots of each player revealed a persistent pattern of muscle activation. Profiles were plotted and insights with respect to player effectiveness were provided. Inspection of EMG dynamics revealed a pair of highest peaks in each channel as the hallmark of golf swing, and a custom application of peak detection for automatic extraction of swing segment was introduced. Various EMG features, encompassing 22 feature sets, were constructed. Feature sets were used individually and also in decision-level fusion for the prediction of shot effectiveness. The prediction of the target attribute, such as club head speed or ball carry distance, was investigated using random forest as the learner in detection and regression tasks. Detection evaluates the personal effectiveness of a shot with respect to the player-specific average, whereas regression estimates the value of target attribute, using EMG features as predictors. Fusion after decision optimization provided the best results: the equal error rate in detection was 24.3% for the speed and 31.7% for the distance; the mean absolute percentage error in regression was 3.2% for the speed and 6.4% for the distance. Proposed EMG feature sets were found to be useful, especially when used in combination. Rankings of feature sets indicated statistics for muscle activity in both the left and right body sides, correlation-based analysis of EMG dynamics and features derived from the properties of two highest peaks as important predictors of personal shot effectiveness. Activation sequence profiles helped in analyzing muscle orchestration during golf shot, exposing a specific avalanche pattern, but data from more players are needed for stronger conclusions. Results demonstrate that information arising from an EMG signal stream is useful for predicting golf shot success, in terms of club head speed and ball carry distance, with acceptable accuracy. Surface EMG data, collected with a goal to automatically evaluate golf player’s performance, enables wearable computing in the field of ambient intelligence and has potential to enhance exercising of a long carry distance drive. Full article
(This article belongs to the Special Issue Wearable Biomedical Sensors)
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<p>Participant body with eight-channel EMG recorder electrodes attached. Electrodes on <span class="html-italic">extensor digitorum communis (EDC)</span> arm muscles can be seen in the front side view (<b>Left</b>); electrodes on <span class="html-italic">flexor carpi radialis (FCR)</span> arm muscles, as well as electrodes on <span class="html-italic">rhomboideus</span> and <span class="html-italic">trapezius</span> muscles can be seen in the back side view (<b>Right</b>). Mapping between a channel number and a muscle: (1) right <span class="html-italic">FCR</span>; (2) right <span class="html-italic">EDC</span>; (3) left <span class="html-italic">FCR</span>; (4) left <span class="html-italic">EDC</span>; (5) right <span class="html-italic">rhomboideus</span>; (6) right <span class="html-italic">trapezius</span>; (7) left <span class="html-italic">rhomboideus</span>; and (8) left <span class="html-italic">trapezius</span>.</p>
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<p>Scatterplot, showing the effectiveness for men (<b>Left</b>) and women (<b>Right</b>) players. Notes: grid lines correspond to sex-specific averages; shots are colored according to the player’s overall effectiveness, where a lighter color means a more effective player, based on average club head speed and average ball carry distance through all of his/her shots.</p>
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<p>EMG signals recorded from eight muscles of golf players G2 (<b>Top</b>) and G6 (<b>Bottom</b>). Note: position in samples on the <span class="html-italic">X</span> (horizontal) axis. Channel numbers correspond to the following muscles: (1) right <span class="html-italic">FCR</span>; (2) right <span class="html-italic">EDC</span>; (3) left <span class="html-italic">FCR</span>; (4) left <span class="html-italic">EDC</span>; (5) right <span class="html-italic">rhomboideus</span>; (6) right <span class="html-italic">trapezius</span>; (7) left <span class="html-italic">rhomboideus</span>; and (8) left <span class="html-italic">trapezius</span>.</p>
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<p>EMG signal pre-processing: raw signal (<b>Top</b>) and normalized rectified signal (<b>Bottom</b>) with the result of Butterworth filtering (black curve). Note: the position is in seconds on the <span class="html-italic">X</span> (horizontal) axis.</p>
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<p>Finding peaks in the filtered EMG signal. Interface window of the <span class="html-italic">ipeak</span> function: entire pre-processed signal (<b>Bottom</b>) with 17 peaks detected and the zoomed-in portion of the signal (<b>Top</b>) containing the two highest peaks (# 10 and # 11). Note: the position is in seconds on the <span class="html-italic">X</span> (horizontal) axis.</p>
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<p>Architecture of the random forest model.</p>
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<p>Activation profiles of eight muscles during golf swing for 16 different golf players. Note: channel 8 (left <span class="html-italic">trapezius</span>) was used as the reference for measuring time differences for remaining channels.</p>
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<p>Decision-level fusion for detection task: evaluation by the detection error trade-off (DET) (<b>Left</b>) and ROC (<b>Right</b>) curves.</p>
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<p>RF permutation-based variable importance in decision-level fusion for detection (<b>Left</b>) and regression (<b>Right</b>) tasks.</p>
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<p>Decision-level fusion for regression task: results for club head speed (<b>Left</b>) and ball carry distance (<b>Right</b>) prediction. Note: the diagonal dotted line corresponds to an ideal prediction.</p>
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<p>Illustration of a biomechanically-correct transition in a golf swing. The golf swing progresses in time on the <span class="html-italic">X</span> (horizontal) axis from left to right, and the speed of player’s body parts is on the <span class="html-italic">Y</span> (vertical) axis.</p>
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<p>Illustration of transition sequences for 14 golf players (∼5 shots each), where color change means the change of rotation direction. The sequence of colors (violet, green, red and blue) for player G15 corresponds to the correct transition sequence (pelvis, thorax, arm and club). Note: position in samples on the <span class="html-italic">X</span> (horizontal) axis is shown, where 0 corresponds to the moment of impact.</p>
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4750 KiB  
Article
Color-Space-Based Visual-MIMO for V2X Communication
by Jai-Eun Kim, Ji-Won Kim, Youngil Park and Ki-Doo Kim
Sensors 2016, 16(4), 591; https://doi.org/10.3390/s16040591 - 23 Apr 2016
Cited by 23 | Viewed by 7091
Abstract
In this paper, we analyze the applicability of color-space-based, color-independent visual-MIMO for V2X. We aim to achieve a visual-MIMO scheme that can maintain the original color and brightness while performing seamless communication. We consider two scenarios of GCM based visual-MIMO for V2X. One [...] Read more.
In this paper, we analyze the applicability of color-space-based, color-independent visual-MIMO for V2X. We aim to achieve a visual-MIMO scheme that can maintain the original color and brightness while performing seamless communication. We consider two scenarios of GCM based visual-MIMO for V2X. One is a multipath transmission using visual-MIMO networking and the other is multi-node V2X communication. In the scenario of multipath transmission, we analyze the channel capacity numerically and we illustrate the significance of networking information such as distance, reference color (symbol), and multiplexing-diversity mode transitions. In addition, in the V2X scenario of multiple access, we may achieve the simultaneous multiple access communication without node interferences by dividing the communication area using image processing. Finally, through numerical simulation, we show the superior SER performance of the visual-MIMO scheme compared with LED-PD communication and show the numerical result of the GCM based visual-MIMO channel capacity versus distance. Full article
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<p>Illustration of the optical V2V communication system.</p>
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<p>Generation example of a constellation diagram for a target color in CIELUV color space (example uses seven LEDs and two bit data symbols).</p>
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<p>Color-space-based, color-independent visual-MIMO tranceiving procedure using image processing.</p>
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<p>Multipath transmission strategies using geometric information.</p>
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<p>Multi-node V2X communication.</p>
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<p>The divided ROI for multi-node V2X communication.</p>
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<p>An example of target color transition in a color-space-based constellation diagram.</p>
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<p>The transition example of a target color of a traffic sign from green to red under GCM based communication between LED and PD.</p>
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<p>SER performance comparison between visual-MIMO and LED-PD communication under color variation.</p>
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<p>Numerical results of GCM based visual-MIMO (Channel capacity <span class="html-italic">vs.</span> Distance).</p>
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<p>Compensation of channel noise by sending a reference color in the color space of CIE1931.</p>
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<p>The illustration of V2V communication using color-independent visual-MIMO.</p>
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2381 KiB  
Article
Unsupervised Event Characterization and Detection in Multichannel Signals: An EEG application
by Angel Mur, Raquel Dormido, Jesús Vega, Natividad Duro and Sebastian Dormido-Canto
Sensors 2016, 16(4), 590; https://doi.org/10.3390/s16040590 - 23 Apr 2016
Cited by 10 | Viewed by 8737
Abstract
In this paper, we propose a new unsupervised method to automatically characterize and detect events in multichannel signals. This method is used to identify artifacts in electroencephalogram (EEG) recordings of brain activity. The proposed algorithm has been evaluated and compared with a supervised [...] Read more.
In this paper, we propose a new unsupervised method to automatically characterize and detect events in multichannel signals. This method is used to identify artifacts in electroencephalogram (EEG) recordings of brain activity. The proposed algorithm has been evaluated and compared with a supervised method. To this end an example of the performance of the algorithm to detect artifacts is shown. The results show that although both methods obtain similar classification, the proposed method allows detecting events without training data and can also be applied in signals whose events are unknown a priori. Furthermore, the proposed method provides an optimal window whereby an optimal detection and characterization of events is found. The detection of events can be applied in real-time. Full article
(This article belongs to the Special Issue Noninvasive Biomedical Sensors)
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<p>Different windows along the <span class="html-italic">MC</span> signal <span class="html-italic">X</span>.</p>
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<p>The channel <span class="html-italic">CH</span><sub>1</sub>(<span class="html-italic">t</span>) of the 64-channel EEG.</p>
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<p>Groups of intervals found using the unsupervised classification (UMED) and a PCA. The <span class="html-italic">L<sub>w</sub><sup>H</sup></span> has 155 samples. The first two principal components contain 55% of the full information. The different clusters are characterized but not identified.</p>
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<p>Groups of intervals found using the unsupervised classification (UMED) and a PCA. The <span class="html-italic">L<sub>w</sub></span> has 128 samples. The first two principal components contain 53% of the full information. The different clusters are characterized but not identified.</p>
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<p>Groups of intervals found using the supervised classification (SM) [<a href="#B8-sensors-16-00590" class="html-bibr">8</a>] and the first two principal components of the <a href="#sensors-16-00590-f004" class="html-fig">Figure 4</a>. The <span class="html-italic">L<sub>w</sub></span> has 128 samples. The first two principal components contain 53% of the full information. The different clusters are identified. Using the <a href="#sensors-16-00590-t001" class="html-table">Table 1</a>: NN intervals are in <span class="html-italic">G</span><sub>1+2</sub>, the EB in <span class="html-italic">G</span><sub>3</sub>, the EUM in <span class="html-italic">G</span><sub>4</sub>, the ELM in <span class="html-italic">G</span><sub>5</sub>, the JM in <span class="html-italic">G</span><sub>6</sub>, and the JC in <span class="html-italic">G</span><sub>7</sub>.</p>
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<p>Events detected between the samples 46,389 and 46,653 using a <span class="html-italic">L<sub>w</sub><sup>H</sup></span> = 155, <span class="html-italic">L<sub>w</sub></span> = 128 and <span class="html-italic">L<sub>w</sub></span> = 165. The signal is a portion of an EEG channel.</p>
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217 KiB  
Review
Sensor Monitoring of Physical Activity to Improve Glucose Management in Diabetic Patients: A Review
by Sandrine Ding and Michael Schumacher
Sensors 2016, 16(4), 589; https://doi.org/10.3390/s16040589 - 23 Apr 2016
Cited by 64 | Viewed by 9882
Abstract
Diabetic individuals need to tightly control their blood glucose concentration. Several methods have been developed for this purpose, such as the finger-prick or continuous glucose monitoring systems (CGMs). However, these methods present the disadvantage of being invasive. Moreover, CGMs have limited accuracy, notably [...] Read more.
Diabetic individuals need to tightly control their blood glucose concentration. Several methods have been developed for this purpose, such as the finger-prick or continuous glucose monitoring systems (CGMs). However, these methods present the disadvantage of being invasive. Moreover, CGMs have limited accuracy, notably to detect hypoglycemia. It is also known that physical exercise, and even daily activity, disrupt glucose dynamics and can generate problems with blood glucose regulation during and after exercise. In order to deal with these challenges, devices for monitoring patients’ physical activity are currently under development. This review focuses on non-invasive sensors using physiological parameters related to physical exercise that were used to improve glucose monitoring in type 1 diabetes (T1DM) patients. These devices are promising for diabetes management. Indeed they permit to estimate glucose concentration either based solely on physical activity parameters or in conjunction with CGM or non-invasive CGM (NI-CGM) systems. In these last cases, the vital signals are used to modulate glucose estimations provided by the CGM and NI-CGM devices. Finally, this review indicates possible limitations of these new biosensors and outlines directions for future technologic developments. Full article
(This article belongs to the Special Issue Noninvasive Biomedical Sensors)
1359 KiB  
Article
Healthcare4VideoStorm: Making Smart Decisions Based on Storm Metrics
by Weishan Zhang, Pengcheng Duan, Xiufeng Chen and Qinghua Lu
Sensors 2016, 16(4), 588; https://doi.org/10.3390/s16040588 - 23 Apr 2016
Viewed by 5645
Abstract
Storm-based stream processing is widely used for real-time large-scale distributed processing. Knowing the run-time status and ensuring performance is critical to providing expected dependability for some applications, e.g., continuous video processing for security surveillance. The existing scheduling strategies’ granularity is too coarse to [...] Read more.
Storm-based stream processing is widely used for real-time large-scale distributed processing. Knowing the run-time status and ensuring performance is critical to providing expected dependability for some applications, e.g., continuous video processing for security surveillance. The existing scheduling strategies’ granularity is too coarse to have good performance, and mainly considers network resources without computing resources while scheduling. In this paper, we propose Healthcare4Storm, a framework that finds Storm insights based on Storm metrics to gain knowledge from the health status of an application, finally ending up with smart scheduling decisions. It takes into account both network and computing resources and conducts scheduling at a fine-grained level using tuples instead of topologies. The comprehensive evaluation shows that the proposed framework has good performance and can improve the dependability of the Storm-based applications. Full article
(This article belongs to the Special Issue Identification, Information & Knowledge in the Internet of Things)
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<p>Storm topology.</p>
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<p>Storm scheduling.</p>
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<p>Healthcare4VideoStorm architecture illustrated as a component-connector view.</p>
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<p>Metric sensor.</p>
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<p>Bottleneck detector: (<b>a</b>) Fuzzy Inference System (<b>b</b>) Kernel Density Estimator.</p>
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<p>Core classes of tuple routing.</p>
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<p>Metric patterns when rescheduling a topology.</p>
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<p>CPU-GPU switching architecture illustrated with background subtraction.</p>
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<p>Topologies for evaluation.</p>
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<p>Router performance under the CPU-intensive bottleneck maker.</p>
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<p>Router performance under the I/O-intensive bottleneck maker.</p>
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<p>Switcher performance under the CPU-intensive bottleneck maker.</p>
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<p>Switcher performance under the I/O-intensive bottleneck maker.</p>
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<p>A general video processing system using Storm.</p>
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6652 KiB  
Article
HybridPLAY: A New Technology to Foster Outdoors Physical Activity, Verbal Communication and Teamwork
by Diego José Díaz, Clara Boj and Cristina Portalés
Sensors 2016, 16(4), 586; https://doi.org/10.3390/s16040586 - 23 Apr 2016
Cited by 13 | Viewed by 8066
Abstract
This paper presents HybridPLAY, a novel technology composed of a sensor and mobile-based video games that transforms urban playgrounds into game scenarios. With this technology we aim to stimulate physical activity and playful learning by creating an entertaining environment in which users can [...] Read more.
This paper presents HybridPLAY, a novel technology composed of a sensor and mobile-based video games that transforms urban playgrounds into game scenarios. With this technology we aim to stimulate physical activity and playful learning by creating an entertaining environment in which users can actively participate and collaborate. HybridPLAY is different from other existing technologies that enhance playgrounds, as it is not integrated in them but can be attached to the different elements of the playgrounds, making its use more ubiquitous (i.e., not restricted to the playgrounds). HybridPLAY was born in 2007 as an artistic concept, and evolved after different phases of research and testing by almost 2000 users around the world (in workshops, artistic events, conferences, etc.). Here, we present the temporal evolution of HybridPLAY with the different versions of the sensors and the video games, and a detailed technical description of the sensors and the way interactions are produced. We also present the outcomes after the evaluation by users at different events and workshops. We believe that HybridPLAY has great potential to contribute to increased physical activity in kids, and also to improve the learning process and monitoring at school centres by letting users create the content of the apps, leading to new narratives and fostering creativity. Full article
(This article belongs to the Special Issue Sensors for Entertainment)
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Graphical abstract

Graphical abstract
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<p>HybridPLAY workflow.</p>
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<p>The HybridPLAY sensor. From left to right, the first, second and third versions.</p>
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<p>First version of the sensor. (<b>a</b>) The different models, according to the elements of the playground; (<b>b</b>) one of the sensors attached to the hobbyhorse.</p>
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<p>Video game example: (<b>a</b>) screenshot of the game Puzzle City; and (<b>b</b>) bracelet to hold a mobile device.</p>
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<p>Kids looking the score in the server screen (<b>a</b>–<b>c</b>). Details of the bracelet with the integrated RFID tag (<b>b</b>).</p>
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<p>Technical components of the third version of HybridPLAY.</p>
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<p>Image of the design process and different prototypes (<b>a</b>) and the final design (<b>b</b>).</p>
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<p>(<b>a</b>) Space Kids and (<b>b</b>) Puzzle City 2.</p>
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<p>Instructions to perform the calibration of the sensor with regards to the element of the playground.</p>
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<p>Screenshot of the video game Moskis.</p>
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<p>Screenshot of the adaptation of the classic arcade video game Pac Man.</p>
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<p>Instructions on how to trigger interaction with the swing.</p>
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<p>Example of the interaction produced in the game HybridEDU with the swing.</p>
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<p>Schematic of the interaction produced by placing the sensor on the slide. The system detects that the child is waiting for jumping.</p>
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<p>Cart of HybridPLAY in the park (<b>a</b>) with the monitor showing the score of the games and at one of the exhibitions (<b>b</b>) with the monitor showing a loop of the video games.</p>
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<p>Seniors playing with HybridPLAY at the elliptical machine (<b>a</b>) and at the ab twister (<b>b</b>).</p>
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<p>Children and parents designing their own games for HybridPLAY at the Medialab-Prado (Madrid, Spain) workshop.</p>
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3124 KiB  
Article
VitiCanopy: A Free Computer App to Estimate Canopy Vigor and Porosity for Grapevine
by Roberta De Bei, Sigfredo Fuentes, Matthew Gilliham, Steve Tyerman, Everard Edwards, Nicolò Bianchini, Jason Smith and Cassandra Collins
Sensors 2016, 16(4), 585; https://doi.org/10.3390/s16040585 - 23 Apr 2016
Cited by 88 | Viewed by 15532
Abstract
Leaf area index (LAI) and plant area index (PAI) are common and important biophysical parameters used to estimate agronomical variables such as canopy growth, light interception and water requirements of plants and trees. LAI can be either measured directly using destructive methods or [...] Read more.
Leaf area index (LAI) and plant area index (PAI) are common and important biophysical parameters used to estimate agronomical variables such as canopy growth, light interception and water requirements of plants and trees. LAI can be either measured directly using destructive methods or indirectly using dedicated and expensive instrumentation, both of which require a high level of know-how to operate equipment, handle data and interpret results. Recently, a novel smartphone and tablet PC application, VitiCanopy, has been developed by a group of researchers from the University of Adelaide and the University of Melbourne, to estimate grapevine canopy size (LAI and PAI), canopy porosity, canopy cover and clumping index. VitiCanopy uses the front in-built camera and GPS capabilities of smartphones and tablet PCs to automatically implement image analysis algorithms on upward-looking digital images of canopies and calculates relevant canopy architecture parameters. Results from the use of VitiCanopy on grapevines correlated well with traditional methods to measure/estimate LAI and PAI. Like other indirect methods, VitiCanopy does not distinguish between leaf and non-leaf material but it was demonstrated that the non-leaf material could be extracted from the results, if needed, to increase accuracy. VitiCanopy is an accurate, user-friendly and free alternative to current techniques used by scientists and viticultural practitioners to assess the dynamics of LAI, PAI and canopy architecture in vineyards, and has the potential to be adapted for use on other plants. Full article
(This article belongs to the Special Issue Sensors for Agriculture)
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<p>Example of an upward looking grapevine canopy image suitable for analysis using VitiCanopy. The image was obtained using the front camera of an iPad4, at a distance of 80 cm between the vine’s cordon and the device.</p>
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<p>VitiCanopy Home page displaying the five main menu tabs as a simplified operations flow chart.</p>
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<p>Relationship between the canopy size measured by analyzing the images using the Matlab method (LAI-Matlab) and VitiCanopy (LAI-vc). The continuous line represents the linear fitting; the dashed line represents the 1:1 relationship.</p>
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<p>Relationship between plant area index (LAI-vc) and effective plant are index (LAIvc<sub>e</sub> = LAI × Ω(0)) measured using the VitiCanopy App for three vineyards located in Langhorne Creek (SA), Hilltops (NSW) and Sunraysia (Vic) during the season 2013–14. The continuous line represents the calculated regression; the dashed line represents the 1:1 relationship.</p>
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<p>Relationship between the canopy size measured using the Licor-2000 (LAI-LAI-2000) and VitiCanopy App (LAI-vc<sub>e</sub>) for three vineyards located in Langhorne Creek (SA), Hilltops (NSW) and Sunraysia (Vic) during the season 2013–14. Error bars correspond to the standard error of the means. The continuous line represents the calculated regression passing through the origin (0,0), the dashed line represents the 1:1 relationship.</p>
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<p>(<b>a</b>) Relationship between the leaf area index (LAI) measured by destructively removing all the leaves (LAI<sub>r</sub>) and using the cover photography App VitiCanopy (LAI-vc<sub>e</sub>) using a common light extinction coefficient (<span class="html-italic">k</span> = 0.7) (method i) for the cv. Shiraz on a VSP trellis system in the McLaren Vale region; (<b>b</b>) Relationship between Real LAI (LAI<sub>r</sub>) and VitiCanopy LAI (LAI-vc<sub>e</sub>) extracting the Y—intercept related to cordon and non-leaf material inclusion. For 6a and 6b, the continuous line represents the calculated regression; the dashed line represents the 1:1 relationship.</p>
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<p>Linear regressions obtained from the comparison between real LAI (LAI<sub>r</sub>) and effective LAI using VitiCanopy (LAI-vc<sub>e</sub>) with different methods to obtain a proxy of light extinction coefficient (<span class="html-italic">k</span>): (<b>a</b>) obtaining a real <span class="html-italic">k</span> (<span class="html-italic">k<sub>r</sub></span>) by inverting Equation (7) (method ii); (<b>b</b>) Lowess linear interpolation model based on canopy cover (<span class="html-italic">f<sub>c</sub></span>) and porosity (Φ) (method iii); (<b>c</b>) <span class="html-italic">k</span> obtained from a linear regression between <span class="html-italic">k<sub>r</sub></span> and large gaps (lg) (method iv) and (<b>d</b>) <span class="html-italic">k</span> obtained from the ratio between image luminance (I) and maximum luminance (Io = 12) (method v).</p>
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405 KiB  
Article
Secure and Cost-Effective Distributed Aggregation for Mobile Sensor Networks
by Kehua Guo, Ping Zhang and Jianhua Ma
Sensors 2016, 16(4), 583; https://doi.org/10.3390/s16040583 - 23 Apr 2016
Cited by 4 | Viewed by 4997
Abstract
Secure data aggregation (SDA) schemes are widely used in distributed applications, such as mobile sensor networks, to reduce communication cost, prolong the network life cycle and provide security. However, most SDA are only suited for a single type of statistics (i.e., [...] Read more.
Secure data aggregation (SDA) schemes are widely used in distributed applications, such as mobile sensor networks, to reduce communication cost, prolong the network life cycle and provide security. However, most SDA are only suited for a single type of statistics (i.e., summation-based or comparison-based statistics) and are not applicable to obtaining multiple statistic results. Most SDA are also inefficient for dynamic networks. This paper presents multi-functional secure data aggregation (MFSDA), in which the mapping step and coding step are introduced to provide value-preserving and order-preserving and, later, to enable arbitrary statistics support in the same query. MFSDA is suited for dynamic networks because these active nodes can be counted directly from aggregation data. The proposed scheme is tolerant to many types of attacks. The network load of the proposed scheme is balanced, and no significant bottleneck exists. The MFSDA includes two versions: MFSDA-I and MFSDA-II. The first one can obtain accurate results, while the second one is a more generalized version that can significantly reduce network traffic at the expense of less accuracy loss. Full article
(This article belongs to the Special Issue Mobile Sensor Computing: Theory and Applications)
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<p>Network model.</p>
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<p>Mapping and encoding step of MFSDA-I.</p>
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<p>Communication cost comparison of RCDAand MFSDA.</p>
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<p>Communication cost comparison of MFSDA-I and MFSDA-II.</p>
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<p>Accuracy evaluation of the MFSDA variant. (<b>a</b>) Error rate of MEAN; (<b>b</b>) error rate of VAR; (<b>c</b>) error rate of STD; (<b>d</b>) error rate of MAX; (<b>e</b>) error rate of MEDIAN; (<b>f</b>) error rate of MIN.</p>
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2069 KiB  
Article
Optimizing Colorimetric Assay Based on V2O5 Nanozymes for Sensitive Detection of H2O2 and Glucose
by Jiaheng Sun, Chunyan Li, Yanfei Qi, Shuanli Guo and Xue Liang
Sensors 2016, 16(4), 584; https://doi.org/10.3390/s16040584 - 22 Apr 2016
Cited by 98 | Viewed by 10384
Abstract
Nanozyme-based chemical sensing is a rapidly emerging field of research. Herein, a simple colorimetric assay for the detection of hydrogen peroxide and glucose based on the peroxidase-like activity of V2O5 nanozymes has been established. In this assay, the effects of [...] Read more.
Nanozyme-based chemical sensing is a rapidly emerging field of research. Herein, a simple colorimetric assay for the detection of hydrogen peroxide and glucose based on the peroxidase-like activity of V2O5 nanozymes has been established. In this assay, the effects of pH, substrate, nanozyme concentrations and buffer solution have been investigated. It was found that compared with 3,3′,5,5′-tetramethylbenzidine (TMB), the enzyme substrate o-phenylenediamine (OPD) seriously interfered with the H2O2 detection. Under the optimal reaction conditions, the resulting sensor displayed a good response to H2O2 with a linear range of 1 to 500 μM, and a detection limit of 1 μM at a signal-to-noise ratio of 3. A linear correlation was established between absorbance intensity and concentration of glucose from 10 to 2000 μM, with a detection limit of 10 μM. The current work presents a simple, cheap, more convenient, sensitive, and easy handling colorimetric assay. Full article
(This article belongs to the Special Issue Colorimetric and Fluorescent Sensor)
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<p>Characterizations of V<sub>2</sub>O<sub>5</sub> nanozymes: (<b>a</b>) FTIR spectrum; (<b>b</b>) XRD pattern; (<b>c</b>) TEM images.</p>
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<p>The catalytic effect of V<sub>2</sub>O<sub>5</sub> nanozymes with TMB (<b>a</b>) and OPD (<b>b</b>) as the substrate in the presence of H<sub>2</sub>O<sub>2</sub>.</p>
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<p>Effects of pH with TMB (<b>a</b>) and OPD (<b>b</b>) substrate, respectively. The error bars represent the standard deviation of three measurements.</p>
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<p>Activities of V<sub>2</sub>O<sub>5</sub> nanozymes in, pH 4.0, 0.2 M buffers, with TMB (<b>a</b>) and OPD (<b>b</b>), respectively. The error bars represent the standard deviation of three measurements.</p>
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<p>Effects of the V<sub>2</sub>O<sub>5</sub> nanozymes concentrations ranging from 0 up to 1 mM in pH 4.0 NaOAc-HOAc buffer solution, with TMB (<b>a</b>) and OPD (<b>b</b>) respectively.</p>
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<p>Steady-state kinetic assay and catalytic mechanism of V<sub>2</sub>O<sub>5</sub> nanozymes as peroxidase mimic.</p>
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<p>Linear calibration plot for H<sub>2</sub>O<sub>2</sub> from 1 to 500 μM in, pH 4.0, 0.2 M NaOAc-HOAc buffers, with TMB (<b>a</b>) and OPD (<b>b</b>) respectively (<span class="html-italic">p</span> &lt; 0.05). The inset shows dependence of the absorbance on the concentration of H<sub>2</sub>O<sub>2</sub>.</p>
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<p>Linear calibration plot for glucose from 10 to 2000 μM (<span class="html-italic">p</span> &lt; 0.05). The inset shows dependence of the absorbance on the concentration of glucose in the range from 0 to 4 mM.</p>
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6128 KiB  
Article
High Temperature Shear Horizontal Electromagnetic Acoustic Transducer for Guided Wave Inspection
by Maria Kogia, Tat-Hean Gan, Wamadeva Balachandran, Makis Livadas, Vassilios Kappatos, Istvan Szabo, Abbas Mohimi and Andrew Round
Sensors 2016, 16(4), 582; https://doi.org/10.3390/s16040582 - 22 Apr 2016
Cited by 38 | Viewed by 8698
Abstract
Guided Wave Testing (GWT) using novel Electromagnetic Acoustic Transducers (EMATs) is proposed for the inspection of large structures operating at high temperatures. To date, high temperature EMATs have been developed only for thickness measurements and they are not suitable for GWT. A pair [...] Read more.
Guided Wave Testing (GWT) using novel Electromagnetic Acoustic Transducers (EMATs) is proposed for the inspection of large structures operating at high temperatures. To date, high temperature EMATs have been developed only for thickness measurements and they are not suitable for GWT. A pair of water-cooled EMATs capable of exciting and receiving Shear Horizontal (SH0) waves for GWT with optimal high temperature properties (up to 500 °C) has been developed. Thermal and Computational Fluid Dynamic (CFD) simulations of the EMAT design have been performed and experimentally validated. The optimal thermal EMAT design, material selection and operating conditions were calculated. The EMAT was successfully tested regarding its thermal and GWT performance from ambient temperature to 500 °C. Full article
(This article belongs to the Section Physical Sensors)
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<p>Thermal EMAT model (<b>a</b>) entire EMAT design; (<b>b</b>) Cooling chamber; (<b>c</b>) Coil.</p>
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<p>Temperature gradient of alumina encapsulated coil (<b>a</b>) 0.75 mm alumina thickness; (<b>b</b>) 1 mm alumina thickness.</p>
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<p>Optimum ceramic thickness graph.</p>
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<p>Temperature gradient of Kapton and alumina encapsulated coil (<b>a</b>) 0.75 mm alumina thickness; (<b>b</b>) 1 mm alumina thickness.</p>
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<p>(<b>a</b>) EMAT temperature against coolant flow velocity; (<b>b</b>) EMAT temperature against coolant temperature.</p>
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<p>Water cooled EMAT (<b>a</b>) temperature gradient of EMAT components at 500 °C; (<b>b</b>) temperature of EMAT components against temperature rise. The temperature range of the magnets, coil and the cooling medium are depicted in figure a.</p>
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<p>(<b>a</b>) EMAT design; (<b>b</b>) EMAT prototype.</p>
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<p>(<b>a</b>) Constantan Coil; (<b>b</b>) Alumina and Kapton encapsulated coil (in mm).</p>
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<p>Experimental setup.</p>
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<p>Signal received by Nd-F-B and SmCo EMAT on steel at (<b>a</b>) room temperature; (<b>b</b>) 250 °C; (<b>c</b>) 500 °C; (<b>d</b>) amplitude drop against temperature rise.</p>
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<p>Signal received by Nd-F-B and SmCo EMAT on stainless steel at (<b>a</b>) room temperature; (<b>b</b>) 250 °C; (<b>c</b>) 500 °C; (<b>d</b>) amplitude drop against temperature rise.</p>
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<p>Measured temperature of EMAT coil and magnets <span class="html-italic">vs.</span> temperature.</p>
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Article
Localized Electrical Impedance Myography of the Biceps Brachii Muscle during Different Levels of Isometric Contraction and Fatigue
by Le Li, Henry Shin, Xiaoyan Li, Sheng Li and Ping Zhou
Sensors 2016, 16(4), 581; https://doi.org/10.3390/s16040581 - 22 Apr 2016
Cited by 43 | Viewed by 8167
Abstract
This study assessed changes in electrical impedance myography (EIM) at different levels of isometric muscle contraction as well as during exhaustive exercise at 60% maximum voluntary contraction (MVC) until task failure. The EIM was performed on the biceps brachii muscle of 19 healthy [...] Read more.
This study assessed changes in electrical impedance myography (EIM) at different levels of isometric muscle contraction as well as during exhaustive exercise at 60% maximum voluntary contraction (MVC) until task failure. The EIM was performed on the biceps brachii muscle of 19 healthy subjects. The results showed that there was a significant difference between the muscle resistance (R) measured during the isometric contraction and when the muscle was completely relaxed. Post hoc analysis shows that the resistance increased at higher contractions (both 60% MVC and MVC), however, there were no significant changes in muscle reactance (X) during the isometric contractions. The resistance also changed during different stages of the fatigue task and there were significant decreases from the beginning of the contraction to task failure as well as between task failure and post fatigue rest. Although our results demonstrated an increase in resistance during isometric contraction, the changes were within 10% of the baseline value. These changes might be related to the modest alterations in muscle architecture during a contraction. The decrease in resistance seen with muscle fatigue may be explained by an accumulation of metabolites in the muscle tissue. Full article
(This article belongs to the Special Issue Noninvasive Biomedical Sensors)
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<p>Experimental setup of EIM measurement during contraction.</p>
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<p>Resistance (<b>A</b>) and Reactance (<b>B</b>) at isometric contraction with two different frequencies (50 kHz and 100 kHz) (mean ± standard deviation, * indicates <span class="html-italic">p</span> &lt; 0.05 between contraction levels).</p>
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<p>Resistance (<b>A</b>) and Reactance (<b>B</b>) at isometric contraction with two different frequencies (50 kHz and 100 kHz) (mean ± standard deviation, * indicates <span class="html-italic">p</span> &lt; 0.05 between contraction levels).</p>
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<p>Resistance (<b>A</b>) and Reactance (<b>B</b>) at fatigue tests with two different frequencies (50 kHz and 100 kHz) (mean ± standard deviation, * indicates <span class="html-italic">p</span> &lt; 0.05 between contraction conditions during fatigue task).</p>
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<p>Resistance (<b>A</b>) and Reactance (<b>B</b>) at fatigue tests with two different frequencies (50 kHz and 100 kHz) (mean ± standard deviation, * indicates <span class="html-italic">p</span> &lt; 0.05 between contraction conditions during fatigue task).</p>
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<p>Correlation between the task failure time and the change of resistance during sustained contraction in fatigue test (<span class="html-italic">p</span> = 0.0159).</p>
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Article
Outlier Detection in GNSS Pseudo-Range/Doppler Measurements for Robust Localization
by Salim Zair, Sylvie Le Hégarat-Mascle and Emmanuel Seignez
Sensors 2016, 16(4), 580; https://doi.org/10.3390/s16040580 - 22 Apr 2016
Cited by 15 | Viewed by 8056
Abstract
In urban areas or space-constrained environments with obstacles, vehicle localization using Global Navigation Satellite System (GNSS) data is hindered by Non-Line Of Sight (NLOS) and multipath receptions. These phenomena induce faulty data that disrupt the precise localization of the GNSS receiver. In this [...] Read more.
In urban areas or space-constrained environments with obstacles, vehicle localization using Global Navigation Satellite System (GNSS) data is hindered by Non-Line Of Sight (NLOS) and multipath receptions. These phenomena induce faulty data that disrupt the precise localization of the GNSS receiver. In this study, we detect the outliers among the observations, Pseudo-Range (PR) and/or Doppler measurements, and we evaluate how discarding them improves the localization. We specify a contrario modeling for GNSS raw data to derive an algorithm that partitions the dataset between inliers and outliers. Then, only the inlier data are considered in the localization process performed either through a classical Particle Filter (PF) or a Rao-Blackwellization (RB) approach. Both localization algorithms exclusively use GNSS data, but they differ by the way Doppler measurements are processed. An experiment has been performed with a GPS receiver aboard a vehicle. Results show that the proposed algorithms are able to detect the ‘outliers’ in the raw data while being robust to non-Gaussian noise and to intermittent satellite blockage. We compare the performance results achieved either estimating only PR outliers or estimating both PR and Doppler outliers. The best localization is achieved using the RB approach coupled with PR-Doppler outlier estimation. Full article
(This article belongs to the Section Physical Sensors)
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<p>(<b>a</b>) Experimental platform with the three GPS visible on the roof of the car; (<b>b</b>,<b>c</b>) trajectory of the experiment, either (<b>b</b>) plotted on Google Earth<math display="inline"> <semantics> <msup> <mrow/> <mi>©</mi> </msup> </semantics> </math> or (<b>c</b>) labeled in terms of the quality of the Real-Time Kinematic (RTK) solution (“ground truth”).</p>
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<p>Skyplot configuration during the experimental data acquisition in the urban area.</p>
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<p>Cumulative distribution function of errors achieved by the four versions of KF, the five versions of particle filters and the two GPS solutions for our experiment of 11 min and 40 s.</p>
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<p><math display="inline"> <semantics> <mrow> <mover accent="true"> <mo>Δ</mo> <mo stretchy="false">˜</mo> </mover> <msub> <mi>m</mi> <mi>j</mi> </msub> </mrow> </semantics> </math> estimations on PR measurements acquired by the different satellites (numbered between 1 and 32). Red markers point out PR outliers detected by NFA.</p>
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<p><math display="inline"> <semantics> <mrow> <mover accent="true"> <mo>Δ</mo> <mo stretchy="false">˜</mo> </mover> <msub> <mover accent="true"> <mi>m</mi> <mo>˙</mo> </mover> <mi>j</mi> </msub> </mrow> </semantics> </math> estimations on Doppler measurements acquired by the different satellites (numbered between 1 and 32). Red markers point out Dp outliers detected by NFA.</p>
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Article
A Practical and Portable Solids-State Electronic Terahertz Imaging System
by Ken Smart, Jia Du, Li Li, David Wang, Keith Leslie, Fan Ji, Xiang Dong Li and Da Zhang Zeng
Sensors 2016, 16(4), 579; https://doi.org/10.3390/s16040579 - 22 Apr 2016
Cited by 7 | Viewed by 6601
Abstract
A practical compact solid-state terahertz imaging system is presented. Various beam guiding architectures were explored and hardware performance assessed to improve its compactness, robustness, multi-functionality and simplicity of operation. The system performance in terms of image resolution, signal-to-noise ratio, the electronic signal modulation [...] Read more.
A practical compact solid-state terahertz imaging system is presented. Various beam guiding architectures were explored and hardware performance assessed to improve its compactness, robustness, multi-functionality and simplicity of operation. The system performance in terms of image resolution, signal-to-noise ratio, the electronic signal modulation versus optical chopper, is evaluated and discussed. The system can be conveniently switched between transmission and reflection mode according to the application. A range of imaging application scenarios was explored and images of high visual quality were obtained in both transmission and reflection mode. Full article
(This article belongs to the Special Issue Infrared and THz Sensing and Imaging)
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<p>Examples of the system improvement steps with varied hardware and the beam guiding schemes.</p>
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<p>A view of the full system mounted on a portable optical plate (450 mm × 750 mm) showing a linearly aligned source-lenses-sample-detector scheme and a removable beam splitter (inset) for changing between transmission and reflection mode.</p>
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<p>Schematic of the quasi-optical THz transmission and reflection imaging system.</p>
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<p>(<b>a</b>) A transmission image of a computer floppy disk; a scanned area of 50 mm × 50 mm at a resolution of 0.5 mm. The black lines indicate the single line scans at vertical line 17 and horizontal line 23; (<b>b</b>) is the photograph of the floppy disk flipped to correspond to scanned image.</p>
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<p>Line scans of the image data: the detected signal level of the transmitted THz beam <span class="html-italic">versus</span> the pixel point (upper <span class="html-italic">x</span>-axis) and spatial position (lower <span class="html-italic">x</span>-axis). (<b>a</b>) corresponds to the single line scans at vertical line 17 in <a href="#sensors-16-00579-f004" class="html-fig">Figure 4</a>a and (<b>b</b>) corresponds to the horizontal line 23 shown in <a href="#sensors-16-00579-f004" class="html-fig">Figure 4</a>a. The upper <span class="html-italic">x</span> axis shows the image pixel points (0.5 mm each step) and lower axis is converted the position points in both figures.</p>
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<p>Imaging of a 50 cents coin and a Kangaroo key ring in a reflection mode (note that the experiment was carried out before the introduction of the cube mounted beam splitter shown in <a href="#sensors-16-00579-f002" class="html-fig">Figure 2</a>).</p>
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<p>Imaging in reflection mode, showing a hidden object in shoe lining.</p>
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<p>Photograph (<b>a</b>) and the transmission THz image (<b>b</b>) of a fresh leaf.</p>
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<p>Real-time detector voltage output V<sub>RF</sub> (t) traces of the modulated THz beam using a mechanical optical chopper (<b>a</b>) and an electronic signal via the TTL port on the AMC THz source (<b>b</b>).</p>
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<p>The THz transmission image of the computer disk acquired using the TTL electronic signal modulation at the same chopper speed of 1 kHz and scanning conditions as that used in <a href="#sensors-16-00579-f004" class="html-fig">Figure 4</a> image modulated with an optic chopper.</p>
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8695 KiB  
Article
Vision-Based Leader Vehicle Trajectory Tracking for Multiple Agricultural Vehicles
by Linhuan Zhang, Tofael Ahamed, Yan Zhang, Pengbo Gao and Tomohiro Takigawa
Sensors 2016, 16(4), 578; https://doi.org/10.3390/s16040578 - 22 Apr 2016
Cited by 18 | Viewed by 6682
Abstract
The aim of this study was to design a navigation system composed of a human-controlled leader vehicle and a follower vehicle. The follower vehicle automatically tracks the leader vehicle. With such a system, a human driver can control two vehicles efficiently in agricultural [...] Read more.
The aim of this study was to design a navigation system composed of a human-controlled leader vehicle and a follower vehicle. The follower vehicle automatically tracks the leader vehicle. With such a system, a human driver can control two vehicles efficiently in agricultural operations. The tracking system was developed for the leader and the follower vehicle, and control of the follower was performed using a camera vision system. A stable and accurate monocular vision-based sensing system was designed, consisting of a camera and rectangular markers. Noise in the data acquisition was reduced by using the least-squares method. A feedback control algorithm was used to allow the follower vehicle to track the trajectory of the leader vehicle. A proportional–integral–derivative (PID) controller was introduced to maintain the required distance between the leader and the follower vehicle. Field experiments were conducted to evaluate the sensing and tracking performances of the leader-follower system while the leader vehicle was driven at an average speed of 0.3 m/s. In the case of linear trajectory tracking, the RMS errors were 6.5 cm, 8.9 cm and 16.4 cm for straight, turning and zigzag paths, respectively. Again, for parallel trajectory tracking, the root mean square (RMS) errors were found to be 7.1 cm, 14.6 cm and 14.0 cm for straight, turning and zigzag paths, respectively. The navigation performances indicated that the autonomous follower vehicle was able to follow the leader vehicle, and the tracking accuracy was found to be satisfactory. Therefore, the developed leader-follower system can be implemented for the harvesting of grains, using a combine as the leader and an unloader as the autonomous follower vehicle. Full article
(This article belongs to the Section Physical Sensors)
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<p>The autonomous follower in the leader-follower system. (<b>a</b>) Sensors arrangements in the autonomous unit; (<b>b</b>) Hardware components of the autonomous follower tracking system.</p>
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<p>Geometrical disposition between the leader and the follower. (<b>a</b>) Leader-follower relative position; (<b>b</b>) Relative position between camera and marker plane; (<b>c</b>). Servo motor implemented with the camera-marker system.</p>
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<p>Image processing for marker detection. (<b>a</b>) Contour image; (<b>b</b>) Detected marker.</p>
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<p>Camera perspective model.</p>
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<p>Model for offsetting vehicle roll effect.</p>
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<p>Relationship and coordinate transformation between the leader and the follower vehicles.</p>
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<p>Field experiments of the leader-follower system. (<b>a</b>) Evaluation of the camera–marker system; (<b>b</b>) Tracking of a trajectory of the leader vehicle.</p>
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<p>Position of the marker. (<b>a</b>) Location of the marker; (<b>b</b>) Relative angle between the marker and the x-axis.</p>
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<p>Linear Regression and Accuracy analysis of the camera observation referenced with the laser observation. (<b>a</b>) Distance; (<b>b</b>) Relative angle; (<b>c</b>) Orientation angle; (<b>d</b>) Distance error; (<b>e</b>) Relative angle error; (<b>f</b>) Orientation angle error.</p>
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<p>Linear Regression and Accuracy analysis of the camera observation referenced with the laser observation. (<b>a</b>) Distance; (<b>b</b>) Relative angle; (<b>c</b>) Orientation angle; (<b>d</b>) Distance error; (<b>e</b>) Relative angle error; (<b>f</b>) Orientation angle error.</p>
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<p>Relative position between the camera and marker before smooth, smoothed, and LRF data. (<b>a</b>) Relative distance; (<b>b</b>) Relative angle.</p>
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<p>Relative position error for camera observation. (<b>a</b>) Relative distance error; (<b>b</b>) Relative angle error.</p>
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<p>Dispersion of camera observation data. (<b>a</b>) Dispersion of relative distance; (<b>b</b>) Dispersion of relative angle.</p>
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<p>Leader trajectory tracking on a straight path. (<b>a</b>)Linear tracking; (<b>b</b>) Parallel tracking.</p>
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<p>Leader trajectory tracking on a turning path. (<b>a</b>)Linear tracking; (<b>b</b>) Parallel tracking.</p>
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<p>Leader trajectory tracking on a zigzag path. (<b>a</b>)Linear tracking; (<b>b</b>) Parallel tracking.</p>
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<p>Leader trajectory tracking on a zigzag path. (<b>a</b>)Linear tracking; (<b>b</b>) Parallel tracking.</p>
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<p>Tracking error between leader and the follower trajectories during tracking on a straight path. (<b>a</b>) Linear tracking; (<b>b</b>) Parallel tracking.</p>
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<p>Tracking error between the leader and the follower trajectories during tracking on a turning path. (<b>a</b>) Linear tracking; (<b>b</b>) Parallel tracking.</p>
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<p>Tracking error between the leader and the follower trajectory during tracking on a zigzag path. (<b>a</b>) Linear tracking; (<b>b</b>) Parallel tracking.</p>
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492 KiB  
Article
A New Elliptical Model for Device-Free Localization
by Qian Lei, Haijian Zhang, Hong Sun and Linling Tang
Sensors 2016, 16(4), 577; https://doi.org/10.3390/s16040577 - 22 Apr 2016
Cited by 30 | Viewed by 5138
Abstract
Device-free localization (DFL) based on wireless sensor networks (WSNs) is expected to detect and locate a person without the need for any wireless devices. Radio tomographic imaging (RTI) has attracted wide attention from researchers as an emerging important technology in WSNs. However, there [...] Read more.
Device-free localization (DFL) based on wireless sensor networks (WSNs) is expected to detect and locate a person without the need for any wireless devices. Radio tomographic imaging (RTI) has attracted wide attention from researchers as an emerging important technology in WSNs. However, there is much room for improvement in localization estimation accuracy. In this paper, we propose a geometry-based elliptical model and adopt the orthogonal matching pursuit (OMP) algorithm. The new elliptical model uses not only line-of-sight information, but also non-line-of-sight information, which divides one ellipse into several areas with different weights. Meanwhile the OMP, which can eliminate extra bright spots in image reconstruction, is used to derive an image estimator. The experimental results demonstrate that the proposed algorithm could improve the accuracy of positioning by up to 23.8% for one person and 33.3% for two persons over some state-of-the-art RTI methods. Full article
(This article belongs to the Section Sensor Networks)
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<p>(<b>a</b>) The monitoring environment used in the experiments; (<b>b</b>) The elliptical model which is used in [<a href="#B18-sensors-16-00577" class="html-bibr">18</a>,<a href="#B19-sensors-16-00577" class="html-bibr">19</a>] representing one link in the monitoring area.</p>
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<p>The communication channels inside one ellipse.</p>
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<p>(<b>a</b>) When <span class="html-italic">β</span> = 0, the relationship between MSE and <span class="html-italic">k</span><sub>1</sub>; (<b>b</b>) When <span class="html-italic">k</span><sub>1</sub> = 2, the relationship between mean-square error (MSE) and <span class="html-italic">β</span>; (<b>c</b>) The weightings of voxels, which is shown as link 2 in <a href="#sensors-16-00577-f001" class="html-fig">Figure 1</a>a; (<b>d</b>) The division of the ellipse in <a href="#sensors-16-00577-f003" class="html-fig">Figure 3</a>c.</p>
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<p>(<b>a</b>) All positions (red rectangles) in the experiment field; (<b>b</b>) The difference between the actual position (red rectangle), the estimated position (white voxel), and the experiment result in [<a href="#B18-sensors-16-00577" class="html-bibr">18</a>] (blue rectangle), when a person stood at coordinate (3 m,3 m); (<b>c</b>) The experiment result in all 35 positions for the localization of one person; (<b>d</b>) As the number of voxels increased, the contrast between two algorithms for the localization of one person; (<b>e</b>) The radio tomographic imaging (RTI) algorithm in the first eight positions for the localization of one person; (<b>f</b>) The proposed algorithm in the first eight positions for the localization of one person.</p>
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<p>(<b>a</b>) The differences between the actual positions (red rectangles), the estimated positions (white voxels), and the experiment results in [<a href="#B18-sensors-16-00577" class="html-bibr">18</a>] (blue rectangles), when two persons stood at coordinates (1 m,5 m) and (6 m,5 m); (<b>b</b>) The result of the experiment for the localizations of two persons.</p>
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Article
Measuring Electrolyte Impedance and Noise Simultaneously by Triangular Waveform Voltage and Principal Component Analysis
by Shanzhi Xu, Peng Wang and Yonggui Dong
Sensors 2016, 16(4), 576; https://doi.org/10.3390/s16040576 - 22 Apr 2016
Cited by 10 | Viewed by 6163
Abstract
In order to measure the impedance variation process in electrolyte solutions, a method of triangular waveform voltage excitation is investigated together with principal component analysis (PCA). Using triangular waveform voltage as the excitation signal, the response current during one duty cycle is sampled [...] Read more.
In order to measure the impedance variation process in electrolyte solutions, a method of triangular waveform voltage excitation is investigated together with principal component analysis (PCA). Using triangular waveform voltage as the excitation signal, the response current during one duty cycle is sampled to construct a measurement vector. The measurement matrix is then constructed by the measurement vectors obtained from different measurements. After being processed by PCA, the changing information of solution impedance is contained in the loading vectors while the response current and noise information is contained in the score vectors. The measurement results of impedance variation by the proposed signal processing method are independent of the equivalent impedance model. The noise-induced problems encountered during equivalent impedance calculation are therefore avoided, and the real-time variation information of noise in the electrode-electrolyte interface can be extracted at the same time. Planar-interdigitated electrodes are experimentally tested for monitoring the KCl concentration variation process. Experimental results indicate that the measured impedance variation curve reflects the changing process of solution conductivity, and the amplitude distribution of the noise during one duty cycle can be utilized to analyze the contact conditions of the electrode and electrolyte interface. Full article
(This article belongs to the Section Physical Sensors)
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<p>Schematic diagram of the impedance measurement system. FPGA: Field-programmable gate array; DDS: Direct digital synthesizer; D/A: Digital-to-analog converter; A/D: Analog-to-digital converter; (І): Current-to-voltage converter; (II): Voltage amplifier. PC: Personal computer.</p>
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<p>Results after principal component analysis (PCA) processing: (<b>a</b>) PC1–PC4 scores plot; (<b>b</b>) PC1–PC4 loadings plot.</p>
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<p>Current before and after PCA processing.</p>
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<p>Comparison of the calculated results. SSA: Singular spectrum analysis. PC1(SSA) + 0.2: PC1 loading curve after SSA processing with a bias of 0.2; PC1 + 0.1: PC1 loading curve with a bias of 0.1; C: Capacitance variation curve.</p>
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<p>Diagram of three kinds of the planar-interdigitated electrodes (IDT) used. Au-IDT: Au electrode on Si substrate; Cu-IDT: Cu electrode on printed circuit board (PCB) substrate; and Au-Cu-IDT: Au electrode on PCB substrate.</p>
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<p>Measurement results of KCl base solution conducted with Au-IDT excited by triangular waveform voltage of different parameters: (<b>a</b>) A = 0.2 V; (<b>b</b>) A = 1 V.</p>
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<p>Measurement results of KCl solution conductivity variation process conducted with Au-IDT: (<b>a</b>) PC1–PC8 scores plot; (<b>b</b>) 3-D image of the reconstructed noise in one sampling period.</p>
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<p>Measurement results of KCl solution conductivity variation process conducted with Au-IDT: (<b>a</b>) PC1 loading curve (after SSA) and the reconstructed noise image of the measurement period (0–20 min); (<b>b</b>) PC1 loading curve (before and after SSA) and theoretical conductivity variation curve of the first stage (0–5 min); (<b>c</b>) PC1 loading curve (before and after SSA) and theoretical conductivity variation curve of the second stage (5–10 min); (<b>d</b>) PC1 loading curve (before and after SSA) and theoretical conductivity variation curve of the third stage (10–20 min).</p>
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<p>Measurement results of KCl solution conductivity variation conducted with the modified Au-IDT covered with self-assembled monolayers (SAM-Au-IDT): (<b>a</b>) PC1–PC8 scores plot; (<b>b</b>) PC1 loading curve (after SSA) and the reconstructed noise image of the measurement period (0–20 min).</p>
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<p>Measurement results of the KCl background solution conducted with Au-IDT: (<b>a</b>) PC1–PC8 scores plot; (<b>b</b>) PC1 loading curve (after SSA) and the residual noise image; (<b>c</b>) The residual noise signal at 360 s.</p>
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<p>Measurement results of Mercaptopropionic Acid (MPA) solution conducted with Au-IDT: (<b>a</b>) PC1–PC8 scores plot; (<b>b</b>) PC1 loading curve (after SSA) and the reconstructed noise image.</p>
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<p>Measurement results of the KCl background solution conducted with Au-Cu-IDT: (<b>a</b>) PC1–PC8 scores plot; (<b>b</b>) PC1 loading curve (after SSA) and the reconstructed noise image.</p>
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<p>Measurement results of the KCl background solution conducted with Cu-IDT: (<b>a</b>) PC1–PC8 scores plot; (<b>b</b>) PC1 loading curve (after SSA) and the reconstructed noise image.</p>
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1999 KiB  
Article
Design and Analysis of Cost-Efficient Sensor Deployment for Tracking Small UAS with Agent-Based Modeling
by Sangmi Shin, Seongha Park, Yongho Kim and Eric T. Matson
Sensors 2016, 16(4), 575; https://doi.org/10.3390/s16040575 - 22 Apr 2016
Cited by 5 | Viewed by 5437
Abstract
Recently, commercial unmanned aerial systems (UAS) have gained popularity. However, these UAS are potential threats to people in terms of safety in public places, such as public parks or stadiums. To reduce such threats, we consider a design, modeling, and evaluation of a [...] Read more.
Recently, commercial unmanned aerial systems (UAS) have gained popularity. However, these UAS are potential threats to people in terms of safety in public places, such as public parks or stadiums. To reduce such threats, we consider a design, modeling, and evaluation of a cost-efficient sensor system that detects and tracks small UAS. In this research, we focus on discovering the best sensor deployments by simulating different types and numbers of sensors in a designated area, which provide reasonable detection rates at low costs. Also, the system should cover the crowded areas more thoroughly than vacant areas to reduce direct threats to people underneath. This research study utilized the Agent-Based Modeling (ABM) technique to model a system consisting of independent and heterogeneous agents that interact with each other. Our previous work presented the ability to apply ABM to analyze the sensor configurations with two types of radars in terms of cost-efficiency. The results from the ABM simulation provide a list of candidate configurations and deployments that can be referred to for applications in the real world environment. Full article
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<p>The three well-known commercial quadcopter unmanned aerial systems (UAS): DJI Phantom 3 [<a href="#B3-sensors-16-00575" class="html-bibr">3</a>] (Left); Parrot AR. Drone 2.0 [<a href="#B4-sensors-16-00575" class="html-bibr">4</a>] (Middle); 3DR IRIS+ [<a href="#B5-sensors-16-00575" class="html-bibr">5</a>] (Right).</p>
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<p>800 × 4000 pixel monochrome map of Central Park used as the target environment (<b>black</b>: roads/trails; <b>white</b>: lawn areas).</p>
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<p>Behavior model verification: examples of results with low detection rates (<b>Left</b>) and high detection rates (<b>Right</b>) from the verification experiment (red line: UAS flight path, circles: positions of the radar).</p>
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<p>Examples of arbitrary flight patterns generated by Robotics Toolbox. (x, y, z in meters).</p>
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<p>Sensor deployments of the best samples (ranking numbers on the top left). Circles represents each radar’s detection range.</p>
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<p>Detection rates including penalties (<span class="html-italic">y</span> axis) by number of each radar (<span class="html-italic">x</span> axis).</p>
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2381 KiB  
Article
Protein Chips for Detection of Salmonella spp. from Enrichment Culture
by Palmiro Poltronieri, Fabio Cimaglia, Enrico De Lorenzis, Maurizio Chiesa, Valeria Mezzolla and Ida Barbara Reca
Sensors 2016, 16(4), 574; https://doi.org/10.3390/s16040574 - 22 Apr 2016
Cited by 9 | Viewed by 7749
Abstract
Food pathogens are the cause of foodborne epidemics, therefore there is a need to detect the pathogens in food productions rapidly. A pre-enrichment culture followed by selective agar plating are standard detection methods. Molecular methods such as qPCR have provided a first rapid [...] Read more.
Food pathogens are the cause of foodborne epidemics, therefore there is a need to detect the pathogens in food productions rapidly. A pre-enrichment culture followed by selective agar plating are standard detection methods. Molecular methods such as qPCR have provided a first rapid protocol for detection of pathogens within 24 h of enrichment culture. Biosensors also may provide a rapid tool to individuate a source of Salmonella contamination at early times of pre-enrichment culture. Forty mL of Salmonella spp. enrichment culture were processed by immunoseparation using the Pathatrix, as in AFNOR validated qPCR protocols. The Salmonella biosensor combined with immunoseparation showed a limit of detection of 100 bacteria/40 mL, with a 400 fold increase to previous results. qPCR analysis requires processing of bead-bound bacteria with lysis buffer and DNA clean up, with a limit of detection of 2 cfu/50 μL. Finally, a protein chip was developed and tested in screening and identification of 5 common pathogen species, Salmonella spp., E. coli, S. aureus, Campylobacter spp. and Listeria spp. The protein chip, with high specificity in species identification, is proposed to be integrated into a Lab-on-Chip system, for rapid and reproducible screening of Salmonella spp. and other pathogen species contaminating food productions. Full article
(This article belongs to the Section Biosensors)
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<p>Scheme of protocol used, from Pathatrix immunoseparation to protein chip detection.</p>
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<p><b>Protein chip detection of bacteria immunoseparated using in-house made magnetic beads.</b> Fluorescence intensity showing the protein chip results of bacteria immunoseparated using three types of magnetic beads: (<b>a</b>) beads made using anti-<span class="html-italic">Salmonella</span> antibody indirectly bound by biotinylated group to streptavidin magnetic beads; (<b>b</b>) anti-Gram negative antibody; (<b>c</b>) Pathatrix beads. Scale: square size 4 mm.</p>
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<p>Assessing the limit of detection of protein chips using serial dilutions of <span class="html-italic">Salmonella</span> spp. Protein chips hybridised with serial dilutions of Salmonella cells after elution by thermal treatment of magnetic beads. Quantification of colony forming units performed in parallel by plating bacteria on XLD-Agar. Each sub-array was hybridised with a serial dilution of <span class="html-italic">Salmonella</span>, 10<sup>6</sup> cfu/mL. (<b>a</b>) 10<sup>5</sup> cfu/mL; (<b>b</b>), 10<sup>4</sup>cfu/mL; (<b>c</b>) 10<sup>3</sup> cfu/mL; (<b>d</b>) and 100 cfu/mL; (<b>e</b>) Signals obtained by direct labelling of bacteria with Alexa 646. Experiments were repeated at least three times. Size of subarrays: 3 × 3 mm.</p>
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<p>Scheme of printed slides in 2 subarrays, with slide holder closing gasket (digits in mm).</p>
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<p>Assessment of performance of protein chips in detection of multiple bacterial species Left Upper line: Scheme of antibodies spotted in the <span class="html-italic">x</span>, <span class="html-italic">y</span> axis. Yellow: anti-<span class="html-italic">E. coli</span> Antibodies; orange: anti-<span class="html-italic">Salmonella</span> Abs; black: anti-<span class="html-italic">C. jejuni</span> Abs; green: anti-<span class="html-italic">Listeria monocytogenes</span> Abs; red: anti-<span class="html-italic">S. aureus</span> Abs. Size of the subarray area is 3 × 3 mm. <span class="html-italic">Salmonella</span> spp. were recognised by anti-<span class="html-italic">Salmonella</span> specific antibodies (<b>b</b>); <span class="html-italic">E. coli</span> (<b>a</b>) was detected in the anti-<span class="html-italic">E.coli</span> Ab spots. (<b>c</b>) <span class="html-italic">C. jejuni</span> was recognised by anti-<span class="html-italic">C. jejuni</span> Abs; (<b>d</b>) <span class="html-italic">Listeria monocytogenes</span> was recognised by anti-<span class="html-italic">Listeria</span> Abs; (<b>e</b>) <span class="html-italic">Staphylococcus aureus</span> was recognised by anti-<span class="html-italic">S. aureus</span> Abs. Experiments were repeated at least three times. Scale in mm. Each subarray area was 3 × 3 mm.</p>
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3682 KiB  
Article
Signal Analysis and Waveform Reconstruction of Shock Waves Generated by Underwater Electrical Wire Explosions with Piezoelectric Pressure Probes
by Haibin Zhou, Yongmin Zhang, Ruoyu Han, Yan Jing, Jiawei Wu, Qiaojue Liu, Weidong Ding and Aici Qiu
Sensors 2016, 16(4), 573; https://doi.org/10.3390/s16040573 - 22 Apr 2016
Cited by 40 | Viewed by 9232
Abstract
Underwater shock waves (SWs) generated by underwater electrical wire explosions (UEWEs) have been widely studied and applied. Precise measurement of this kind of SWs is important, but very difficult to accomplish due to their high peak pressure, steep rising edge and very short [...] Read more.
Underwater shock waves (SWs) generated by underwater electrical wire explosions (UEWEs) have been widely studied and applied. Precise measurement of this kind of SWs is important, but very difficult to accomplish due to their high peak pressure, steep rising edge and very short pulse width (on the order of tens of μs). This paper aims to analyze the signals obtained by two kinds of commercial piezoelectric pressure probes, and reconstruct the correct pressure waveform from the distorted one measured by the pressure probes. It is found that both PCB138 and Müller-plate probes can be used to measure the relative SW pressure value because of their good uniformities and linearities, but none of them can obtain precise SW waveforms. In order to approach to the real SW signal better, we propose a new multi-exponential pressure waveform model, which has considered the faster pressure decay at the early stage and the slower pressure decay in longer times. Based on this model and the energy conservation law, the pressure waveform obtained by the PCB138 probe has been reconstructed, and the reconstruction accuracy has been verified by the signals obtained by the Müller-plate probe. Reconstruction results show that the measured SW peak pressures are smaller than the real signal. The waveform reconstruction method is both reasonable and reliable. Full article
(This article belongs to the Section Physical Sensors)
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<p>Schematic diagram of the SW generator based on UEWE.</p>
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<p>Typical waveforms of current and resistive voltage.</p>
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<p>Pressure probes arrangements in the water tank.</p>
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<p>20 repeated temporal pressure waveforms at the distance of 260 mm from discharge channel. (<b>a</b>) Pressure waveforms obtained by the PCB138 probe with the SW arrival times aligned; (<b>b</b>) distribution of the SW arrival times obtained by the PCB138 probe; (<b>c</b>) pressure waveforms obtained by the Müller-plate probe with the SW arrival times aligned; (<b>d</b>) distribution of the SW arrival times obtained by the Müller-plate probe.</p>
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<p>20 repeated temporal pressure waveforms at the distance of 260 mm from discharge channel. (<b>a</b>) Pressure waveforms obtained by the PCB138 probe with the SW arrival times aligned; (<b>b</b>) distribution of the SW arrival times obtained by the PCB138 probe; (<b>c</b>) pressure waveforms obtained by the Müller-plate probe with the SW arrival times aligned; (<b>d</b>) distribution of the SW arrival times obtained by the Müller-plate probe.</p>
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<p>Sensitive element of a piezoelectric probe.</p>
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<p>Pressure signals obtained by the PCB138 probe with different incident angles at the distance of 460 mm (<b>a</b>) Consistency of the obtained pressure waveforms; (<b>b</b>) rising edge of pressure signal with different incident angles.</p>
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<p>Temporal waveforms obtained by pressure probes <span class="html-italic">vs.</span> distances. (<b>a</b>) Müller-plate probe; (<b>b</b>) PCB138 probe.</p>
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<p>Dependence of the SW peak pressures and fitted values on the distance from the discharge channel.</p>
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<p>Typical time-dependent pressure waveforms obtained with both pressure probes at the distance of 260 mm.</p>
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<p>Decay constants obtained by the Müller-plate probe <span class="html-italic">vs.</span> distance.</p>
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<p>Dependence SW speed behind shock front on pressure.</p>
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<p>SW peak pressures obtained by the TOF method.</p>
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<p>Reconstructed pressure signals based on three types of waveforms.</p>
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<p>Peak pressure evaluation with the Müller-plate probe signal.</p>
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7778 KiB  
Article
A High-Speed Vision-Based Sensor for Dynamic Vibration Analysis Using Fast Motion Extraction Algorithms
by Dashan Zhang, Jie Guo, Xiujun Lei and Changan Zhu
Sensors 2016, 16(4), 572; https://doi.org/10.3390/s16040572 - 22 Apr 2016
Cited by 71 | Viewed by 8992
Abstract
The development of image sensor and optics enables the application of vision-based techniques to the non-contact dynamic vibration analysis of large-scale structures. As an emerging technology, a vision-based approach allows for remote measuring and does not bring any additional mass to the measuring [...] Read more.
The development of image sensor and optics enables the application of vision-based techniques to the non-contact dynamic vibration analysis of large-scale structures. As an emerging technology, a vision-based approach allows for remote measuring and does not bring any additional mass to the measuring object compared with traditional contact measurements. In this study, a high-speed vision-based sensor system is developed to extract structure vibration signals in real time. A fast motion extraction algorithm is required for this system because the maximum sampling frequency of the charge-coupled device (CCD) sensor can reach up to 1000 Hz. Two efficient subpixel level motion extraction algorithms, namely the modified Taylor approximation refinement algorithm and the localization refinement algorithm, are integrated into the proposed vision sensor. Quantitative analysis shows that both of the two modified algorithms are at least five times faster than conventional upsampled cross-correlation approaches and achieve satisfactory error performance. The practicability of the developed sensor is evaluated by an experiment in a laboratory environment and a field test. Experimental results indicate that the developed high-speed vision-based sensor system can extract accurate dynamic structure vibration signals by tracking either artificial targets or natural features. Full article
(This article belongs to the Section Physical Sensors)
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<p>High-speed visual measuring system. (<b>a</b>) experimental setup; (<b>b</b>) camera head and optical lens.</p>
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<p>Basic procedure of the implementation.</p>
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<p>Procedure of maximum cross-correlation (MCC) motion extraction algorithm in 2D frequency domain.</p>
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<p>Flowchart of refinement using Taylor approximation with the reformative iteration operation.</p>
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<p>Number of iterations using the modified Taylor approximation refinement in the simulation test.</p>
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<p>Comparisons of displacement extraction results between the actual input and the MCC with modified Taylor refinement.</p>
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<p>Example of the quadratic surface fitting refinement: (<b>a</b>) nine integer level cross-correlation values for curve fitting; (<b>b</b>) the fitting quandratic surface, and the triangle marker is the refined subpixel estimation of the best-matching location.</p>
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<p>Comparisons of displacement extraction results between the actual input and the MCC with subpixel localization refinement.</p>
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<p>Experiment setup in moving platform experiment: (<b>a</b>) experimental device; (<b>b</b>) the selected artificial target and natural structure target.</p>
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<p>Measurement comparisons between the grating ruler sensor and the vision-based sensor: (<b>a</b>) results using an artificial target; (<b>b</b>) results using a natural structure feature.</p>
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<p>Sound barrier experiment setup: (<b>a</b>) the experiment environment; (<b>b</b>) experimental setup; (<b>c</b>) Image captured by the developed visual measuring system.</p>
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<p>Vibration extraction results and their Fourier spectrums in the sound barrier experiment.</p>
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1084 KiB  
Article
Design of Secure ECG-Based Biometric Authentication in Body Area Sensor Networks
by Steffen Peter, Bhanu Pratap Reddy, Farshad Momtaz and Tony Givargis
Sensors 2016, 16(4), 570; https://doi.org/10.3390/s16040570 - 22 Apr 2016
Cited by 48 | Viewed by 10135
Abstract
Body area sensor networks (BANs) utilize wireless communicating sensor nodes attached to a human body for convenience, safety, and health applications. Physiological characteristics of the body, such as the heart rate or Electrocardiogram (ECG) signals, are promising means to simplify the setup process [...] Read more.
Body area sensor networks (BANs) utilize wireless communicating sensor nodes attached to a human body for convenience, safety, and health applications. Physiological characteristics of the body, such as the heart rate or Electrocardiogram (ECG) signals, are promising means to simplify the setup process and to improve security of BANs. This paper describes the design and implementation steps required to realize an ECG-based authentication protocol to identify sensor nodes attached to the same human body. Therefore, the first part of the paper addresses the design of a body-area sensor system, including the hardware setup, analogue and digital signal processing, and required ECG feature detection techniques. A model-based design flow is applied, and strengths and limitations of each design step are discussed. Real-world measured data originating from the implemented sensor system are then used to set up and parametrize a novel physiological authentication protocol for BANs. The authentication protocol utilizes statistical properties of expected and detected deviations to limit the number of false positive and false negative authentication attempts. The result of the described holistic design effort is the first practical implementation of biometric authentication in BANs that reflects timing and data uncertainties in the physical and cyber parts of the system. Full article
(This article belongs to the Special Issue Security and Privacy in Sensor Networks)
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<p>A BAN comprises sensors attached to a human body. Electrocardiography (ECG) data can ensure that sensors, attached to the same body (<b>A,B,C</b>) trust each other but do not trust sensors (<b>E</b>) and devices (<b>D</b>) that are not attached to the same body.</p>
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<p>Characteristics of the heart signal and Inter-Pulse-Intervals (IPI) between peaks.</p>
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<p>Development flow.</p>
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<p>Schematic of our sensor processing board: the instrumentation amplifier obtains the difference of the sensor inputs, before the single signal is filtered and amplified.</p>
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<p>Five seconds of gathered sensor data after processing on our sensor board. Visible are the ECG characteristics, but also some residing high frequency artifacts.</p>
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<p>Steps of the digital processing: the ECG needs to be filtered, peaks are detected and validated. Output is a table of Q, R, and S values.</p>
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<p>Signal and detected QRS peaks for two QRS complexes after Pan-Tompkins. Note that a third erroneous QRS complex is detected at time stamp 4.8 s.</p>
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<p>Photo of our experimental setup: electrodes with sensor board in front, the RaspberryPi board at the back.</p>
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<p>Block diagram of the Simulink Model. (<b>A</b>) data acquisition; (<b>B</b>) data conversion; (<b>C</b>) output; (<b>D</b>) lowpass filter; (<b>E</b>) Pan–Tompkins QRS detection; and (<b>F</b>) time tracker.</p>
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<p>Sampling rate trade-offs: (<b>A</b>) memory to error rate; and (<b>B</b>) processing time.</p>
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<p>Distribution of (<b>A</b>) measured IPIs; (<b>B</b>) difference between two adjacent measurements; and (<b>C</b>) measurement errors between sensors.</p>
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<p>Message sequence chart for the biometric authentication protocol between Sensor nodes <math display="inline"> <semantics> <msub> <mi>S</mi> <mn>1</mn> </msub> </semantics> </math> and <math display="inline"> <semantics> <msub> <mi>S</mi> <mn>2</mn> </msub> </semantics> </math>, with processing steps for <math display="inline"> <semantics> <msub> <mi>S</mi> <mn>1</mn> </msub> </semantics> </math>. The authentication is successful if the last two steps succeed.</p>
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<p>Rejected authentications (false negatives) for measured truthful authentication attempts, (<b>A</b>) for different number of samples; and (<b>B</b>) for different dynamic ranges.</p>
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<p>Accepted authentications (false positives) for forged authentication attempts, (<b>A</b>) for different number of samples; and (<b>B</b>) for different dynamic ranges.</p>
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<p>Impact of increased basis variance (e.g., more noise) on the allowed thresholds to limit false positives and false negatives, for (<b>A</b>) 8 samples at 48 dB, and (<b>B</b>) 16 samples at 60 dB.</p>
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4113 KiB  
Article
Vibration Monitoring Using Fiber Optic Sensors in a Lead-Bismuth Eutectic Cooled Nuclear Fuel Assembly
by Ben De Pauw, Alfredo Lamberti, Julien Ertveldt, Ali Rezayat, Katrien Van Tichelen, Steve Vanlanduit and Francis Berghmans
Sensors 2016, 16(4), 571; https://doi.org/10.3390/s16040571 - 21 Apr 2016
Cited by 23 | Viewed by 6549
Abstract
Excessive fuel assembly vibrations in nuclear reactor cores should be avoided in order not to compromise the lifetime of the assembly and in order to prevent the occurrence of safety hazards. This issue is particularly relevant to new reactor designs that use liquid [...] Read more.
Excessive fuel assembly vibrations in nuclear reactor cores should be avoided in order not to compromise the lifetime of the assembly and in order to prevent the occurrence of safety hazards. This issue is particularly relevant to new reactor designs that use liquid metal coolants, such as, for example, a molten lead-bismuth eutectic. The flow of molten heavy metal around and through the fuel assembly may cause the latter to vibrate and hence suffer degradation as a result of, for example, fretting wear or mechanical fatigue. In this paper, we demonstrate the use of optical fiber sensors to measure the fuel assembly vibration in a lead-bismuth eutectic cooled installation which can be used as input to assess vibration-related safety hazards. We show that the vibration characteristics of the fuel pins in the fuel assembly can be experimentally determined with minimal intrusiveness and with high precision owing to the small dimensions and properties of the sensors. In particular, we were able to record local strain level differences of about 0.2 μϵ allowing us to reliably estimate the vibration amplitudes and modal parameters of the fuel assembly based on optical fiber sensor readings during different stages of the operation of the facility, including the onset of the coolant circulation and steady-state operation. Full article
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<p>Concept drawing and photograph of the seven-pin fuel assembly.</p>
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<p>Owing to the phase-correlation approach to demodulation, the reflected spectral information of the FBGs and the (temperature) controlled environment, the strain resolution (determined as the standard deviation of the noise) was approximately 0.2 <math display="inline"> <semantics> <mrow> <mi mathvariant="sans-serif">μ</mi> <mi mathvariant="sans-serif">ϵ</mi> </mrow> </semantics> </math>.</p>
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<p>Scheme of an optical fiber with draw tower gratings (DTGs) embedded in a small groove near the surface of the pin.</p>
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<p>Photograph and scheme of the test facility containing the fuel assembly at SCK·CEN. The inset shows an enlarged image of the T-section holding the egress locations of the optical fibers.</p>
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<p>(<b>Top</b>): The LBE flow velocity during the course of the test procedure; middle: Corresponding average strain values as measured with <span class="html-italic">all</span> the FBGs on <span class="html-italic">all</span> fuel pins; (<b>Bottom</b>): rms value of the strain AC component of the middle figure; inset: Illustration of the high-pass filtering applied to the strain measurements to eliminate the drag (<span class="html-italic">i.e.</span>, the DC component (<b>red</b>)) and obtain the vibration (AC component).</p>
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<p>(<b>Left</b>): rms vibration amplitude and corresponding standard deviation averaged over all FBGs per fuel pin at an LBE flow of 4 m/s. The central fuel pin exhibits a slightly higher vibration amplitude compared to the peripheral fuel pins; (<b>Right</b>): The rms vibration amplitude measured with the different FBGs on the central fuel pin.</p>
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<p>Experimentally estimated mode shapes and approximate eigen-frequency and damping ranges during external excitation of the fuel pins.</p>
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<p>Rigid body “mode shape” occurring as a consequence of the fuel pin fixation or the support structure vibration. The additional FBG located in the capillary measures the relative movement from the fuel pin to its supports. Therefore, only that FBG identifies the rigid body mode.</p>
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3945 KiB  
Article
Impulse Magnetization of Nd-Fe-B Sintered Magnets for Sensors
by Marek Przybylski, Dariusz Kapelski, Barbara Ślusarek and Sławomir Wiak
Sensors 2016, 16(4), 569; https://doi.org/10.3390/s16040569 - 21 Apr 2016
Cited by 7 | Viewed by 8233
Abstract
Magnetization of large Nd-Fe-B sintered permanent magnets is still challenging. This type of permanent magnet is electrically conductive, so impulse magnetization causes a flow of eddy currents which prevent magnetization of the whole volume of the magnet. The paper deals with the impulse [...] Read more.
Magnetization of large Nd-Fe-B sintered permanent magnets is still challenging. This type of permanent magnet is electrically conductive, so impulse magnetization causes a flow of eddy currents which prevent magnetization of the whole volume of the magnet. The paper deals with the impulse magnetization of sintered Nd-Fe-B permanent magnets and shows a method for the determination of suitable parameters for the supply system. The necessary magnetic field strength for magnetization of the magnet to saturation was determined. The optimal magnetizing fixture supply voltage for magnetization to saturation was determined from simulations in PSpice software, finite element analyses in Maxwell 15 and measurements. Measurements of magnetic induction on the surface of the Nd-Fe-B magnet are also presented to ensure that a magnet with 70 mm diameter and 20 mm in height is fully saturated. Full article
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<p>Measurements of (<b>a</b>) magnetic flux density as a function of magnetic field strength B = f(H) and magnetic polarization as a function of magnetic field strength J = f(H) magnetization curves; (<b>b</b>) J = f(H) demagnetization curves of an Nd-Fe-B permanent magnet.</p>
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<p>Measurements of (<b>a</b>) magnetic flux density as a function of magnetic field strength B = f(H) and magnetic polarization as a function of magnetic field strength J = f(H) magnetization curves; (<b>b</b>) J = f(H) demagnetization curves of an Nd-Fe-B permanent magnet.</p>
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<p>Measurements of B = f(H) demagnetization curves of an Nd-Fe-B permanent magnet.</p>
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<p>Measurements of (<b>a</b>) magnetic remanence Br and (<b>b</b>) coercivity of magnetic polarization H<sub>cJ</sub> as a function of magnetizing magnetic field strength H<sub>mag</sub>.</p>
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<p>Electric diagram of the impulse magnetizer with a magnetizing fixture.</p>
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<p>(<b>a</b>) Measurements of impulse magnetization currents for different voltages; (<b>b</b>) comparison of impulse magnetization currents for voltage U<sub>c</sub> = 3200 V.</p>
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<p>Measurements of (<b>a</b>) magnetic flux density in the middle of magnetization coil and (<b>b</b>) current, for U<sub>c</sub> = 3200 V magnetization voltage as a function of time [<a href="#B25-sensors-16-00569" class="html-bibr">25</a>].</p>
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<p>Simulation of magnetic flux density as a function of time in the middle of magnetizing coil in Maxwell 15.</p>
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<p>FEM simulations of magnetic induction in the Nd-Fe-B sintered magnet for different capacitor voltages, time t = 2.6 ms.</p>
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<p>FEM <b>s</b>imulations of magnetic induction in the centre of an Nd-Fe-B magnet as a function of capacitor voltages.</p>
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<p>FEM simulations in magnetizing fixture and Nd-Fe-B magnet for U<sub>c</sub> = 2800 V, I<sub>m</sub> = 1032 A, t = 2.6 ms.</p>
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<p>Measurements of magnetic induction on the surface of the magnet, for different capacitor voltages.</p>
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<p>Photos of magnetic poles on the surface of N38 type Nd-Fe-B magnet for magnetization voltages (<b>a</b>) for 1600 V and (<b>b</b>) for 2800 V.</p>
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Article
Reconstructing Face Image from the Thermal Infrared Spectrum to the Visible Spectrum
by Brahmastro Kresnaraman, Daisuke Deguchi, Tomokazu Takahashi, Yoshito Mekada, Ichiro Ide and Hiroshi Murase
Sensors 2016, 16(4), 568; https://doi.org/10.3390/s16040568 - 21 Apr 2016
Cited by 4 | Viewed by 6826
Abstract
During the night or in poorly lit areas, thermal cameras are a better choice instead of normal cameras for security surveillance because they do not rely on illumination. A thermal camera is able to detect a person within its view, but identification from [...] Read more.
During the night or in poorly lit areas, thermal cameras are a better choice instead of normal cameras for security surveillance because they do not rely on illumination. A thermal camera is able to detect a person within its view, but identification from only thermal information is not an easy task. The purpose of this paper is to reconstruct the face image of a person from the thermal spectrum to the visible spectrum. After the reconstruction, further image processing can be employed, including identification/recognition. Concretely, we propose a two-step thermal-to-visible-spectrum reconstruction method based on Canonical Correlation Analysis (CCA). The reconstruction is done by utilizing the relationship between images in both thermal infrared and visible spectra obtained by CCA. The whole image is processed in the first step while the second step processes patches in an image. Results show that the proposed method gives satisfying results with the two-step approach and outperforms comparative methods in both quality and recognition evaluations. Full article
(This article belongs to the Special Issue Infrared and THz Sensing and Imaging)
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<p>Image examples in different spectra: (<b>a</b>) in the visible spectrum; (<b>b</b>) in the thermal infrared spectrum.</p>
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<p>Process flow of the proposed method: (<b>a</b>) training process; (<b>b</b>) reconstruction process.</p>
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<p>Examples of patches taken from a face image.</p>
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<p>Examples of reconstructed images by various methods. Each row indicates a person and the columns represent images of: (<b>a</b>) ground-truth; (<b>b</b>) proposed method; (<b>c</b>) holistic LLE (Locally Linear Embedding); (<b>d</b>) patch-Based LLE; (<b>e</b>) patch-Based 1NN (Nearest Neighbor); (<b>f</b>) patch-Based <span class="html-italic">k</span>-NN.</p>
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<p>A heat map representation of the confusion matrix of the recognition evaluation. It goes from dark blue to dark red, where the representations of higher values are close to dark red.</p>
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<p>Visual examples in various steps of the proposed method: (<b>a</b>) thermal infrared input; (<b>b</b>) globally reconstructed images; (<b>c</b>) residual images; (<b>d</b>) fully reconstructed images; (<b>e</b>) ground-truth images.</p>
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<p>Type B examples of reconstructed images by various methods. Each row indicates a person and the columns represent images of: (<b>a</b>) ground-truth; (<b>b</b>) proposed method; (<b>c</b>) holistic LLE; (<b>d</b>) patch-Based LLE; (<b>e</b>) patch-Based 1NN; (<b>f</b>) patch-Based <span class="html-italic">k</span>-NN.</p>
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<p>Type B examples of reconstructed images with various number of training data. Each row indicates a person and the columns represent: (<b>a</b>) ground-truth images; (<b>b</b>) reconstructed images from 40 people’s training data; (<b>c</b>) reconstructed images from 70 people’s training data; (<b>d</b>) reconstructed images from 100 people’s training data; (<b>e</b>) reconstructed images from 130 people’s training data; (<b>f</b>) reconstructed images from 160 people’s training data.</p>
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Article
A Novel Method to Enhance Pipeline Trajectory Determination Using Pipeline Junctions
by Hussein Sahli and Naser El-Sheimy
Sensors 2016, 16(4), 567; https://doi.org/10.3390/s16040567 - 21 Apr 2016
Cited by 38 | Viewed by 6375
Abstract
Pipeline inspection gauges (pigs) have been used for many years to perform various maintenance operations in oil and gas pipelines. Different pipeline parameters can be inspected during the pig journey. Although pigs use many sensors to detect the required pipeline parameters, matching these [...] Read more.
Pipeline inspection gauges (pigs) have been used for many years to perform various maintenance operations in oil and gas pipelines. Different pipeline parameters can be inspected during the pig journey. Although pigs use many sensors to detect the required pipeline parameters, matching these data with the corresponding pipeline location is considered a very important parameter. High-end, tactical-grade inertial measurement units (IMUs) are used in pigging applications to locate the detected problems of pipeline using other sensors, and to reconstruct the trajectories of the pig. These IMUs are accurate; however, their high cost and large sizes limit their use in small diameter pipelines (8″ or less). This paper describes a new methodology for the use of MEMS-based IMUs using an extended Kalman filter (EKF) and the pipeline junctions to increase the position parameters’ accuracy and to reduce the total RMS errors even during the unavailability of above ground markers (AGMs). The results of this new proposed method using a micro-electro-mechanical systems (MEMS)-based IMU revealed that the position RMS errors were reduced by approximately 85% compared to the standard EKF solution. Therefore, this approach will enable the mapping of small diameter pipelines, which was not possible before. Full article
(This article belongs to the Section Physical Sensors)
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<p>Smart Pipeline Inspection Gauge (Nord Stream AG).</p>
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<p>Main pig tool components.</p>
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<p>Pipeline joints: (<b>a</b>) flange type; (<b>b</b>) push-on type; (<b>c</b>) welding type.</p>
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<p>Accelerometer output—MEMS (SiIMU02).</p>
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<p>Accelerometer output—LN200.</p>
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<p>Mexican Hat mother wavelet.</p>
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<p>Pattern detected using WL.</p>
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<p>Pig defined axes.</p>
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<p>Algorithm for corrected state estimation.</p>
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<p>Selecting threshold criteria.</p>
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<p>Trajectories—Case #1.</p>
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<p>Position Errors-EKF &amp; EKF/PLJ Scenario #1.</p>
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<p>Maximum Position Error—Scenario #1.</p>
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<p>RMS Position Errors—Scenario #1.</p>
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<p>Trajectories—Scenario #2.</p>
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<p>Positions Errors—EKF &amp; EKF/PLJ Scenario #2.</p>
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<p>Maximum Position Errors—Scenario #2.</p>
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<p>RMS Positions Errors—Scenario #2.</p>
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Article
Stability Analysis of Multi-Sensor Kalman Filtering over Lossy Networks
by Shouwan Gao, Pengpeng Chen, Dan Huang and Qiang Niu
Sensors 2016, 16(4), 566; https://doi.org/10.3390/s16040566 - 20 Apr 2016
Cited by 9 | Viewed by 4375
Abstract
This paper studies the remote Kalman filtering problem for a distributed system setting with multiple sensors that are located at different physical locations. Each sensor encapsulates its own measurement data into one single packet and transmits the packet to the remote filter via [...] Read more.
This paper studies the remote Kalman filtering problem for a distributed system setting with multiple sensors that are located at different physical locations. Each sensor encapsulates its own measurement data into one single packet and transmits the packet to the remote filter via a lossy distinct channel. For each communication channel, a time-homogeneous Markov chain is used to model the normal operating condition of packet delivery and losses. Based on the Markov model, a necessary and sufficient condition is obtained, which can guarantee the stability of the mean estimation error covariance. Especially, the stability condition is explicitly expressed as a simple inequality whose parameters are the spectral radius of the system state matrix and transition probabilities of the Markov chains. In contrast to the existing related results, our method imposes less restrictive conditions on systems. Finally, the results are illustrated by simulation examples. Full article
(This article belongs to the Section Sensor Networks)
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<p>Distributed systems.</p>
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<p>Diagram of a networked filtering system under distributed sensing.</p>
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<p>Stable and unstable regions.</p>
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<p>The error covariance matrix <math display="inline"> <semantics> <msub> <mi>P</mi> <mi>k</mi> </msub> </semantics> </math> and channel state <math display="inline"> <semantics> <msub> <mi>S</mi> <mi>k</mi> </msub> </semantics> </math> with <math display="inline"> <semantics> <mrow> <mfenced separators="" open="(" close=")"> <msub> <mi>q</mi> <mn>1</mn> </msub> <mo>,</mo> <mspace width="4pt"/> <msub> <mi>q</mi> <mn>2</mn> </msub> </mfenced> <mo>=</mo> <mfenced separators="" open="(" close=")"> <mn>0</mn> <mo>.</mo> <mn>8</mn> <mo>,</mo> <mspace width="4pt"/> <mn>0</mn> <mo>.</mo> <mn>9</mn> </mfenced> </mrow> </semantics> </math>: (<b>a</b>) The error covariance; (<b>b</b>) the associated channel state.</p>
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<p>The error covariance matrix <math display="inline"> <semantics> <msub> <mi>P</mi> <mi>k</mi> </msub> </semantics> </math> and channel state <math display="inline"> <semantics> <msub> <mi>S</mi> <mi>k</mi> </msub> </semantics> </math> with <math display="inline"> <semantics> <mrow> <mfenced separators="" open="(" close=")"> <msub> <mi>q</mi> <mn>1</mn> </msub> <mo>,</mo> <mspace width="4pt"/> <msub> <mi>q</mi> <mn>2</mn> </msub> </mfenced> <mo>=</mo> <mfenced separators="" open="(" close=")"> <mn>0</mn> <mo>.</mo> <mn>2</mn> <mo>,</mo> <mspace width="4pt"/> <mn>0</mn> <mo>.</mo> <mn>2</mn> </mfenced> </mrow> </semantics> </math>: (<b>a</b>) The error covariance; (<b>b</b>) the associated channel state.</p>
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<p>The error covariance matrix <math display="inline"> <semantics> <msub> <mi>P</mi> <mi>k</mi> </msub> </semantics> </math> and channel state <math display="inline"> <semantics> <msub> <mi>S</mi> <mi>k</mi> </msub> </semantics> </math> with <math display="inline"> <semantics> <mrow> <mfenced separators="" open="(" close=")"> <msub> <mi>q</mi> <mn>1</mn> </msub> <mo>,</mo> <mspace width="4pt"/> <msub> <mi>q</mi> <mn>2</mn> </msub> </mfenced> <mo>=</mo> <mfenced separators="" open="(" close=")"> <mn>0</mn> <mo>.</mo> <mn>6</mn> <mo>,</mo> <mspace width="4pt"/> <mn>0</mn> <mo>.</mo> <mn>8</mn> </mfenced> </mrow> </semantics> </math>: (<b>a</b>) The error covariance; (<b>b</b>) the associated channel state.</p>
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<p>The error covariance matrix <math display="inline"> <semantics> <msub> <mi>P</mi> <mi>k</mi> </msub> </semantics> </math> and channel state <math display="inline"> <semantics> <msub> <mi>S</mi> <mi>k</mi> </msub> </semantics> </math> with <math display="inline"> <semantics> <mrow> <mfenced separators="" open="(" close=")"> <msub> <mi>q</mi> <mn>1</mn> </msub> <mo>,</mo> <mspace width="4pt"/> <msub> <mi>q</mi> <mn>2</mn> </msub> </mfenced> <mo>=</mo> <mfenced separators="" open="(" close=")"> <mn>0</mn> <mo>.</mo> <mn>6</mn> <mo>,</mo> <mspace width="4pt"/> <mn>0</mn> <mo>.</mo> <mn>8</mn> </mfenced> </mrow> </semantics> </math>: (<b>a</b>) The error covariance; (<b>b</b>) the associated channel state.</p>
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Article
A Comparative Study of the Applied Methods for Estimating Deflection of the Vertical in Terrestrial Geodetic Measurements
by Luca Vittuari, Maria Alessandra Tini, Pierguido Sarti, Eugenio Serantoni, Alessandra Borghi, Monia Negusini and Sébastien Guillaume
Sensors 2016, 16(4), 565; https://doi.org/10.3390/s16040565 - 20 Apr 2016
Cited by 19 | Viewed by 6614
Abstract
This paper compares three different methods capable of estimating the deflection of the vertical (DoV): one is based on the joint use of high precision spirit leveling and Global Navigation Satellite Systems (GNSS), a second uses astro-geodetic measurements and the third gravimetric geoid [...] Read more.
This paper compares three different methods capable of estimating the deflection of the vertical (DoV): one is based on the joint use of high precision spirit leveling and Global Navigation Satellite Systems (GNSS), a second uses astro-geodetic measurements and the third gravimetric geoid models. The working data sets refer to the geodetic International Terrestrial Reference Frame (ITRF) co-location sites of Medicina (Northern, Italy) and Noto (Sicily), these latter being excellent test beds for our investigations. The measurements were planned and realized to estimate the DoV with a level of precision comparable to the angular accuracy achievable in high precision network measured by modern high-end total stations. The three methods are in excellent agreement, with an operational supremacy of the astro-geodetic method, being faster and more precise than the others. The method that combines leveling and GNSS has slightly larger standard deviations; although well within the 1 arcsec level, which was assumed as threshold. Finally, the geoid model based method, whose 2.5 arcsec standard deviations exceed this threshold, is also statistically consistent with the others and should be used to determine the DoV components where local ad hoc measurements are lacking. Full article
(This article belongs to the Section Remote Sensors)
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<p>Area of IRA-INAF observatory of Medicina (Northern Italy) (satellite image courtesy of Google Earth<sup>®</sup>).</p>
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<p>Area of the IRA-INAF observatory of Noto (Sicily) (satellite image courtesy of Google Earth<sup>®</sup>).</p>
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<p>Relation between the geoid undulation N and the deflection of the vertical <span class="html-italic">ε</span>. (Adapted from [<a href="#B27-sensors-16-00565" class="html-bibr">27</a>]).</p>
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<p>Zeiss Ni1 analogic measurement of the height difference between GNSS-ARP and the South leveling bolt at site Medicina. The inset shows the reference height marker: a bolt on top of a 1.5 m coated metal rod hammered into the ground.</p>
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<p>Deflection of the vertical (DoV) components <span class="html-italic">ξ</span> (North) and <span class="html-italic">η</span> (East) calculated from the ITALGEO2005 grid at the Medicina site. The orange dot indicates the point where the DoV was estimated using the GNSS-LEV method; the black star identifies the location of the DoV measured using QDaedalus.</p>
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<p>DoV components <span class="html-italic">ξ</span> (North) and <span class="html-italic">η</span> (East) calculated from the ITALGEO2005 grid at Noto site. The orange dots indicate the point for which the DoV was estimated using the GNSS-LEV method; the black stars identify the locations where the DoV was measured using QDaedalus.</p>
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Article
Dynamic Measurement for the Diameter of A Train Wheel Based on Structured-Light Vision
by Zheng Gong, Junhua Sun and Guangjun Zhang
Sensors 2016, 16(4), 564; https://doi.org/10.3390/s16040564 - 20 Apr 2016
Cited by 17 | Viewed by 13299
Abstract
Wheels are very important for the safety of a train. The diameter of the wheel is a significant parameter that needs regular inspection. Traditional methods only use the contact points of the wheel tread to fit the rolling round. However, the wheel tread [...] Read more.
Wheels are very important for the safety of a train. The diameter of the wheel is a significant parameter that needs regular inspection. Traditional methods only use the contact points of the wheel tread to fit the rolling round. However, the wheel tread is easily influenced by peeling or scraping. Meanwhile, the circle fitting algorithm is sensitive to noise when only three points are used. This paper proposes a dynamic measurement method based on structured-light vision. The axle of the wheelset and the tread are both employed. The center of the rolling round is determined by the axle rather than the tread only. Then, the diameter is calculated using the center and the contact points together. Simulations are performed to help design the layout of the sensors, and the influences of different noise sources are also analyzed. Static and field experiments are both performed, and the results show it to be quite stable and accurate. Full article
(This article belongs to the Section Physical Sensors)
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<p>Measurement system structure. S1–S8: Structured-light sensors; T: electromagnetic sensor.</p>
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<p>Structured-light vision model. (1) Camera; (2) laser projector; (3) measured object.</p>
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<p>The images of the planar targets. (<b>a</b>) The planar target image for the intrinsic parameters’ calibration. The target contains 10 × 10 checkers at the interval of 10 mm, and the precision is 0.02 mm; (<b>b</b>) The planar target image for the structured light calibration. The target contains a 7 × 7 dot matrix at the interval of 12 mm, and the precision is 0.02 mm.</p>
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<p>The images for the global calibration. (<b>a</b>) The target image of the camera for the wheel tread measurement; (<b>b</b>) the target image of the camera for the wheelset axle measurement.</p>
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<p>Image of the laser stripe. (<b>a</b>) Image of the wheel tread; (<b>b</b>) image of the axle of the wheelset.</p>
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<p>The image processing result of <a href="#sensors-16-00564-f005" class="html-fig">Figure 5</a>. (<b>a</b>) The result of <a href="#sensors-16-00564-f005" class="html-fig">Figure 5</a>a; (<b>b</b>) the result of <a href="#sensors-16-00564-f005" class="html-fig">Figure 5</a>b.</p>
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<p>The profiles of the wheelset and tread. (<b>a</b>) The profile of half wheelset; (<b>b</b>) the profile of wheel tread; AB: the wheel rim plane; BD: the wheel flange; C: the flange vertex; DF: the wheel tread; E: the contact point.</p>
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<p>The wheel tread measurement. (<b>a</b>) The sensors for tread measurement; (<b>b</b>) the result of S1; (<b>c</b>) the result of S2; (<b>d</b>) the result of S3.</p>
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<p>The wheelset axle measurement. (<b>a</b>) The sensor for the axle; (<b>b</b>) the result of S4.</p>
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<p>Determine the radius of the wheel. (<b>a</b>) The feature points in the 3D coordinate frame; (<b>b</b>) the projection of the feature points to the wheel rim plane.</p>
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<p>The simulation frame. The diameter of the wheel is set to 840 mm, and dL is the distance from <b><span class="html-italic">O1</span></b> to the wheel rim plane.</p>
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<p>Diameter RMS error to the 3D noise of the structured-light sensors.</p>
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<p>Diameter RMS error to the distribution angle of the lasers on the wheel rim plane.</p>
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<p>Deformation of the wheelset.</p>
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<p>Diameter RMS error to the angle of bending and the distance from <b><span class="html-italic">O1</span></b> to the rim plane.</p>
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<p>Diameter RMS error to the angle of the bend with the distance dL of 200 mm.</p>
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<p>Diameter RMS error to the angle of bending with the geometrical error.</p>
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<p>The static experiment. (<b>a</b>) The experiment platform; (<b>b</b>) the laser profiles on the wheelset; (<b>c</b>) the laser images captured by the cameras.</p>
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<p>The 3D laser profiles.</p>
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<p>The diameter results of ten static measurements.</p>
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<p>Wheelset dynamic measurement system installed on the railway bed.</p>
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<p>One set of laser images of a wheel.</p>
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<p>The manual measurement. (<b>a</b>) Using the diameter caliper; (<b>b</b>) using the 3D scanner; (<b>c</b>) the 3D shape result of the scanner.</p>
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<p>The diameter results of the wheelset axle.</p>
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<p>The comparison between the system result and the diameter caliper. (<b>a</b>) The diameter result; (<b>b</b>) the diameter error.</p>
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Article
A Stimuli-Responsive Biosensor of Glucose on Layer-by-Layer Films Assembled through Specific Lectin-Glycoenzyme Recognition
by Huiqin Yao, Qianqian Gan, Juan Peng, Shan Huang, Meilin Zhu and Keren Shi
Sensors 2016, 16(4), 563; https://doi.org/10.3390/s16040563 - 20 Apr 2016
Cited by 13 | Viewed by 6171
Abstract
The research on intelligent bioelectrocatalysis based on stimuli-responsive materials or interfaces is of great significance for biosensors and other bioelectronic devices. In the present work, lectin protein concanavalin A (Con A) and glycoenzyme glucose oxidase (GOD) were assembled into {Con A/GOD}n layer-by-layer [...] Read more.
The research on intelligent bioelectrocatalysis based on stimuli-responsive materials or interfaces is of great significance for biosensors and other bioelectronic devices. In the present work, lectin protein concanavalin A (Con A) and glycoenzyme glucose oxidase (GOD) were assembled into {Con A/GOD}n layer-by-layer (LbL) films by taking advantage of the biospecific lectin-glycoenzyme affinity between them. These film electrodes possess stimuli-responsive properties toward electroactive probes such as ferrocenedicarboxylic acid (Fc(COOH)2) by modulating the surrounding pH. The CV peak currents of Fc(COOH)2 were quite large at pH 4.0 but significantly suppressed at pH 8.0, demonstrating reversible stimuli-responsive on-off behavior. The mechanism of stimuli-responsive property of the films was explored by comparative experiments and attributed to the different electrostatic interaction between the films and the probes at different pH. This stimuli-responsive films could be used to realize active/inactive electrocatalytic oxidation of glucose by GOD in the films and mediated by Fc(COOH)2 in solution, which may establish a foundation for fabricating novel stimuli-responsive electrochemical biosensors based on bioelectrocatalysis with immobilized enzymes. Full article
(This article belongs to the Special Issue Microbial and Enzymatic Biosensors)
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<p>QCM frequency shift (−ΔF) with assembly step of {Con A/GOD}<sub>n</sub> LbL films on Au/MPS/PDDA surface with adsorption steps: Con A (▲) and GOD (○).</p>
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<p>(<b>A</b>) CVs in pH 7.0 buffers at 0.2 V·s<sup>−</sup><sup>1</sup> for {Con A/GOD}<sub>n</sub> films assembled on PG/PDDA electrode with different number of bilayers (n): (<b>a</b>) 0, (<b>b</b>) 1, (<b>c</b>) 3, (<b>d</b>) 5 and (<b>e</b>) 7; (<b>B</b>) Effect of number of bilayers on the surface concentration of GOD (Γ*) for {Con A/GOD}<sub>n</sub>.</p>
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<p>(<b>A</b>) CVs of 0.5 mM Fc(COOH)<sub>2</sub> at 0.1 V·s<sup>−</sup><sup>1</sup> for {Con A/GOD}<sub>5</sub> films in buffers at pH (<b>a</b>) 4.0 and (<b>b</b>) 8.0; (<b>B</b>) Influence of solution pH on (<b>a</b>) CV oxidation peak current (I<sub>pa</sub>) and (<b>b</b>) peak separation (ΔE<sub>p</sub>) of 0.5 mM Fc(COOH)<sub>2</sub> at 0.1 V·s<sup>−</sup><sup>1</sup> for {Con A/GOD}<sub>5</sub> films.</p>
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<p>(<b>A</b>) Dependence of CV oxidation peak current (I<sub>pa</sub>) of Fc(COOH)<sub>2</sub> at 0.1 V·s<sup>−</sup><sup>1</sup> on solution pH switched between pH 4.0 and 8.0 for the same {Con A/GOD}<sub>5</sub> films; (<b>B</b>) EIS responses of 10 mM Fe(CN)<sub>6</sub><sup>3−/4−</sup> at 0.17 V on solution pH switched between (<b>a</b>) pH 4.0, (<b>b</b>) 8.0 of the first cycle, (<b>c</b>) pH 4.0 and (<b>d</b>) 8.0 of the second cycle for {Con A/GOD}<sub>5</sub> films. Inset is a magnification of curve a and curve c.</p>
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<p>SEM top views of {Con A/GOD}<sub>5</sub> films assembled on PG/PDDA surface after the films were immersed in buffers containing 0.5 mM Fc(COOH)<sub>2</sub> at pH (<b>A</b>) 4.0 and (<b>B</b>) 8.0 for 30 min, and there is no substantial difference in the structures.</p>
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<p>CVs of (<b>A</b>) 1 mM Ru(NH<sub>3</sub>)<sub>6</sub>Cl<sub>3</sub>; (<b>B</b>) 0.5 mM FcMeOH; (<b>C</b>) 0.5 mM hydroquinone; (<b>D</b>) 0.2 mM Fc(COOH); and (<b>E</b>) K<sub>3</sub>Fe(CN)<sub>6</sub> at 0.1 V·s<sup>−1</sup> for {Con A/GOD}<sub>5</sub> films in buffers at pH (<b>a</b>) 4.0 and (<b>b</b>) 8.0.</p>
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<p>(<b>A</b>) CVs of {Con A/GOD}<sub>5</sub> films at 0.005 V·s<sup>−1</sup> in pH 4.0 buffers containing 0.5 mM Fc(COOH)<sub>2</sub> with (<b>a</b>) 0, (<b>b</b>) 3.0, (<b>c</b>) 5.5, (<b>d</b>) 6.5, and (<b>e</b>) 7.0 mM glucose; (<b>B</b>) Amperometric responses of {Con A/GOD}<sub>5</sub> films at 0.4 V in buffers containing 0.5 mM Fc(COOH)<sub>2</sub> upon successive addition of 0.5 mM glucose at pH (<b>a</b>) 4.0 and (<b>b</b>) 8.0. Inset: dependence of amperometric oxidation peak currents (I<sub>pa</sub>) on concentration of glucose in systems at pH (<b>a</b>) 4.0 and (<b>b</b>) 8.0.</p>
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<p>(<b>A</b>) CVs of {Con A/GOD}<sub>5</sub> films at 0.005 V·s<sup>−1</sup> in solutions containing 0.5 mM Fc(COOH)<sub>2</sub>, 7.0 mM glucose at pH (<b>a</b>) 4.0 and (<b>b</b>) 8.0; (<b>B</b>) Dependence of CV catalytic I<sub>pa</sub> at 0.005 V·s<sup>−1</sup> on solution pH switched between pH 4.0 and 8.0, which tuned by alternate addition of 10 mM ethyl butyrate (black square) and 6 mM urea (red square) into unbuffered solutions containing 5 units·mL<sup>−1</sup> esterase, 15 units·mL<sup>−1</sup> urease, 0.5 mM Fc(COOH)<sub>2</sub>, and 7.0 mM glucose for the same {Con A/GOD}<sub>5</sub> films.</p>
Full article ">Scheme 1
<p>Schematic picture of the {Con A/GOD}<sub>n</sub> LbL film assembly.</p>
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12062 KiB  
Article
Mass Sensitivity Optimization of a Surface Acoustic Wave Sensor Incorporating a Resonator Configuration
by Wenchang Hao, Jiuling Liu, Minghua Liu, Yong Liang and Shitang He
Sensors 2016, 16(4), 562; https://doi.org/10.3390/s16040562 - 20 Apr 2016
Cited by 35 | Viewed by 7914
Abstract
The effect of the sensitive area of the two-port resonator configuration on the mass sensitivity of a Rayleigh surface acoustic wave (R-SAW) sensor was investigated theoretically, and verified in experiments. A theoretical model utilizing a 3-dimensional finite element method (FEM) approach was established [...] Read more.
The effect of the sensitive area of the two-port resonator configuration on the mass sensitivity of a Rayleigh surface acoustic wave (R-SAW) sensor was investigated theoretically, and verified in experiments. A theoretical model utilizing a 3-dimensional finite element method (FEM) approach was established to extract the coupling-of-modes (COM) parameters in the absence and presence of mass loading covering the electrode structures. The COM model was used to simulate the frequency response of an R-SAW resonator by a P-matrix cascading technique. Cascading the P-matrixes of unloaded areas with mass loaded areas, the sensitivity for different sensitive areas was obtained by analyzing the frequency shift. The performance of the sensitivity analysis was confirmed by the measured responses from the silicon dioxide (SiO2) deposited on different sensitive areas of R-SAW resonators. It is shown that the mass sensitivity varies strongly for different sensitive areas, and the optimal sensitive area lies towards the center of the device. Full article
(This article belongs to the Section Physical Sensors)
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Graphical abstract

Graphical abstract
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<p>The schematic of a two-port R-SAW resonator with three IDTs.</p>
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<p>The schematic of the COM model for typical resonator configuration.</p>
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<p>The schematic of the periodic electrodes covering a piezoelectric substrate model.</p>
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<p>Meshed periodic structure in <a href="#sensors-16-00562-f003" class="html-fig">Figure 3</a>.</p>
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<p>Displacement profiles of periodic shorted-grating on ST-X Quartz: (<b>a</b>) eigenfrequency <span class="html-italic">f</span><sub>sc−</sub> = 312.539 (MHz); (<b>b</b>) eigenfrequency <span class="html-italic">f</span><sub>sc+</sub> = 314.528 (MHz).</p>
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<p>Input admittance of periodic IDT on ST-X quartz.</p>
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<p>Input admittance of periodic IDT on ST-2°X quartz: the red dashed box area shows the counteracted extrema in <a href="#sensors-16-00562-f006" class="html-fig">Figure 6</a>.</p>
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<p>The schematic of a layered periodic model with embedded electrodes.</p>
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<p>Displacement profiles of periodic layered shorted-grating on ST-X quartz: (<b>a</b>) eigenfrequency <span class="html-italic">f′</span><sub>sc−</sub> = 311.666 (MHz); (<b>b</b>) eigenfrequency <span class="html-italic">f′</span><sub>sc+</sub> = 312.466 (MHz).</p>
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<p>Input admittance of periodic layered IDT on ST-X quartz.</p>
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<p>The schematic of the <span class="html-italic">P</span>-matrix in the IDT section.</p>
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<p>The schematic of <span class="html-italic">P</span>-matrix in IDT section.</p>
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<p>The schematic of mass deposited along the <span class="html-italic">x</span>-axis from A to F on the two-port SAW resonator.</p>
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<p>The frequency responses for non-loaded and different sensitive areas shown in <a href="#sensors-16-00562-f013" class="html-fig">Figure 13</a> with mass loaded of the resonator.</p>
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<p>(<b>a</b>) The structure of the SAW resonator device; (<b>b</b>) the frequency response of the device.</p>
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<p>Measured frequency responses caused by (<b>a</b>) area B loaded and (<b>b</b>) area F loaded by SiO<sub>2</sub>.</p>
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<p>The simulated and measured mass sensitivity for different surface areas, each position being demonstrated by repeated measurements.</p>
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