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Search Results (401)

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13 pages, 2523 KiB  
Article
Enhanced Non-Invasive Diagnosis of Female Urinary Incontinence Using Static and Functional Transperineal Ultrasonography
by Milosz Pietrus, Kazimierz Pityński, Maciej W. Socha, Iwona Gawron, Robert Biskupski-Brawura-Samaha and Marcin Waligóra
Diagnostics 2024, 14(22), 2549; https://doi.org/10.3390/diagnostics14222549 - 14 Nov 2024
Viewed by 318
Abstract
Background/Objectives: To investigate the utility of transperineal ultrasound in detecting stress urinary incontinence (SUI) and identify optimal anatomical and functional parameters. Methods: Thirty-four women presenting with SUI with or without pelvic organ prolapse between 2012 and 2016 were studied. The control [...] Read more.
Background/Objectives: To investigate the utility of transperineal ultrasound in detecting stress urinary incontinence (SUI) and identify optimal anatomical and functional parameters. Methods: Thirty-four women presenting with SUI with or without pelvic organ prolapse between 2012 and 2016 were studied. The control group included patients without SUI who underwent surgery for mild gynecologic disorders or pelvic organ prolapse. The relationship between selected ultrasound parameters and SUI was determined. Results: Among the 20 variables measured in ultrasonography using 4 angles and the bladder–symphysis distance (BSD) values, we found that the difference in the BSD obtained at rest and during the Valsalva maneuver (odds ratio [OR]: 1.15, 95% confidence interval [CI]: 1.05–1.27, p = 0.004), the mean urethral diameter (UD; OR: 4.29, 95% CI: 2.07–8.83, p = 0.0001), and the occurrence of the funneling sign during the Valsalva maneuver (OR: 21; 95% CI: 6.1–71.9, p < 0.0001) were associated with urinary incontinence in the logistic regression analysis. The optimal cut-off point for BSD was >8 mm (area under the curve (AUC), 0.71; sensitivity, 91.2%; specificity, 56.8%; p = 0.001) and that for UD was >6 mm (AUC, 0.84; sensitivity, 82.1%; specificity, 73%; p < 0.001). Conclusions: Transperineal ultrasonography is a useful tool for detecting SUI. Our findings highlighted the utility of several sonographic parameters, mainly the urethral diameter, in the diagnosis of urinary incontinence. Full article
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Figure 1

Figure 1
<p>Bladder–symphysis distance in patients with and without urinary incontinence.</p>
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<p>Angles assessed in ultrasonography in patients with and without urinary incontinence.</p>
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<p>Urethral diameters. Data are presented as median and interquartile range. The box plots represent the distribution of urethral diameters measured in millimeters for individuals with and without urinary incontinence (UI). Comparisons between groups were made using the Mann–Whitney U test.</p>
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<p>Funneling and urethral rotation signs. Bars represent the percentage of individuals exhibiting the funneling sign at rest, during the Valsalva maneuver, and total urethral rotation. Comparisons between groups (urinary incontinence [UI] vs. non-UI) were made using the chi-square test.</p>
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<p>Receiver operating characteristic curve for the identification of urinary incontinence. We assessed variables shown to be significant in logistic regression: BSD difference between rest and during the Valsalva maneuver with a cut-off point of &gt;8 mm (area under the curve, 0.71; sensitivity, 91.2%; specificity, 56.8%; <span class="html-italic">p</span> = 0.001) and mean urethral diameter with a cut-off point of &gt;6 mm (area under the curve, 0.84; sensitivity, 82.1%; specificity, 73%; <span class="html-italic">p</span> &lt; 0.001). BSD, bladder–symphysis distance.</p>
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19 pages, 6930 KiB  
Article
Deterministic Trajectory Design and Attitude Maneuvers of Gradient-Index Solar Sail in Interplanetary Transfers
by Marco Bassetto, Giovanni Mengali and Alessandro A. Quarta
Appl. Sci. 2024, 14(22), 10463; https://doi.org/10.3390/app142210463 - 13 Nov 2024
Viewed by 395
Abstract
A refractive sail is a special type of solar sail concept, whose membrane exposed to the Sun’s rays is covered with an advanced engineered film made of micro-prisms. Unlike the well-known reflective solar sail, an ideally flat refractive sail is able to generate [...] Read more.
A refractive sail is a special type of solar sail concept, whose membrane exposed to the Sun’s rays is covered with an advanced engineered film made of micro-prisms. Unlike the well-known reflective solar sail, an ideally flat refractive sail is able to generate a nonzero thrust component along the sail’s nominal plane even when the Sun’s rays strike that plane perpendicularly, that is, when the solar sail attitude is Sun-facing. This particular property of the refractive sail allows heliocentric orbital transfers between orbits with different values of the semilatus rectum while maintaining a Sun-facing attitude throughout the duration of the flight. In this case, the sail control is achieved by rotating the structure around the Sun–spacecraft line, thus reducing the size of the control vector to a single (scalar) parameter. A gradient-index solar sail (GIS) is a special type of refractive sail, in which the membrane film design is optimized though a transformation optics-based method. In this case, the membrane film is designed to achieve a desired refractive index distribution with the aid of a waveguide array to increase the sail efficiency. This paper analyzes the optimal transfer performance of a GIS with a Sun-facing attitude (SFGIS) in a series of typical heliocentric mission scenarios. In addition, this paper studies the attitude control of the Sun-facing GIS using a simplified mathematical model, in order to investigate the effective ability of the solar sail to follow the (optimal) variation law of the rotation angle around the radial direction. Full article
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Figure 1

Figure 1
<p>Sketch of the SFGIS with the normal unit vector <math display="inline"><semantics> <mover accent="true"> <mi mathvariant="bold-italic">n</mi> <mo stretchy="false">^</mo> </mover> </semantics></math> and the reference unit vector <math display="inline"><semantics> <mover accent="true"> <mi mathvariant="bold-italic">m</mi> <mo stretchy="false">^</mo> </mover> </semantics></math>, whose directions are fixed in a (spacecraft) body reference frame. Note that the sail nominal plane <math display="inline"><semantics> <mi mathvariant="script">P</mi> </semantics></math> is perpendicular to the Sun–spacecraft line, and the unit vector <math display="inline"><semantics> <mover accent="true"> <mi mathvariant="bold-italic">m</mi> <mo stretchy="false">^</mo> </mover> </semantics></math> belongs to the <math display="inline"><semantics> <mi mathvariant="script">P</mi> </semantics></math> plane. The conceptual scheme of the waveguide array was adapted from Ref. [<a href="#B1-applsci-14-10463" class="html-bibr">1</a>], courtesy of Dr. Shengping Gong.</p>
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<p>Sketch of the Radial–Transverse–Normal (RTN) reference frame <math display="inline"><semantics> <msub> <mi mathvariant="script">T</mi> <mi>RTN</mi> </msub> </semantics></math> of unit vectors <math display="inline"><semantics> <mrow> <mo stretchy="false">{</mo> <msub> <mover accent="true"> <mi mathvariant="bold-italic">i</mi> <mo stretchy="false">^</mo> </mover> <mi mathvariant="normal">R</mi> </msub> <mo>,</mo> <mspace width="0.166667em"/> <msub> <mover accent="true"> <mi mathvariant="bold-italic">i</mi> <mo stretchy="false">^</mo> </mover> <mi mathvariant="normal">T</mi> </msub> <mo>,</mo> <mspace width="0.166667em"/> <msub> <mover accent="true"> <mi mathvariant="bold-italic">i</mi> <mo stretchy="false">^</mo> </mover> <mi mathvariant="normal">N</mi> </msub> <mo stretchy="false">}</mo> </mrow> </semantics></math>. The sail clock angle <math display="inline"><semantics> <mrow> <mi>δ</mi> <mo>∈</mo> <msup> <mrow> <mo>[</mo> <mn>0</mn> <mo>,</mo> <mspace width="0.166667em"/> <mn>360</mn> <mo>]</mo> </mrow> <mo>∘</mo> </msup> </mrow> </semantics></math> is the single control parameter of an SFGIS-propelled spacecraft.</p>
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<p>Dimensionless components <math display="inline"><semantics> <mrow> <mo>{</mo> <msub> <mi>a</mi> <msub> <mi>p</mi> <mi mathvariant="normal">R</mi> </msub> </msub> <mo>/</mo> <msub> <mi>a</mi> <mi>c</mi> </msub> <mo>,</mo> <mspace width="0.166667em"/> <msub> <mi>a</mi> <msub> <mi>p</mi> <mi mathvariant="normal">T</mi> </msub> </msub> <mo>/</mo> <msub> <mi>a</mi> <mi>c</mi> </msub> <mo>,</mo> <mspace width="0.166667em"/> <msub> <mi>a</mi> <msub> <mi>p</mi> <mi mathvariant="normal">N</mi> </msub> </msub> <mo>/</mo> <msub> <mi>a</mi> <mi>c</mi> </msub> <mo>}</mo> </mrow> </semantics></math> of the propulsive acceleration vector as a function of the sail clock angle <math display="inline"><semantics> <mrow> <mi>δ</mi> <mo>∈</mo> <msup> <mrow> <mo>[</mo> <mn>0</mn> <mo>,</mo> <mspace width="0.166667em"/> <mn>360</mn> <mo>]</mo> </mrow> <mo>∘</mo> </msup> </mrow> </semantics></math>, when the solar distance is one astronomical unit.</p>
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<p>Time variation in the (unconstrained) sail clock angle <math display="inline"><semantics> <mi>δ</mi> </semantics></math> in the minimum-time Earth–Venus mission scenario when <math display="inline"><semantics> <mrow> <msub> <mi>a</mi> <mi>c</mi> </msub> <mo>=</mo> <mn>0.175</mn> <mspace width="0.166667em"/> <mi>mm</mi> <mo>/</mo> <msup> <mi mathvariant="normal">s</mi> <mn>2</mn> </msup> </mrow> </semantics></math>. Blue dot → starting point; red square → arrival point.</p>
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<p>Ecliptic projection and isometric view of the rapid transfer trajectory in an Earth–Venus mission scenario, when <math display="inline"><semantics> <mrow> <msub> <mi>a</mi> <mi>c</mi> </msub> <mo>=</mo> <mn>0.175</mn> <mspace width="0.166667em"/> <mi>mm</mi> <mo>/</mo> <msup> <mi mathvariant="normal">s</mi> <mn>2</mn> </msup> </mrow> </semantics></math> and the sail clock angle <math display="inline"><semantics> <mi>δ</mi> </semantics></math> is unconstrained. The <span class="html-italic">z</span>-axis of the isometric view is exaggerated to highlight the three-dimensionality of the transfer trajectory. Black line → spacecraft transfer trajectory; blue line → Earth’s orbit; red line → Venus’s orbit; filled star → perihelion; blue dot → starting point; red square → arrival point; orange dot → the Sun.</p>
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<p>Time variation of the (unconstrained) sail clock angle <math display="inline"><semantics> <mi>δ</mi> </semantics></math> in a minimum-time Earth–asteroid 433 Eros mission scenario when <math display="inline"><semantics> <mrow> <msub> <mi>a</mi> <mi>c</mi> </msub> <mo>=</mo> <mn>0.175</mn> <mspace width="0.166667em"/> <mi>mm</mi> <mo>/</mo> <msup> <mi mathvariant="normal">s</mi> <mn>2</mn> </msup> </mrow> </semantics></math>. The legend is reported in <a href="#applsci-14-10463-f004" class="html-fig">Figure 4</a>.</p>
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<p>Ecliptic projection and isometric view of the rapid transfer trajectory in an Earth–asteroid 433 Eros mission scenario, when <math display="inline"><semantics> <mrow> <msub> <mi>a</mi> <mi>c</mi> </msub> <mo>=</mo> <mn>0.175</mn> <mspace width="0.166667em"/> <mi>mm</mi> <mo>/</mo> <msup> <mi mathvariant="normal">s</mi> <mn>2</mn> </msup> </mrow> </semantics></math> and unconstrained sail clock angle <math display="inline"><semantics> <mi>δ</mi> </semantics></math>. The legend is reported in <a href="#applsci-14-10463-f005" class="html-fig">Figure 5</a>.</p>
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<p>Minimum flight time as a function of the characteristic acceleration <math display="inline"><semantics> <mrow> <msub> <mi>a</mi> <mi>c</mi> </msub> <mo>∈</mo> <mrow> <mo>[</mo> <mn>0.1</mn> <mo>,</mo> <mspace width="0.166667em"/> <mn>0.2</mn> <mo>]</mo> </mrow> <mspace width="0.166667em"/> <mi>mm</mi> <mo>/</mo> <msup> <mi mathvariant="normal">s</mi> <mn>2</mn> </msup> </mrow> </semantics></math> in an Earth–Venus orbit-to-orbit transfer. The black dot refers to the special case of <math display="inline"><semantics> <mrow> <msub> <mi>a</mi> <mi>c</mi> </msub> <mo>=</mo> <mn>0.175</mn> <mspace width="0.166667em"/> <mi>mm</mi> <mo>/</mo> <msup> <mi mathvariant="normal">s</mi> <mn>2</mn> </msup> </mrow> </semantics></math> discussed in the first part of the section.</p>
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<p>Ecliptic projection and isometric view of the rapid transfer trajectory in an Earth–Mars mission scenario, when <math display="inline"><semantics> <mrow> <msub> <mi>a</mi> <mi>c</mi> </msub> <mo>=</mo> <mn>0.175</mn> <mspace width="0.166667em"/> <mi>mm</mi> <mo>/</mo> <msup> <mi mathvariant="normal">s</mi> <mn>2</mn> </msup> </mrow> </semantics></math> and the sail clock angle <math display="inline"><semantics> <mi>δ</mi> </semantics></math> is unconstrained. The legend is reported in <a href="#applsci-14-10463-f005" class="html-fig">Figure 5</a>.</p>
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<p>Time variation of the (unconstrained) sail clock angle <math display="inline"><semantics> <mi>δ</mi> </semantics></math> in a minimum-time Earth–Mars mission scenario when <math display="inline"><semantics> <mrow> <msub> <mi>a</mi> <mi>c</mi> </msub> <mo>=</mo> <mn>0.175</mn> <mspace width="0.166667em"/> <mi>mm</mi> <mo>/</mo> <msup> <mi mathvariant="normal">s</mi> <mn>2</mn> </msup> </mrow> </semantics></math>. The legend is reported in <a href="#applsci-14-10463-f004" class="html-fig">Figure 4</a>.</p>
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<p>Ecliptic projection and isometric view of the rapid transfer trajectory of an Earth–Mercury mission scenario, when <math display="inline"><semantics> <mrow> <msub> <mi>a</mi> <mi>c</mi> </msub> <mo>=</mo> <mn>0.175</mn> <mspace width="0.166667em"/> <mi>mm</mi> <mo>/</mo> <msup> <mi mathvariant="normal">s</mi> <mn>2</mn> </msup> </mrow> </semantics></math> and the sail clock angle <math display="inline"><semantics> <mi>δ</mi> </semantics></math> is unconstrained. The legend is reported in <a href="#applsci-14-10463-f005" class="html-fig">Figure 5</a>.</p>
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<p>Time variation in the (unconstrained) sail clock angle <math display="inline"><semantics> <mi>δ</mi> </semantics></math> in a minimum-time Earth–Mercury mission scenario when <math display="inline"><semantics> <mrow> <msub> <mi>a</mi> <mi>c</mi> </msub> <mo>=</mo> <mn>0.175</mn> <mspace width="0.166667em"/> <mi>mm</mi> <mo>/</mo> <msup> <mi mathvariant="normal">s</mi> <mn>2</mn> </msup> </mrow> </semantics></math>. The legend is reported in <a href="#applsci-14-10463-f004" class="html-fig">Figure 4</a>.</p>
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<p>Time variation of the constrained sail clock angle <math display="inline"><semantics> <mi>δ</mi> </semantics></math> in a minimum-time Earth–Venus mission scenario when <math display="inline"><semantics> <mrow> <msub> <mi>a</mi> <mi>c</mi> </msub> <mo>=</mo> <mn>0.175</mn> <mspace width="0.166667em"/> <mi>mm</mi> <mo>/</mo> <msup> <mi mathvariant="normal">s</mi> <mn>2</mn> </msup> </mrow> </semantics></math>. The legend is reported in <a href="#applsci-14-10463-f004" class="html-fig">Figure 4</a>. (<b>a</b>) Case of <math display="inline"><semantics> <mrow> <mi mathvariant="script">I</mi> <mo>=</mo> <msub> <mi mathvariant="script">I</mi> <mrow> <mo>①</mo> </mrow> </msub> </mrow> </semantics></math>; (<b>b</b>) Case of <math display="inline"><semantics> <mrow> <mi mathvariant="script">I</mi> <mo>=</mo> <msub> <mi mathvariant="script">I</mi> <mrow> <mo>②</mo> </mrow> </msub> </mrow> </semantics></math>.</p>
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<p>Sun–spacecraft distance <span class="html-italic">r</span> as a function of time in a minimum-time Earth–Venus mission scenario when <math display="inline"><semantics> <mrow> <msub> <mi>a</mi> <mi>c</mi> </msub> <mo>=</mo> <mn>0.175</mn> <mspace width="0.166667em"/> <mi>mm</mi> <mo>/</mo> <msup> <mi mathvariant="normal">s</mi> <mn>2</mn> </msup> </mrow> </semantics></math>. The legend is reported in <a href="#applsci-14-10463-f004" class="html-fig">Figure 4</a>. (<b>a</b>) Case of <math display="inline"><semantics> <mrow> <mi mathvariant="script">I</mi> <mo>=</mo> <msub> <mi mathvariant="script">I</mi> <mrow> <mo>①</mo> </mrow> </msub> </mrow> </semantics></math>; (<b>b</b>) Case of <math display="inline"><semantics> <mrow> <mi mathvariant="script">I</mi> <mo>=</mo> <msub> <mi mathvariant="script">I</mi> <mrow> <mo>②</mo> </mrow> </msub> </mrow> </semantics></math>.</p>
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<p>Sketch of an SFGIS with two control vanes. The force due to the solar radiation pressure acting on the two moving surfaces is applied at the vane pressure center <math display="inline"><semantics> <msub> <mi>C</mi> <mi>p</mi> </msub> </semantics></math>. The rotation of the surfaces, denoted by <math display="inline"><semantics> <mi>β</mi> </semantics></math>, is the vane control angle.</p>
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<p>Closed-loop control scheme with saturation of the input to the system.</p>
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<p>Results of the numerical simulation when <math display="inline"><semantics> <mrow> <mi>k</mi> <mo>≃</mo> <mn>9.1724</mn> <mo>×</mo> <msup> <mn>10</mn> <mrow> <mo>−</mo> <mn>8</mn> </mrow> </msup> <mspace width="0.166667em"/> <mi>rad</mi> <mo>/</mo> <msup> <mi mathvariant="normal">s</mi> <mn>2</mn> </msup> </mrow> </semantics></math>.</p>
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<p>Minimum settling time <math display="inline"><semantics> <msub> <mi>t</mi> <mi>s</mi> </msub> </semantics></math> to perform a rotation of <math display="inline"><semantics> <mrow> <msub> <mi>δ</mi> <mi>ref</mi> </msub> <mo>=</mo> <mn>1</mn> <mspace width="0.166667em"/> <mi>rad</mi> </mrow> </semantics></math> around <span class="html-italic">z</span> as a function of <span class="html-italic">k</span>.</p>
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<p>Optimal control parameters of the PDF controller as a function of <span class="html-italic">k</span>.</p>
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12 pages, 253 KiB  
Review
A Study to Investigate the Role and Challenges Associated with the Use of Deep Learning in Autonomous Vehicles
by Nojood O. Aljehane
World Electr. Veh. J. 2024, 15(11), 518; https://doi.org/10.3390/wevj15110518 - 12 Nov 2024
Viewed by 481
Abstract
The application of deep learning in autonomous vehicles has surged over the years with advancements in technology. This research explores the integration of deep learning algorithms into autonomous vehicles (AVs), focusing on their role in perception, decision-making, localization, mapping, and navigation. It shows [...] Read more.
The application of deep learning in autonomous vehicles has surged over the years with advancements in technology. This research explores the integration of deep learning algorithms into autonomous vehicles (AVs), focusing on their role in perception, decision-making, localization, mapping, and navigation. It shows how deep learning, as a part of machine learning, mimics the human brain’s neural networks, enabling advancements in perception, decision-making, localization, mapping, and overall navigation. Techniques like convolutional neural networks are used for image detection and steering control, while deep learning is crucial for path planning, automated parking, and traffic maneuvering. Localization and mapping are essential for AVs’ navigation, with deep learning-based object detection mechanisms like Faster R-CNN and YOLO proving effective in real-time obstacle detection. Apart from the roles, this study also revealed that the integration of deep learning in AVs faces challenges such as dataset uncertainty, sensor challenges, and model training intricacies. However, these issues can be addressed through the increased standardization of sensors and real-life testing for model training, and advancements in model compression technologies can optimize the performance of deep learning in AVs. This study concludes that deep learning plays a crucial role in enhancing the safety and reliability of AV navigation. This study contributes to the ongoing discourse on the optimal integration of deep learning in AVs, aiming to foster their safety, reliability, and societal acceptance. Full article
(This article belongs to the Special Issue Deep Learning Applications for Electric Vehicles)
16 pages, 1085 KiB  
Article
Effect of a Sensorimotor Training Program for Aerial Maneuvers in Junior Surfers
by Pedro Seixas, Raul Oliveira, Isabel Carita, Ian Davis and Miguel Moreira
Appl. Sci. 2024, 14(22), 10159; https://doi.org/10.3390/app142210159 - 6 Nov 2024
Viewed by 358
Abstract
The purpose of this study was to examine the impact of a sensorimotor training program on maximum ankle dorsiflexion (ankle DF), coordination, dynamic balance and postural control, and lower-limb muscle power, in competitive junior surfers, and its relation to parameters of sensorimotor control [...] Read more.
The purpose of this study was to examine the impact of a sensorimotor training program on maximum ankle dorsiflexion (ankle DF), coordination, dynamic balance and postural control, and lower-limb muscle power, in competitive junior surfers, and its relation to parameters of sensorimotor control required to perform aerial maneuvers. Twelve junior competitive surfers followed a 7-week sensorimotor training program, being assessed pre- and post-program with the knee-to-wall test (KW), Y-Balance test—lower quarter (YBT-LQ), and the countermovement jump test (CMJ). Post-training assessment revealed positive effects on the KW (ankle DF) distance, which increased approximately 2 cm (p < 0.001) for both ankles, and all scores for the YTB-LQ (coordination, dynamic balance, and postural control) variables increased, being significant (p < 0.005) for some reach distances (YBT-LQ—Anterior Left, YBT-LQ—Postero-medial Left, and YTB-LQ Anterior Right). YBT-LQ Anterior Reach Asymmetry also improved by decreasing 1.62 cm (p < 0.001) and the CMJ height (lower limb muscle power) increased 2.89 cm (p < 0.001). The training program proved to effectively enhance parameters of physical performance for this sample, including ankle DF, coordination, dynamic balance, postural control, and lower limb muscle power. This tailored-made task approach can help to optimize surfing performance capabilities and contribute to reducing the risk of injuries while performing aerials. Full article
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Figure 1
<p>Pre- and post-training means and standard deviation values of ankle dorsiflexion (cm) with knee-to-wall (KW) test.</p>
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<p>Pre and post-training measures of lower limb muscle power, assessed with the CMJa test (cm).</p>
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18 pages, 6141 KiB  
Article
Optimizing Solid Rocket Missile Trajectories: A Hybrid Approach Using an Evolutionary Algorithm and Machine Learning
by Carlo Ferro, Matteo Cafaro and Paolo Maggiore
Aerospace 2024, 11(11), 912; https://doi.org/10.3390/aerospace11110912 - 6 Nov 2024
Viewed by 484
Abstract
This paper introduces a novel approach for modeling and optimizing the trajectory and behavior of small solid rocket missiles. The proposed framework integrates a six-degree-of-freedom (6DoF) simulation environment experimentally tuned for accuracy, with a combination of genetic algorithms (GAs) and machine learning (ML) [...] Read more.
This paper introduces a novel approach for modeling and optimizing the trajectory and behavior of small solid rocket missiles. The proposed framework integrates a six-degree-of-freedom (6DoF) simulation environment experimentally tuned for accuracy, with a combination of genetic algorithms (GAs) and machine learning (ML) to enhance the performance of the missile path. In the initial phase, a GA is employed to optimize the missile’s trajectory for efficient target acquisition, defining key launch parameters such as the ramp angle and lateral maneuver force to minimize positional errors and to ensure effective target engagement. Following trajectory optimization, the derived data are used to train an ML model that predicts setup parameters, significantly reducing computational costs and time. This close integration enables real-time adjustments for acquiring moving targets, thereby improving accuracy and minimizing maneuvering costs. This study also explores the application of fluidic thrust vectoring for small rockets, providing an innovative solution to enhance maneuverability and control, especially at low speeds. The proposed framework was validated using experimental launch data from the Icarus Team. The methodology offers a robust and cost-effective solution for precision targeting and improved maneuverability in aerospace and defense contexts. Full article
(This article belongs to the Section Astronautics & Space Science)
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Figure 1
<p>Patented section view of small rocket with integrated cooling and thrust vectoring.</p>
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<p>Reference frames.</p>
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<p>Model overview.</p>
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<p>A schematic of the classification NN.</p>
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<p>A schematic of the regression NN.</p>
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<p>Optimal trajectory calculation: (<b>a</b>) workflow diagram, (<b>b</b>) target grid, (<b>c</b>) post-processing graph.</p>
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<p>NN training and extraction of the model.</p>
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<p>GA optimization algorithm: (<b>a</b>) time contour plot, (<b>b</b>) zenith contour plot, (<b>c</b>) maneuver angle contour plot, (<b>d</b>) accuracy contour plot, (<b>e</b>) accuracy histogram, (<b>f</b>) typical trajectory.</p>
Full article ">Figure 8 Cont.
<p>GA optimization algorithm: (<b>a</b>) time contour plot, (<b>b</b>) zenith contour plot, (<b>c</b>) maneuver angle contour plot, (<b>d</b>) accuracy contour plot, (<b>e</b>) accuracy histogram, (<b>f</b>) typical trajectory.</p>
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<p>GA optimization algorithm with restricted domain: (<b>a</b>) time contour plot, (<b>b</b>) zenith contour plot, (<b>c</b>) maneuver angle contour plot, (<b>d</b>) accuracy contour plot, (<b>e</b>) accuracy histogram, (<b>f</b>) typical trajectory.</p>
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<p>GA optimization algorithm with restricted domain: (<b>a</b>) time contour plot, (<b>b</b>) zenith contour plot, (<b>c</b>) maneuver angle contour plot, (<b>d</b>) accuracy contour plot, (<b>e</b>) accuracy histogram, (<b>f</b>) typical trajectory.</p>
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<p>Performance of NN classification algorithm: (<b>a</b>) neural network zenith angle; (<b>b</b>) GA zenith angle. (<b>c</b>) the network’s proficiency; (<b>d</b>) the confusion matrix.</p>
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<p>Performance of NN classification algorithm under the different zenith angles: (<b>a</b>,<b>b</b>) 0°, (<b>c</b>,<b>d</b>) 15°, (<b>e</b>,<b>f</b>) 30°, and (<b>g</b>,<b>h</b>) 45°.</p>
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<p>Performance of NN classification algorithm under the different zenith angles: (<b>a</b>,<b>b</b>) 0°, (<b>c</b>,<b>d</b>) 15°, (<b>e</b>,<b>f</b>) 30°, and (<b>g</b>,<b>h</b>) 45°.</p>
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<p>Different batch performance evaluations with NN: (<b>a</b>) time contour plot, (<b>b</b>) zenith contour plot, (<b>c</b>) maneuver angle contour plot, (<b>d</b>) accuracy contour plot, (<b>e</b>) accuracy histogram, (<b>f</b>) typical trajectory.</p>
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<p>Different batch performance evaluations with NN: (<b>a</b>) time contour plot, (<b>b</b>) zenith contour plot, (<b>c</b>) maneuver angle contour plot, (<b>d</b>) accuracy contour plot, (<b>e</b>) accuracy histogram, (<b>f</b>) typical trajectory.</p>
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<p>Aerodynamic forces and moment coefficients expressed in body axes (x, longitudinal; y and z, transversal axes): (<b>a</b>) force coefficient along z body axis, (<b>b</b>) force coefficient along x body axis, (<b>c</b>) moment coefficient around y body axis.</p>
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<p>Aerodynamic forces and moment coefficients expressed in body axes (x, longitudinal; y and z, transversal axes): (<b>a</b>) force coefficient along z body axis, (<b>b</b>) force coefficient along x body axis, (<b>c</b>) moment coefficient around y body axis.</p>
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21 pages, 36914 KiB  
Article
Development of a Novel Tailless X-Type Flapping-Wing Micro Air Vehicle with Independent Electric Drive
by Yixin Zhang, Song Zeng, Shenghua Zhu, Shaoping Wang, Xingjian Wang, Yinan Miao, Le Jia, Xinyu Yang and Mengqi Yang
Biomimetics 2024, 9(11), 671; https://doi.org/10.3390/biomimetics9110671 - 3 Nov 2024
Viewed by 584
Abstract
A novel tailless X-type flapping-wing micro air vehicle with two pairs of independent drive wings is designed and fabricated in this paper. Due to the complexity and unsteady of the flapping wing mechanism, the geometric and kinematic parameters of flapping wings significantly influence [...] Read more.
A novel tailless X-type flapping-wing micro air vehicle with two pairs of independent drive wings is designed and fabricated in this paper. Due to the complexity and unsteady of the flapping wing mechanism, the geometric and kinematic parameters of flapping wings significantly influence the aerodynamic characteristics of the bio-inspired flying robot. The wings of the vehicle are vector-controlled independently on both sides, enhancing the maneuverability and robustness of the system. Unique flight control strategy enables the aircraft to have multiple flight modes such as fast forward flight, sharp turn and hovering. The aerodynamics of the prototype is analyzed via the lattice Boltzmann method of computational fluid dynamics. The chordwise flexible deformation of the wing is implemented via designing a segmented rigid model. The clap-and-peel mechanism to improve the aerodynamic lift is revealed, and two air jets in one cycle are shown. Moreover, the dynamics experiment for the novel vehicle is implemented to investigate the kinematic parameters that affect the generation of thrust and maneuver moment via a 6-axis load cell. Optimized parameters of the flapping wing motion and structure are obtained to improve flight dynamics. Finally, the prototype realizes controllable take-off and flight from the ground. Full article
(This article belongs to the Section Locomotion and Bioinspired Robotics)
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<p>Designed configuration and related details display of the prototype.</p>
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<p>Onboard electronic system structure.</p>
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<p>Bionic wings with different membrane materials and wing vein distribution.</p>
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<p>Double crank-rocker mechanism.</p>
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<p>Clap-and-peel mechanism during the flapping wing process. (<b>a</b>) Clap of the real butterfly; (<b>b</b>) Near clap; (<b>c</b>) Leading edges touch together; (<b>d</b>) Peel of the real butterfly; (<b>e</b>) Completely clap; (<b>f</b>) Initial peel; (<b>g</b>) End of peel of the real butterfly; (<b>h</b>) Trailing edges separate; (<b>i</b>) Completely peel.</p>
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<p>Tailless vector control schematic diagram of the prototype. (<b>a</b>) Altitude control; (<b>b</b>) Yaw control; (<b>c</b>) Pitch control (head up); (<b>d</b>) Pitch control (head down); (<b>e</b>) Roll control (clockwise); (<b>f</b>) Roll control (counterclockwise).</p>
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<p>PD attitude feedback control system for the X-type tailless FMAV.</p>
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<p>(<b>a</b>) Initial location diagram of various parts of prototype model in Xflow; (<b>b</b>) Model of X-type FMAV in Adams; (<b>c</b>) Visualization of the vortex structure of the flexible model in the Xflow flow field.</p>
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<p>Experiment setup for force, torque and power measurements.</p>
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<p>Vicon system setup for attitude angle (pitch <math display="inline"><semantics> <mi>θ</mi> </semantics></math>, roll <math display="inline"><semantics> <mi>ϕ</mi> </semantics></math> and yaw <math display="inline"><semantics> <mi>ψ</mi> </semantics></math>), angular rates (<span class="html-italic">p</span>, <span class="html-italic">q</span>, <span class="html-italic">r</span>) and spatial position (<math display="inline"><semantics> <mrow> <mi>x</mi> <mo>,</mo> <mi>y</mi> <mo>,</mo> <mi>z</mi> </mrow> </semantics></math>) real-time measurements using a frame rate of 150 Hz.</p>
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<p>Simulation results of the wing flow field of the X-type FMAV: (<b>a</b>) at t = 0.015 s, the vorticity isosurface around the aircraft; (<b>b</b>) at t = 0.025 s, that is, when the wings clap together, vertical z-direction cutting plane, velocity vector field diagram at z = 0.1 m.</p>
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<p>Instantaneous aerodynamic forces in X-, Y- and Z-axis for 4 cycles of hovering FMAV.</p>
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<p>The cutting plane in the vertical z direction during the first flapping stroke of hovering flight, the frame-by-frame screenshot of vector velocity field at z = 0.1 m, and the flapping period is T = 0.05 s.</p>
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<p>Visualization results of isosurface based on vorticity from an oblique downward 45° viewing angle at (<b>a</b>) t = T/4, (<b>b</b>) T/2, (<b>c</b>) 3T/4, and (<b>d</b>) T, respectively.</p>
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<p>Simulation results of flow field at the end of the first cycle of hovering flight of the X-type FMAV: (<b>a</b>) the visualized image of front view vorticity isosurface; (<b>b</b>) the screenshot of velocity field at x = 0 m of cutting plane, perpendicul to the X-axis; (<b>c</b>) the screenshot of velocity field at z = 0.1 m of cutting plane, perpendicular to Z-axis.</p>
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<p>Generation of force and torques in three axes for a range of control inputs. (<b>a</b>) Yaw control; (<b>b</b>) Pitch control; (<b>c</b>) Roll control.</p>
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<p>Free flight test of the prototype. (<b>a</b>) Take-off test of prototype with rope constraints; (<b>b</b>) A 3D trajectory plot of the X-type FMAV.</p>
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20 pages, 5107 KiB  
Article
A Decision Model for Ship Overtaking in Straight Waterway Channels
by Nian Liu, Yong Shen, Fei Lin and Yihua Liu
J. Mar. Sci. Eng. 2024, 12(11), 1976; https://doi.org/10.3390/jmse12111976 - 2 Nov 2024
Viewed by 395
Abstract
Overtaking situations are commonly encountered in maritime navigation, and the overtaking process involves various risk factors that significantly contribute to collision incidents. It is crucial to conduct research on the maneuvering behaviors and decision-making processes associated with ship overtaking. This paper proposes a [...] Read more.
Overtaking situations are commonly encountered in maritime navigation, and the overtaking process involves various risk factors that significantly contribute to collision incidents. It is crucial to conduct research on the maneuvering behaviors and decision-making processes associated with ship overtaking. This paper proposes a method based on the analysis of ship maneuvering performance to investigate overtaking behaviors in navigational channels. A relative motion model is established for both the overtaking and the overtaken vessels, and the inter-vessel distance is calculated, taking into account the psychological perceptions of the ship’s driver. A decision-making model for ship overtaking is presented to provide a safety protocol for overtaking maneuvers. Applying this method to overtaking data from the South Channel shows that it effectively characterizes both the permissible overtaking space and the driver’s overtaking desire. Additionally, it enables the prediction of optimal overtaking timing and strategies based on short-term trajectory forecasts. Thus, this method not only offers a safe overtaking plan for vessels but also provides auxiliary information for decision making in intelligent ship navigation. Full article
(This article belongs to the Section Ocean Engineering)
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<p>Ship overtaking situation.</p>
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<p>Analysis of ship overtaking phases.</p>
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<p>Schematic diagram of the ship-to-ship effect.</p>
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<p>Schematic diagram of the ship’s overtaking phase.</p>
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<p>Schematic diagram of virtual force directions.</p>
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<p>Distribution of ship driver’s concerns.</p>
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<p>Schematic diagram of a ship’s overtaking time field.</p>
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<p>Three-dimensional schematic of the field.</p>
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<p>Non-contact force.</p>
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<p>Dynamic overtaking space.</p>
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<p>Minimum distance between ship field in port and starboard space.</p>
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<p>Three systems.</p>
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<p>The variation in <math display="inline"><semantics> <mrow> <msubsup> <mrow> <mi>S</mi> </mrow> <mrow> <mi>i</mi> <mi>j</mi> </mrow> <mrow> <mo>∗</mo> </mrow> </msubsup> </mrow> </semantics></math> with differrent values of <math display="inline"><semantics> <mrow> <mi>γ</mi> </mrow> </semantics></math>.</p>
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<p>Vessel’s lateral force.</p>
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<p>Vessel’s yawing moment.</p>
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<p>Changes in the distance between the overtaking vessel “ORIENTAL GLORY” and the overtaken vessel “RUNFABAOBOAT”.</p>
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<p>Changes in speed of the overtaking vessel “ORIENTAL GLORY”.</p>
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<p>Overtaking decision model.</p>
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16 pages, 10062 KiB  
Article
Energy Consumption Performance of a VTOL UAV In and Out of Ground Effect by Flight Test
by Shanfei Su, Xiaowen Shan, Peng Yu and Hao Wang
Drones 2024, 8(11), 625; https://doi.org/10.3390/drones8110625 - 30 Oct 2024
Viewed by 358
Abstract
Current research on ground-effect unmanned aerial vehicles (UAVs) predominantly centers on numerical aerodynamic optimization and stability analysis in the ground effect, leaving a significant gap in the thorough examination of flight performance through flight tests. This study presents the design of a vertical [...] Read more.
Current research on ground-effect unmanned aerial vehicles (UAVs) predominantly centers on numerical aerodynamic optimization and stability analysis in the ground effect, leaving a significant gap in the thorough examination of flight performance through flight tests. This study presents the design of a vertical takeoff and landing (VTOL) ground-effect UAV, featuring a vector motor configuration. The control system utilizes a decoupled strategy based on position and attitude, enabling stable altitude control in the low-altitude ground-effect region. Comprehensive flight tests were conducted to evaluate the UAV’s flight stability and energy consumption in the ground-effect region. The results reveal that the ground-effect UAV successfully performed rapid takeoff maneuvers and maintained stable forward flight in the designated ground-effect region. In the span-dominated ground-effect region, a significant 33% reduction in flight current was observed, leading to a corresponding 33% decrease in total power consumption compared to flight conditions outside the ground effect. These findings highlight a substantial improvement in flight performance under the influence of ground effect. The real-time flight data produced by this system provides valuable insights for optimizing the design of VTOL ground-effect UAVs. Full article
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<p>Aerodynamic performance and eigenvalue root locus distribution as a function of height [<a href="#B19-drones-08-00625" class="html-bibr">19</a>].</p>
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<p>Aerodynamic performance and eigenvalue root locus distribution as a function of height [<a href="#B19-drones-08-00625" class="html-bibr">19</a>].</p>
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<p>Egretta30 flight system.</p>
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<p>Data transmission system.</p>
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<p>Force analysis diagram.</p>
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<p>Framework of the proposed controller.</p>
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<p>Estimation and control of altitude [<a href="#B28-drones-08-00625" class="html-bibr">28</a>].</p>
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<p>The smoke generation device for flow visualization.</p>
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<p>Reference trajectory for one flight test mission in the ground-effect region.</p>
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<p>Flow visualization of the wingtip vortices at various ground-effect heights. The time points <span class="html-italic">t</span><sub>1</sub> and <span class="html-italic">t</span><sub>2</sub> represent the instances when the wingtip vortex is most pronounced and when it enters the dissipation phase, respectively.</p>
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<p>Attitude tracking of flight stability test.</p>
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<p>Altitude-holding test in span-dominated ground-effect regions.</p>
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<p>Corresponding altitude holding and ground speed.</p>
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<p>Attitude-tracking performance in various ground-effect regions.</p>
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<p>Propulsive control inputs in various ground-effect regions.</p>
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<p>Power consumption in various ground-effect regions.</p>
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19 pages, 9816 KiB  
Article
Mission Planning Method for Dense Area Target Observation Based on Clustering Agile Satellites
by Chuanyi Yu, Xin Nie, Yuan Chen and Yilin Chen
Electronics 2024, 13(21), 4244; https://doi.org/10.3390/electronics13214244 - 29 Oct 2024
Viewed by 468
Abstract
To address the mission planning challenge for agile satellites in dense point target observation, a clustering strategy based on an ant colony algorithm and a heuristic simulated genetic annealing optimization algorithm are proposed. First, the imaging observation process of agile satellites is analyzed, [...] Read more.
To address the mission planning challenge for agile satellites in dense point target observation, a clustering strategy based on an ant colony algorithm and a heuristic simulated genetic annealing optimization algorithm are proposed. First, the imaging observation process of agile satellites is analyzed, and an improved ant colony algorithm is employed to optimize the clustering of observation tasks, enabling the satellites to complete more observation tasks efficiently with a more stable attitude. Second, to solve for the optimal group target observation sequence and achieve higher total observation benefits, a task planning model based on multi-target observation benefits and attitude maneuver energy consumption is established, considering the visible time windows of targets and the time constraints between adjacent targets. To overcome the drawbacks of traditional simulated annealing and genetic algorithms, which are prone to local optimal solution and a slow convergence speed, a novel Simulated Genetic Annealing Algorithm is designed while optimizing the sum of target observation weights and yaw angles while also accounting for factors such as target visibility windows and satellite attitude transition times between targets. Ultimately, the feasibility and efficiency of the proposed algorithm are substantiated by comparing its performance against traditional heuristic optimization algorithms using a dataset comprising large-scale dense ground targets. Full article
(This article belongs to the Section Artificial Intelligence)
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<p>Satellite observation attitude.</p>
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<p>Task clustering.</p>
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<p>Group division.</p>
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<p>Task planning.</p>
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<p>SA-GA process.</p>
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<p>The rule of 0–1 encoding.</p>
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<p>Crossover operation.</p>
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<p>Mutation operation.</p>
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<p>Point target distribution map.</p>
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<p>Iteration benefit comparison.</p>
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<p>The benefit of each algorithm run.</p>
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<p>Iteration benefit comparison.</p>
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<p>The benefit of each algorithm run.</p>
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<p>Benefits before and after clustering.</p>
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<p>Benefits before and after clustering.</p>
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22 pages, 1480 KiB  
Article
Work of Breathing for Aviators: A Missing Link in Human Performance
by Victoria Ribeiro Rodrigues, Rheagan A. Pratt, Chad L. Stephens, David J. Alexander and Nicholas J. Napoli
Life 2024, 14(11), 1388; https://doi.org/10.3390/life14111388 - 28 Oct 2024
Viewed by 544
Abstract
In this study, we explore the work of breathing (WoB) experienced by aviators during the Anti-G Straining Maneuver (AGSM) to improve pilot safety and performance. Traditional airflow models of WoB fail to adequately distinguish between breathing rate and inspiratory frequency, leading to potentially [...] Read more.
In this study, we explore the work of breathing (WoB) experienced by aviators during the Anti-G Straining Maneuver (AGSM) to improve pilot safety and performance. Traditional airflow models of WoB fail to adequately distinguish between breathing rate and inspiratory frequency, leading to potentially inaccurate assessments. This mismatch can have serious implications, particularly in critical flight situations where understanding the true respiratory workload is essential for maintaining performance. To address these limitations, we used a non-sinusoidal model that captures the complexities of WoB under high inspiratory frequencies and varying dead space conditions. Our findings indicate that the classical airflow model tends to underestimate WoB, particularly at elevated inspiratory frequencies ranging from 0.5 to 2 Hz, where resistive forces play a significant role and elastic forces become negligible. Additionally, we show that an increase in dead space, coupled with high-frequency breathing, elevates WoB, heightening the risk of dyspnea among pilots. Interestingly, our analysis reveals that higher breathing rates lead to a decrease in total WoB, an unexpected finding suggesting that refining breathing patterns could help pilots optimize their energy expenditure. This research highlights the importance of examining the relationship between alveolar ventilation, breathing rate, and inspiratory frequency in greater depth within realistic flight scenarios. These insights indicate the need for targeted training programs and adaptive life-support systems to better equip pilots for managing respiratory challenges in high-stress situations. Ultimately, our research lays the groundwork for enhancing respiratory support for aviators, contributing to safer and more efficient flight operations. Full article
(This article belongs to the Section Physiology and Pathology)
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<p>Idealized representation of inspired instantaneous flow as sine wave utilizing a pneumotachogram.</p>
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<p>Breakdown of WoB forces using the Classical Sinusoidal Model. The overall internal WoB is composed of three key components: (1) Elastic work, which includes the effort required to overcome the elastic recoil of both the lungs and chest wall; (2) Viscous work, which accounts for the resistance posed by tissues, including lung and chest wall resistance; and (3) Turbulent work, which encompasses the effort needed to overcome airway resistance, including both intrinsic airway resistance and additional resistance from airway devices and circuits. The circles in the figure show where the viscous and turbulent forces overtake the elastic forces.</p>
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<p>A pictorial example of different waveforms. A waveform is considered sinusoidal if <math display="inline"><semantics> <mrow> <msub> <mi>T</mi> <mi>I</mi> </msub> <mo>=</mo> <msub> <mi>T</mi> <mi>E</mi> </msub> </mrow> </semantics></math> for a singular breath. Non-sinusoidal waveforms consider <math display="inline"><semantics> <msub> <mi>T</mi> <mi>I</mi> </msub> </semantics></math> and <math display="inline"><semantics> <msub> <mi>T</mi> <mi>E</mi> </msub> </semantics></math> dynamic, and examples of these dynamics are conveyed in (graphs <b>A</b>–<b>C</b>).</p>
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<p>Percentage change in WoB between the Classical Sinusoidal Model and the Non-Sinusoidal Model for both low and high inspiratory flows, considering an alveolar ventilation of 6 L/min. A positive percentage change indicates that the Non-Sinusoidal Model results in a higher WoB compared to the Classical Model.</p>
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<p>Percentage change in WoB between the Classical Sinusoidal Model and the Non-Sinusoidal Model for both low and high inspiratory flows, considering an alveolar ventilation of 30 L/min. A positive percentage change indicates that the Non-Sinusoidal Model results in a higher WoB compared to the Classical Model.</p>
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<p>Elastic, Viscous and Turbulent Force breakdown for various inspiratory frequencies for an alveolar ventilation of 6 L/min model.</p>
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<p>Frequency and dead space effects on WoB at resting alveolar ventilation (6 L/min). The red circles indicate the optimal breathing rate for a given dead space.</p>
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<p>Frequency and dead space effects on WoB at high alveolar ventilation (30 L/min). The red circles indicate the optimal breathing rate for a given dead space.</p>
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23 pages, 3336 KiB  
Article
Insensitive Mechanism-Based Nonlinear Model Predictive Guidance for UAVs Intercepting Maneuvering Targets with Input Constraints
by Danpeng Huang, Mingjie Zhang, Taideng Zhan and Jianjun Ma
Drones 2024, 8(11), 608; https://doi.org/10.3390/drones8110608 - 24 Oct 2024
Viewed by 692
Abstract
This paper proposed an innovative guidance strategy, denoted as NMPC-IM, which integrates the Insensitive Mechanism (IM) with Nonlinear Model Predictive Control (NMPC) for Unmanned Aerial Vehicle (UAV) pursuit-evasion scenarios, with the aim of effectively intercepting maneuvering targets with consideration of input constraints while [...] Read more.
This paper proposed an innovative guidance strategy, denoted as NMPC-IM, which integrates the Insensitive Mechanism (IM) with Nonlinear Model Predictive Control (NMPC) for Unmanned Aerial Vehicle (UAV) pursuit-evasion scenarios, with the aim of effectively intercepting maneuvering targets with consideration of input constraints while minimizing average energy expenditure. Firstly, the basic principle of IM is proposed, and it is transformed into an additional cost function in NMPC. Secondly, in order to estimate the states of maneuvering target, a fixed-time sliding mode disturbance observer is developed. Thirdly, the UAV’s interception task is formulated into a comprehensive Quadratic Programming (QP) problem, and the NMPC-IM guidance strategy is presented, which is then improved by the adjustment of parameters and determination of maximum input. Finally, numerical simulations are carried out to validate the effectiveness of the proposed method, and the simulation results show that the NMPC-IM guidance strategy can decrease average energy expenditure by mitigating the impact of the target’s maneuverability, optimizing the UAV’s trajectory during the interception process. Full article
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<p>The UAV pursuit-evasion scenario. The blue and orange conical areas are the variable range of orientation angles of the UAV and the target, respectively, and represent their maneuvering capabilities, and also the constraints of control input. Larger top angles of the cones mean more maneuverability.</p>
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<p>Kinematics between UAV (<span class="html-italic">M</span>) and target (<span class="html-italic">T</span>).</p>
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<p>The structure of NMPC-IM in guidance.</p>
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<p>The basic idea of IM.</p>
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<p>Step-by-step schematic of Insensitive Mechanism.</p>
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<p>Different <math display="inline"><semantics> <msub> <mi>y</mi> <mi>d</mi> </msub> </semantics></math> in NMPC-IM: (<b>a</b>) Trajectories. (<b>b</b>) Control input. Green represents <math display="inline"><semantics> <mrow> <msub> <mi>y</mi> <mi>d</mi> </msub> <mo>=</mo> <msqrt> <mi>r</mi> </msqrt> </mrow> </semantics></math> and blue represents <math display="inline"><semantics> <mrow> <msub> <mi>y</mi> <mi>d</mi> </msub> <mo>=</mo> <mn>1</mn> <mo>/</mo> <msqrt> <mi>r</mi> </msqrt> </mrow> </semantics></math>.</p>
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<p>Comparisons of PNG and pure NMPC-IM (<math display="inline"><semantics> <mrow> <msub> <mi>a</mi> <mi>T</mi> </msub> <mo>=</mo> <mn>20</mn> <mo form="prefix">sin</mo> <mrow> <mo>(</mo> <mi>t</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> g): (<b>a</b>) Trajectories. (<b>b</b>) Control input. Green represents PNG and purple represents pure NMPC-IM.</p>
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<p>Comparisons of PNG and pure NMPC-IM (<math display="inline"><semantics> <mrow> <msub> <mi>a</mi> <mi>T</mi> </msub> <mo>=</mo> <mn>15</mn> <mo form="prefix">sin</mo> <mrow> <mo>(</mo> <mn>1.5</mn> <mi>t</mi> <mo>)</mo> </mrow> </mrow> </semantics></math> g): (<b>a</b>) Trajectories. (<b>b</b>) Control input. Green represents PNG and purple represents pure NMPC-IM.</p>
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<p>Different <math display="inline"><semantics> <msub> <mi>k</mi> <mi>t</mi> </msub> </semantics></math> in Maximum Input Determination: (<b>a</b>) Trajectories. (<b>b</b>) Control input.</p>
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<p>Comparisons of PNG, NMPC, NMPC-IM (sin): (<b>a</b>) Trajectories. (<b>b</b>) Control input. (<b>c</b>) Prediction horizon of NMPC-IM.</p>
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<p>Individually considerate of IM: (<b>a</b>) Trajectories. (<b>b</b>) Control input. (<b>c</b>) Prediction horizon.</p>
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<p>Comparisons of PNG, NMPC, NMPC-IM (exp): (<b>a</b>) Trajectories. (<b>b</b>) Control input. (<b>c</b>) Prediction horizon of NMPC-IM.</p>
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<p>Different initial heading angles of <span class="html-italic">M</span>: (<b>a</b>) Trajectories. (<b>b</b>) Control input.</p>
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<p>Addition of disturbance observer: (<b>a</b>) Trajectories. (<b>b</b>) Control input. <math display="inline"><semantics> <mrow> <mo>(</mo> <msub> <mi>t</mi> <mi>f</mi> </msub> <mo>,</mo> <mi>s</mi> <mi>u</mi> <mo>)</mo> </mrow> </semantics></math> = (36.64 s, 1.4346 g). (<b>c</b>) Prediction horizon of NMPC-IM. (<b>d</b>) Estimated and true values of <math display="inline"><semantics> <msub> <mi>a</mi> <mrow> <mi>T</mi> <mi>r</mi> </mrow> </msub> </semantics></math>. (<b>e</b>) Estimated and true values of <math display="inline"><semantics> <msub> <mi>a</mi> <mrow> <mi>T</mi> <mi>θ</mi> </mrow> </msub> </semantics></math>.</p>
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20 pages, 584 KiB  
Article
Cognitive Radar Waveform Selection for Low-Altitude Maneuvering-Target Tracking: A Robust Information-Aided Fusion Method
by Xiang Feng, Ping Sun, Lu Zhang, Guangle Jia, Jun Wang and Zhiquan Zhou
Remote Sens. 2024, 16(21), 3951; https://doi.org/10.3390/rs16213951 - 23 Oct 2024
Viewed by 621
Abstract
In this paper, we introduce an innovative interacting multiple-criterion selection (IMCS) idea to design the optimal radar waveform, aimingto reduce tracking error and enhance tracking performance. This method integrates the multiple-hypothesis tracking (MHT) and Rao–Blackwellized particle filter (RBPF) algorithms to tackle maneuvering First-Person-View [...] Read more.
In this paper, we introduce an innovative interacting multiple-criterion selection (IMCS) idea to design the optimal radar waveform, aimingto reduce tracking error and enhance tracking performance. This method integrates the multiple-hypothesis tracking (MHT) and Rao–Blackwellized particle filter (RBPF) algorithms to tackle maneuvering First-Person-View (FPV) drones in a three-dimensional low-altitude cluttered environment. A complex hybrid model, combining linear and nonlinear states, is constructed to describe the high maneuverability of the target. Based on the interacting multiple model (IMM) framework, our proposed IMCS method employs several waveform selection criteria as models and determines the optimal criterion with the highest probability to select waveform parameters. The simulation results indicate that the MHT–RBPF algorithm, using the IMCS method for adaptive parameter selection, exhibits high accuracy and robustness in tracking a low-altitude maneuvering target, resulting in lower root mean square error (RMSE) compared with fixed- or single-waveform selection mechanisms. Full article
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Graphical abstract

Graphical abstract
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<p>Low-altitude maneuvering-target tracking process of a radar system.</p>
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<p>The selection results of different parameter ranges and intervals.</p>
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<p>RMSEs from the selection of different waveform libraries.</p>
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<p>Tracking result using the IMCS–MHT–RBPF algorithm.</p>
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<p>RMSE for the IMCS–MHT–RBPF algorithm.</p>
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<p>RMSEs of each target state component for the IMCS–MHT–RBPF algorithm.</p>
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<p>Patterns of selected waveform parameters (Gaussian pulse length and sweep frequency).</p>
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<p>Index of the selected criterion at each time instant. (1: Max-Q; 2: Min-MSE; 3: Max-MI; 4: Min-Gate).</p>
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<p>RMSE of different clutter-processing methods for state estimation.</p>
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<p>Tracking results using different waveform selection criteria.</p>
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<p>RMSE of different waveform selection criteria.</p>
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<p>Patterns of selected pulse lengths using different waveform selection criteria.</p>
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<p>Patterns of selected sweep frequencies using different waveform selection criteria.</p>
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17 pages, 4394 KiB  
Article
Real-Time Semantic Segmentation of 3D LiDAR Point Clouds for Aircraft Engine Detection in Autonomous Jetbridge Operations
by Ihnsik Weon, Soongeul Lee and Juhan Yoo
Appl. Sci. 2024, 14(21), 9685; https://doi.org/10.3390/app14219685 - 23 Oct 2024
Viewed by 600
Abstract
This paper presents a study on aircraft engine identification using real-time 3D LiDAR point cloud segmentation technology, a key element for the development of automated docking systems in airport boarding facilities, known as jetbridges. To achieve this, 3D LiDAR sensors utilizing a spinning [...] Read more.
This paper presents a study on aircraft engine identification using real-time 3D LiDAR point cloud segmentation technology, a key element for the development of automated docking systems in airport boarding facilities, known as jetbridges. To achieve this, 3D LiDAR sensors utilizing a spinning method were employed to gather surrounding environmental 3D point cloud data. The raw 3D environmental data were then filtered using the 3D RANSAC technique, excluding ground data and irrelevant apron areas. Segmentation was subsequently conducted based on the filtered data, focusing on aircraft sections. For the segmented aircraft engine parts, the centroid of the grouped data was computed to determine the 3D position of the aircraft engine. Additionally, PointNet was applied to identify aircraft engines from the segmented data. Dynamic tests were conducted in various weather and environmental conditions, evaluating the detection performance across different jetbridge movement speeds and object-to-object distances. The study achieved a mean intersection over union (mIoU) of 81.25% in detecting aircraft engines, despite experiencing challenging conditions such as low-frequency vibrations and changes in the field of view during jetbridge maneuvers. This research provides a strong foundation for enhancing the robustness of jetbridge autonomous docking systems by reducing the sensor noise and distortion in real-time applications. Our future research will focus on optimizing sensor configurations, especially in environments where sea fog, snow, and rain are frequent, by combining RGB image data with 3D LiDAR information. The ultimate goal is to further improve the system’s reliability and efficiency, not only in jetbridge operations but also in broader autonomous vehicle and robotics applications, where precision and reliability are critical. The methodologies and findings of this study hold the potential to significantly advance the development of autonomous technologies across various industrial sectors. Full article
(This article belongs to the Section Mechanical Engineering)
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<p>Configuration of the jetbridge autonomous sensor system [<a href="#B18-applsci-14-09685" class="html-bibr">18</a>].</p>
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<p>Schematics of the jetbridge system used for automation [<a href="#B18-applsci-14-09685" class="html-bibr">18</a>].</p>
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<p>The 3D point cloud data for the aircraft and jetbridge on the apron (no ground filter).</p>
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<p>The 3D point cloud data for the aircraft and jetbridge on the apron (ground filtered).</p>
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<p>Real 3D point cloud data (.pcd) format (x, y, z, intensity).</p>
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<p>Aircraft engine detection model for the PointNet algorithm.</p>
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<p>The 3D LiDAR data of aircraft engines used for training process.</p>
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<p>Center of the jetbridge and distance between the jetbridge and engine.</p>
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<p>Result of the segmentation with the PointNet model (daytime). Jetbridge(blue box).</p>
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<p>Jetbridge cabin degree and distance error between the jetbridge and engine (daytime).</p>
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<p>Jetbridge cabin degree and distance error between the Jetbridge (blue box) and engine (nighttime).</p>
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19 pages, 11487 KiB  
Article
Real-Time Analysis and Digital Twin Modeling for CFD-Based Air Valve Control During Filling Procedures
by Duban A. Paternina-Verona, Oscar E. Coronado-Hernández, Modesto Pérez-Sánchez and Helena M. Ramos
Water 2024, 16(21), 3015; https://doi.org/10.3390/w16213015 - 22 Oct 2024
Viewed by 820
Abstract
Air exchange in pressurized water pipelines is an essential but complex aspect of pipeline modeling and operation. Implementing effective air management strategies can yield numerous benefits, enhancing the system’s energy efficiency, reliability, and safety. This paper comprehensively evaluates an irregular profile pipeline filling [...] Read more.
Air exchange in pressurized water pipelines is an essential but complex aspect of pipeline modeling and operation. Implementing effective air management strategies can yield numerous benefits, enhancing the system’s energy efficiency, reliability, and safety. This paper comprehensively evaluates an irregular profile pipeline filling procedure involving air-release through an air valve. The analysis includes real-time data tests and numerical simulations using Computational Fluid Dynamics (CFD). A Digital Twin model was proposed and applied to filling maneuvers in water installations. In particular, this research considers an often-overlooked aspect, such as filling a pipe with an irregular profile rather than a simple straight pipe. CFD simulations have proven to capture the main features of the transient event, which are suitable for tracking the air-water interface, the unsteady water flow, and the evolution of the trapped air pocket. Thus, they provide thorough and reliable information for real-time operational processes in the industry, focusing on the filling pressure and geometry of the air-valve hydraulic system. Additionally, this study provides details regarding the application of an efficient Digital Twin CFD approach, demonstrating its feasibility in optimizing the filling procedure in pipes with irregular profiles. Full article
(This article belongs to the Special Issue Hydrodynamics in Pressurized Pipe Systems)
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<p>Components of the proposed Digital Twin for filling maneuvers.</p>
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<p>A schematic experimental setup with details on the accessories used.</p>
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<p>Mesh configuration and boundaries of CFD model: (<b>a</b>) air valve device; (<b>b</b>) walls of the elbow at the left branch; (<b>c</b>) walls of the elbow at the right branch; (<b>d</b>) mesh detail on the right horizontal branch of the pipeline; and (<b>e</b>) detail of pipe cross-section.</p>
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<p>Comparison of the air pocket pressure of the 3D CFD model with experimental measurements: (<b>a</b>) Test 1; (<b>b</b>) Test 2; (<b>c</b>) Test 3; (<b>d</b>) Test 4; (<b>e</b>) Test 5; and (<b>f</b>) Test 6.</p>
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<p>Validation of results: (<b>a</b>) DT model with categorization used for ML/CFD improvement, (<b>b</b>) analysis of results for Test 1.</p>
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<p>Dynamic of rapid filling in Test 5: (<b>a</b>) contours of air-water interaction from 3D CFD model, and (<b>b</b>) video frames from the observed experiment.</p>
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<p>Evolution of the fraction of water available in the pipeline during the filling process: (<b>a</b>) Test 2; and (<b>b</b>) Test 5.</p>
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<p>Numerical pattern of air outflow through air valve in 3D CFD model: (<b>a</b>) Test 2; and (<b>b</b>) Test 5.</p>
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<p>Air streamlines during the expulsion of trapped air for Test 2: (<b>a</b>) overview; (<b>b</b>) close-up at the highest point.</p>
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19 pages, 5686 KiB  
Article
Mathematical Model of Horizontal Track Conflict Prevention Algorithm in Detect-and-Avoid Framework
by Suli Wang, Yunsong Lin and Yuan Zhang
Drones 2024, 8(10), 595; https://doi.org/10.3390/drones8100595 - 18 Oct 2024
Viewed by 537
Abstract
With the proliferation of Unmanned Aerial Vehicle (UAV) technology, the demand for effective collision avoidance technology has intensified. The DAIDALUS algorithm, devised by NASA Langley Research Center under the Detect-and-Avoid (DAA) framework, provides conflict prevention bands for remotely piloted UAVs navigating in intricate [...] Read more.
With the proliferation of Unmanned Aerial Vehicle (UAV) technology, the demand for effective collision avoidance technology has intensified. The DAIDALUS algorithm, devised by NASA Langley Research Center under the Detect-and-Avoid (DAA) framework, provides conflict prevention bands for remotely piloted UAVs navigating in intricate airspace. The algorithm computes the bands in two distinct phases: Conflict and Recovery. The formal model for both phases has been established and implemented through iterative programming approaches. However, the mathematical model remains incomplete. Therefore, based on the model, this paper proposes the mathematical model for the two phases of the horizontal track conflict prevention algorithm. Firstly, Cauchy’s inequality is proposed to formulate the model that addresses trajectory conflicts considering the UAV non-instantaneous maneuvering dynamics model, and then a prudent maneuvering strategy is designed to optimize the model for the recovery phase. Finally, the execution procedure of the algorithm within the two-stage mathematical model is also detailed. The results demonstrate that the proposed model achieves a higher precision in the preventive bands, implements an effective collision avoidance strategy, and consistently aligns with the DAIDALUS model while offering a larger buffer time or distance. This work theoretically validates the formal model of the DAIDLAUS algorithm and provides insights for further refinement. Full article
(This article belongs to the Section Drone Design and Development)
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<p>Sketch map of the mathematical model for calculating the prevention bands under instantaneous and non-instantaneous horizontal maneuvers within the well-clear zone in the relative coordinate system. (<b>a</b>) Instantaneous maneuver scenarios. (<b>b</b>) Proposed non-instantaneous maneuver scenarios.</p>
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<p>Schematic diagram of violation areas of the well-clear zone for instantaneous and non-instantaneous track maneuvers of the ownship in the absolute coordinate system. (<b>a</b>) The diagram under instantaneous maneuvers. (<b>b</b>) Proposed diagram under non-instantaneous maneuvers.</p>
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<p>Sketch map of the mathematical model of the conflict prevention algorithm in the recovery phase of the proposed model.</p>
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<p>Two-dimensional trajectory graphs for Scene 1.</p>
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<p>Two-dimensional trajectory graphs for Scene 2.</p>
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<p>Two-dimensional trajectory graphs for Scene 3.</p>
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<p>Trajectory graphs for Scene 4. (<b>a</b>) Two-dimensional trajectory graphs. (<b>b</b>) Three-dimensional trajectory graphs.</p>
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<p>Trajectory graphs for Scene 5. (<b>a</b>) Two-dimensional trajectory graphs. (<b>b</b>) Three-dimensional trajectory graphs.</p>
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<p>Trajectory graphs for Scene 6. (<b>a</b>) Two-dimensional trajectory graphs. (<b>b</b>) Three-dimensional trajectory graphs.</p>
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<p>Trajectory graphs for Scene 7. (<b>a</b>) Two-dimensional trajectory graphs. (<b>b</b>) Three-dimensional trajectory graphs.</p>
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<p>Trajectory graphs for Scene 8. (<b>a</b>) Two-dimensional trajectory graphs. (<b>b</b>) Three-dimensional trajectory graphs.</p>
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<p>Trajectory graphs for Scene 9. (<b>a</b>) Two-dimensional trajectory graphs. (<b>b</b>) Three-dimensional trajectory graphs.</p>
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<p>Variation curves of the time difference (ΔTcpa) and the distance difference (ΔDcpa) at the closest point of approach (CPA) during flights across all scenarios. (<b>a</b>) Variation curves of the time difference (ΔTcpa). (<b>b</b>) Variation curves of the distance difference (ΔDcpa).</p>
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