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Search Results (2,834)

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17 pages, 5645 KiB  
Article
Kinematic Analysis of Plasticization and Transportation System of Tri-Screw Dynamic Extruder
by Bin Xue, Jun Li, Qu Yang, Guiting Wu, Danxiang Wei, Yijie Ding, Zhenbin Du and Mingshi Huang
Polymers 2024, 16(23), 3252; https://doi.org/10.3390/polym16233252 - 22 Nov 2024
Viewed by 330
Abstract
With the growing demand for high-performance polymer composites, conventional single- and twin-screw extruders often fall short of meeting industrial requirements for effective mixing and compounding. This research investigates the kinematic behavior of the plasticization and transport mechanisms in tri-screw extruders when subjected to [...] Read more.
With the growing demand for high-performance polymer composites, conventional single- and twin-screw extruders often fall short of meeting industrial requirements for effective mixing and compounding. This research investigates the kinematic behavior of the plasticization and transport mechanisms in tri-screw extruders when subjected to a vibrational force field. The study specifically examines how applying vibrational force technology can improve the efficiency of polymer mixing. Vibration force field means that in a three-screw mechanism, an axial vibration is applied to the middle screw to produce a vibration force field. Through the development of mathematical and physical models, this study analyzed the motion dynamics of the screw and the influence of a vibrational force field on polymer transport and mixing efficiency. The findings indicate that, in comparison to traditional twin-screw extruders, tri-screw systems can achieve higher shear and elongational rates, leading to enhanced polymer mixing uniformity. Furthermore, applying an axial vibrational force field significantly influenced the shear and elongational strain rates of the material, thereby optimizing its rheological behavior and processing quality. This research not only establishes a theoretical foundation for the design and optimization of tri-screw extruders but also opens new pathways for the efficient processing of high-viscosity composite materials. Full article
(This article belongs to the Section Polymer Processing and Engineering)
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<p>Three-screw dynamic extruder.</p>
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<p>Cross-sectional profile of screw.</p>
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<p>Establishment of coordinate system of three-screw plasticizing conveying system and marking of main geometric dimensions.</p>
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<p>Geometric relationship of screw size.</p>
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<p>Position relationship of M point.</p>
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<p>Diagram of the relationship between the clearance between two screws and rotation.</p>
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<p>Velocity diagram between two screws.</p>
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<p>The plane expansion diagram of screw spiral section.</p>
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<p>Velocity diagram between two screws.</p>
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<p>Relationship between circumferential shear deformation rate of screw surface and vibration amplitude and frequency.</p>
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<p>Relationship between circumferential average shear deformation rate with vibration amplitude and frequency.</p>
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<p>Relationship between axial tensile deformation rate of screw surface and amplitude and frequency.</p>
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<p>Relationship between axial tension deformation rate with vibration amplitude and frequency.</p>
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16 pages, 3422 KiB  
Article
Development of Rehabilitation Glove: Soft Robot Approach
by Tomislav Bazina, Marko Kladarić, Ervin Kamenar and Goran Gregov
Actuators 2024, 13(12), 472; https://doi.org/10.3390/act13120472 - 22 Nov 2024
Viewed by 167
Abstract
This study describes the design, simulation, and development process of a rehabilitation glove driven by soft pneumatic actuators. A new, innovative finger soft actuator design has been developed through detailed kinematic and workspace analysis of anatomical fingers and their actuators. The actuator design [...] Read more.
This study describes the design, simulation, and development process of a rehabilitation glove driven by soft pneumatic actuators. A new, innovative finger soft actuator design has been developed through detailed kinematic and workspace analysis of anatomical fingers and their actuators. The actuator design combines cylindrical and ribbed geometries with a reinforcing element—a thicker, less extensible structure—resulting in an asymmetric cylindrical bellow actuator driven by positive pressure. The performance of the newly designed actuator for the rehabilitation glove was validated through numerical simulation in open-source software. The simulation results indicate actuators’ compatibility with human finger trajectories. Additionally, a rehabilitation glove was 3D-printed from soft materials, and the actuator’s flexibility and airtightness were analyzed across different wall thicknesses. The 0.8 mm wall thickness and thermoplastic polyurethane (TPU) material were chosen for the final design. Experiments confirmed a strong linear relationship between bending angle and pressure variations, as well as joint elongation and pressure changes. Next, pseudo-rigid kinematic models were developed for the index and little finger soft actuators, based solely on pressure and link lengths. The workspace of the soft actuator, derived through forward kinematics, was visually compared to that of the anatomical finger and experimentally recorded data. Finally, an ergonomic assessment of the complete rehabilitation glove in interaction with the human hand was conducted. Full article
(This article belongs to the Section Actuators for Robotics)
17 pages, 2390 KiB  
Article
An Attempt to Establish a Mathematical Model for an Unconventional Worm Gear with Bearings
by Simion Haragâș, Roland Ninacs, Ovidiu Buiga, Lucian Tudose, Alexandru Haragâș, Ioana Monica Sas-Boca and Felicia Aurora Cristea
Appl. Sci. 2024, 14(23), 10833; https://doi.org/10.3390/app142310833 - 22 Nov 2024
Viewed by 277
Abstract
The aim of this paper is to develop a mathematical model for an unconventional worm gear consisting of a globoid worm and a worm wheel where the teeth are bearings. Using rolling elements such the teeth of the worm wheel (ball bearings) transforms [...] Read more.
The aim of this paper is to develop a mathematical model for an unconventional worm gear consisting of a globoid worm and a worm wheel where the teeth are bearings. Using rolling elements such the teeth of the worm wheel (ball bearings) transforms the sliding friction to rolling friction during the process of worm gear meshing, improving power. The geometry of the component elements of the gear is analyzed in correlation with its kinematics. After the creation of the mathematical model, it is validated both analytically (through complex graphic representations) and experimentally (by creating, for a particular case, the 3D model and the concrete physical model (prototype) of the gear through 3D printing). Full article
(This article belongs to the Special Issue Machine Tools, Advanced Manufacturing and Precision Manufacturing)
12 pages, 1402 KiB  
Article
Influence of the Initial Guess on the Estimation of Knee Ligament Parameters via Optimization Procedures
by Ilias Theodorakos and Michael Skipper Andersen
Bioengineering 2024, 11(12), 1183; https://doi.org/10.3390/bioengineering11121183 - 22 Nov 2024
Viewed by 260
Abstract
Optimization procedures provide ligament parameters by minimizing the difference between experimental measurements and computational simulations. Literature values are used as initial guesses of ligament parameters for these optimization procedures. However, it remains unknown how these values affect the estimation of ligament parameters. This [...] Read more.
Optimization procedures provide ligament parameters by minimizing the difference between experimental measurements and computational simulations. Literature values are used as initial guesses of ligament parameters for these optimization procedures. However, it remains unknown how these values affect the estimation of ligament parameters. This study evaluates the effects of the initial guess on estimations of ligament parameters. A synthetic data set was generated using a subject-specific knee computational model, reference ligament parameters and simulated laxity tests. Subsequently, ligament parameters were estimated using an optimization routine and four different initial guesses. The distance of these initial guesses from their true values ranged from 0 to 3.5 kN and from 0 to 3.6% for the stiffness and reference strains, respectively. The optimized ligament parameters had an average absolute mean error ranging from 0.15 (0.09) kN and 0.08 (0.04)% to 3.67 (2.46) kN and 1.25 (0.76)%, while the kinematic error remained below 1 mm and 1.2° for all conditions. Our results showed that the estimations of the ligament parameters worsened as the initial guesses moved farther away from their true values. Moreover, the optimization procedure resulted in suboptimal ligament parameters that provided similar behavior to the true laxity behavior, which is an alarming finding that should be further investigated. Full article
(This article belongs to the Special Issue Biomechanics of Sports Injuries)
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<p>The tibiofemoral computational model. The implemented ligaments are represented by red lines. The articular cartilage is represented by blue color. The anatomical reference systems of the femur and the tibia are represented by yellow and green colors, respectively.</p>
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<p>The laxity profile of the synthetic data generated using the computational model and the reference ligament parameter.</p>
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<p>Optimized ligament parameters for different sets of initial guesses (IGs). The red asterisks show the respective initial guess values, while the black line represents the reference values.</p>
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<p>Ligament force–strain curves for the anterior cruciate (ACL), posterior cruciate (PCL), medial collateral (MCL) and lateral collateral (LCL) ligaments. The curves using the reference ligament parameters (synthetic data) and the optimized values for the different initial guesses (IG) are presented.</p>
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11 pages, 1096 KiB  
Article
Quantification of Ground Reaction Forces During the Follow Through in Trained Male Cricket Fast Bowlers: A Laboratory-Based Study
by Jeffrey Fleming, Corey Perrett, Onesim Melchi, Jodie McClelland and Kane Middleton
Sports 2024, 12(12), 316; https://doi.org/10.3390/sports12120316 - 22 Nov 2024
Viewed by 218
Abstract
Ground reaction forces (GRFs) are known to be high during front foot contact of fast bowling deliveries in cricket. There is a lack of published data on the GRFs during follow through foot contacts. The aim of this study was to quantify and [...] Read more.
Ground reaction forces (GRFs) are known to be high during front foot contact of fast bowling deliveries in cricket. There is a lack of published data on the GRFs during follow through foot contacts. The aim of this study was to quantify and compare peak GRFs and impulse of the delivery stride and the follow through of fast bowling deliveries. Ten trained male fast bowlers (ball release speed mean ± SD; 32.6 ± 2.3 m/s) competing in the Men’s Victorian Premier League participated in the study. Peak GRF and impulse data were collected using in-ground force plates in a laboratory setting. Linear mixed modelling of GRFs and impulse showed a significant effect of foot strike (p < 0.001). Front foot contact had the greatest magnitude of peak vertical GRF (5.569 ± 0.334 BW) but was not significantly greater than back foot recontact (4.471 ± 0.285 BW) (p = 0.07). Front foot impact had the greatest vertical impulse (0.408 ± 0.018 BW·s) but was similar to back foot (0.377 ± 0.012 BW·s) and front foot (0.368 ± 0.006 BW·s) recontacts (p = 0.070 to 0.928). The high GRF and impulse during the follow through highlights the need for further kinetic and kinematic research on this phase of the fast bowling delivery. Full article
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<p>Schematic of testing set-up. Set-up 1 was used to collect data for back foot contact (BF1) on force plate 1 (FP1), front foot contact (FF1) on force plate 2 (FP2), and back foot recontact (BF2) on force plate 3 (FP3). Set-up 2 was used to collect data for front foot contact (FF1) on force plate 1 (FP1), back foot recontact (BF2) on force plate 2 (FP2), and front foot recontact (FF2) on force plate 3 (FP3).</p>
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<p>Scatter plot combined with a box plot to illustrate the distribution of the vertical ground reaction force (GRF) data collected at each foot strike. Scatter plot points are colour-coded by participant to aid in visualising both intra-participant and inter-participant variability of the data. Colour coding of participants is consistent across figures. The full width line represents the median of the data. The upper and lower hinges of the boxes represent the first and third quartiles of data, respectively, the whiskers extending to the largest or smallest value no more than 1.5 times the distance between the first and third quartile. To aid in discerning individual data points, a random amount of noise has been added to the x value for each scatter plot point; the y values are unaltered. * Denotes estimated marginal mean of foot strikes are different to at least the 0.05 level.</p>
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<p>Scatter plot combined with a box plot to illustrate the distribution of the vertical impulse data collected at each foot strike. Scatter plot points are colour-coded by participant to aid in visualising both intra-participant and inter-participant variability of the data. Colour coding of participants is consistent across figures. The full width line represents the median of the data. The upper and lower hinges of the boxes represent the first and third quartiles of data, respectively, the whiskers extending to the largest or smallest value no more than 1.5 times the distance between the first and third quartile. To aid in discerning individual data points a random amount of noise has been added to the x value for each scatter plot point, the y values are unaltered. * Denotes estimated marginal mean of foot strikes are different to at least the 0.05 level.</p>
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27 pages, 7577 KiB  
Article
Design and Experiment of Obstacle Avoidance Mower in Orchard
by Yi Yang, Yichuan He, Zhihui Tang and Hong Zhang
Agriculture 2024, 14(12), 2099; https://doi.org/10.3390/agriculture14122099 - 21 Nov 2024
Viewed by 216
Abstract
In order to solve the problem of mowing between plants in Xinjiang trunk orchards, an obstacle avoidance mower suitable for trunk orchard planting mode was designed. The whole structure, working principle and main parameter design of the obstacle avoidance mower are introduced. The [...] Read more.
In order to solve the problem of mowing between plants in Xinjiang trunk orchards, an obstacle avoidance mower suitable for trunk orchard planting mode was designed. The whole structure, working principle and main parameter design of the obstacle avoidance mower are introduced. The finite element analysis and kinematic analysis of the cutter are carried out on the premise of using a Y-shaped cutter and its arrangement, and the condition that the inter-row mower does not leak is determined. Through the modal analysis of the frame, the range of the first six natural frequencies of the frame is determined and compared with the frequency of the main excitation source of the machine to determine the rationality of the frame design. On the premise of simplifying the inter-plant obstacle avoidance mechanism into a two-dimensional model for kinematics analysis, the motion parameters of the key components of the machine were determined. At the same time, the virtual kinematics simulation single-factor test of the designed inter-plant obstacle avoidance device was carried out with the help of ADAMS 2020 software. Through the reduction in and calculation of the motion trajectory of the simulation test, it was finally determined that the forward speed of the machine, the elastic coefficient of the reset spring and the compression speed of the hydraulic cylinder were the main influencing factors of the inter-plant obstacle avoidance mower. The orthogonal test was designed and the optimal solution of the three test factors was determined. The optimal solution is taken for further field test verification. The results show that when the tractor forward speed is 1.5 km∙h−1, the hydraulic cylinder compression speed is 225 mm∙s−1, and the elastic coefficient of the reset spring is 29 N∙mm−1, the average leakage rate between the orchard plants is 7.64%, and the obstacle avoidance pass rate is 100%. The working stability is strong and meets the design requirements. Full article
(This article belongs to the Section Agricultural Technology)
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Figure 1
<p>The overall structure diagram of the orchard inter-plant obstacle avoidance mower. 1: Suspension device; 2: hydraulic oil tank; 3: transmission belt shell; 4: belt pulley drive shaft; 5: cylindrical guide rail; 6: cooling fan; 7: frame; 8: lawn mower roller; 9: lawn mower; 10: telescopic rod; 11: hydraulic directional valve; 12: obstacle avoidance disc; 13: obstacle avoidance rod; 14: spring; 15: obstacle avoidance disc bracket; 16: inter-row mower; 17: protective disc; 18: pressing roller; 19: stent; 20: gear box.</p>
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<p>Transmission system diagram of mower. 1. Mowing roller. 2. Hydraulic pump. 3. Transfer box. 4. Transmission shaft. 5. Drive pulley. 6. Drive pulley. 7. Belt. 8. Input shaft.</p>
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<p>The arrangement of pins on the roller shaft. (<b>a</b>) Helix arrangement. (<b>b</b>) Symmetrical arrangement. (<b>c</b>) Interlaced arrangement. (<b>d</b>) Symmetrical staggered arrangement.</p>
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<p>Cutter meshing diagram.</p>
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<p>Cutter statics simulation results. (<b>a</b>) Equivalent elastic deformation cloud diagram of cutter. (<b>b</b>) Cutter displacement deformation cloud map. (<b>c</b>) Cutter stress deformation cloud diagram.</p>
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<p>Cutter trajectory diagram.</p>
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<p>Three-dimensional model of frame.</p>
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<p>Frame finite element model.</p>
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<p>Frame of the first six-order modal analysis diagram.</p>
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<p>Automatic obstacle avoidance device between plants. 1. Hydraulic motor. 2. Cutterhead. 3. Connecting shaft. 4. Breakthrough rod. 5. Control valve. 6. Connecting plate. 7. Cylinder.</p>
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<p>Motion diagram of automatic obstacle avoidance device between plants. 1. Cutterhead. 2. Cutterhead connecting plate. 3. Connecting plate. 4. Hydraulic cylinder. Note: N is the position of the cutter head under the compression state of the hydraulic cylinder; n′ is the position of the cutter head in the elongation state of the hydraulic cylinder; R is the radius of the cutter head and the length of the hydraulic cylinder in the compressed state; l<sub>1</sub> is the length of the hydraulic cylinder in compression state. <math display="inline"><semantics> <mrow> <msubsup> <mrow> <mi mathvariant="normal">l</mi> </mrow> <mrow> <mn>1</mn> </mrow> <mrow> <mo>´</mo> </mrow> </msubsup> </mrow> </semantics></math> the length of the hydraulic cylinder in the telescopic state; L is the distance between the position of the hydraulic cylinder and the connecting plate; l<sub>3</sub> is the position of both ends of the connecting plate; l<sub>4</sub> is the distance between the midpoint of the cutter connection plate of the cutter head; l<sub>5</sub> is the distance between the center of the cutter head in the two middle states; l<sub>6</sub> is the distance between the two connection points in two states; l<sub>7</sub> is the distance between point O and E′; l<sub>8</sub> is the distance between two points of DE; l<sub>9</sub> is the distance between EE′; <math display="inline"><semantics> <mrow> <mi>α</mi> </mrow> </semantics></math> is the angle between OA and AB; <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>α</mi> </mrow> <mrow> <mn>1</mn> </mrow> </msub> </mrow> </semantics></math> is the angle between BA and B′A; θ<sub>1</sub> is the angle between OA and OB. θ<sub>2</sub> is the angle between OA and OB′; <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>α</mi> </mrow> <mrow> <mn>2</mn> </mrow> </msub> </mrow> </semantics></math> is the angle between OD and OB; <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>α</mi> </mrow> <mrow> <mn>3</mn> </mrow> </msub> </mrow> </semantics></math> is the angle between OD′ and OB′; <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>α</mi> </mrow> <mrow> <mn>4</mn> </mrow> </msub> </mrow> </semantics></math> is the angle between OB and OB′; <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>α</mi> </mrow> <mrow> <mn>5</mn> </mrow> </msub> </mrow> </semantics></math> is the angle between OD and OB′; <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>α</mi> </mrow> <mrow> <mn>6</mn> </mrow> </msub> </mrow> </semantics></math> is the angle between OD and OD′; <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>α</mi> </mrow> <mrow> <mn>7</mn> </mrow> </msub> </mrow> </semantics></math> is the angle between OE and OD; <math display="inline"><semantics> <mrow> <msub> <mrow> <mi>α</mi> </mrow> <mrow> <mn>8</mn> </mrow> </msub> </mrow> </semantics></math> is the angle between D′ D and OD; and h is the vertical distance between the center of the cutter head in the two states.</p>
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<p>Simulation model of obstacle avoidance mowing device between plants. 1. Grassland 2. Pear tree. 3. Pear tree spacing. 4. Rack. 5. Barrier plate. 6. Barrier rod.</p>
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<p>Constraint relationship diagram of obstacle avoidance mower between orchard plants. 1. Obstacle avoidance disc drive. 2. Fixed pair. 3. Rotating pair. 4. Axis rotation drive.</p>
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<p>Model validation information.</p>
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<p>Simulation operation process of obstacle avoidance lawn mower in orchard. Note: (<b>a</b>): inter-row mowing operation stage; (<b>b</b>): obstacle avoidance rod touch tree stage; (<b>c</b>): inter-row obstacle avoidance stage; (<b>d</b>): obstacle avoidance end stage.</p>
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<p>Area of cutter cutting area.</p>
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<p>The influence curve of various factors on the working efficiency of the inter-plant obstacle avoidance mower. (<b>a</b>) The relationship between the forward speed of the machine and the leakage cutting rate. (<b>b</b>) The relationship between the compression speed of hydraulic cylinder and the leakage cutting rate. (<b>c</b>) Relationship between elastic coefficient of reset spring and leakage cutting rate. (<b>d</b>) The relationship between cutter diameter and leakage cutting rate.</p>
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<p>Effects of interaction of various factors on the rate of missing cutting between plants. (<b>a</b>) The interaction of AC on missing cutting G1 between plants. (<b>b</b>) The interaction of BC on missing cutting G1 between plants. (<b>c</b>) The interaction of AB on missing cutting G1 between plants.</p>
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<p>Optimal parameter combination configuration diagram.</p>
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<p>(<b>a</b>) Test site. (<b>b</b>) Obstacle avoidance mower prototype.</p>
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<p>Field test verification. (<b>a</b>) Before mowing operation. (<b>b</b>) After mowing operation (between rows). (<b>c</b>) After mowing operation (between plants).</p>
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30 pages, 15227 KiB  
Review
A Survey of Planar Underactuated Mechanical System
by Zixin Huang, Chengsong Yu, Ba Zeng, Xiangyu Gong and Hongjian Zhou
Machines 2024, 12(12), 829; https://doi.org/10.3390/machines12120829 - 21 Nov 2024
Viewed by 180
Abstract
Planar underactuated mechanical systems have been a popular research issue in the area of mechanical systems and nonlinear control. This paper reviews the current research status of control methods for a class of planar underactuated manipulator (PUM) systems containing a single passive joint. [...] Read more.
Planar underactuated mechanical systems have been a popular research issue in the area of mechanical systems and nonlinear control. This paper reviews the current research status of control methods for a class of planar underactuated manipulator (PUM) systems containing a single passive joint. Firstly, the general dynamics model and kinematics model of the PUM are given, and its control characteristics are introduced; secondly, according to the distribution position characteristics of the passive joints, the PUM is classified into the passive first joint system, the passive last joint system, and the passive intermediate joint system, and the analysis and discussion are carried out in respect to the existing intelligent control methods. Finally, in response to the above discussion, we provide a brief theoretical analysis and summarize the challenges faced by PUM, i.e., uncertainty and robustness of the system, unified control methods and research on underactuated systems with uncontrollable multi-passive joints; at the same time, the practical applications have certain limitations that need to be implemented subsequently, i.e., anti-jamming, multi-planar underactuated robotic arm co-control and spatial underactuated robotic arm system development. Aiming at the above challenges and problems in the control of PUM systems, we elaborate on them in points, and put forward the research directions and related ideas for future work, taking into account the contributions of the current work. Full article
(This article belongs to the Section Machine Design and Theory)
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Figure 1
<p>Physical structure of planar <span class="html-italic">n</span>-DoF manipulator.</p>
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<p>Physical structure of planar <math display="inline"><semantics> <mrow> <msup> <mi mathvariant="normal">A</mi> <mi>m</mi> </msup> <msup> <mi>PA</mi> <mi>n</mi> </msup> </mrow> </semantics></math> manipulator.</p>
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<p>Structural sketch of the planar <math display="inline"><semantics> <mrow> <msup> <mi mathvariant="normal">A</mi> <mi>m</mi> </msup> <msup> <mi>PA</mi> <mi>n</mi> </msup> </mrow> </semantics></math> manipulator.</p>
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<p>Physical structure of planar Acrobot manipulator.</p>
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<p>Physical structure of planar PAA manipulator system.</p>
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<p>Physical structure of planar manipulator system. (<b>a</b>) PA manipulator system. (<b>b</b>) PAAA manipulator system. (<b>c</b>) <math display="inline"><semantics> <mrow> <msup> <mi>PA</mi> <mi>n</mi> </msup> </mrow> </semantics></math> manipulator system. (<b>d</b>) PAPA manipulator system.</p>
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<p>Acrobot simulation results (First data set). (<b>a</b>) angle. (<b>b</b>) angular velocity. (<b>c</b>) torque.</p>
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<p>Pendubot simulation results (First data set). (<b>a</b>) angle. (<b>b</b>) angular velocity. (<b>c</b>) torque.</p>
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<p>Acrobot simulation results (Second data set). (<b>a</b>) angle. (<b>b</b>) angular velocity. (<b>c</b>) torque.</p>
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<p>Pendubot simulation results (Second data set). (<b>a</b>) angle. (<b>b</b>) angular velocity. (<b>c</b>) torque.</p>
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<p>Physical structure of planar Pendubot manipulator system.</p>
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<p>Physical structure of planar AAP manipulator system.</p>
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<p>Physical structure of planar <math display="inline"><semantics> <mrow> <msup> <mi mathvariant="normal">A</mi> <mi>m</mi> </msup> </mrow> </semantics></math>P <math display="inline"><semantics> <mrow> <mo>(</mo> <mi>m</mi> <mo>&gt;</mo> <mn>2</mn> <mo>)</mo> </mrow> </semantics></math> manipulator system.</p>
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<p>Physical structure of planar APA manipulator system.</p>
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<p>Physical structure of planar <math display="inline"><semantics> <mrow> <msup> <mi mathvariant="normal">A</mi> <mi>m</mi> </msup> <mrow> <msup> <mi>PA</mi> <mi>n</mi> </msup> <mrow> <mo>(</mo> <mi>m</mi> <mo>≥</mo> <mn>1</mn> <mo>,</mo> <mi>n</mi> <mo>≥</mo> <mn>1</mn> <mo>,</mo> <mi>m</mi> <mo>+</mo> <mi>n</mi> <mo>≥</mo> <mn>2</mn> <mo>)</mo> </mrow> </mrow> </mrow> </semantics></math> manipulator system.</p>
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20 pages, 6819 KiB  
Article
Analysis and Experimentation on the Motion Characteristics of a Dragon Fruit Picking Robot Manipulator
by Kairan Lou, Zongbin Wang, Bin Zhang, Qiu Xu, Wei Fu, Yang Gu and Jinyi Liu
Agriculture 2024, 14(11), 2095; https://doi.org/10.3390/agriculture14112095 - 20 Nov 2024
Viewed by 287
Abstract
Due to the complex growth positions of dragon fruit and the difficulty in robotic picking, this paper proposes a six degrees of freedom dragon fruit picking robot and investigates the manipulator’s motion characteristics to address the adaptive motion issues of the picking manipulator. [...] Read more.
Due to the complex growth positions of dragon fruit and the difficulty in robotic picking, this paper proposes a six degrees of freedom dragon fruit picking robot and investigates the manipulator’s motion characteristics to address the adaptive motion issues of the picking manipulator. Based on the agronomic characteristics of dragon fruit cultivation, the structural design of the robot and the dimensions of its manipulator were determined. A kinematic model of the dragon fruit picking robot based on screw theory was established, and the workspace of the manipulator was analyzed using the Monte Carlo method. Furthermore, a dynamic model of the manipulator based on the Kane equation was constructed. Performance experiments under trajectory and non-trajectory planning showed that trajectory planning significantly reduced power consumption and peak torque. Specifically, Joint 3’s power consumption decreased by 62.28%, and during the picking, placing, and resetting stages, the peak torque of Joint 4 under trajectory planning was 10.14 N·m, 12.57 N·m, and 16.85 N·m, respectively, compared to 12.31 N·m, 15.69 N·m, and 22.13 N·m under non-trajectory planning. This indicated that the manipulator operates with less impact and smoother motion under trajectory planning. Comparing the dynamic model simulation and actual testing, the maximum absolute error in the joint torques was −2.76 N·m, verifying the correctness of the dynamic equations. Through field picking experiments, it was verified that the machine’s picking success rate was 66.25%, with an average picking time of 42.4 s per dragon fruit. The manipulator operated smoothly during each picking process. In the study, the dragon fruit picking manipulator exhibited good stability, providing the theoretical foundation and technical support for intelligent dragon fruit picking. Full article
(This article belongs to the Section Agricultural Technology)
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<p>Cultivation model and picking method in a dragon fruit orchard. (<b>a</b>) Cultivation mode; (<b>b</b>) Picking method.</p>
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<p>Dragon fruit picking robot joint motion directions and three-dimensional structure diagram. 1. Tracked chassis; 2. Manipulator base; 3. Joint 1; 4. Link 1; 5. Joint 2; 6. Joint 3; 7. Joint 4; 8. Joint 5; 9. Joint 6; 10. Link 2; 11. Link 3; 12. Link 4; 13. Link 5; 14. Vision system; 15. End effector; 16. Motor; 17. Coupling; 18. Screw mechanism; 19. Linkage mechanism; 20. Picking bucket.</p>
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<p>The initial position of the manipulator.</p>
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<p>Schematic diagram of the manipulator.</p>
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<p>Schematic diagram of the manipulator. 1. Robot body; 2. Host computer; 3. 36 V lithium-ion battery; 4. Lower level controller; 5. Depth camera.</p>
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<p>Dragon fruit picking robot workspace composite diagram. (<b>a</b>) Three-dimensional workspace; (<b>b</b>) <span class="html-italic">xoy</span> projection plane; (<b>c</b>) <span class="html-italic">xoz</span> projection plane; (<b>d</b>) <span class="html-italic">yoz</span> projection plane.</p>
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<p>Joint 3 to Joint 6 average power consumption per second. (<b>a</b>) Joint 3; (<b>b</b>) Joint 4; (<b>c</b>) Joint 5; (<b>d</b>) Joint 6.</p>
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<p>Joint 4 velocity and torque curves for each stage. (<b>a</b>) The p1 stage rotational speed; (<b>b</b>) The p2 stage rotational speed; (<b>c</b>) The p3 stage rotational speed; (<b>d</b>) The p1 stage torque; (<b>e</b>) The p2 stage torque; (<b>f</b>) The p3 stage torque.</p>
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<p>Torque variation curves of joints during the p3 stage. (<b>a</b>) Torque based on experimental platform; (<b>b</b>) Torque based on MATLAB simulation and its error chart.</p>
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<p>Field testing of dragon fruit picking robot. (<b>a</b>) Object recognition; (<b>b</b>) Moving towards the picking position; (<b>c</b>) Shearing and twisting; (<b>d</b>) Fruit picking.</p>
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18 pages, 6723 KiB  
Article
Design and Development of 10,000-Meter Class Autonomous Underwater Vehicle
by Jiali Xu, Zhaopeng Du, Xianqing Huang, Chong Ren, Shuai Fa and Shaoqiong Yang
J. Mar. Sci. Eng. 2024, 12(11), 2097; https://doi.org/10.3390/jmse12112097 - 19 Nov 2024
Viewed by 374
Abstract
As a significant subset of unmanned underwater vehicles (UUVs), autonomous underwater vehicles (AUVs) possess the capability to autonomously execute tasks. Characterized by its flexibility, cost-effectiveness, extensive operational range, and robust environmental adaptability, AUV has emerged as the primary technological apparatus for deep-sea exploration [...] Read more.
As a significant subset of unmanned underwater vehicles (UUVs), autonomous underwater vehicles (AUVs) possess the capability to autonomously execute tasks. Characterized by its flexibility, cost-effectiveness, extensive operational range, and robust environmental adaptability, AUV has emerged as the primary technological apparatus for deep-sea exploration and research. In this paper, we present the design of a 10,000 m class AUV equipped with capabilities such as fixed-depth navigation, regional autonomous cruising, full-depth video recording, and temperature and salinity profiling. Initially, we outline the comprehensive design of the AUV, detailing its structural configuration, system components, functional module arrangement, and operational principles. Subsequently, we compute the hydrodynamic parameters using a spatial kinematics model. Finally, the AUV designed in this paper is tested for its functions and performance, such as fixed-depth sailing, maximum speed, and maximum diving depth, and its reliability and practicability are verified. Full article
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<p>The outline structure of 10,000 m deep-sea AUV.</p>
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<p>Overall structure of the AUV.</p>
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<p>Overall structure of the AUV.</p>
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<p>The detailed internal structure of each module of the 10,000 m AUV. (<b>a</b>) Deflector module. (<b>b</b>) Propellant module. (<b>c</b>) Control module.</p>
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<p>The detailed internal structure of each module of the 10,000 m AUV. (<b>a</b>) Deflector module. (<b>b</b>) Propellant module. (<b>c</b>) Control module.</p>
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<p>The system composition block diagram of the AUV.</p>
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<p>Schematic diagram of the working process of the 10,000 m class AUV.</p>
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<p>AUV inertial coordinate system and body coordinate system.</p>
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<p>AUV velocity coordinate system and body coordinate system.</p>
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<p>The schematic diagram of the control strategy framework.</p>
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<p>The depth, velocity, and pitch angle variation with time.</p>
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<p>Launching and recycling of the AUV during the direct sailing test at fixed depth.</p>
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<p>The variation of diving depth and pitch angle of the AUV during the direct sailing test at fixed depth.</p>
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<p>The trajectory of the AUV during the timeout load jettison function test.</p>
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<p>The maximum speed test of the AUV.</p>
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<p>Time sequence of underwater movements of the AUV during 2000 m shallow-sea trial.</p>
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<p>Underwater motion sequence of the AUV during 10,000 m deep-sea trial.</p>
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18 pages, 3616 KiB  
Article
Theoretical Analysis of Shaft Wall Damage and Failure Under Impacting of Ore-Rock Falling in Vertical Ore Pass
by Qiangying Ma, Chi Ma, Jiaoqun Li, Zengxiang Lu and Zhiguo Xia
Appl. Sci. 2024, 14(22), 10695; https://doi.org/10.3390/app142210695 - 19 Nov 2024
Viewed by 306
Abstract
The impact of ore-rock blocks on the shaft wall of a vertical ore pass is a crucial cause of shaft wall damage and failure. Based on the structure and parameters of the ore pass in a case mine, the first collision’s position of [...] Read more.
The impact of ore-rock blocks on the shaft wall of a vertical ore pass is a crucial cause of shaft wall damage and failure. Based on the structure and parameters of the ore pass in a case mine, the first collision’s position of the ore-rock block with respect to the ore pass wall and the angle between the impacting direction of the ore-rock block and the horizontal plane before and after the collision are investigated via a kinematic analysis. The normal and tangential analysis models of ore rock impacting the shaft wall are established and analyzed based on contact mechanics. The results show that: (1) based on the kinematic analysis of ore rock moving in the ore pass and on the colliding condition of the ore-rock block the first time that it collides with the ore pass wall, the coordinates and angles of the collision are proposed; (2) the impacting process of ore rock is categorized into elastic compression, elastic–plastic compression, and rebound of the shaft wall material. The relationship between the normal impact force and the penetrating depth is determined, and the slipping distance of the ore-rock block along the shaft wall and the lost volume of the shaft material are established. (3) The wall material’s normal, tangential, and total restitution coefficient is acquired. (4) The total lost volume during the collision is obtained through the analysis and solution of the model. (5) Based on the characteristics and parameters of the ore pass in the case mine, the influence of the impact velocity and angle of the ore-rock block on the restitution coefficient, maximum normal intrusion depth, maximum tangential displacement, and volume loss of the shaft wall are analyzed by using relevant formulas. Full article
(This article belongs to the Special Issue Advanced Methodology and Analysis in Coal Mine Gas Control)
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<p>Layout of the main ore pass in the Shunfeng iron mine, a case mine located in Northeast China.</p>
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<p>Spatial motion model of the ore-rock block entering the ore pass: (<b>a</b>) longitudinal projection along the length of the unloading chute; (<b>b</b>) a top view of figure (<b>a</b>).</p>
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<p>Contact model between the moving ore-rock block and the ore pass wall. (<b>a</b>) Calculation model of the moving ore-rock block impacting the ore pass wall and the yellow part is the deformation area of the ore pass wall; (<b>b</b>) decomposition of the velocity of the moving ore-rock block when it collides with the ore pass wall.</p>
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<p>Calculation model of the lost volume of the ore pass wall. The shaded part in the figure is the lost volume of the ore pass wall: (<b>a</b>) profile along the center line of the ore pass, located at the point of the maximum intrusion depth of the ore-rock block; (<b>b</b>) section perpendicular to the center line of the ore pass, located at the point of maximum intrusion depth of the ore-rock block. The A.C. line in this figure represents the original surface of the ore pass wall and B is the point of maximum intrusion depth on the ore pass wall.</p>
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<p>The influence of <span class="html-italic">v</span><sub>1</sub> variations on NRC and TRC. The red lines represent the NRCs, and the blue lines represent the tangential ones.</p>
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<p>Influence of the ore-rock block radius <span class="html-italic">R</span> and of the impact velocity <span class="html-italic">v</span><sub>1</sub> on the intrusion depth.</p>
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<p>Influence of the rock block radius <span class="html-italic">R</span> change and of the impact velocity <span class="html-italic">v</span><sub>1</sub> on the tangential displacement.</p>
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<p>Influence of the rock block radius <span class="html-italic">R</span> change and of the impact velocity <span class="html-italic">v</span><sub>1</sub> on the volume loss of the shaft wall.</p>
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<p>Characteristics of the damage to the ore pass wall resulting from impact with and cutting of ore-rock block: (<b>a</b>) characteristics of the damage to the ore pass wall according to Yue Y et al. [<a href="#B26-applsci-14-10695" class="html-bibr">26</a>]; (<b>b</b>) analysis of the damage characteristics of the ore pass wall—the yellow circles show the impact traces on the ore pass wall caused by the collision with the ore-rock blocks and the black ellipses show the damage caused by the impact with a sharp surface. The height meter shows the lower half of the ore pass model.</p>
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45 pages, 5829 KiB  
Article
Geometric Constraint Programming (GCP) Implemented Through GeoGebra to Study/Design Planar Linkages
by Raffaele Di Gregorio and Tommaso Cinti
Machines 2024, 12(11), 825; https://doi.org/10.3390/machines12110825 - 18 Nov 2024
Viewed by 376
Abstract
In the study and design of planar mechanisms, graphical techniques for solving kinematic analysis/synthesis and kinetostatics problems have regained interest due to the availability of advanced drawing tools (e.g., CAD software). These techniques offer a deeper physical understanding of a mechanism’s behavior, which [...] Read more.
In the study and design of planar mechanisms, graphical techniques for solving kinematic analysis/synthesis and kinetostatics problems have regained interest due to the availability of advanced drawing tools (e.g., CAD software). These techniques offer a deeper physical understanding of a mechanism’s behavior, which can enhance a designer’s intuition and help students develop their skills. Geometric Constraint Programming (GCP) is the term used to describe this modern approach to implementing these techniques. GeoGebra is an open-source platform designed for the interactive learning and teaching of mathematics and related STEM disciplines. It offers an object-oriented programming language and a wide range of geometric tools that can be leveraged to implement GCP. This work presents a systematic technique for studying and designing planar linkages, based on Assur’s groups and GeoGebra’s tools. Although some kinematic analyses and syntheses of planar linkages using GeoGebra have been previously introduced, the proposed systematic approach is novel and could serve as a guide for implementing similar problem-solving methods in other graphical environments. Several case studies will be presented to illustrate this novel approach in detail. Full article
(This article belongs to the Collection Machines, Mechanisms and Robots: Theory and Applications)
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<p>Dyad types (<span class="html-italic">i</span> and <span class="html-italic">j</span> are the two links of the dyad, the green elements are the free endings of the dyad, the red parameters are the geometric constants of the dyad): (<b>a</b>) RRR, (<b>b</b>) RRP, (<b>c</b>) RPR, (<b>d</b>) RRP, and (<b>e</b>) RPP.</p>
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<p>Driving links (link <span class="html-italic">j</span> is the driving link; link <span class="html-italic">i</span> is a link of the studied linkage whose motion is known): (<b>a</b>) driving link with actuated R-pair and (<b>b</b>) driving link with actuated P-pair.</p>
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<p>RRR dyad: (<b>a</b>) reference dynamic sketch, (<b>b</b>) vector diagram of the velocity loop associated to the sketch, and (<b>c</b>) vector diagram of the acceleration loop associated to the sketch.</p>
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<p>RRP dyad: (<b>a</b>) reference dynamic sketch, (<b>b</b>) vector diagram of the velocity loop associated to the sketch, and (<b>c</b>) vector diagram of the acceleration loop associated to the sketch.</p>
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<p>RPR dyad: (<b>a</b>) reference dynamic sketch, (<b>b</b>) vector diagram of the velocity loop associated to the sketch, and (<b>c</b>) vector diagram of the acceleration loop associated to the sketch.</p>
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<p>PRP dyad: (<b>a</b>) reference dynamic sketch, (<b>b</b>) vector diagram of the velocity loop associated to the sketch, and (<b>c</b>) vector diagram of the acceleration loop associated to the sketch.</p>
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<p>RPP dyad: (<b>a</b>) reference dynamic sketch, (<b>b</b>) vector diagram of the velocity loop associated to the sketch, and (<b>c</b>) vector diagram of the acceleration loop associated to the sketch.</p>
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<p>Coupler curve generated in GeoGebra.</p>
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<p>Four-bar linkage: dynamic sketch and velocity/acceleration diagrams generated in GeoGebra for the case of constant angular velocity of the crank (ω<sub>2</sub> = 2π/3 rad/s and α<sub>2</sub> = 0 rad/s<sup>2</sup>) at the instant of motion t = 0.5 s (all the measurement units are in <a href="#app1-machines-12-00825" class="html-app">SI</a>).</p>
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<p>General geometric solution of the kinetostatic analysis of four-bar linkages, at the instant of motion t = 0.54 s (all the measurement units are in <a href="#app1-machines-12-00825" class="html-app">SI</a>), implemented in GeoGebra in the case in which the crank rotates at constant angular velocity (ω<sub>2</sub> = 2π/3 rad/s and α<sub>2</sub> = 0 rad/s<sup>2</sup>) and the R-pair centered at A is actuated. Only the inertial loads are applied to the links. On the linkage sketch, the blue (green (violet)) lines of action and forces refer to the case in which only link 3 (link 4 (link 2)) is loaded, whereas the red forces are the resultants obtained through the superposition principle.</p>
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<p>Diagram of the generalized torque M<sub>12</sub> as a function of time, t, during one full cycle of crank motion, that is, for t ranging from 0 s to 3 s, generated in GeoGebra.</p>
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<p>Shaper mechanism: dynamic sketch and velocity/acceleration diagrams generated in GeoGebra for the case of constant angular velocity of the crank (ω<sub>2</sub> = 1 rad/s and α<sub>2</sub> = 0 rad/s<sup>2</sup>) at the instant of motion t = 4.27 s (all the measurement units are in <a href="#app1-machines-12-00825" class="html-app">SI</a>).</p>
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24 pages, 9386 KiB  
Article
Toward Improving Human Training by Combining Wearable Full-Body IoT Sensors and Machine Learning
by Nazia Akter, Andreea Molnar and Dimitrios Georgakopoulos
Sensors 2024, 24(22), 7351; https://doi.org/10.3390/s24227351 - 18 Nov 2024
Viewed by 486
Abstract
This paper proposes DigitalUpSkilling, a novel IoT- and AI-based framework for improving and personalising the training of workers who are involved in physical-labour-intensive jobs. DigitalUpSkilling uses wearable IoT sensors to observe how individuals perform work activities. Such sensor observations are continuously processed to [...] Read more.
This paper proposes DigitalUpSkilling, a novel IoT- and AI-based framework for improving and personalising the training of workers who are involved in physical-labour-intensive jobs. DigitalUpSkilling uses wearable IoT sensors to observe how individuals perform work activities. Such sensor observations are continuously processed to synthesise an avatar-like kinematic model for each worker who is being trained, referred to as the worker’s digital twins. The framework incorporates novel work activity recognition using generative adversarial network (GAN) and machine learning (ML) models for recognising the types and sequences of work activities by analysing an individual’s kinematic model. Finally, the development of skill proficiency ML is proposed to evaluate each trainee’s proficiency in work activities and the overall task. To illustrate DigitalUpSkilling from wearable IoT-sensor-driven kinematic models to GAN-ML models for work activity recognition and skill proficiency assessment, the paper presents a comprehensive study on how specific meat processing activities in a real-world work environment can be recognised and assessed. In the study, DigitalUpSkilling achieved 99% accuracy in recognising specific work activities performed by meat workers. The study also presents an evaluation of the proficiency of workers by comparing kinematic data from trainees performing work activities. The proposed DigitalUpSkilling framework lays the foundation for next-generation digital personalised training. Full article
(This article belongs to the Special Issue Wearable and Mobile Sensors and Data Processing—2nd Edition)
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<p>DigitalUpSkilling framework.</p>
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<p>Hybrid GAN-ML activity classification.</p>
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<p>Skill proficiency assessment.</p>
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<p>(<b>a</b>) Placement of sensors; (<b>b</b>) sensors and straps; (<b>c</b>) alignment of sensors with the participant’s movements.</p>
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<p>Work environment for the data collection: (<b>a</b>) boning area; (<b>b</b>) slicing area.</p>
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<p>Dataflow of the study.</p>
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<p>(<b>a</b>) Worker performing boning; (<b>b</b>) worker’s real-time digital twin; (<b>c</b>) digital twins showing body movements along with real-time graphs of the joint’s movements.</p>
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<p>Comparison of the error rates of the different ML models.</p>
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<p>Confusion matrices: (<b>a</b>) boning; (<b>b</b>) slicing with pitch and roll from right-hand sensors.</p>
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<p>Distribution of the activity classification: (<b>a</b>) boning; (<b>b</b>) slicing.</p>
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<p>Accuracy of the GAN for different percentages of synthetic data: (<b>a</b>) boning; (<b>b</b>) slicing.</p>
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<p>Accuracy of the GAN with different percentages of synthetic data (circled area showing drop in the accuracy): (<b>a</b>) boning; (<b>b</b>) slicing.</p>
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<p>Classification accuracy with the GAN, SMOTE, and ENN (circled area showing improvement in the accuracy): (<b>a</b>) boning; (<b>b</b>) slicing.</p>
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<p>Distribution of right-hand pitch and roll mean (in degree).</p>
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<p>Comparison of the engagement in boning (W1: Worker 1; W2: Worker 2).</p>
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<p>Comparison of the engagement in slicing.</p>
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<p>Comparison of the accelerations of the right hand.</p>
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<p>Comparison of the accelerations of the right-hand.</p>
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<p>Comparisons of abduction, rotation, and flexion of the right shoulder during boning activities: (<b>a</b>) worker 1; (<b>b</b>) worker 2.</p>
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19 pages, 15352 KiB  
Article
Evaluation of Dynamics of a Freight Wagon Model with Viscous Damping
by Rafał Melnik, Seweryn Koziak, Jarosław Seńko, Ján Dižo and Jacek Caban
Appl. Sci. 2024, 14(22), 10624; https://doi.org/10.3390/app142210624 - 18 Nov 2024
Viewed by 326
Abstract
The aim of this work was to perform a simulation analysis of the dynamics of a freight wagon with a variant vibration damping: dry friction and viscous damping. The following mathematical models of the damping characteristics are presented: the Maxwell model and the [...] Read more.
The aim of this work was to perform a simulation analysis of the dynamics of a freight wagon with a variant vibration damping: dry friction and viscous damping. The following mathematical models of the damping characteristics are presented: the Maxwell model and the Kolsch model. The differences among the types of damping were first analyzed based on the dynamic responses of the 1 DOF model. Simulation studies were then carried out in a VI-Rail environment with the use of S-curved track models comprising short straight sections connecting the curves. The track models differed in the values of curve radii, cant, and length, which made it possible to run at different speeds. The multibody model of the vehicle represents a typical two-axle freight wagon. The dynamics of the wagon model were investigated for two states: empty and laden. Standard kinematic and dynamic values were compared in order to investigate if the nature of the damping has a significant impact on the dynamic properties of a freight wagon. The analysis of the simulation study showed that replacing dry friction damping with the viscous one can generally reduce forces acting on the wheel–rail contact, which, in turn, can be related to improving the running behavior of wagons while reducing the negative impact on the track. Full article
(This article belongs to the Section Mechanical Engineering)
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<p>UIC double-link suspension of a single-axle running gear. (<b>a</b>) Running gear model; (<b>b</b>) Diagram of a double-link connecting parabolic springs to a vehicle frame.</p>
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<p>DB 665 bogie with parabolic springs.</p>
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<p>Y25 bogie with parabolic springs: (<b>a</b>) Running gear model; (<b>b</b>) Diagram of the friction damper with Lenoir link (adapted from [<a href="#B4-applsci-14-10624" class="html-bibr">4</a>]).</p>
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<p>A three-piece bogie [<a href="#B4-applsci-14-10624" class="html-bibr">4</a>].</p>
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<p>TF 25 bogie [<a href="#B4-applsci-14-10624" class="html-bibr">4</a>].</p>
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<p>Physical model of the wagon: (<b>a</b>) Simulation model in VI-Rail MD 2010 13.0 software; (<b>b</b>) Diagram of the wagon model.</p>
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<p>The Maxwell model of a suspension damper.</p>
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<p>Characteristics of the Maxwell model with constant damping <span class="html-italic">c</span> and for different stiffness <span class="html-italic">k</span> values, an excitation frequency <span class="html-italic">f</span> = 1 Hz, and an amplitude <span class="html-italic">A</span> = 0.005 m.</p>
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<p>The Kolsch dry friction model.</p>
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<p>Characteristics of the Kolsch friction damper model, excitation frequency <span class="html-italic">f</span> = 1 Hz, and amplitude <span class="html-italic">A</span> = 0.005 m.</p>
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<p>Comparison of vertical vibrations of a vehicle model body with dry friction and viscous damping: (<b>a</b>) Vehicle body free vibration; (<b>b</b>) Phase portrait.</p>
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<p>Plan view of the simulated S-curved tracks: (<b>a</b>) the first track: R = 150 m, length = 220 m; (<b>b</b>) the second track: R = 320 m, length = 950 m.</p>
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<p>Simplified model of a rail vehicle running on a canted track.</p>
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<p>The vertical forces of the left wheel of the first wheelset: (<b>a</b>) The empty wagon; (<b>b</b>) The laden wagon.</p>
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<p>The vertical forces of the right wheel of the first wheelset: (<b>a</b>) The empty wagon; (<b>b</b>) The laden wagon.</p>
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<p>Sum of lateral forces of the first wheelset: (<b>a</b>) The empty wagon; (<b>b</b>) The laden wagon.</p>
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<p>The sum of lateral forces of the second wheelset: (<b>a</b>) The empty wagon; (<b>b</b>) The laden wagon.</p>
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<p>Vertical forces of a left and right wheel of the first wheelset: (<b>a</b>) Relative changes of the 99.85% percentile; (<b>b</b>) The RMS value.</p>
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<p>A sum of guiding forces: (<b>a</b>) Relative changes of the 99.85% percentile; (<b>b</b>) The RMS values.</p>
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<p>Lateral displacement of the second wheelset in the first simulation track: (<b>a</b>) The empty wagon; (<b>b</b>) The laden wagon.</p>
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<p>Angles of attack of the second wheelset in the first simulation track: (<b>a</b>) The empty wagon; (<b>b</b>) The laden wagon.</p>
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<p>RMS values of dissipated power by dry friction dampers and viscous dampers in the track with curves of R = 150 m, v = 50 km/h: (<b>a</b>) The empty wagon; (<b>b</b>) The laden wagon.</p>
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<p>RMS values of dissipated power by dry friction dampers and viscous dampers in the track with curves of R = 320 m, v = 80 km/h: (<b>a</b>) The empty wagon; (<b>b</b>) The laden wagon.</p>
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14 pages, 933 KiB  
Article
Olfactory Profile and Stochastic Analysis: An Innovative Approach for Predicting the Physicochemical Characteristics of Recycled Waste Cooking Oils for Sustainable Biodiesel Production
by Suelen Conceição de Carvalho, Maryana Mathias Costa Silva, Adriano Francisco Siqueira, Mariana Pereira de Melo, Domingos Sávio Giordani, Tatiane de Oliveira Souza Senra and Ana Lucia Gabas Ferreira
Sustainability 2024, 16(22), 9998; https://doi.org/10.3390/su16229998 - 16 Nov 2024
Viewed by 426
Abstract
The efficient, economical, and sustainable production of biodiesel from waste cooking oils (WCOs) depends on the availability of simple, rapid, and low-cost methods to test the quality of potential feedstocks. The aim of this study was to establish the applicability of stochastic modeling [...] Read more.
The efficient, economical, and sustainable production of biodiesel from waste cooking oils (WCOs) depends on the availability of simple, rapid, and low-cost methods to test the quality of potential feedstocks. The aim of this study was to establish the applicability of stochastic modeling of e-nose profiles in the evaluation of recycled WCO characteristics. Olfactory profiles of 10 WCOs were determined using a Sensigent Cyranose® 320 chemical vapor-sensing device with a 32 sensor-array, and a stepwise multiple linear regression (MLR) analysis was performed to select stochastic parameters (explanatory variables) for inclusion in the final predictive models of the physicochemical properties of the WCOs. The most important model parameters for the characterization of WCOs were those relating to the time of inception of the e-nose signal “plateau” and to the concentration of volatile organic compounds (VOCs) in the sensor region. A comparison of acid values, peroxide values, water contents, and kinematic viscosities predicted by the MLR models with those determined by conventional laboratory methods revealed that goodness of fit and predictor accuracy varied from good to excellent, with all metric values >90%. Combining e-nose profiling with stochastic modeling was successful in predicting the physicochemical characteristics of WCOs and could be used to select suitable raw materials for efficient and sustainable biodiesel production. Full article
(This article belongs to the Section Waste and Recycling)
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<p>Scatter plots showing the (<b>a</b>) acid value, (<b>b</b>) peroxide value, (<b>c</b>) water content, and (<b>d</b>) kinematic viscosity predicted by multiple linear regression vs. the corresponding values observed for samples of waste cooking oils. The solid red line represents the model estimates, the dashed line indicates the 95% predictability interval, and the dots denote the olfactory profiles of the 10 WCOs analyzed. Ten olfactory profiles were obtained for each sample, totalizing 100 olfactory profiles for each of the response variables.</p>
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<p>Scatter plot showing 10-fold R<sup>2</sup> and R<sup>2</sup> adjusted obtained for four models.</p>
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32 pages, 11087 KiB  
Article
Path Planning and Motion Control of Robot Dog Through Rough Terrain Based on Vision Navigation
by Tianxiang Chen, Yipeng Huangfu, Sutthiphong Srigrarom and Boo Cheong Khoo
Sensors 2024, 24(22), 7306; https://doi.org/10.3390/s24227306 - 15 Nov 2024
Viewed by 655
Abstract
This article delineates the enhancement of an autonomous navigation and obstacle avoidance system for a quadruped robot dog. Part one of this paper presents the integration of a sophisticated multi-level dynamic control framework, utilizing Model Predictive Control (MPC) and Whole-Body Control (WBC) from [...] Read more.
This article delineates the enhancement of an autonomous navigation and obstacle avoidance system for a quadruped robot dog. Part one of this paper presents the integration of a sophisticated multi-level dynamic control framework, utilizing Model Predictive Control (MPC) and Whole-Body Control (WBC) from MIT Cheetah. The system employs an Intel RealSense D435i depth camera for depth vision-based navigation, which enables high-fidelity 3D environmental mapping and real-time path planning. A significant innovation is the customization of the EGO-Planner to optimize trajectory planning in dynamically changing terrains, coupled with the implementation of a multi-body dynamics model that significantly improves the robot’s stability and maneuverability across various surfaces. The experimental results show that the RGB-D system exhibits superior velocity stability and trajectory accuracy to the SLAM system, with a 20% reduction in the cumulative velocity error and a 10% improvement in path tracking precision. The experimental results also show that the RGB-D system achieves smoother navigation, requiring 15% fewer iterations for path planning, and a 30% faster success rate recovery in challenging environments. The successful application of these technologies in simulated urban disaster scenarios suggests promising future applications in emergency response and complex urban environments. Part two of this paper presents the development of a robust path planning algorithm for a robot dog on a rough terrain based on attached binocular vision navigation. We use a commercial-of-the-shelf (COTS) robot dog. An optical CCD binocular vision dynamic tracking system is used to provide environment information. Likewise, the pose and posture of the robot dog are obtained from the robot’s own sensors, and a kinematics model is established. Then, a binocular vision tracking method is developed to determine the optimal path, provide a proposal (commands to actuators) of the position and posture of the bionic robot, and achieve stable motion on tough terrains. The terrain is assumed to be a gentle uneven terrain to begin with and subsequently proceeds to a more rough surface. This work consists of four steps: (1) pose and position data are acquired from the robot dog’s own inertial sensors, (2) terrain and environment information is input from onboard cameras, (3) information is fused (integrated), and (4) path planning and motion control proposals are made. Ultimately, this work provides a robust framework for future developments in the vision-based navigation and control of quadruped robots, offering potential solutions for navigating complex and dynamic terrains. Full article
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<p>Simplified box model of the Lite3P quadruped robotic dog.</p>
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<p>Internal sensor arrangement of the quadruped robotic dog.</p>
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<p>Dynamic control flowchart.</p>
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<p>MPC flowchart.</p>
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<p>WBC flowchart [<a href="#B30-sensors-24-07306" class="html-bibr">30</a>].</p>
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<p>Robot coordinates and joint point settings [<a href="#B30-sensors-24-07306" class="html-bibr">30</a>].</p>
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<p>Intel D435i and velodyne LIDAR.</p>
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<p>ICP diagram.</p>
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<p>Comparison of before and after modifying the perception region.</p>
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<p>Point cloud processing flowchart.</p>
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<p>{p, v} generation: (<b>a</b>) the creation of {p, v} pairs for collision points; (<b>b</b>) the process of generating anchor points and repulsive vectors for dynamic obstacle avoidance [<a href="#B41-sensors-24-07306" class="html-bibr">41</a>].</p>
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<p>Overall framework of 2D EGO-Planner.</p>
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<p>Robot initialization and control process in Gazebo simulation: (<b>a</b>) Gazebo environment creation, (<b>b</b>) robot model import, (<b>c</b>) torque balance mode activation, and (<b>d</b>) robot stepping and rotation in simulation.</p>
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<p>Joint rotational angles of FL and RL legs.</p>
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<p>Joint angular velocities of FL and RL legs.</p>
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<p>Torque applied to FL and RL joints during the gait cycle.</p>
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<p>The robot navigating in a simple environment using a camera.</p>
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<p>The robot navigating in a complex environment using a camera.</p>
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<p>A 2D trajectory showing start and goal positions, obstacles, and rough path.</p>
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<p>Initial environment setup.</p>
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<p>The robot starts navigating in a simple environment with a static obstacle (brown box).</p>
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<p>Dynamic Obstacle 1 introduced: the robot detects a new obstacle and recalculates its path.</p>
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<p>Dynamic Obstacle 2 introduced: after avoiding the first obstacle, a second obstacle is introduced and detected by the planner.</p>
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<p>Approaching the target: the robot adjusts its path to approach the target point as the distance shortens.</p>
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<p>Reaching the target: the robot completes its path and reaches the designated target point.</p>
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<p>Real-time B-spline trajectory updates in response to dynamic obstacles. Set 1 (orange) shows the initial path avoiding static obstacles. When the first dynamic obstacle is detected, the EGO-Planner updates the path (Set 2, blue) using local optimization. A second obstacle prompts another adjustment (Set 3, green), guiding the robot smoothly towards the target as trajectory updates become more frequent.</p>
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<p>The robot navigating a simple environment using SLAM.</p>
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<p>The robot navigating a complex environment using SLAM.</p>
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<p>A 2D trajectory showing start and goal positions, obstacles, and the planned path in a complex environment using SLAM.</p>
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<p>Navigation based on RGB-D camera.</p>
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<p>Navigation based on SLAM.</p>
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<p>Velocity deviation based on RGB-D camera.</p>
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<p>Velocity deviation based on SLAM.</p>
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<p>Cumulative average iterations.</p>
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<p>Cumulative success rate.</p>
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