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28 pages, 8007 KiB  
Review
Stimuli-Responsive Polymer Actuator for Soft Robotics
by Seewoo Kim, Sang-Nam Lee, Ambrose Ashwin Melvin and Jeong-Woo Choi
Polymers 2024, 16(18), 2660; https://doi.org/10.3390/polym16182660 - 21 Sep 2024
Abstract
Polymer actuators are promising, as they are widely used in various fields, such as sensors and soft robotics, for their unique properties, such as their ability to form high-quality films, sensitivity, and flexibility. In recent years, advances in structural and fabrication processes have [...] Read more.
Polymer actuators are promising, as they are widely used in various fields, such as sensors and soft robotics, for their unique properties, such as their ability to form high-quality films, sensitivity, and flexibility. In recent years, advances in structural and fabrication processes have significantly improved the reliability of polymer sensing-based actuators. Polymer actuators have attracted considerable attention for use in artificial or biohybrid systems, as they have the potential to operate under diverse conditions with high durability. This review briefly describes different types of polymer actuators and provides an understanding of their working mechanisms. It focuses on actuation modes controlled by diverse or multiple stimuli. Furthermore, it discusses the fabrication processes of polymer actuators; the fabrication process is an important consideration in the development of high-quality actuators with sensing properties for a wide range of applications in soft robotics. Additionally, the high potential of polymer actuators for use in sensing technology is examined, and the latest developments in the field of polymer actuators, such as the development of biohybrid polymers and the use of polymer actuators in 4D printing, are briefly described. Full article
(This article belongs to the Special Issue Flexible Devices Based on Functional Polymers)
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Figure 1
<p>Schematic classification of stimuli-responsive polymer actuators by types of external stimuli, fabrication methods, and types.</p>
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<p>(<b>a</b>) Operation model of custom-developed microelectronics devices for device interfacing and experimental controlling. (<b>b</b>) Setpoint, feedback, and output curves of a typical feedback-driven positioning experiment. Position feedback was provided by integrated magnetic sensors. The proportional gain constant was set to <span class="html-italic">K</span><sub>P</sub> = 200. Reprinted with permission from reference [<a href="#B29-polymers-16-02660" class="html-bibr">29</a>]. (<b>c</b>) A photograph of the c-PEDOT:PSS-PET substrate immersed in water. (<b>d</b>) Plots of the normalized thickness (upper) and optical transmittance of the c-PEDOT:PSS films (lower) concerning the duration of immersion in DI water and phosphate-buffered saline (PBS). Reprinted with permission from reference [<a href="#B30-polymers-16-02660" class="html-bibr">30</a>]. (<b>e</b>) Schematic illustration of the actuation mechanism in the case of a trilayer conjugated polymer. Reprinted with permission from reference [<a href="#B26-polymers-16-02660" class="html-bibr">26</a>]. (<b>f</b>) Prospective 3D printed soft robot, where both the EP actuator and robotic body are printed using a single printing process. Cut-away view to show the internal components. Reprinted with permission from reference [<a href="#B28-polymers-16-02660" class="html-bibr">28</a>].</p>
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<p>(<b>a</b>) Schematic illustration of the preparation process. Reprinted with permission from reference [<a href="#B35-polymers-16-02660" class="html-bibr">35</a>]. (<b>b</b>) Photograph and schematic illustration of the ultrahigh-molecular-weight gel [<a href="#B36-polymers-16-02660" class="html-bibr">36</a>]. (<b>c</b>) Photograph of a flat individual polyelectrolyte-based GPE (PGPE) and of an LED powered by a 2.4 V device; here, two 1.2 V PGPE supercapacitor devices are connected in series. Reprinted with permission from reference [<a href="#B34-polymers-16-02660" class="html-bibr">34</a>].</p>
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<p>(<b>a</b>) The biohybrid composite fabrication steps are conducted using bovine pericardium (BP). Step I: intact BP is divided into three portions for processing, and the first portion is left untreated. Step II: the second portion of the sac is decellularized using sodium deoxycholate. Step III: coating of polycaprolactone: chitosan polymer layer on the decellularized BP via electrospinning. Reprinted with permission from reference [<a href="#B43-polymers-16-02660" class="html-bibr">43</a>]. (<b>b</b>) Electronic functionalization of plant roots. ETE-S polymerizes on the roots of intact bean plants catalyzed by endogenous plant cell wall peroxidases and H<sub>2</sub>O<sub>2</sub>. Reprinted with permission from reference [<a href="#B48-polymers-16-02660" class="html-bibr">48</a>]. (<b>c</b>) Ejection of guest–host granular hydrogel from the syringe through a 27 G needle onto a surface, and two-component granular hydrogels injected into rat hearts either with myocardial infarction (MI) or no MI. Reprinted with permission from reference [<a href="#B47-polymers-16-02660" class="html-bibr">47</a>].</p>
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<p>(<b>a</b>) The molecular mechanism of the dual-SME. Black dots: net points; blue lines: molecular chains of low mobility below <span class="html-italic">T</span><sub>trans</sub>; red lines: molecular chains of high mobility above <span class="html-italic">T</span><sub>trans</sub>. Reprinted with permission from reference [<a href="#B53-polymers-16-02660" class="html-bibr">53</a>]. (<b>b</b>) The alignment of polymer chains, i.e., entangled in their permanent form and aligned when stretched in their temporary form. Reprinted with permission from reference [<a href="#B52-polymers-16-02660" class="html-bibr">52</a>]. (<b>c</b>) Schematic demonstration of this smart shape-memory textile used in a smart cloth. Reprinted with permission from reference [<a href="#B55-polymers-16-02660" class="html-bibr">55</a>].</p>
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<p>(<b>a</b>) Various actuator constructions using conducting polymers differ in bulk expansion, bending bilayer, buckling trilayer, and bending trilayer in air. Reprinted with permission from reference [<a href="#B56-polymers-16-02660" class="html-bibr">56</a>]. (<b>b</b>) Photograph and schematic illustration depicting the structure and assembly procedure of the actuator. Reprinted with permission from reference [<a href="#B57-polymers-16-02660" class="html-bibr">57</a>].</p>
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<p>Thermal sensing actuator design principle. (<b>a</b>) Schematics showing the hand withdrawal reflex consists of a thermoreceptor, sensory neurons, spinal cord, motor neurons, and muscle. (<b>b</b>) Working mechanism of the TSA simulating the function of hand withdrawal reflex, with thermal sensing potential (V<sub>thermal</sub>), action potential (V<sub>action</sub>) and a smart control system. Reprinted with permission from reference [<a href="#B60-polymers-16-02660" class="html-bibr">60</a>]. (<b>c</b>) Image of the fiber temperature sensor sewn onto the tip of a hand glove. (<b>d</b>) Temperature response of the fiber sensor to repetitive touch of a hot (45 °C) or cold (5 °C) object. Reprinted with permission from reference [<a href="#B61-polymers-16-02660" class="html-bibr">61</a>].</p>
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<p>(<b>a</b>) Photoactuation of the polymer ribbons incorporating H1 [<a href="#B62-polymers-16-02660" class="html-bibr">62</a>]. Thickness 25 μm. (<b>b</b>,<b>c</b>) Linear dichroism of azobenzene-doped ultra-drawn ultrahigh-molecular-weight polyethylene films. Insets are photographs taken of the corresponding ultra-drawn films, with the transmission axis of the polarizer at 0° indicated in white. Reprinted with permission from reference [<a href="#B63-polymers-16-02660" class="html-bibr">63</a>].</p>
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<p>(<b>a</b>) Schematic representation of a magnetically active strain sensor on a PET film with resistance variation correlation with the magnetic actuator displacement after correction of the low-frequency offset. Inset resistance variation correlation with the magnetic actuator displacement after correction of the low-frequency offset. Reprinted with permission from reference [<a href="#B64-polymers-16-02660" class="html-bibr">64</a>]. Novel dual-alignment processing method for HPMSA to align magnetic particles and PVDF crystals. (<b>b</b>) Random Fe<sub>3</sub>O<sub>4</sub>, f-CNT, and amorphous and crystal phases of PVDF. (<b>c</b>) Magnetic alignment: movement of f-CNT and PVDF crystals due to Fe<sub>3</sub>O<sub>4</sub> alignment with an external magnetic field. (<b>d</b>) Mechanical alignment: further alignment of Fe<sub>3</sub>O<sub>4</sub>, f-CNT, and PVDF crystals (transformation from amorphous phase) with mechanical uniaxial stretching of HPMSA [<a href="#B65-polymers-16-02660" class="html-bibr">65</a>].</p>
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<p>(<b>a</b>) Initial emf response (squares) and response after 6 months (circles) to pH for an ISE with a PDMA membrane (doped with ionophore and ionic sites) photographed onto a polypropylene-based electrode body and nano-graphite solid contact, relative to a free-flowing double-junction reference electrode. The pH was adjusted by the addition of 1.0 M HCl or 1.0 M NaOH to 10 mM sodium phosphate buffer solution (pH 7.1). The pH shown on the x-axis was measured using a pH glass electrode.Reprinted with permission from reference [<a href="#B68-polymers-16-02660" class="html-bibr">68</a>]. (<b>b</b>) schematic representation of our pH sensor consisting of a PANI membrane on interdigital electrodes supported by a PI substrate. The transformation of PANI protonated in acid solution and deprotonated in basic solution [<a href="#B69-polymers-16-02660" class="html-bibr">69</a>].</p>
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<p>(<b>a</b>) The schematics of the fabricated p(D-<span class="html-italic">co</span>-M) sensor and the copolymer’s predominant protonation state at various pH values. Reprinted with permission from reference [<a href="#B72-polymers-16-02660" class="html-bibr">72</a>]. (<b>b</b>) A schematic diagram representing the deposition of gas molecules on the surface of a conducting polymer composite film consisting of inorganic nanoparticles. Reprinted with permission from reference [<a href="#B73-polymers-16-02660" class="html-bibr">73</a>].</p>
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<p>Proposes structures of (<b>a</b>) SC/PEA/KB(10) and (<b>b</b>) PSCD⊃PEA/KB(10). Reprinted with permission from reference [<a href="#B74-polymers-16-02660" class="html-bibr">74</a>]. Schematic illustration of the wearable FSS for real-time stress management. (<b>b</b>) Schematic illustration of the wearable FSS that enables cortisol monitoring through a CNT-based sensor with an MIP. (<b>c</b>) Schematic illustration of a single fabric sensor and magnified image of the fabric sensor. (<b>d</b>) Schematic illustration and current response in cortisol recognition. The red solid line indicates the current response after cortisol recognition. Reprinted with permission from reference [<a href="#B75-polymers-16-02660" class="html-bibr">75</a>].</p>
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<p>Electrosynthesis strategies are based on the direct formation of quinones. Schematic representations of the electro-crosslinking, through direct electro-oxidation of catechol/gallon moieties of (<b>a</b>) PAH/bis catechol film [<a href="#B77-polymers-16-02660" class="html-bibr">77</a>]. (<b>b</b>) Representation of Al<sup>3+</sup>/TA@AgNP film assembly. Reproduced with permission from reference [<a href="#B78-polymers-16-02660" class="html-bibr">78</a>].</p>
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<p>(<b>a</b>) Schematic illustration of constructing a mesoporous CP layer on 2D functionalized surfaces. (<b>a</b>) Simplified schematic diagram of PS-b-PEO. (<b>b</b>) PS-b-PEO dissolved in the mixed solution to form spherical micelles. (<b>c</b>) The micelles are tightly arranged on the GO surface. (<b>d</b>) Micelles attract Py monomers to form complex micelles. (<b>e</b>) Monomer polymerizes in situ to form a polymer network. (<b>f</b>) Removal of the template to obtain sandwich-structured mesoporous PPy nanosheets [<a href="#B80-polymers-16-02660" class="html-bibr">80</a>]. (<b>g</b>) Schematic illustration of the synthesis route employed for the preparation via RAFT-mediated aqueous polymerization-induced disassembly (PIDA). Reproduced with permission from reference [<a href="#B81-polymers-16-02660" class="html-bibr">81</a>].</p>
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<p>(<b>a</b>) Dispersion polymerization of tulip-derived α-methylene γ-butylrolactone (MBL). Reproduced with permission from reference [<a href="#B89-polymers-16-02660" class="html-bibr">89</a>]. (<b>b</b>) Schematic illustrating the Au assembly process of polymer substrates. Reproduced with permission from reference [<a href="#B90-polymers-16-02660" class="html-bibr">90</a>].</p>
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<p>(<b>a</b>) CP formation by reacting metal ions with bridging ligands and also CP formation via polymerization of MCMs. Reproduced with permission from reference [<a href="#B97-polymers-16-02660" class="html-bibr">97</a>]. (<b>b</b>) The recycling process of shape-memory polymers in repeated programming and photoinduced 4D printing. (<b>c</b>) The recovery angle versus time of LMPCs in a total of 25 cycles while irradiating with 808 nm laser (0.3 W/cm<sup>2</sup>) for 60 s. Reproduced with permission from reference [<a href="#B98-polymers-16-02660" class="html-bibr">98</a>].</p>
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15 pages, 4554 KiB  
Article
Curvature Sensing and Control of Soft Continuum Robots Using e-Textile Sensors
by Eric Vincent Galeta, Ayman A. Nada, Ibrahim Hameed and Haitham El-Hussieny
Appl. Syst. Innov. 2024, 7(5), 84; https://doi.org/10.3390/asi7050084 - 13 Sep 2024
Abstract
Soft continuum robots, with their flexible and deformable structures, excel in tasks requiring delicate manipulation and navigation through complex environments. Accurate shape sensing is vital to enhance their performance, safety, and adaptability. Unlike rigid sensors, soft sensors conform to the robot’s flexible surfaces, [...] Read more.
Soft continuum robots, with their flexible and deformable structures, excel in tasks requiring delicate manipulation and navigation through complex environments. Accurate shape sensing is vital to enhance their performance, safety, and adaptability. Unlike rigid sensors, soft sensors conform to the robot’s flexible surfaces, ensuring consistent measurement of shape and motion. This paper introduces a new approach using soft e-textile resistive sensors, which integrate seamlessly with the robot’s structure. These sensors adjust their resistance in response to movements, capturing multidimensional force data. A deep Convolutional Neural Network (CNN) decodes the sensor signals, enabling precise shape estimation and control. Our findings indicate that soft e-textile sensors may surpass traditional rigid sensors in shape sensing and control, significantly improving the functionality of soft continuum robots in challenging applications. Full article
(This article belongs to the Section Control and Systems Engineering)
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<p>The sensor design utilizes piezoresistive textile material and copper electrodes to detect changes in pressure and strain.</p>
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<p>Diagram depicting the design of our soft force sensor with stacked layers [<a href="#B27-asi-07-00084" class="html-bibr">27</a>].</p>
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<p>Diagram of the Soft E-Textile Sensor Interface: This illustration highlights the e-textile sensor at the center, flanked by copper electrodes, and encased within fabric insulation layers.</p>
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<p>A single-section continuum robot is equipped with a soft e-textile sensor featuring 16 sensing points arranged in a 4 × 4 matrix.</p>
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<p>The CNN architectures used to estimate the curvature of the soft robot from sensor readings.</p>
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<p>A block diagram of the continuum robot Jacobian-based shape control approach utilizing the soft e-textile sensor with the proposed CNN shape sensing model.</p>
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<p>The experimental setup includes a cable-driven continuum robot, IMU, soft e-textile sensor, and Arduino UNO for estimating the robot’s shape.</p>
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<p>(<b>a</b>) Variation in sensor readings from the 4 × 4 matrix of e-textile sensing points labeled <math display="inline"><semantics> <msub> <mi>A</mi> <mn>0</mn> </msub> </semantics></math> to <math display="inline"><semantics> <msub> <mi>A</mi> <mn>15</mn> </msub> </semantics></math> capturing the continuum robot’s deformation in relation to changes in the robot’s curvature <math display="inline"><semantics> <mi>κ</mi> </semantics></math> in (<b>b</b>).</p>
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<p>Graph illustrating the mean squared error (MSE) for training and validation losses during the training of the CNN-based shape sensing model for continuum robots over 500 epochs.</p>
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<p>Comparison of target versus estimated values for the validation dataset of the robot’s parameters <math display="inline"><semantics> <mi>κ</mi> </semantics></math> and <math display="inline"><semantics> <mi>ϕ</mi> </semantics></math> using the CNN-based shape sensing model.</p>
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<p>(<b>a</b>) Training losses depicted as mean squared error (MSE) for five deep neural network (DNN) models during 5-fold cross-validation, and (<b>b</b>) the corresponding mean and standard deviations of these losses. Architectures with more number of neocons are having intense red colors.</p>
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<p>Results of the Jacobian-based control used for reaching the reference desired shape parameter (<math display="inline"><semantics> <mi>κ</mi> </semantics></math>) at (<b>a</b>) <math display="inline"><semantics> <mrow> <mi>K</mi> <mo>=</mo> <mn>0.25</mn> </mrow> </semantics></math> and (<b>c</b>) <math display="inline"><semantics> <mrow> <mi>K</mi> <mo>=</mo> <mn>0.5</mn> </mrow> </semantics></math> gains, while controlling the shape parameter (<math display="inline"><semantics> <mi>ϕ</mi> </semantics></math>) at (<b>b</b>) <math display="inline"><semantics> <mrow> <mi>K</mi> <mo>=</mo> <mn>0.25</mn> </mrow> </semantics></math> and (<b>d</b>) <math display="inline"><semantics> <mrow> <mi>K</mi> <mo>=</mo> <mn>0.5</mn> </mrow> </semantics></math> gain values.</p>
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<p>End-effector tracking performance of the proposed Jacobian-based control to command the robot’s tip follow desired trajectory in (<b>a</b>) <span class="html-italic">x</span>- and (<b>b</b>) <span class="html-italic">y</span>-directions.</p>
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13 pages, 6005 KiB  
Article
Facile One-Pot Preparation of Polypyrrole-Incorporated Conductive Hydrogels for Human Motion Sensing
by Zunhui Zhao, Jiahao Liu, Jun Lv, Bo Liu, Na Li and Hangyu Zhang
Sensors 2024, 24(17), 5814; https://doi.org/10.3390/s24175814 - 7 Sep 2024
Abstract
Conductive hydrogels have been widely used in soft robotics, as well as skin-attached and implantable bioelectronic devices. Among the candidates of conductive fillers, conductive polymers have become popular due to their intrinsic conductivity, high biocompatibility, and mechanical flexibility. However, it is still a [...] Read more.
Conductive hydrogels have been widely used in soft robotics, as well as skin-attached and implantable bioelectronic devices. Among the candidates of conductive fillers, conductive polymers have become popular due to their intrinsic conductivity, high biocompatibility, and mechanical flexibility. However, it is still a challenge to construct conductive polymer-incorporated hydrogels with a good performance using a facile method. Herein, we present a simple method for the one-pot preparation of conductive polymer-incorporated hydrogels involving rapid photocuring of the hydrogel template followed by slow in situ polymerization of pyrrole. Due to the use of a milder oxidant, hydrogen peroxide, for polypyrrole synthesis, the photocuring of the hydrogel template and the growing of polypyrrole proceeded in an orderly manner, making it possible to prepare conductive polymer-incorporated hydrogels in one pot. The preparation process is facile and extensible. Moreover, the obtained hydrogels exhibit a series of properties suitable for biomedical strain sensors, including good conductivity (2.49 mS/cm), high stretchability (>200%), and a low Young’s modulus (~30 kPa) that is compatible with human skin. Full article
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<p>Schematic diagram for the preparation process of the CPHs through the one-pot method.</p>
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<p>Various interactions among components of the PPy/PA/PSBMA hydrogel.</p>
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<p>UV–Vis spectra of PPy/PA/PSBMA hydrogel during PPy polymerization.</p>
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<p>FT-IR and XPS spectra of the hydrogels. (<b>a</b>) FT-IR spectra of the PSBMA hydrogel, PA/PSBMA hydrogel, and PPy/PA/PSBMA hydrogel. (<b>b</b>) XPS spectra of the PPy/PA/PSBMA hydrogel. (<b>c</b>) Magnified spectra of the N1s area.</p>
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<p>The tensile stress and strain curves of the PPy/PA/PSBMA hydrogels with different cross-linking degrees.</p>
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<p>Sensing performance of the PPy/PA/PSBMA hydrogel as a strain sensor. (<b>a</b>) Electrical resistance and strain curves. The original data is represented by a blue line and the linear-fitted curve is represented by a red dashed line. (<b>b</b>) The response and recovery times of the hydrogel. (<b>c</b>) Real-time response curve measured at variable strains. (<b>d</b>) Real-time response curve measured at changeable frequencies. (<b>e</b>) Cycling durability of the hydrogel strain sensor.</p>
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<p>Application of the PPy/PA/PSBMA hydrogel for motion detection. The hydrogel could be used to monitor the movements of the (<b>a</b>) neck, (<b>b</b>) knees, (<b>c</b>) ankles, (<b>d</b>) wrists, and (<b>e</b>) the variations in gesture.</p>
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<p>Trials of the hydrogel fabrication using different materials through the one-pot preparation method. (<b>a</b>) PPy/PA/PAAm. (<b>b</b>) PPy/PA/PAA. (<b>c</b>) PPy/PA/P (AAm-co-AA). (<b>d</b>) PPy/PA/PHEMA. (<b>e</b>) PPy/PA/PSBMA-APS. (<b>f</b>) PANI/PA/PSBMA.</p>
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32 pages, 6972 KiB  
Review
Gels/Hydrogels in Different Devices/Instruments—A Review
by Md Murshed Bhuyan and Jae-Ho Jeong
Gels 2024, 10(9), 548; https://doi.org/10.3390/gels10090548 - 23 Aug 2024
Viewed by 369
Abstract
Owing to their physical and chemical properties and stimuli-responsive nature, gels and hydrogels play vital roles in diverse application fields. The three-dimensional polymeric network structure of hydrogels is considered an alternative to many materials, such as conductors, ordinary films, constituent components of machines [...] Read more.
Owing to their physical and chemical properties and stimuli-responsive nature, gels and hydrogels play vital roles in diverse application fields. The three-dimensional polymeric network structure of hydrogels is considered an alternative to many materials, such as conductors, ordinary films, constituent components of machines and robots, etc. The most recent applications of gels are in different devices like sensors, actuators, flexible screens, touch panels, flexible storage, solar cells, batteries, and electronic skin. This review article addresses the devices where gels are used, the progress of research, the working mechanisms of hydrogels in those devices, and future prospects. Preparation methods are also important for obtaining a suitable hydrogel. This review discusses different methods of hydrogel preparation from the respective raw materials. Moreover, the mechanism by which gels act as a part of electronic devices is described. Full article
(This article belongs to the Special Issue Applications of Gels in Energy Materials and Devices)
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<p>Conductive hydrogels used in different devices (reused with permission [<a href="#B35-gels-10-00548" class="html-bibr">35</a>]).</p>
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<p>Properties of hydrogels for application to different devices.</p>
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<p>Property versus cross-linked density graph for correlating shear modulus, (G) swelling ratio (Q), and molecular diffusivity (D).</p>
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<p>Fabrication and structure of (<b>a</b>) PVAGMA-MCC hydrogel cross-linked by tannic acid and (<b>b</b>) borax cross-linked TOCN/PVA composite gel and its SEM photograph [<a href="#B43-gels-10-00548" class="html-bibr">43</a>].</p>
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<p>Fabrication and structure of (<b>a</b>) PVAGMA-MCC hydrogel cross-linked by tannic acid and (<b>b</b>) borax cross-linked TOCN/PVA composite gel and its SEM photograph [<a href="#B43-gels-10-00548" class="html-bibr">43</a>].</p>
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<p>Application of hydrogels in different sectors.</p>
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<p>Different preparation methods of gel/hydrogel.</p>
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<p>Different hydrogel-based sensors.</p>
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<p>Polyacrylamide (PAAM)/chitosan (CS) hydrogel showing angle of bend for strain sensor.</p>
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<p>Different stimuli-responsive hydrogel actuators.</p>
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<p>Schematic illustration of PSPA-based hydrogel’s electroactuation on applied electric field. (<b>a</b>) At zero time, (<b>b</b>) bending characteristics of PASA-based hydrogel at 2 min, and (<b>c</b>) at 4 min.</p>
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<p>Illustration of central touch analysis to find the connections between the current versus touch location of 1D touch strip.</p>
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<p>(<b>a</b>) GG/PEDOT:PSS model and (<b>b</b>) comparison curves of I–V for the different gel electrolytes in DSSCs (reused with permission [<a href="#B140-gels-10-00548" class="html-bibr">140</a>]).</p>
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<p>Hydrogel network as electrolyte for battery flexible battery system.</p>
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<p>Agar/polyacrylamide DN hydrogels as soft endoscope.</p>
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<p>Thermal stability and insulation characteristics. (<b>a</b>,<b>b</b>) Relationship of thermal conductivity with density, temperature, and wavelength; (<b>c</b>) comparison of thermal insulation between ZAG and commercial barrier for an aero-engine (CFM56) [<a href="#B183-gels-10-00548" class="html-bibr">183</a>].</p>
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19 pages, 4449 KiB  
Article
Development of an Adaptive Force Control Strategy for Soft Robotic Gripping
by Ian MacDonald and Rickey Dubay
Appl. Sci. 2024, 14(16), 7354; https://doi.org/10.3390/app14167354 - 20 Aug 2024
Viewed by 391
Abstract
Using soft materials in robotic mechanisms has become a common solution to overcome many challenges associated with the rigid bodies frequently used in robotics. Compliant mechanisms allow the robot to adapt to objects and perform a broader range of tasks, unlike rigid bodies [...] Read more.
Using soft materials in robotic mechanisms has become a common solution to overcome many challenges associated with the rigid bodies frequently used in robotics. Compliant mechanisms allow the robot to adapt to objects and perform a broader range of tasks, unlike rigid bodies that are generally designed for specific applications. However, soft robotics presents its own set of challenges in both design and implementation, particularly in sensing and control. These challenges are abundant when dealing with the force control problem of a compliant gripping mechanism. The ability to effectively regulate the applied force of a gripper is a critical task in many control operations, as it allows the precise manipulation of objects, which drives the need for enhanced force control strategies for soft or flexible grippers. Standard sensing techniques, such as motor current monitoring and strain-based sensors, add complexities and uncertainties when establishing mathematical models of soft grippers to the required gripping forces. In addition, the soft gripper creates a complex non-linear system, compounded by adding an adhesive-type sensor. This work develops a unique visual force sensor trained on synthetic data generated using finite element analysis (FEA) and implemented by integrating a non-linear model reference adaptive controller (MRAC) to control gripping force on a fixed 6-DOF robot. The robot can be placed on a mobile platform to perform various tasks. The virtual FEA sensor and controller, combined, are termed virtual reference adaptive control (VRAC). The VRAC was compared to other methods and achieved comparable control sensing and control performance while reducing the complexity of the sensor requirements and its integration. The VRAC strategy effectively controlled the gripping force by driving the dynamics to match the desired performance after a limited amount of training cycles. The controller proposed in this work was designed to be generally applicable to most objects that the gripper will interact with and easily adaptable to a wide variety of soft grippers. Full article
(This article belongs to the Special Issue Advanced Technologies in AI Mobile Robots)
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<p>Festo fin ray gripper [<a href="#B1-applsci-14-07354" class="html-bibr">1</a>].</p>
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<p>Computer vision force-sensing workflow.</p>
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<p>Gripper–camera assembly.</p>
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<p>Ansys deformation simulation using fin ray finger and 50 mm round object.</p>
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<p>Ansys deformation simulation using fin ray finger and 10 mm round object.</p>
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<p>Autoencoder structure.</p>
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<p>High-level cascaded control scheme.</p>
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<p>Model reference adaptive control for gripper force control.</p>
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<p>Binary cross-entropy loss of autoencoder training process.</p>
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<p>Fin ray with occlusions reconstructed using fin ray.</p>
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<p>Force profile for 50 mm object. (<b>a</b>) Training data capture setup with 50 mm round object; (<b>b</b>) force comparison between load cell sensor and visual sensor for 50 mm round training object.</p>
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<p>Force profile for 10 mm object. (<b>a</b>) Training data capture setup with 10 mm round object; (<b>b</b>) force comparison between load cell sensor and visual sensor for 10 mm round training object.</p>
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<p>Force profile for novel 25 mm object. (<b>a</b>) Novel 25 mm object data capture setup; (<b>b</b>) force comparison between load cell sensor and visual sensor for a novel 25 mm object.</p>
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<p>Closed-loop force control performance of MRAC controller on fin ray fingers.</p>
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<p>Evolution of controller gains.</p>
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<p>Gripping test using learned parameters found in <a href="#applsci-14-07354-f014" class="html-fig">Figure 14</a>.</p>
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42 pages, 18854 KiB  
Review
A Review of Perception Technologies for Berry Fruit-Picking Robots: Advantages, Disadvantages, Challenges, and Prospects
by Chenglin Wang, Weiyu Pan, Tianlong Zou, Chunjiang Li, Qiyu Han, Haoming Wang, Jing Yang and Xiangjun Zou
Agriculture 2024, 14(8), 1346; https://doi.org/10.3390/agriculture14081346 - 12 Aug 2024
Viewed by 795
Abstract
Berries are nutritious and valuable, but their thin skin, soft flesh, and fragility make harvesting and picking challenging. Manual and traditional mechanical harvesting methods are commonly used, but they are costly in labor and can damage the fruit. To overcome these challenges, it [...] Read more.
Berries are nutritious and valuable, but their thin skin, soft flesh, and fragility make harvesting and picking challenging. Manual and traditional mechanical harvesting methods are commonly used, but they are costly in labor and can damage the fruit. To overcome these challenges, it may be worth exploring alternative harvesting methods. Using berry fruit-picking robots with perception technology is a viable option to improve the efficiency of berry harvesting. This review presents an overview of the mechanisms of berry fruit-picking robots, encompassing their underlying principles, the mechanics of picking and grasping, and an examination of their structural design. The importance of perception technology during the picking process is highlighted. Then, several perception techniques commonly used by berry fruit-picking robots are described, including visual perception, tactile perception, distance measurement, and switching sensors. The methods of these four perceptual techniques used by berry-picking robots are described, and their advantages and disadvantages are analyzed. In addition, the technical characteristics of perception technologies in practical applications are analyzed and summarized, and several advanced applications of berry fruit-picking robots are presented. Finally, the challenges that perception technologies need to overcome and the prospects for overcoming these challenges are discussed. Full article
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<p>Traditional harvesting device of berry fruits: (<b>a</b>) The artificial-assisted single-drive device for picking multi-fruit strawberries from Ref. [<a href="#B5-agriculture-14-01346" class="html-bibr">5</a>]. (<b>b</b>) The crankshaft vibration threshing and harvesting equipment for wine grapes from Ref. [<a href="#B6-agriculture-14-01346" class="html-bibr">6</a>].</p>
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<p>Application of perception technology in berry fruit picking: (<b>a</b>) The vision system-based end-effector for grape picking robots from Ref. [<a href="#B15-agriculture-14-01346" class="html-bibr">15</a>]. (<b>b</b>) The kiwifruit harvesting robot is based on deep learning from Ref. [<a href="#B16-agriculture-14-01346" class="html-bibr">16</a>]. (<b>c</b>) A modular autonomous strawberry-picking robot and its end-effector from Ref. [<a href="#B17-agriculture-14-01346" class="html-bibr">17</a>].</p>
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<p>Picking steps and grasping standardized processes of berry-picking robots.</p>
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<p>Classification of mobile platforms for berry fruit-picking robots. The mobile base is Yuhesen Technology and PAL Robotics.</p>
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<p>Process of analyzing the kinematics of the manipulator of a berry fruit-picking robot.</p>
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<p>Classification of end-effector for berry fruit-picking robots.</p>
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<p>Part of the end-effector for berry fruit picking: (<b>a</b>) The fuzzy control of a robotic gripper for efficient strawberry harvesting from Ref. [<a href="#B58-agriculture-14-01346" class="html-bibr">58</a>]. (<b>b</b>) The tendon-driven soft robotic gripper for blackberry harvesting from Ref. [<a href="#B59-agriculture-14-01346" class="html-bibr">59</a>]. (<b>c</b>) The ridge planting strawberry picking manipulator from Ref. [<a href="#B60-agriculture-14-01346" class="html-bibr">60</a>]. (<b>d</b>) The harvesting robot for table-top cultivated strawberries and its end-effector from Ref. [<a href="#B61-agriculture-14-01346" class="html-bibr">61</a>]. Copyright 2019, IEEE. (<b>e</b>) A robotic kiwifruit harvester and its end-effector from Ref. [<a href="#B62-agriculture-14-01346" class="html-bibr">62</a>].</p>
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<p>Object detection techniques applied to berry fruit picking: (<b>a</b>) Detection of kiwifruit in the orchard using improved YOLOv3—tiny model from Ref. [<a href="#B113-agriculture-14-01346" class="html-bibr">113</a>]. Copyright 2021, Springer Nature. (<b>b</b>) Detection of cherry fruits based on the improved YOLOv4 model from Ref. [<a href="#B106-agriculture-14-01346" class="html-bibr">106</a>]. Copyright 2023, Springer Nature. (<b>c</b>) Visual localization of the picking points for a ridge-planting strawberry from Ref. [<a href="#B112-agriculture-14-01346" class="html-bibr">112</a>]. (<b>d</b>) Tomato detection based on modified YOLOv3 framework from Ref. [<a href="#B110-agriculture-14-01346" class="html-bibr">110</a>].</p>
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<p>Semantic segmentation techniques applied to berry fruit picking: (<b>a</b>) Counting of grapevine berries using convolutional neural networks from Ref. [<a href="#B123-agriculture-14-01346" class="html-bibr">123</a>]. (<b>b</b>) Bayberry segmentation is based on a multi-module convolutional neural network from Ref. [<a href="#B122-agriculture-14-01346" class="html-bibr">122</a>]. (<b>c</b>) Recognition of strawberry ripeness combining Mask R-CNN from Ref. [<a href="#B116-agriculture-14-01346" class="html-bibr">116</a>]. (<b>d</b>) A transformer-based Mask R-CNN for tomato detection and segmentation from Ref. [<a href="#B121-agriculture-14-01346" class="html-bibr">121</a>].</p>
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<p>Instance segmentation techniques applied to berry fruit picking: (<b>a</b>) Quantifying blueberries in the wild using instance segmentation. from Ref. [<a href="#B124-agriculture-14-01346" class="html-bibr">124</a>]. (<b>b</b>) Mask R-CNN for instance segmentation of grape cluster from Ref. [<a href="#B126-agriculture-14-01346" class="html-bibr">126</a>]. (<b>c</b>) Deep learning method for strawberry instance segmentation from Ref. [<a href="#B131-agriculture-14-01346" class="html-bibr">131</a>]. (<b>d</b>) A segmentation method for waxberry image from Ref. [<a href="#B127-agriculture-14-01346" class="html-bibr">127</a>].</p>
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<p>Tactile perception applied to berry fruit-picking robots: (<b>a</b>) A multi-finger gripper and its grasping grape cluster from Ref. [<a href="#B137-agriculture-14-01346" class="html-bibr">137</a>]. (<b>b</b>) A gripper for delicate harvesting of strawberries from Ref. [<a href="#B138-agriculture-14-01346" class="html-bibr">138</a>]. (<b>c</b>) Grasping perception of kiwifruit gripper and its structure from Ref. [<a href="#B139-agriculture-14-01346" class="html-bibr">139</a>]. (<b>d</b>) A sweet pepper harvesting robot and its gripper’s structure from Ref. [<a href="#B141-agriculture-14-01346" class="html-bibr">141</a>]. (<b>e</b>) A gripper with capacitive object size detection from Ref. [<a href="#B143-agriculture-14-01346" class="html-bibr">143</a>]. (<b>f</b>) The structure of the capacitive sensor and its application from Ref. [<a href="#B144-agriculture-14-01346" class="html-bibr">144</a>]. Copyright 2023, IEEE. (<b>g</b>) PE sensor integrated on a robotic hand and its grasping from Ref. [<a href="#B146-agriculture-14-01346" class="html-bibr">146</a>]. (<b>h</b>) A dynamic tactile sensor and its application from Ref. [<a href="#B145-agriculture-14-01346" class="html-bibr">145</a>]. (<b>i</b>) A finger of the end-effector with a triboelectric sensor is used to monitor the tactile aspect of the robot from Ref. [<a href="#B149-agriculture-14-01346" class="html-bibr">149</a>]. (<b>j</b>) A finger of end-effector with triboelectric sensor and its application from Ref. [<a href="#B147-agriculture-14-01346" class="html-bibr">147</a>].</p>
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<p>Distance measurement-related technology applied to berry fruit-picking robots: (<b>a</b>) A pneumatic finger-like end-effector and harvesting cherry tomato from Ref. [<a href="#B159-agriculture-14-01346" class="html-bibr">159</a>]. (<b>b</b>) The strawberry localization in a ridge planting from Ref. [<a href="#B158-agriculture-14-01346" class="html-bibr">158</a>]. (<b>c</b>) A strawberry harvesting robot with a cable-driven gripper from Ref. [<a href="#B32-agriculture-14-01346" class="html-bibr">32</a>]. (<b>d</b>) A tomato harvesting robot with LiDAR from Ref. [<a href="#B162-agriculture-14-01346" class="html-bibr">162</a>]. (<b>e</b>) A gripper with laser beam sensor and its application from Ref. [<a href="#B160-agriculture-14-01346" class="html-bibr">160</a>]. (<b>f</b>) A tomato harvesting robot with LiDAR from Ref. [<a href="#B161-agriculture-14-01346" class="html-bibr">161</a>]. (<b>g</b>) Detection of wild blueberry using an ultrasonic sensor from Ref. [<a href="#B163-agriculture-14-01346" class="html-bibr">163</a>]. Copyright 2009, ASABE. (<b>h</b>) Optical sensing and LiDAR to determine tomato plant spacing from Ref. [<a href="#B164-agriculture-14-01346" class="html-bibr">164</a>]. (<b>i</b>) Adaptive end-effector with multimodal sensors for tomato-harvesting robots from Ref. [<a href="#B165-agriculture-14-01346" class="html-bibr">165</a>].</p>
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<p>Switching sensors related technology applied to berry fruit-picking robots. (<b>a</b>) The cherry tomato picking robot with photoelectric switches from Ref. [<a href="#B169-agriculture-14-01346" class="html-bibr">169</a>]. (<b>b</b>) A soft gripper with photoelectric switches for kiwifruit from Ref. [<a href="#B170-agriculture-14-01346" class="html-bibr">170</a>]. (<b>c</b>) A berry-picking robot with proximity switches from Ref. [<a href="#B173-agriculture-14-01346" class="html-bibr">173</a>]. (<b>d</b>) A harvesting robot with a vacuum sensor for sweet pepper from Ref. [<a href="#B178-agriculture-14-01346" class="html-bibr">178</a>]. (<b>e</b>) An underactuated gripper with a pressure sensor for grasping grape cluster from Ref. [<a href="#B174-agriculture-14-01346" class="html-bibr">174</a>]. Copyright 2023, IEEE.</p>
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<p>The characteristics of the perception techniques.</p>
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<p>Advanced technologies applied to berry fruit harvesting: (<b>a</b>) Fruit picking using physical twinning from Ref. [<a href="#B181-agriculture-14-01346" class="html-bibr">181</a>]. (<b>b</b>) A Bubble casts soft robotics by grasping small fruits from Ref. [<a href="#B182-agriculture-14-01346" class="html-bibr">182</a>]. Copyright 2021, Springer Nature. (<b>c</b>) A hydraulically amplified self-healing electrostatic actuator with muscle-like performance and its application. From Ref. [<a href="#B183-agriculture-14-01346" class="html-bibr">183</a>].</p>
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18 pages, 3470 KiB  
Article
Soft Robots: Computational Design, Fabrication, and Position Control of a Novel 3-DOF Soft Robot
by Martin Garcia, Andrea-Contreras Esquen, Mark Sabbagh, Devin Grace, Ethan Schneider, Turaj Ashuri, Razvan Cristian Voicu, Ayse Tekes and Amir Ali Amiri Moghadam
Machines 2024, 12(8), 539; https://doi.org/10.3390/machines12080539 - 7 Aug 2024
Viewed by 618
Abstract
This paper presents the computational design, fabrication, and control of a novel 3-degrees-of-freedom (DOF) soft parallel robot. The design is inspired by a delta robot structure. It is engineered to overcome the limitations of traditional soft serial robot arms, which are typically low [...] Read more.
This paper presents the computational design, fabrication, and control of a novel 3-degrees-of-freedom (DOF) soft parallel robot. The design is inspired by a delta robot structure. It is engineered to overcome the limitations of traditional soft serial robot arms, which are typically low in structural stiffness and blocking force. Soft robotic systems are becoming increasingly popular due to their inherent compliance match to that of human body, making them an efficient solution for applications requiring direct contact with humans. The proposed soft robot consists of three soft closed-loop kinematic chains, each of which includes a soft actuator and a compliant four-bar arm. The complex nonlinear dynamics of the soft robot are numerically modeled, and the model is validated experimentally using a 6-DOF electromagnetic position sensor. This research contributes to the growing body of literature in the field of soft robotics, providing insights into the computational design, fabrication, and control of soft parallel robots for use in a variety of complex applications. Full article
(This article belongs to the Section Robotics, Mechatronics and Intelligent Machines)
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<p>Design of rigid and soft delta robots. (RJ: revolute joint).</p>
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<p>Comparison of (<b>a</b>) bending movement of rigid and soft links and (<b>b</b>) lateral movement of rigid and compliant upper links.</p>
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<p>CAD model and the prototype of the proposed soft delta robot.</p>
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<p>Experimental setup to prove the concept and validate the model.</p>
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<p>Working principle of tendon-driven actuators.</p>
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<p>Frame assignment for the soft delta robot.</p>
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<p>Workspace of the soft robot.</p>
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<p>Kinematic model of the robot. (<b>a</b>) Horizontal trajectory; (<b>b</b>) joint angles.</p>
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<p>Kinematic model of the robot. (<b>a</b>) Vertical trajectory; (<b>b</b>) joint angles.</p>
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<p>Simscape model of (<b>a</b>) soft link, (<b>b</b>) compliant four-bar, and (<b>c</b>) single SL-CFB.</p>
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<p>MATLAB Simscape model of the soft delta robot.</p>
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<p>Validation of the Simscape model through experimental data.</p>
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<p>Comparison of Simscape and experimental system response for circular motion (planar trajectory).</p>
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<p>Comparison of Simscape and experimental system response for helical trajectory (spatial motion).</p>
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<p>Neural network structure.</p>
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<p>Closed-loop control using PID and NN/KNN as kinematic model.</p>
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<p>Open- and closed-loop responses. (<b>a</b>) Analytical model, open loop; (<b>b</b>) KNN regression, open loop; (<b>c</b>) neural network, open loop; (<b>d</b>) KNN regression, closed loop; (<b>e</b>) neural network, closed loop.</p>
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19 pages, 6835 KiB  
Article
Development and Investigation of a Grasping Analysis System with Two-Axis Force Sensors at Each of the 16 Points on the Object Surface for a Hardware-Based FinRay-Type Soft Gripper
by Takahide Kitamura, Kojiro Matsushita, Naoki Nakatani and Shunsei Tsuchiyama
Sensors 2024, 24(15), 4896; https://doi.org/10.3390/s24154896 - 28 Jul 2024
Viewed by 479
Abstract
The FinRay soft gripper achieves passive enveloping grasping through its functional flexible structure, adapting to the contact configuration of the object to be grasped. However, variations in beam position and thickness lead to different behaviors, making it important to research the relationship between [...] Read more.
The FinRay soft gripper achieves passive enveloping grasping through its functional flexible structure, adapting to the contact configuration of the object to be grasped. However, variations in beam position and thickness lead to different behaviors, making it important to research the relationship between structure and force. Conventional research using FEM simulations has tested various virtual FinRay models but replicating phenomena such as buckling and slipping has been challenging. While hardware-based methods that involve installing sensors on the gripper and the object to analyze their states have been attempted, no studies have focused on the tangential contact force related to slipping. Therefore, we developed a 16-way object contact force measurement device incorporating two-axis force sensors into each of the 16 segmented objects and compared the normal and tangential components of the enveloping grasping force of the FinRay soft gripper under two types of contact friction conditions. In the first experiment, the proposed device was compared with a device containing a six-axis force sensor in one segmented object, confirming that the proposed device has no issues with measurement performance. In the second experiment, comparisons of the proposed device were made under various conditions: two contact friction states, three object contact positions, and two object motion states. The results demonstrated that the proposed device could decompose and analyze the grasping force into its normal and tangential components for each segmented object. Moreover, low friction conditions result in a wide contact area with lower tangential frictional force and a uniform normal pushing force, achieving effective enveloping grasping. Full article
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<p>Arrangement of each beam in the FinRay structure (<b>left</b>) and the passive deformation mechanism (<b>right</b>).</p>
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<p>Conceptual diagram of the distributed contact force measurement device with a built-in object to be grasped. (<b>a</b>) Introduction of measurement equipment: (<b>i</b>) Overall view; (<b>ii</b>) 16 measuring point numbers, (<b>b</b>) additions and design changes in the direction of the measurement axis, (<b>c</b>) an aluminum contact blade (shape of the contact area), and (<b>d</b>) force sensor size and mounting method.</p>
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<p>Back and forth action mechanisms for the contact force measurement device. (<b>a</b>) Installation of the laser range finder and view of the laser-irradiated surface, (<b>b</b>) switching mechanism for forward/backward movement of the object (upper image: sliding mechanism; lower image: screw-fixing mechanism), and (<b>c</b>) contact positions of three types of cylindrical objects.</p>
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<p>Parallel opening/closing mechanism of the FinRay soft gripper and finger design with a marker base. (<b>a</b>) Appearance of the FinRay soft gripper and the size and structure of the opening and closing mechanisms, (<b>b</b>) size of the FinRay structure and the location and size of the marker base, and (<b>c</b>) method of fixing the FinRay structure to the moving part of the opening/closing mechanism (T-slot type).</p>
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<p>Conceptual diagram of the structural deformation measurement device using camera images and flow of image processing and analysis of marker trajectories. (<b>a</b>) Relationship between the USB camera, motor, and PC (PC3 for controlling gripper motors 1, 2, and camera base motor 3) that made up the device; (<b>b</b>) initial image; (<b>c</b>) Gaussian smoothing image; (<b>d</b>) masking image; (<b>e</b>) binarized image; (<b>f</b>) recording of the center of gravity using a Kalman filter and numbering of recognition blobs; (<b>g</b>) unit conversion of blob center-of-gravity coordinates (pixel to mm); (<b>h</b>) smoothing with Savitzky–Golay filter; and (<b>i</b>) numbering position.</p>
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<p>The 1/16-type measurement device using a 6-axis force sensor and the measurement method for channels 1–8 (1ch to 8ch) directions of 16 divisions (same for channels 9–16).</p>
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<p>The 1/16-type measurement device using a 6-axis force sensor and the measurement method from 1ch to 8ch directions of 16 divisions (same from 9ch to 16ch). On the left is the distribution of normal force and on the right is the distribution of frictional force. (<b>a</b>) High friction condition, (<b>b</b>) low friction condition.</p>
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<p>The 16/16-type measurement device using a 6-axis force sensor and the measurement method from 1ch to 8ch directions of 16 divisions (same from 9ch to 16ch). On the left is the distribution of normal force and on the right is the distribution of frictional force. (<b>a</b>) High friction condition, (<b>b</b>) low friction condition.</p>
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<p>Normal and frictional force distribution and vector display for a high friction contact surface and cylindrical object under “fixed” conditions. (<b>a</b>) Contact start position: L = +20 mm, green; (<b>b</b>) contact start position: L = +10 mm, blue; and (<b>c</b>) contact start position: L = 0 mm, red.</p>
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<p>Normal and frictional force distribution and vector display for a low friction contact surface and cylindrical object under “fixed” conditions. (<b>a</b>) Contact start position: L = +20 mm, green; (<b>b</b>) contact start position: L = +10 mm, blue; (<b>c</b>) contact start position: L = 0 mm, red; and (<b>d</b>) structural deformation by marker tracking (high friction condition: red; low friction condition: blue).</p>
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<p>Normal and frictional force distribution and vector display for a high friction contact surface and cylindrical object under “non-fixed” conditions. (<b>a</b>) Contact start position: L = +20 mm, green; (<b>b</b>) contact start position: L = +10, blue mm; and (<b>c</b>) contact start position: L = 0 mm, red.</p>
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<p>Normal and frictional force distribution and vector display for a low friction contact surface and cylindrical object under “non-fixed” conditions. (<b>a</b>) Contact start position: L = +20 mm, green; (<b>b</b>) contact start position: L = +10 mm, blue; (<b>c</b>) contact start position: L = 0 mm, red; and (<b>d</b>) structural deformation by marker tracking (high friction condition: red; low friction condition: blue).</p>
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<p>Displacement of the laser range finder in a movable object state under object-movable condition: “non-fixed” (top: L = +20mm / middle: L = +10mm / bottom: L = 0mm). (<b>a</b>) High friction condition; (<b>b</b>) low friction condition.</p>
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17 pages, 4958 KiB  
Article
Characterizing the Sensing Response of Carbon Nanocomposite-Based Wearable Sensors on Elbow Joint Using an End Point Robot and Virtual Reality
by Amit Chaudhari, Rakshith Lokesh, Vuthea Chheang, Sagar M. Doshi, Roghayeh Leila Barmaki, Joshua G. A. Cashaback and Erik T. Thostenson
Sensors 2024, 24(15), 4894; https://doi.org/10.3390/s24154894 - 28 Jul 2024
Viewed by 669
Abstract
Physical therapy is often essential for complete recovery after injury. However, a significant population of patients fail to adhere to prescribed exercise regimens. Lack of motivation and inconsistent in-person visits to physical therapy are major contributing factors to suboptimal exercise adherence, slowing the [...] Read more.
Physical therapy is often essential for complete recovery after injury. However, a significant population of patients fail to adhere to prescribed exercise regimens. Lack of motivation and inconsistent in-person visits to physical therapy are major contributing factors to suboptimal exercise adherence, slowing the recovery process. With the advancement of virtual reality (VR), researchers have developed remote virtual rehabilitation systems with sensors such as inertial measurement units. A functional garment with an integrated wearable sensor can also be used for real-time sensory feedback in VR-based therapeutic exercise and offers affordable remote rehabilitation to patients. Sensors integrated into wearable garments offer the potential for a quantitative range of motion measurements during VR rehabilitation. In this research, we developed and validated a carbon nanocomposite-coated knit fabric-based sensor worn on a compression sleeve that can be integrated with upper-extremity virtual rehabilitation systems. The sensor was created by coating a commercially available weft knitted fabric consisting of polyester, nylon, and elastane fibers. A thin carbon nanotube composite coating applied to the fibers makes the fabric electrically conductive and functions as a piezoresistive sensor. The nanocomposite sensor, which is soft to the touch and breathable, demonstrated high sensitivity to stretching deformations, with an average gauge factor of ~35 in the warp direction of the fabric sensor. Multiple tests are performed with a Kinarm end point robot to validate the sensor for repeatable response with a change in elbow joint angle. A task was also created in a VR environment and replicated by the Kinarm. The wearable sensor can measure the change in elbow angle with more than 90% accuracy while performing these tasks, and the sensor shows a proportional resistance change with varying joint angles while performing different exercises. The potential use of wearable sensors in at-home virtual therapy/exercise was demonstrated using a Meta Quest 2 VR system with a virtual exercise program to show the potential for at-home measurements. Full article
(This article belongs to the Special Issue Advances in Sensor Technologies for Wearable Applications)
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<p>The process for preparing a uniform dispersion of carbon nanotubes for dip coating.</p>
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<p>(<b>a</b>) Schematic of the specimen utilized for uniaxial testing in the warp direction; (<b>b</b>) scanning electron micrograph of weft knit fabric showing the looped structure and (<b>c</b>) schematic of a compression sleeve with a carbon nanotube sensor sewn onto the elbow location.</p>
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<p>Sketches showing arm movements used for testing (<b>a</b>) Constant amplitude straight line movement task for a displacement of 30 cm in the vertical direction; (<b>b</b>) variable amplitude straight line movement task from 30 cm to 5 cm when the handle moves from the start point to points 1-6, where the amplitude decreases by 5 cm between each point; (<b>c</b>) in-plane two-dimensional movement of the arm in diamond path with angle measured at four end points; and (<b>d</b>) in the plane two-dimensional movement of the arm in a circular path with an angle measured at four end points. The arrow indicates the direction of movement.</p>
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<p>(<b>a</b>) Virtual model of the Kinarm in a home family room setting created in VR environment, (<b>b</b>) in-plane two-dimensional movement of the hand following a diamond path, and (<b>c</b>) in-plane movement of the hand following a circular path. The user moves the handle from point 1 to point 2, 3, and 4, following straight line and circular paths.</p>
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<p>(<b>a</b>) Surface morphology of a fiber in a knit fabric before and after the carbon nanocomposite coating; (<b>b</b>) sensor response when tested for the uniaxial stretch in the warp direction for 10%, 20%, and 30% strain levels; and (<b>c</b>) resistance change against strain with a gauge factor of ~35 at low strains.</p>
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<p>The calibration curve generated with the participant with a compression sleeve on the arm for increasing change in elbow flexion angle.</p>
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<p>(<b>a</b>) Resistance change (%) in the arm flexion from moving start point to end point with a total change in angle of 53°, showing repeatability of the sensor response and (<b>b</b>) resistance response of sleeve in variable amplitude straight line motion with change in elbow angle when handle moves from start point to points 1–6, starting from an amplitude of 30 cm and decreasing by 5 cm for each subsequent point.</p>
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<p>Elbow angle change was calculated using a goniometer during activity for points 1, 2, 3, and 4, and the change in angle was extrapolated from the calibration curve using resistance change values for the different sections of circular and diamond paths between points 1, 2, 3, and 4. Dotted boxes separates the data for circular and diamond path segments.</p>
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<p>Response of the sensor in compression sleeve during elbow motion with virtual reality task (<b>a</b>) diamond path tracing, and (<b>b</b>) circular path tracing with a deviation from the intended path (dashed area of the second cycle). The user moves handles from point 1 to points 2, 3, and 4, following a straight (for diamond path) or circular path. A dotted encircled point is a mistake made by the participant while performing a circular task.</p>
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<p>Calibration curve with resistance change plotted against change in elbow angle during flexion, while performing the tasks on Kinarm end point robot and VR.</p>
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<p>Participant testing with commercial stretching exercise available on Oculus Quest with CNT sensor on the sleeve in one hand and sleeve response, percentage resistance change, for the three different types of stretch exercises. Mountains and valleys in the resistance curve and the corresponding arm positions during stretch 2 are shown with arrows.</p>
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27 pages, 2864 KiB  
Review
Recent Advances in the 3D Printing of Conductive Hydrogels for Sensor Applications: A Review
by Xiaoxu Liang, Minghui Zhang, Cheong-Meng Chong, Danlei Lin, Shiji Chen, Yumiao Zhen, Hongyao Ding and Hai-Jing Zhong
Polymers 2024, 16(15), 2131; https://doi.org/10.3390/polym16152131 - 26 Jul 2024
Viewed by 558
Abstract
Conductive hydrogels, known for their flexibility, biocompatibility, and conductivity, have found extensive applications in fields such as healthcare, environmental monitoring, and soft robotics. Recent advancements in 3D printing technologies have transformed the fabrication of conductive hydrogels, creating new opportunities for sensing applications. This [...] Read more.
Conductive hydrogels, known for their flexibility, biocompatibility, and conductivity, have found extensive applications in fields such as healthcare, environmental monitoring, and soft robotics. Recent advancements in 3D printing technologies have transformed the fabrication of conductive hydrogels, creating new opportunities for sensing applications. This review provides a comprehensive overview of the advancements in the fabrication and application of 3D-printed conductive hydrogel sensors. First, the basic principles and fabrication techniques of conductive hydrogels are briefly reviewed. We then explore various 3D printing methods for conductive hydrogels, discussing their respective strengths and limitations. The review also summarizes the applications of 3D-printed conductive hydrogel-based sensors. In addition, perspectives on 3D-printed conductive hydrogel sensors are highlighted. This review aims to equip researchers and engineers with insights into the current landscape of 3D-printed conductive hydrogel sensors and to inspire future innovations in this promising field. Full article
(This article belongs to the Special Issue Development of Applications of Polymer-Based Sensors and Actuators)
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<p>Number of publications over the last five years (from 2019 to 2023) using the keywords “conductive hydrogel”, “3D print”, “sensor”, and their combination, using Web of Science.</p>
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<p>Various types of conductive hydrogels: (<b>a</b>) electronic conductive hydrogels (ECH), (<b>b</b>) ion conductive hydrogels (ICH), and (<b>c</b>) composite conductive hydrogels (CCH).</p>
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<p>(<b>I</b>) Schematic diagram of properties of PPNGC hydrogel [<a href="#B111-polymers-16-02131" class="html-bibr">111</a>]. (<b>II</b>) Conductivity and strain-sensing ability of 3D-printable triple-network composite hydrogels. (<b>a</b>) Hydrogel is immersed in PBS (10 mM), and the Na+/K+/Ca2+ ions are attracted by SMF. (<b>b</b>) Conductivity of the SMF/RSF/PAM hydrogel-based strain sensor with different compression ratios. (<b>c</b>) Photographs of the LED light before and after compression. Strain sensors of hydrogels under (<b>d</b>) compression and (<b>e</b>) tensile loading. (<b>f</b>) Relative resistance changes and (<b>g</b>) GF variations of the composite hydrogel-based sensors under the applied tension. Relative resistance changes upon (<b>h</b>) two and (<b>i</b>) three movements of the strain sensor on the fingers. [<a href="#B112-polymers-16-02131" class="html-bibr">112</a>].</p>
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<p>(<b>I</b>) Digital photographs and corresponding relative resistance change of the poly(ACMO)/Pt sensor attached to the (<b>a</b>) finger, (<b>b</b>) elbow, (<b>c</b>) knee, (<b>d</b>,<b>e</b>) throat, and (<b>f</b>) wrist [<a href="#B74-polymers-16-02131" class="html-bibr">74</a>]. (<b>II</b>) Schematic of the preparation procedure and properties of 3D reactive printing of the PHH hydrogels (polyaniline hybrid hydrogels) [<a href="#B32-polymers-16-02131" class="html-bibr">32</a>].</p>
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<p>(<b>I</b>) Performance of a flexible electrode made of the printed hydrogel for capturing human neural signals. (<b>a</b>) Illustration of the 3D printed flexible electrode acting as a human-machine interface. (<b>b</b>) The EOG of the nerve of horizontal rotation of the eye balls: the opposite signals indicate the EOG of right and left eyeballs. (<b>c</b>) The EOG signal of blinking the eyes. (<b>d</b>) The EEG signal of blinking the eyes. (<b>e</b>) The Fourier transformation of the signal of closing the eyes and relaxing. (<b>f</b>) The Fourier transformation of the signal of opening the eyes and focusing to show the neural activity [<a href="#B106-polymers-16-02131" class="html-bibr">106</a>]. (<b>II</b>) (<b>a</b>) Schematic illustration of the manufacturing process of epidermal PAINT hydrogel electrodes with direct ink writing. (<b>b</b>) Schematic of electrode setup for ECG tests. (<b>c</b>) Biopotential ECG signals monitored with Ag/AgCl coated gel and PAINT hydrogel electrodes of identical surface area. (<b>d</b>) Frequency-amplitude spectrogram of the recorded ECG. (<b>e</b>) Schematic of electrode setup for sEMG tests. (<b>f</b>) sEMG of fist motions monitored with Ag/AgCl coated gel and PAINT hydrogel electrodes of identical surface area. (<b>g</b>) Signal-to-noise ratios show a 16.7% improvement for the fist clenching sEMG and an 87.5% improvement for the finger extension sEMG with the PAINT hydrogel. (<b>h</b>) Comparison between commercial and PAINT electrodes during eye closure sFES. (<b>i</b>) Resistance as a function of stimulation current during sFES of the eye closure [<a href="#B2-polymers-16-02131" class="html-bibr">2</a>].</p>
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<p>(<b>I</b>) Humidity sensitivity and potential applications of the graphene nanoplate–carbon nanotube (GC) humidity sensor. (<b>a</b>) A filter with sensor function and (<b>b</b>) its application scenarios; (<b>c</b>) The resistance changes of the GC sensor from the indoor environment to the high humidity environment and back to the indoor environment; (<b>d</b>) Cyclic testing of the GC humidity sensor; (<b>e</b>) Respiration testing results of normal breath, fast breath, and deep breath [<a href="#B115-polymers-16-02131" class="html-bibr">115</a>]. (<b>II</b>) Wireless temperature monitor based on PNCMA-78 deep eutectic gel. (<b>a</b>) Thermal conductivity of PNCMA-78 gel. (<b>b</b>) Photo of the wireless body temperature monitor, while the meaning of the non-English term is Bluetooth networking. (<b>c</b>) Infrared images captured body surface temperature at 25 °C, artificial heating, and returning to 25 °C. (<b>d</b>) Temperature-time curves drawn by the data collected on the mobile phone. (<b>e</b>) Temperature change curves in three states by using a deep eutectic gel sensor and an infrared camera, respectively [<a href="#B117-polymers-16-02131" class="html-bibr">117</a>]. (<b>III</b>) pH response of PEDOT:PSS/hydrophilic polyurethanes (HPU) hydrogel-based sensor. (<b>a</b>) an example of the electrical response of PEDOT:PSS/HPU hydrogels to the pH change from neutral to pH 3 over time with inset showing an image of the sample with electrical connections and (<b>b</b>) correlation between resistance and pH of the solution for PEDOT:PSS/HPU hydrogels. (<b>c</b>) Schematic illustration of the impact of pH on molecular structure of PEDOT:PSS [<a href="#B123-polymers-16-02131" class="html-bibr">123</a>]. (<b>IV</b>) Temperature changes of poly (N-isopropyl acrylamide) (PNIPAAM) /L3/ carbon nanotubes (CNTs) hydrogels (<b>A</b>) after NIR light exposure. Relative resistance changes of PNIPAM/L3/CNT hydrogels under NIR light exposure (<b>B</b>). Photographs of the increased light intensity after NIR light exposure (<b>C</b>) [<a href="#B38-polymers-16-02131" class="html-bibr">38</a>].</p>
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<p>(<b>I</b>) Instant current–time response curves, repeatability, and sensing mechanisms of the corresponding metabolites of printed biosensors when metabolite solutions with different concentrations were pumped into the channel in an alternating manner (flow velocity: 200 μL/min). (<b>a</b>,<b>d</b>) TG-WE detects triglyceride. (<b>b</b>,<b>e</b>) LA-WE detects lactate. (<b>c</b>,<b>f</b>) Glu-WE detects glucose. The insets in (<b>a</b>–<b>c</b>) show the schematic sensing mechanisms of the corresponding metabolites by the PAni hydrogel/PtNP enzymatic biosensors [<a href="#B78-polymers-16-02131" class="html-bibr">78</a>]. (<b>II</b>) (<b>a</b>) Scheme of the glucose sensor based on GOx-loaded H/G4–PANI hydrogel for the detection of glucose. (<b>b</b>) The image of the glucose sensor. (<b>c</b>) Cyclic voltammograms of glucose sensor in the presence of different concentrations of glucose. Inset indicates the linear correlation of cathodic peak current with the concentration of glucose. (<b>d</b>) UV–Vis absorption spectra of the H/G4–PANI hydrogel film measured in HCl solution. Inset are the photographic images of the H/G4–PANI hydrogel film at different applied potentials. (<b>e</b>) Potential and chronoamperometry curves of the H/G4–PANI hydrogel film [<a href="#B130-polymers-16-02131" class="html-bibr">130</a>].</p>
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18 pages, 6367 KiB  
Article
Sensor-Enhanced Smart Gripper Development for Automated Meat Processing
by Kristóf Takács, Bence Takács, Tivadar Garamvölgyi, Sándor Tarsoly, Márta Alexy, Kristóf Móga, Imre J. Rudas, Péter Galambos and Tamás Haidegger
Sensors 2024, 24(14), 4631; https://doi.org/10.3390/s24144631 - 17 Jul 2024
Viewed by 1099
Abstract
Grasping and object manipulation have been considered key domains of Cyber-Physical Systems (CPS) since the beginning of automation, as they are the most common interactions between systems, or a system and its environment. As the demand for automation is spreading to increasingly complex [...] Read more.
Grasping and object manipulation have been considered key domains of Cyber-Physical Systems (CPS) since the beginning of automation, as they are the most common interactions between systems, or a system and its environment. As the demand for automation is spreading to increasingly complex fields of industry, smart tools with sensors and internal decision-making become necessities. CPS, such as robots and smart autonomous machinery, have been introduced in the meat industry in recent decades; however, the natural diversity of animals, potential anatomical disorders and soft, slippery animal tissues require the use of a wide range of sensors, software and intelligent tools. This paper presents the development of a smart robotic gripper for deployment in the meat industry. A comprehensive review of the available robotic grippers employed in the sector is presented along with the relevant recent research projects. Based on the identified needs, a new mechatronic design and early development process of the smart gripper is described. The integrated force sensing method based on strain measurement and magnetic encoders is described, including the adjacent laboratory and on-site tests. Furthermore, a combined slip detection system is presented, which relies on an optical flow-based image processing algorithm using the video feed of a built-in endoscopic camera. Basic user tests and application assessments are presented. Full article
(This article belongs to the Section Smart Agriculture)
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<p>Livestock statistics from the European Union. (<b>a</b>) Distribution of pig meat production in 2019. (<b>b</b>) Production of different meat products in the EU, million tonnes. Source: Agriculture, forestry and fishery statistics [<a href="#B1-sensors-24-04631" class="html-bibr">1</a>]. Data source: Eurostat.</p>
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<p>Examples of robotic grippers: simple strong pneumatic 2-finger meat industry gripper from DMRI (<b>top left</b>, image credit: DMRI), underactuated soft-gripper from Soft Robotics (<b>bottom left</b>, image credit: <a href="http://www.softroboticsinc.com" target="_blank">www.softroboticsinc.com</a>, accessed on: 2 July 2024), and the force controlled OnRobot RG2 2-finger gripper delicately holding a pig kidney (<b>right</b>, image credit: Óbuda University).</p>
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<p>Early conceptual simulated setup of the Meat Factory Cell (<b>a</b>), and the real MFC at the Max Rubner Institute, Kulmbach, Germany (<b>b</b>). The Carcass Handling Unit is holding and manipulating the attached carcass, and the two robots are equipped with intelligent end-of-arm-toolings: RGB-D camera, knife/saw and gripper. (Simulation made with RobotStudio (v2021, ABB Ltd, Zürich, Switzerland), image credit: Óbuda University [<a href="#B28-sensors-24-04631" class="html-bibr">28</a>]).</p>
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<p>Images of a pig carcass fixed in the Carcass Handling Unit before and after the evisceration process. (<b>a</b>) Photo of the pig before the trachea-gripping taken by the RealSense RGB-D camera attached to one of the robots. The trachea and the gripping target point are successfully localized by the neural network (purple bounding-box and the labeled point in the middle). Image credit: ByteMotion. (<b>b</b>) The carcass in the CHU after the evisceration process. The limbs are already cut off, and the saddle, the belly and the viscera are separated and ready to be loaded onto the rack. Image credit: Óbuda University and NMBU.</p>
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<p>CAD models constructed during the design process of the gripper prototype. (<b>a</b>) The 1st conceptual design with 2 × 2 fingers and a cutting blade. (<b>b</b>) The final CAD model of the 1st prototype. (<b>c</b>) The finger design allows the grasping of objects up to 60 mm in diameter, with up to 40 mm radial displacement. The red arrow shows the constrained motion of the target object due to the synchronized encircling motion of the fingers. Furthermore, due to the constant closing torque and the decreasing lever arm (R2 &lt; R1), the clamping force increases (F2 &gt; F1) when the soft tissue is squeezed between the fingers, ensuring that a shape-locking grasp is achieved.</p>
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<p>CAD models constructed during the design process of the gripper prototype. (<b>a</b>) The 1st conceptual design with 2 × 2 fingers and a cutting blade. (<b>b</b>) The final CAD model of the 1st prototype. (<b>c</b>) The finger design allows the grasping of objects up to 60 mm in diameter, with up to 40 mm radial displacement. The red arrow shows the constrained motion of the target object due to the synchronized encircling motion of the fingers. Furthermore, due to the constant closing torque and the decreasing lever arm (R2 &lt; R1), the clamping force increases (F2 &gt; F1) when the soft tissue is squeezed between the fingers, ensuring that a shape-locking grasp is achieved.</p>
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<p>The final gripper model attached to the ABB IRB 4600 robot (<b>a</b>), its CAD model with improved finger design (<b>c</b>), and the timing belts in the power transmission system (<b>b</b>). The wires in the middle of the gripper transmit the sensory data of the strain gauges to the microcontroller.</p>
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<p>The smart slip detection system of the gripper. The camera is placed at the front of the gripper, and the synchronized encircling motion of the fingers ensures that the grasped object is pressed to the protective lens in front of the camera. The visualized optical flow field of the circular ROI shows the direction of the movement too. (<b>a</b>) Placement of the endoscopic camera at the front of the gripper behind the protective lens. (<b>b</b>) Typical camera frame with visualized optical flow and adjacent parameters computed.</p>
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<p>Resultant force data acquired during manual pig cuttings with the gripper prototype. (<b>a</b>) Plot of the forces measured during the cutting of the 4 limbs. (<b>b</b>) Plot of the forces acting during the evisceration process by pulling the trachea without any cuts made. At the peak force value (about 350 N at T = 26 s), the trachea cracked, resulting in some oscillation and then a steep fall; thus, this value became the maximum payload for further mechanical calculations.</p>
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<p>Force limitation mode test—exemplary data. The target force value is incremented by 10 N and denoted by the vertical black lines. The solid lines indicate the clamping force on the target object placed between the two fingers, measured by the 4 sensors (L and R denote sensors of the left and right side fingers, respectively), and the dotted lines denote the angular positions. The unit of the left-side Y axis strongly correlates to Newtons; however, due to uncompensated non-linearity at higher forces, the use of standard units might not be accurate.</p>
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<p>Graph of the clamping force measured on the fingers, and angular position measurements when the target object is off-center. The object (a pig’s leg) is initially positioned to the right; hence, the right-side force values increase while the left-side values merely become noisy (due to the mechanical connection between the two sides). The black lines at the top of the graph (labeled “Asymmetry”) denote the time-points when the device detected asymmetry and triggered a real-time warning to the system. The unit of the left-side Y axis strongly correlates to Newtons; however, due to uncompensated non-linearity at higher forces, the use of standard units might not be accurate.</p>
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<p>New concept of robotic red meat processing—the Meat Factory Cell (MFC) from the RoBUTCHER consortium. Based on Mason et al. [<a href="#B32-sensors-24-04631" class="html-bibr">32</a>].</p>
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26 pages, 10151 KiB  
Article
Development, Experimental, and Numerical Characterisation of Novel Flexible Strain Sensors for Soft Robotics Applications
by Sylvester Ndidiamaka Nnadi, Ivor Ajadalu, Amir Rahmani, Aliyu Aliyu, Khaled Elgeneidy, Allahyar Montazeri and Behnaz Sohani
Robotics 2024, 13(7), 103; https://doi.org/10.3390/robotics13070103 - 11 Jul 2024
Viewed by 729
Abstract
Medical and agricultural robots that interact with living tissue or pick fruit require tactile and flexible sensors to minimise or eliminate damage. Until recently, research has focused on the development of robots made of rigid materials, such as metal or plastic. Due to [...] Read more.
Medical and agricultural robots that interact with living tissue or pick fruit require tactile and flexible sensors to minimise or eliminate damage. Until recently, research has focused on the development of robots made of rigid materials, such as metal or plastic. Due to their complex configuration, poor spatial adaptability and low flexibility, rigid robots are not fully applicable in some special environments such as limb rehabilitation, fragile objects gripping, human–machine interaction, and locomotion. All these should be done in an accurate and safe manner for them to be useful. However, the design and manufacture of soft robot parts that interact with living tissue or fragile objects is not as straightforward. Given that hyper-elasticity and conductivity are involved, conventional (subtractive) manufacturing can result in wasted materials (which are expensive), incompatible parts due to different physical properties, and high costs. In this work, additive manufacturing (3D printing) is used to produce a conductive, composite flexible sensor. Its electrical response was tested based on various physical conditions. Finite element analysis (FEA) was used to characterise its deformation and stress behaviour for optimisation to achieve functionality and durability. Also, a nonlinear regression model was developed for the sensor’s performance. Full article
(This article belongs to the Section Soft Robotics)
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<p>Design 2, two turns: (<b>a</b>) track width = 1.5 mm; height = 0.8 mm; track spacing = 1 mm; (<b>b</b>) track width = 1.5 mm; height = 1.2 mm; track spacing = 1 mm; (<b>c</b>) track width = 1.5 mm; height = 1.6 mm; track spacing = 1 mm; (<b>d</b>) track width = 1.5 mm; height = 2.0 mm; track spacing = 1 mm.</p>
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<p>(<b>a</b>) The fabrication and printing procedures for a flexible strain sensor; (<b>b</b>) 3D-printed flexible strain sensors with an industrial strain sensor for experiments [<a href="#B2-robotics-13-00103" class="html-bibr">2</a>].</p>
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<p>The 3D models of fixed curvature testing pieces for the experiment.</p>
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<p>(<b>a</b>) Circuit diagram of data acquisition circuit (DAQ) for experiments. (<b>b</b>) Sensor testing setup [<a href="#B22-robotics-13-00103" class="html-bibr">22</a>].</p>
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<p>(<b>a</b>) Circuit diagram of data acquisition circuit (DAQ) for experiments. (<b>b</b>) Sensor testing setup [<a href="#B22-robotics-13-00103" class="html-bibr">22</a>].</p>
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<p>Mesh convergence—maximum deformation vs. mesh elements.</p>
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<p>Showing simulation boundary limits: (<b>a</b>) fixed support and (<b>b</b>) applied force.</p>
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<p>All flexible strain sensor resistance measurements for (<b>a</b>) flat positions (<b>b</b>) 20 mm curvature.</p>
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<p>Signal conditioning and processing of time series data for the flexible strain sensors.</p>
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<p>Showing maximum deflections for one turn: (<b>a</b>) 0.8 mm; (<b>b</b>) 1.2 mm; (<b>c</b>) 1.6 mm; (<b>d</b>) 2.0 mm.</p>
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<p>Cross-plot of experimental and predicted dimensionless resistance analysis of the data.</p>
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<p>The novel strain sensors with the rehabilitation hand glove.</p>
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<p>Rehabilitation hand glove.</p>
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<p>Showing design 1, one turn: (<b>a</b>) track width = 2.5 mm; height = 0.8 mm; track spacing = 2 mm; (<b>b</b>) track width = 2.5 mm; height = 1.2 mm; track spacing = 2 mm; (<b>c</b>) track width = 2.5 mm; height = 0.8 mm; track spacing = 2 mm; (<b>d</b>) track width = 2.5 mm; height = 0.8 mm; track spacing = 2 mm.</p>
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<p>Showing design 3, three turns: (<b>a</b>) track width = 0.9 mm; height = 0.8 mm; track spacing = 0.9 mm; (<b>b</b>) track width = 0.9 mm; height = 1.2 mm; track spacing = 0.9 mm; (<b>c</b>) track width = 0.9 mm; height = 1.6 mm; track spacing = 0.9 mm; (<b>d</b>) track width = 0.9 mm; height = 2.0 mm; track spacing = 0.9 mm.</p>
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<p>All flexible strain sensors’ resistance measurements for (<b>a</b>) 40 mm curvature; (<b>b</b>) 60 mm curvature; and (<b>c</b>) 80 mm curvature.</p>
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<p>(<b>a</b>) Impacts of thickness, one turn, and curvatures on resistance. (<b>b</b>) Impacts of thickness, two turns, and curvatures on resistance. (<b>c</b>) Impacts of thickness, three turns, and curvatures on resistance.</p>
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<p>Impacts of curvatures on resistance of the industrial sensor.</p>
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<p>(<b>a</b>) SD as a percentage of the mean resistance of flexible strain sensors in turn one. (<b>b</b>) SD as a percentage of the mean resistance of flexible strain sensors in turn two. (<b>c</b>) SD as a percentage of the mean resistance of flexible strain sensors in turn three.</p>
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<p>Showing maximum deflections for two turns: (<b>a</b>) 0.8 mm; (<b>b</b>) 1.2 mm; (<b>c</b>) 1.6 mm; and (<b>d</b>) 2.0 mm.</p>
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<p>Showing maximum deformations for three turns: (<b>a</b>) 0.8 mm; (<b>b</b>) 1.2 mm; (<b>c</b>) 1.6 mm; and (<b>d</b>) 2.0 mm.</p>
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<p>Showing maximum equivalent stress for one turn: (<b>a</b>) 0.8 mm; (<b>b</b>) 1.2 mm; (<b>c</b>) 1.6 mm; and (<b>d</b>) 2.0 mm.</p>
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<p>Showing maximum equivalent stress for two turns: (<b>a</b>) 0.8 mm; (<b>b</b>) 1.2 mm; (<b>c</b>) 1.6 mm; and (<b>d</b>) 2.0 mm.</p>
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<p>Showing maximum equivalent stress for three turns: (<b>a</b>) 0.8 mm; (<b>b</b>) 1.2 mm; (<b>c</b>) 1.6 mm; and (<b>d</b>) 2.0 mm.</p>
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26 pages, 4851 KiB  
Article
Light-Fueled Self-Propulsion of Liquid Crystal Elastomer-Engined Automobiles in Zero-Energy Modes
by Zongsong Yuan, Yuntong Dai, Junxiu Liu and Kai Li
Mathematics 2024, 12(13), 2109; https://doi.org/10.3390/math12132109 - 4 Jul 2024
Viewed by 522
Abstract
The defining attribute of self-excited motion is its capability to extract energy from a stable environment and regulate it autonomously, making it an extremely promising innovation for microdevices, autonomous robotics, sensor technologies, and energy generation. Based on the concept of an automobile, we [...] Read more.
The defining attribute of self-excited motion is its capability to extract energy from a stable environment and regulate it autonomously, making it an extremely promising innovation for microdevices, autonomous robotics, sensor technologies, and energy generation. Based on the concept of an automobile, we propose a light-fueled self-propulsion of liquid crystal elastomer-engined automobiles in zero-energy mode. This system utilizes a wheel comprising a liquid crystal elastomer (LCE) turntable as an engine, a wheel with conventional material and a linkage. The dynamic behavior of the self-propulsion automobile under steady illumination is analyzed by integrating a nonlinear theoretical model with an established photothermally responsive LCE model. We performed the analysis using the fourth-order Runge–Kutta method. The numerical findings demonstrate the presence of two separate motion patterns in the automobile system: a static pattern and a self-propulsion pattern. The correlation between the energy input and energy dissipation from damping is essential to sustain the repetitive motion of the system. This study delves deeper into the crucial requirements for initiating self-propulsion and examines the effect of critical system parameters on the motion of the system. The proposed system with zero-energy mode motions has the advantage of a simple structural design, easy control, low friction and stable kinematics, and it is very promising for many future uses, including energy harvesting, monitoring, soft robotics, medical devices, and micro- and nano-devices. Full article
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<p>Self-propulsion automobile system based on LCE turntable. (<b>a</b>) Initial state; (<b>b</b>) enlarged view of the engine; (<b>c</b>) reference state; (<b>d</b>) current state; (<b>e</b>) force analysis of the wheels; (<b>f</b>) force analysis of the mass ball. The mass ball continuously enters the heating zone and moves outward under the tension of the LCE rope. This movement creates a torque difference that allows the system to maintain a cyclic motion.</p>
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<p>Time courses and phase trajectories of the LCE turntable-engined automobile system. (<b>a</b>,<b>b</b>) Static pattern with parameters of <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>T</mi> <mo>¯</mo> </mover> <mn>0</mn> </msub> <mo>=</mo> <mn>0</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>θ</mi> <mn>0</mn> </msub> <mo>=</mo> <mn>0.5</mn> <mi>π</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>α</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.3</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>g</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>β</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>R</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>2.5</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>k</mi> <mo>¯</mo> </mover> <mi>l</mi> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>k</mi> <mo>¯</mo> </mover> <mi>s</mi> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>θ</mi> <mo>=</mo> <mn>0.25</mn> <mi>π</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>δ</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>w</mi> <mo>¯</mo> </mover> <mn>0</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>. (<b>c</b>,<b>d</b>) Self-propulsion pattern with parameters of <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>T</mi> <mo>¯</mo> </mover> <mn>0</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>θ</mi> <mn>0</mn> </msub> <mo>=</mo> <mn>0.5</mn> <mi>π</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>α</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.3</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>g</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>β</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>R</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>2.5</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>k</mi> <mo>¯</mo> </mover> <mi>l</mi> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>k</mi> <mo>¯</mo> </mover> <mi>s</mi> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>θ</mi> <mo>=</mo> <mn>0.25</mn> <mi>π</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>δ</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>w</mi> <mo>¯</mo> </mover> <mn>0</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>. The LCE turntable-engined automobile system involves two motion patterns under steady illumination, namely, static pattern and self-propulsion pattern.</p>
Full article ">Figure 3
<p>(<b>a</b>) Driving torque as a function of rotation angle; (<b>b</b>) damping torque as a function of rotation angle; (<b>c</b>) time dependence of LCE rope length; (<b>d</b>) time dependence of self-propulsion speed; (<b>e</b>) time dependence of tension of LCE rope; (<b>f</b>) tension of LCE rope as a function of rotation angle.</p>
Full article ">Figure 4
<p>Self-propulsion of the automobile system over a one cycle under the conditions of <a href="#mathematics-12-02109-f002" class="html-fig">Figure 2</a>c,d. Under steady illumination, the automobile system will exhibit continuous forward self-propulsion.</p>
Full article ">Figure 5
<p>Phase diagram of LCE turntable-engined automobile with respect to limit temperature <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>T</mi> <mo>¯</mo> </mover> <mn>0</mn> </msub> </mrow> </semantics></math> and thermal contraction coefficient <math display="inline"><semantics> <mover accent="true"> <mi>α</mi> <mo>¯</mo> </mover> </semantics></math> for <math display="inline"><semantics> <mrow> <msub> <mi>θ</mi> <mn>0</mn> </msub> <mo>=</mo> <mn>0.5</mn> <mi>π</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>g</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>β</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>R</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>2.5</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>k</mi> <mo>¯</mo> </mover> <mi>l</mi> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>k</mi> <mo>¯</mo> </mover> <mi>s</mi> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>θ</mi> <mo>=</mo> <mn>0.25</mn> <mi>π</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>δ</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>w</mi> <mo>¯</mo> </mover> <mn>0</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>. When the combination of limit temperature <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>T</mi> <mo>¯</mo> </mover> <mn>0</mn> </msub> </mrow> </semantics></math> and thermal contraction coefficient <math display="inline"><semantics> <mover accent="true"> <mi>α</mi> <mo>¯</mo> </mover> </semantics></math> is in the shaded region, the automobile can self-propel in a periodic and continuous fashion; otherwise, it remains static.</p>
Full article ">Figure 6
<p>Effect of gravitational acceleration <math display="inline"><semantics> <mover accent="true"> <mi>g</mi> <mo>¯</mo> </mover> </semantics></math> on the self-propulsion of the system, with <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>T</mi> <mo>¯</mo> </mover> <mn>0</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>θ</mi> <mn>0</mn> </msub> <mo>=</mo> <mn>0.5</mn> <mi>π</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>α</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.3</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>β</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>R</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>2.5</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>k</mi> <mo>¯</mo> </mover> <mi>l</mi> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>k</mi> <mo>¯</mo> </mover> <mi>s</mi> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>δ</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>θ</mi> <mo>=</mo> <mn>0.25</mn> <mi>π</mi> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>w</mi> <mo>¯</mo> </mover> <mn>0</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>. (<b>a</b>) Limit cycles; (<b>b</b>) self-propulsion speed and mass ball amplitude.</p>
Full article ">Figure 7
<p>Effect of limit temperature <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>T</mi> <mo>¯</mo> </mover> <mn>0</mn> </msub> </mrow> </semantics></math> on the self-propulsion of the system, with <math display="inline"><semantics> <mrow> <msub> <mi>θ</mi> <mn>0</mn> </msub> <mo>=</mo> <mn>0.5</mn> <mi>π</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>α</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.3</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>g</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>δ</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>R</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>2.5</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>k</mi> <mo>¯</mo> </mover> <mi>l</mi> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>k</mi> <mo>¯</mo> </mover> <mi>s</mi> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>δ</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.001</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>θ</mi> <mo>=</mo> <mn>0.25</mn> <mi>π</mi> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>w</mi> <mo>¯</mo> </mover> <mn>0</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>. (<b>a</b>) Limit cycles; (<b>b</b>) self-propulsion speed and mass ball amplitude.</p>
Full article ">Figure 8
<p>Effect of thermal contraction coefficient <math display="inline"><semantics> <mover accent="true"> <mi>α</mi> <mo>¯</mo> </mover> </semantics></math> on the self-propulsion of the system, with <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>T</mi> <mo>¯</mo> </mover> <mn>0</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>θ</mi> <mn>0</mn> </msub> <mo>=</mo> <mn>0.5</mn> <mi>π</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>g</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>β</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>R</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>2.5</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>k</mi> <mo>¯</mo> </mover> <mi>l</mi> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>k</mi> <mo>¯</mo> </mover> <mi>s</mi> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>θ</mi> <mo>=</mo> <mn>0.25</mn> <mi>π</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>δ</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math> and <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>w</mi> <mo>¯</mo> </mover> <mn>0</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>. (<b>a</b>) Limit cycles; (<b>b</b>) self-propulsion speed and mass ball amplitude.</p>
Full article ">Figure 9
<p>Effect of LCE turntable radius <math display="inline"><semantics> <mover accent="true"> <mi>R</mi> <mo>¯</mo> </mover> </semantics></math> on the self-propulsion of the system, with <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>T</mi> <mo>¯</mo> </mover> <mn>0</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>θ</mi> <mn>0</mn> </msub> <mo>=</mo> <mn>0.5</mn> <mi>π</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>α</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.3</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>g</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>β</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>k</mi> <mo>¯</mo> </mover> <mi>l</mi> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>k</mi> <mo>¯</mo> </mover> <mi>s</mi> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>δ</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>θ</mi> <mo>=</mo> <mn>0.25</mn> <mi>π</mi> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>w</mi> <mo>¯</mo> </mover> <mn>0</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>. (<b>a</b>) Limit cycles; (<b>b</b>) self-propulsion speed and mass ball amplitude.</p>
Full article ">Figure 10
<p>Effect of damping factor <math display="inline"><semantics> <mover accent="true"> <mi>β</mi> <mo>¯</mo> </mover> </semantics></math> on the self-propulsion of the system, with <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>T</mi> <mo>¯</mo> </mover> <mn>0</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>θ</mi> <mn>0</mn> </msub> <mo>=</mo> <mn>0.5</mn> <mi>π</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>α</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.3</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>g</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>R</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>2.5</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>k</mi> <mo>¯</mo> </mover> <mi>l</mi> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>k</mi> <mo>¯</mo> </mover> <mi>s</mi> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>δ</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>θ</mi> <mo>=</mo> <mn>0.25</mn> <mi>π</mi> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>w</mi> <mo>¯</mo> </mover> <mn>0</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>. (<b>a</b>) Limit cycles; (<b>b</b>) self-propulsion speed and mass ball amplitude.</p>
Full article ">Figure 11
<p>Effect of rolling resistance coefficient <math display="inline"><semantics> <mover accent="true"> <mi>δ</mi> <mo>¯</mo> </mover> </semantics></math> on the self-propulsion of the system, with <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>T</mi> <mo>¯</mo> </mover> <mn>0</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>θ</mi> <mn>0</mn> </msub> <mo>=</mo> <mn>0.5</mn> <mi>π</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>α</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.3</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>g</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>β</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>R</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>2.5</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>k</mi> <mo>¯</mo> </mover> <mi>l</mi> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>k</mi> <mo>¯</mo> </mover> <mi>s</mi> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>θ</mi> <mo>=</mo> <mn>0.25</mn> <mi>π</mi> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>w</mi> <mo>¯</mo> </mover> <mn>0</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>. (<b>a</b>) Limit cycles; (<b>b</b>) self-propulsion speed and mass ball amplitude.</p>
Full article ">Figure 12
<p>Effect of elastic stiffness <math display="inline"><semantics> <msub> <mover accent="true"> <mi>k</mi> <mo>¯</mo> </mover> <mi>l</mi> </msub> </semantics></math> of LCE rope on the self-propulsion of the system, with <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>T</mi> <mo>¯</mo> </mover> <mn>0</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>θ</mi> <mn>0</mn> </msub> <mo>=</mo> <mn>0.5</mn> <mi>π</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>α</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.3</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>g</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>β</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>R</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>2.5</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>k</mi> <mo>¯</mo> </mover> <mi>s</mi> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>δ</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>θ</mi> <mo>=</mo> <mn>0.25</mn> <mi>π</mi> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>w</mi> <mo>¯</mo> </mover> <mn>0</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>. (<b>a</b>) Limit cycles; (<b>b</b>) self-propulsion speed and mass ball amplitude.</p>
Full article ">Figure 13
<p>Effect of elastic stiffness <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>k</mi> <mo>¯</mo> </mover> <mi>s</mi> </msub> </mrow> </semantics></math> of spring on the self-propulsion of the system, with <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>T</mi> <mo>¯</mo> </mover> <mn>0</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mi>θ</mi> <mn>0</mn> </msub> <mo>=</mo> <mn>0.5</mn> <mi>π</mi> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>α</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.3</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>g</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>β</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>R</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>2.5</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>k</mi> <mo>¯</mo> </mover> <mi>l</mi> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>δ</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>θ</mi> <mo>=</mo> <mn>0.25</mn> <mi>π</mi> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>w</mi> <mo>¯</mo> </mover> <mn>0</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>. (<b>a</b>) Limit cycles; (<b>b</b>) self-propulsion speed and mass ball amplitude.</p>
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<p>Effect of illumination zone angle <math display="inline"><semantics> <mrow> <msub> <mi>θ</mi> <mn>0</mn> </msub> </mrow> </semantics></math> on the self-propulsion of the system, with <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>T</mi> <mo>¯</mo> </mover> <mn>0</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>α</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.3</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>g</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>β</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>R</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>2.5</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>k</mi> <mo>¯</mo> </mover> <mi>l</mi> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>k</mi> <mo>¯</mo> </mover> <mi>s</mi> </msub> <mo>=</mo> <mn>10</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mover accent="true"> <mi>δ</mi> <mo>¯</mo> </mover> <mo>=</mo> <mn>0.01</mn> </mrow> </semantics></math>, <math display="inline"><semantics> <mrow> <mi>θ</mi> <mo>=</mo> <mn>0.25</mn> <mi>π</mi> </mrow> </semantics></math>, and <math display="inline"><semantics> <mrow> <msub> <mover accent="true"> <mi>w</mi> <mo>¯</mo> </mover> <mn>0</mn> </msub> <mo>=</mo> <mn>1</mn> </mrow> </semantics></math>. (<b>a</b>) Limit cycles; (<b>b</b>) self-propulsion speed and mass ball amplitude.</p>
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13 pages, 5334 KiB  
Article
Enhanced Dendrite Resistance in Reversible Electrochemical Pneumatic Batteries with Nanoimprinted Nanowire Anodes for Jamming Robots
by Junyu Ge, Yuchen Zhao, Yifan Wang and Hong Li
Batteries 2024, 10(7), 225; https://doi.org/10.3390/batteries10070225 - 24 Jun 2024
Viewed by 647
Abstract
Traditional electric robots often rely on heavy gear units or expensive force–torque sensors, whereas pneumatic robots offer a cost-effective and simple alternative. However, their dependence on noisy and bulky pneumatic systems, such as compressed air technology, limits their portability and adaptability. To overcome [...] Read more.
Traditional electric robots often rely on heavy gear units or expensive force–torque sensors, whereas pneumatic robots offer a cost-effective and simple alternative. However, their dependence on noisy and bulky pneumatic systems, such as compressed air technology, limits their portability and adaptability. To overcome these challenges, we have developed a reversible electrochemical pneumatic battery (REPB) that is compact, noise-free, energy-efficient, and portable. This innovative REPB, principled by the electrochemical redox reactions of zinc–air batteries, can simultaneously supply both electric and pneumatic power, either positive or negative pressure. Its modular, multi-stack structure allows for the easy customization of power output and capacity to suit various applications. We demonstrate the utility of REPB through its application in jamming robots, such as a novel soft yet robust gripper that merges the strengths of hard and soft grippers, enabling universal robotic gripping. This work presents a groundbreaking approach to powering devices that require pneumatic support. Full article
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<p>Schematic of Zn nanowire fabrication. (<b>a</b>) Prepared template and Zn foil. (<b>b</b>) Ultrasonic nanoimprinting process. (<b>c</b>) Assembly after nanoimprinting. (<b>d</b>) Fabricated Zn nanowire electrode.</p>
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<p>Schematic of prototype designed for reversible electrochemical pneumatic battery.</p>
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<p>Design and fabrication of gripper’s main components. (<b>a</b>) Three-dimensional-printed structured fabrics. (<b>b</b>) Fabricated palm-shaped variable-stiffness gripper.</p>
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<p>Schematic of zinc–air battery.</p>
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<p>Discharge measurements of Zn foil and Zn nanowires.</p>
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<p>Cycling measurements of Zn foil and Zn nanowires.</p>
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<p>SEM images of Zn foil and Zn nanowires before and after reaction. (<b>a</b>,<b>b</b>) Zn foil before and after cycling measurements. Scale bars of (<b>a</b>,<b>b</b>) are 10 μm. (<b>c</b>,<b>d</b>) Zn nanowires before and after cycling measurements. Scale bars of (<b>c</b>,<b>d</b>) are 1 μm.</p>
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<p>XPS spectra of O1s region for Zn foil and Zn nanowire samples after reaction. In this figure, the red line represents the peak related to ZnO, the blue line represents the peak related to Zn(OH)<sub>2</sub>, the green line is the fitted result, and the grey line is the measured result.</p>
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<p>The LSV spectra of the Zn foil and Zn nanowire samples after 150 cycles.</p>
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<p>Relationship between pressure and time under different gas volumes.</p>
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<p>The REPB connected to a palm-shaped variable stiffness gripper. (<b>a</b>) The gas connection system between the REPB and the gripper. (<b>b</b>) The gripper grasping an object.</p>
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23 pages, 4827 KiB  
Article
Motion Coordination of Multiple Autonomous Mobile Robots under Hard and Soft Constraints
by Spyridon Anogiatis, Panagiotis S. Trakas and Charalampos P. Bechlioulis
Electronics 2024, 13(11), 2128; https://doi.org/10.3390/electronics13112128 - 29 May 2024
Cited by 1 | Viewed by 619
Abstract
This paper presents a distributed approach to the motion control problem for a platoon of unicycle robots moving through an unknown environment filled with static obstacles under multiple hard and soft operational constraints. Each robot has an onboard camera to determine its relative [...] Read more.
This paper presents a distributed approach to the motion control problem for a platoon of unicycle robots moving through an unknown environment filled with static obstacles under multiple hard and soft operational constraints. Each robot has an onboard camera to determine its relative position in relation to its predecessor and proximity sensors to detect and avoid nearby obstascles. Moreover, no robot apart from the leader can independently localize itself within the given workspace. To overcome this limitation, we propose a novel distributed control protocol for each robot of the fleet, utilizing the Adaptive Performance Control (APC) methodology. By utilizing the APC approach to address input constraints via the on-line modification of the error specifications, we ensure that each follower effectively tracks its predecessor without encountering collisions with obstacles, while simultaneously maintaining visual contact with its preceding robot, thus ensuring the inter-robot visual connectivity. Finally, extensive simulation results are presented to demonstrate the effectiveness of the presented control system along with a real-time experiment conducted on an actual robotic system to validate the feasibility of the proposed approach in real-world scenarios. Full article
(This article belongs to the Special Issue Path Planning for Mobile Robots, 2nd Edition)
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<p>Robot <math display="inline"><semantics> <msub> <mi mathvariant="script">R</mi> <mi>i</mi> </msub> </semantics></math> tracking its predecessor <math display="inline"><semantics> <mrow> <msub> <mi mathvariant="script">R</mi> <mrow> <mi>i</mi> <mo>−</mo> <mn>1</mn> </mrow> </msub> <mo>.</mo> </mrow> </semantics></math></p>
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<p>Saturation function to address diamond-shaped constraints; <math display="inline"><semantics> <msub> <mi>u</mi> <mi>d</mi> </msub> </semantics></math> denotes the desired control input and <math display="inline"><semantics> <mrow> <mi>σ</mi> <mo>(</mo> <msub> <mi>u</mi> <mi>d</mi> </msub> <mo>)</mo> </mrow> </semantics></math> denotes the feasible, constrained, control input based on the radial distance of <math display="inline"><semantics> <msub> <mi>u</mi> <mi>d</mi> </msub> </semantics></math> from the origin.</p>
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<p>Algorithm Flowchart describing the proposed control approach (<a href="#FD8-electronics-13-02128" class="html-disp-formula">8</a>)–(<a href="#FD30-electronics-13-02128" class="html-disp-formula">30</a>).</p>
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<p>Consecutive snapshots of the robot fleet (the red circle is the leader while the cyan ones are the followers) navigating through the given workspace. Each camera’s field of view is given by the black-colored quadrant.</p>
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<p>Consecutive snapshots of the robot fleet (the red circle is the leader while the cyan ones are the followers) navigating through the given workspace. Each camera’s field of view is given by the black-colored quadrant.</p>
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<p>Distance and angle of view error response of each robot follower agent along with their dedicated performance function boundaries; red line is the upper bound, blue line is the lower bound and black line is the respected error.</p>
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<p>Linear and angular (desired (blue) and actual (red)) velocities of each robot.</p>
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<p>The trajectories of each robot on the simulated mapped workspace.</p>
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<p>Distance and Angle of View error response during the simulation in Gazebo; red line depicts the upper bound of each respected error, blue line is the lower bound and black line signifies the error.</p>
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<p>Linear and angular desired and actual velocities for each robot agent during the simulation in Gazebo; red line is the actual saturated velocity while blue is the corresponding desired velocity.</p>
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<p>Real World Experiment workspace along with robots.</p>
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<p>Error response of inter-robot distance and angle of view for the real world experiment; red line depicts the upper adaptive performance bound, while blue line is the lower adaptive performance and black line denote the respected errors.</p>
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<p>Linear and Angular Commanded Velocities given during the real-world experiment in the Laboratory. Red are the actual saturated velocities proposed in this paper while blue the desired velocities.</p>
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