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15 pages, 6315 KiB  
Article
Effect of Various Nanofillers on Piezoelectric Nanogenerator Performance of P(VDF-TrFE) Nanocomposite Thin Film
by Sangkwon Park and Hafiz Muhammad Abid Yaseen
Nanomaterials 2025, 15(5), 403; https://doi.org/10.3390/nano15050403 - 6 Mar 2025
Viewed by 242
Abstract
Flexible polymer-based piezoelectric nanogenerators (PENGs) have gained significant interest due to their ability to deliver clean and sustainable energy for self-powered electronics and wearable devices. Recently, the incorporation of fillers into the ferroelectric polymer matrix has been used to improve the relatively low [...] Read more.
Flexible polymer-based piezoelectric nanogenerators (PENGs) have gained significant interest due to their ability to deliver clean and sustainable energy for self-powered electronics and wearable devices. Recently, the incorporation of fillers into the ferroelectric polymer matrix has been used to improve the relatively low piezoelectric properties of polymer-based PENGs. In this study, we investigated the effect of various nanofillers such as titania (TiO2), zinc oxide (ZnO), reduced graphene oxide (rGO), and lead zirconate titanate (PZT) on the PENG performance of the nanocomposite thin films containing the nanofillers in poly(vinylidene fluoride-co-trifluoro ethylene) (P(VDF-TrFE)) matrix. The nanocomposite films were prepared by depositing molecularly thin films of P(VDF-TrFE) and nanofiller nanoparticles (NPs) spread at the air/water interface onto the indium tin oxide-coated polyethylene terephthalate (ITO-PET) substrate, and they were characterized by measuring their microstructures, crystallinity, β-phase contents, and piezoelectric coefficients (d33) using SEM, FT-IR, XRD, and quasi-static meter, respectively. Multiple PENGs incorporating various nanofillers within the polymer matrix were developed by assembling thin film-coated substrates into a sandwich-like structure. Their piezoelectric properties, such as open-circuit output voltage (VOC) and short-circuit current (ISC), were analyzed. As a result, the PENG containing 4 wt% PZT, which was named P-PZT-4, showed the best performance of VOC of 68.5 V with the d33 value of 78.2 pC/N and β-phase content of 97%. The order of the maximum VOC values for the PENGs of nanocomposite thin films containing various nanofillers was PZT (68.5 V) > rGO (64.0 V) > ZnO (50.9 V) > TiO2 (48.1 V). When the best optimum PENG was integrated into a simple circuit comprising rectifiers and a capacitor, it demonstrated an excellent two-dimensional power density of 20.6 μW/cm2 and an energy storage capacity of 531.4 μJ within 3 min. This piezoelectric performance of PENG with the optimized nanofiller type and content was found to be superior when it was compared with those in the literature. This PENG comprising nanocomposite thin film with optimized nanofiller type and content shows a potential application for a power source for low-powered electronics such as wearable devices. Full article
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Figure 1
<p>Illustration of preparation procedure of nanocomposite LS film and their PENG device.</p>
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<p>SEM micrographs of nanocomposite LS thin films of (<b>a</b>) P, (<b>b</b>) P-TiO<sub>2</sub>-4, (<b>c</b>) P-TiO<sub>2</sub>-40, (<b>d</b>) P-ZnO-2, (<b>e</b>) P-ZnO-20, (<b>f</b>) P-ZnO-40, (<b>g</b>) P-PZT-2, (<b>h</b>) P-PZT-20, and (<b>i</b>) P-PZT-40 with 50 μm scale bars.</p>
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<p>XRD patterns, FT-IR spectra, crystallinity, and β-phase content profiles as a function of nanofiller content for the nanocomposite thin films of (<b>a</b>–<b>c</b>) P-TiO<sub>2</sub>, (<b>d</b>–<b>f</b>) P-ZnO, (<b>g</b>–<b>i</b>) P-rGO, and (<b>j</b>–<b>l</b>) P-PZT series.</p>
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<p>Piezoelectric coefficient (<span class="html-italic">d</span><sub>33</sub>) values as a function of nanofiller content for the nanocomposite thin films of (<b>a</b>) P-TiO<sub>2</sub>, (<b>b</b>) P-ZnO, (<b>c</b>) P-rGO, and (<b>d</b>) P-PZT series.</p>
Full article ">Figure 5
<p><span class="html-italic">V<sub>OC</sub></span> signals of PENG devices and maximum peak-to-peak <span class="html-italic">V<sub>OC</sub></span> values as a function of nanofiller content for the nanocomposite thin films of (<b>a</b>,<b>b</b>) P-TiO<sub>2</sub>, (<b>c</b>,<b>d</b>) P-ZnO, (<b>e</b>,<b>f</b>) P-rGO, and (<b>g</b>,<b>h</b>) P-PZT series.</p>
Full article ">Figure 5 Cont.
<p><span class="html-italic">V<sub>OC</sub></span> signals of PENG devices and maximum peak-to-peak <span class="html-italic">V<sub>OC</sub></span> values as a function of nanofiller content for the nanocomposite thin films of (<b>a</b>,<b>b</b>) P-TiO<sub>2</sub>, (<b>c</b>,<b>d</b>) P-ZnO, (<b>e</b>,<b>f</b>) P-rGO, and (<b>g</b>,<b>h</b>) P-PZT series.</p>
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<p>(<b>a</b>) The maximum <span class="html-italic">V<sub>OC</sub></span> values for different optimum PENGs containing different nanofillers (with the surface pressure of 5 mN/m), (<b>b</b>) <span class="html-italic">I<sub>SC</sub></span> signals for the PZT PENGs as a function of nanofiller content, and (<b>c</b>) stability of the optimized PZT-based PENG for 1000 s.</p>
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<p>(<b>a</b>) Potential profiles and (<b>b</b>) energy storage values for the optimal PENG of thin film containing 4 wt% PZT with different capacitors.</p>
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16 pages, 2591 KiB  
Article
Carbon Dioxide Selectivity over Ethane in Promising Bis Tri (Fluoromethylsulfonyl) Imide-Based Ionic Liquids
by Eric Quaye, Amr Henni and Ezeddin Shirif
Molecules 2025, 30(5), 984; https://doi.org/10.3390/molecules30050984 - 20 Feb 2025
Viewed by 231
Abstract
This research addresses the critical challenge of CO2 capture by exploring innovative ways to avoid ethane (C2H6) co-absorption in natural gas sweetening operations. The solubility of Ethane (C2H6) was measured in three ionic liquids [...] Read more.
This research addresses the critical challenge of CO2 capture by exploring innovative ways to avoid ethane (C2H6) co-absorption in natural gas sweetening operations. The solubility of Ethane (C2H6) was measured in three ionic liquids (ILs) with similar anions, 1-decyl-3-methyl imidazolium bis (trifluoro methylsulfonyl imide) [IL-1], 1-hexadecyl-3-methylimidazolium bis (trifluoro methylsulfonyl imide) [IL-2], and triethytetra-decyl ammonium bis (trifluoromethylsulfonyl imide) [IL-3]. The solubility experiments were investigated at 303.15 K and 343.15 K with pressures reaching 1.2 MPa. Among the ILs, [IL-2] exhibited the highest ethane absorption capacity due to its extended alkyl chain. The Peng-Robinson equation of state (PR-EoS) and three (3) distinct mixing rules provided robust correlations for the solubility data. Results demonstrate the inferior performance of [IL-1], [IL-2], and [IL-3] compared to Selexol/Genosorb 1753. The selectivity of Ethane (C2H6) over CO2 was determined, with the overall selectivity ranking as follows: [IL-1] > [IL-3] > [IL-2]. A comparison of these selectivity values with published IL data indicated that these three ILs are most effective when used in applications targeting CO2 capture in the absence of Ethane (C2H6), such as in the case of flue gas. They will most probably be used with an amine blend. Additionally, the Enthalpy and entropy of absorption provided valuable insights, demonstrating Ethane’s weaker interactions and lower solubility than CO2. These findings emphasize the critical role of IL structure in determining ethane solubility and highlight the potential of customized ILs for optimizing gas-separation processes. Full article
(This article belongs to the Section Molecular Liquids)
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<p>Ethane validation test with Florusse et al. [<a href="#B8-molecules-30-00984" class="html-bibr">8</a>] and Henni et al. [<a href="#B9-molecules-30-00984" class="html-bibr">9</a>] at 323.15 K.</p>
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<p>(<b>a</b>) C<sub>2</sub>H<sub>6</sub> absorption in IL-1; (<b>b</b>) C<sub>2</sub>H<sub>6</sub> absorption in IL-2; (<b>c</b>) C<sub>2</sub>H<sub>6</sub> solubility in IL-3.</p>
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<p>Henry’s Gas law constant (H) comparison for C<sub>2</sub>H<sub>6</sub> absorption between ILs in this study versus published ILs [<a href="#B9-molecules-30-00984" class="html-bibr">9</a>,<a href="#B12-molecules-30-00984" class="html-bibr">12</a>] and Selexol/Genesorb 1753 [<a href="#B10-molecules-30-00984" class="html-bibr">10</a>] at (<b>a</b>) 323.15 K and (<b>b</b>) 343.15 K.</p>
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<p>(<b>a</b>) Comparison to CO<sub>2</sub>/C<sub>2</sub>H<sub>6</sub> selectivity data for ILs published by Nath and Henni et al. [<a href="#B12-molecules-30-00984" class="html-bibr">12</a>] and Rayer al. [<a href="#B10-molecules-30-00984" class="html-bibr">10</a>] at 323 K; (<b>b</b>) at 343.15 K.</p>
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<p>Densities of the ILs used in this work.</p>
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24 pages, 7558 KiB  
Review
Graphene-Enhanced Piezoelectric Nanogenerators for Efficient Energy Harvesting
by Joydip Sengupta and Chaudhery Mustansar Hussain
C 2025, 11(1), 3; https://doi.org/10.3390/c11010003 - 1 Jan 2025
Viewed by 951
Abstract
Graphene-based piezoelectric nanogenerators (PENGs) have emerged as a promising technology for sustainable energy harvesting, offering significant potential in powering next-generation electronic devices. This review explores the integration of graphene, a highly conductive and mechanically robust two-dimensional (2D) material, with PENG to enhance their [...] Read more.
Graphene-based piezoelectric nanogenerators (PENGs) have emerged as a promising technology for sustainable energy harvesting, offering significant potential in powering next-generation electronic devices. This review explores the integration of graphene, a highly conductive and mechanically robust two-dimensional (2D) material, with PENG to enhance their energy conversion efficiency. Graphene’s unique properties, including its exceptional electron mobility, high mechanical strength, and flexibility, allow for the development of nanogenerators with superior performance compared to conventional PENGs. When combined with piezoelectric materials, polymers, graphene serves as both an active layer and a charge transport medium, boosting the piezoelectric response and output power. The graphene-based PENGs can harvest mechanical energy from various sources, including vibrations, human motion, and ambient environmental forces, making them ideal for applications in wearable electronics, and low-power devices. This paper provides an overview of the fabrication techniques, material properties, and energy conversion mechanisms of graphene-based PENGs, and integration into real-world applications. The findings demonstrate that the incorporation of graphene enhances the performance of PENG, paving the way for future innovations in energy-harvesting technologies. Full article
(This article belongs to the Special Issue New Advances in Graphene Synthesis and Applications)
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Graphical abstract

Graphical abstract
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<p>Graphene and its derivatives (reproduced with permission from [<a href="#B13-carbon-11-00003" class="html-bibr">13</a>]).</p>
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<p>Different methods of graphene synthesis (reproduced with permission from [<a href="#B26-carbon-11-00003" class="html-bibr">26</a>]).</p>
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<p>Diagrammatic representations of energy harvesters utilizing (<b>a</b>) the piezoelectric effect, (<b>b</b>) the triboelectric effect, (<b>c</b>) the thermoelectric effect, and (<b>d</b>) the pyroelectric effect (reproduced with permission from [<a href="#B46-carbon-11-00003" class="html-bibr">46</a>]).</p>
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<p>Schematic diagram and operating mechanism of tri-layer piezoelectric nanogenerator (reproduced with permission from [<a href="#B91-carbon-11-00003" class="html-bibr">91</a>]).</p>
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<p>(Clockwise from top left) The original photo of the flexible transparent ZnSi<sub>2</sub>O<sub>4</sub>–graphene–piezoelectric nanogenerator device, schematic of the tetragonal crystal structure of Zn<sub>2</sub>SiO<sub>4</sub> nanorods, SEM image of as-grown Zn<sub>2</sub>SiO<sub>4</sub>, piezoelectric output voltage generated from the transparent and flexible nanogenerator under various pressures under forward connection, schematic diagram of the graphene–ZnSi<sub>2</sub>O<sub>4</sub> piezoelectric device (reproduced with permission from [<a href="#B92-carbon-11-00003" class="html-bibr">92</a>]).</p>
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<p>Voltage output generated from (<b>a</b>) finger tapping, (<b>b</b>) finger bending, (<b>c</b>) heel stepping, (<b>d</b>) toe stepping, and (<b>e</b>) knee bending is illustrated, with the inset depicting each motion during energy harvesting. (<b>f</b>) The durability and stability of the piezoelectric nanogenerator (PENG) were evaluated at a frequency of 5 Hz and a strain of 6 N after 1000 and 5000 cycles, followed by an additional two weeks of testing. (<b>g</b>) A full-bridge rectifier circuit was implemented to illuminate the LEDs, as shown in the accompanying photo displaying the circuit connections and the LEDs powered by the PENG. (<b>h</b>) The charging behavior of the 2.2 μF capacitor is also presented (reproduced with permission from [<a href="#B93-carbon-11-00003" class="html-bibr">93</a>]).</p>
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<p>(<b>a</b>) The schematic of the nanogenerator fabrication process. (<b>i</b>) The pristine PU sponge. (<b>ii</b>) The PU sponge coated with GO on both internal and external surfaces. (<b>iii</b>) GO reduced using L-AA to form RGO, with a bottom electrode affixed. (<b>iv</b>) Growth of ZnO nanowires on the RGO surface. (<b>v</b>) A thin sputtered Au layer is applied on top of the sample, along with an attachment of the top electrode. (<b>vi</b>) PDMS is infused within the pores of the nanogenerator structure. Insets in <a href="#carbon-11-00003-f007" class="html-fig">Figure 7</a> depict the microstructure at each stage. (<b>b</b>) A photograph of the fully assembled nanogenerator (reproduced with permission from [<a href="#B94-carbon-11-00003" class="html-bibr">94</a>]).</p>
Full article ">Figure 8
<p>Sensing features of the device include (<b>a</b>) finger tapping, (<b>b</b>) walking and jogging, (<b>c</b>) finger bending, and (<b>d</b>) LED activation (reproduced with permission from [<a href="#B96-carbon-11-00003" class="html-bibr">96</a>]).</p>
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<p>(<b>a</b>) Piezoelectric output voltage, (<b>b</b>) output current from the GQDs/PVDF-HFP composite device under vertical compressive force in forward connection, (<b>c</b>) piezoelectric output voltage response during hand/wrist movements, and (<b>d</b>) output voltage generated under breathing conditions (reproduced with permission from [<a href="#B97-carbon-11-00003" class="html-bibr">97</a>]).</p>
Full article ">Scheme 1
<p>A schematic representation illustrating the potential of graphene in nanogenerator (NG) fabrication.</p>
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14 pages, 1879 KiB  
Article
Evaluation of Machine Learning Applications for the Complex Near-Critical Phase Behavior Modelling of CO2–Hydrocarbon Systems
by Daulet Magzymov, Meruyert Makhatova, Zhasulan Dairov and Murat Syzdykov
Appl. Sci. 2024, 14(23), 11140; https://doi.org/10.3390/app142311140 - 29 Nov 2024
Cited by 1 | Viewed by 606
Abstract
The objective of this study was to evaluate the capability of machine learning models to accurately predict complex near-critical phase behavior in CO2–hydrocarbon systems, which are crucial for enhanced oil recovery and carbon storage applications. We compared the physical Peng–Robinson equation [...] Read more.
The objective of this study was to evaluate the capability of machine learning models to accurately predict complex near-critical phase behavior in CO2–hydrocarbon systems, which are crucial for enhanced oil recovery and carbon storage applications. We compared the physical Peng–Robinson equation of state model to machine learning algorithms under varying temperatures, pressures, and composition, including challenging near-critical scenarios. We used a direct neural network model and two hybrid model approaches to capture physical behavior in comprehensive compositional space. While all the models showed great performance during training and validation, the Direct Model exhibited unphysical behavior in compositional space, such as fluctuations in equilibrium constants and tie-line crossing. Hybrid Model 1, integrating a single Rachford–Rice iteration for physical constraints, showed an improved consistency in phase predictions. Hybrid Model 2, utilizing logarithmic transformations to better handle nonlinearities in equilibrium constants, further enhanced the accuracy and provided smoother predictions, particularly in the near-critical region. Overall, the hybrid models demonstrated a superior ability to balance computational efficiency and physical accuracy, closely aligning with the reference of the Peng–Robinson equation of state. This study highlights the importance of incorporating physical constraints into machine learning models for reliable phase behavior predictions, especially under near-critical conditions. Full article
(This article belongs to the Special Issue Advanced Drilling, Cementing, and Oil Recovery Technologies)
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Figure 1
<p>Model scenarios: (<b>a</b>) Direct Model, (<b>b</b>) Hybrid Model 1, and (<b>c</b>) Hybrid Model 2.</p>
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<p>Reference case generated using Peng–Robinson equation of state: (<b>a</b>) near-critical conditions of 80 atm and 60 °C; and (<b>b</b>) regular conditions of 75 atm and 60 °C.</p>
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<p>Machine learning (neural network) training, validation, and testing using 4000 flash calculation samples (pressure [80 atm to 40 atm], temperature [57 °C to 67 °C], and overall composition of CO<sub>2</sub>-C4-C10 [0 to 1]) for (<b>a</b>) Direct Model, (<b>b</b>) Hybrid Model 1, and (<b>c</b>) Hybrid Model 2.</p>
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<p>Ternary diagram generated using the direct machine learning model (<span class="html-italic">x<sub>i</sub></span>, <span class="html-italic">y<sub>i</sub></span>): (<b>a</b>) near-critical conditions of 80 atm and 60 °C; and (<b>b</b>) regular conditions of 75 atm and 60 °C.</p>
Full article ">Figure 5
<p>Ternary diagram generated using Hybrid Model 1—Ki → RR → <span class="html-italic">x<sub>i</sub></span>, <span class="html-italic">y<sub>i</sub></span>: (<b>a</b>) near-critical conditions of 80 atm and 60 °C; and (<b>b</b>) regular conditions of 75 atm and 60 °C.</p>
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<p>Ternary diagram generated using Hybrid Model 2—log(<span class="html-italic">x<sub>i</sub></span>), log(<span class="html-italic">y<sub>i</sub></span>) → Ki → RR → <span class="html-italic">x<sub>i</sub></span>, <span class="html-italic">y<sub>i</sub></span>: (<b>a</b>) near-critical conditions of 80 atm and 60 °C; and (<b>b</b>) regular conditions 75 atm and 60 °C.</p>
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<p>Ternary diagrams for far-from-critical conditions of 50 atm and 60 °C: (<b>a</b>) Peng–Robinson EoS; (<b>b</b>) Direct Model; (<b>c</b>) Hybrid Model 1; and (<b>d</b>) Hybrid Model 2.</p>
Full article ">
13 pages, 326 KiB  
Article
New Families of Frequency-Hopping Sequence Sets with a Low-Hit-Zone
by Limengnan Zhou and Hanzhou Wu
Entropy 2024, 26(11), 948; https://doi.org/10.3390/e26110948 - 5 Nov 2024
Viewed by 630
Abstract
As a means of spread spectrum communication, frequency-hopping technology has good performance in anti-jamming, multiple-access, security, covert communications, and so on. In order to meet the needs of different frequency-hopping multiple-access (FHMA) communication scenarios, the research on frequency-hopping sequence (FHS) sets with a [...] Read more.
As a means of spread spectrum communication, frequency-hopping technology has good performance in anti-jamming, multiple-access, security, covert communications, and so on. In order to meet the needs of different frequency-hopping multiple-access (FHMA) communication scenarios, the research on frequency-hopping sequence (FHS) sets with a low-hit-zone (LHZ) is now becoming more and more crucial. In this paper, a general construction to obtain new families of LHZ-FHS sets is achieved via interleaving technique. Subsequently, based on two different shift sequences, two classes of LHZ-FHS sets with new flexible parameters not covered in the related literature are presented. The requirements for our new LHZ-FHS sets to obtain optimality or near-optimality with respect to the Peng–Fan–Lee bound are also introduced. Furthermore, as long as the base FHS set is fixed, the performances of new LHZ-FHS sets can be analyzed, such that the parameters of all appropriate shift sequences to obtain desired LHZ-FHS sets are also fixed. Full article
(This article belongs to the Special Issue Advances in Information and Coding Theory, the Third Edition)
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<p>The maximum PHC values of FHS set <span class="html-italic">B</span> under different time delays (<math display="inline"><semantics> <mi>τ</mi> </semantics></math>).</p>
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<p>The PHC performance of the LHZ-FHS set <span class="html-italic">B</span>.</p>
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<p>The maximum PHC values of FHS set <span class="html-italic">C</span> under different time delay <math display="inline"><semantics> <mi>τ</mi> </semantics></math>.</p>
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<p>The PHC performance of the LHZ-FHS set <span class="html-italic">C</span>.</p>
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10 pages, 3420 KiB  
Article
Flexible Composites with Rare-Earth Element Doped Polycrystalline Particles for Piezoelectric Nanogenerators
by Yanzhe Fan, Zihan Jia, Zhuo Zhang, Shengfei Gu, Wenya Du and Dabin Lin
Micromachines 2024, 15(11), 1280; https://doi.org/10.3390/mi15111280 - 22 Oct 2024
Viewed by 3713
Abstract
Energy harvesting plays an important role in advancing personalized wearables by enabling continuous monitoring, enhancing wearable functionality and facilitating sustainable solutions. We aimed to develop a flexible piezoelectric energy harvesting system based on inorganic piezoelectric materials that convert mechanical energy into electricity to [...] Read more.
Energy harvesting plays an important role in advancing personalized wearables by enabling continuous monitoring, enhancing wearable functionality and facilitating sustainable solutions. We aimed to develop a flexible piezoelectric energy harvesting system based on inorganic piezoelectric materials that convert mechanical energy into electricity to power a wide range of mobile and portable electronic devices. There is significant interest in flexible piezoelectric energy harvesting systems that use inorganic piezoelectric materials due to their exceptional physical features and prospective applications. Herein, we successfully demonstrated a flexible piezoelectric nanogenerator (PENG) designed by the co-doped rare-earth element ceramics (RE-PMN-PT) embedded in PVDF and PDMS composite film and attained a significant output performance while avoiding electrical poling process. The impact of dielectric characteristics on the electrical output of nanogenerators was investigated, together with the structure of the composites. The Sm/La-PMN-PT particles effectively amplify both the voltage and current output, showcasing their potential to power portable and wearable devices, as demonstrated by their capacity to illuminate LEDs. The maximal output power of 2 mW was correlated with the high voltage (220 V) and current (90 µA) of Sm/La-PMN-PT/PVDF, which demonstrated that the device has the potential for energy harvesting in biomedical applications. Full article
(This article belongs to the Section A:Physics)
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<p>(<b>a</b>) Schematic of preparation of Sm/La-PMN-PT based PVDF and PDMS nanocomposite for PENG devices: grinding ceramic disks into powders, mixing powders with PVDF or PDMS solutions, spin coating the mixture, casting the solutions, curing the mixture at high temperature to form the sol film, and fabricating the PENG devices. (<b>b</b>) The photo of Sm/La-PMN-PT ceramic disks. (<b>c</b>) The photo of Sm/La-PMN-PT/PVDF and Sm/La-PMN-PT/PDMS PENG devices. (<b>d</b>) The bending status of the composite film. (<b>e</b>) The devices can be wrapped on the surface of the cylinder.</p>
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<p>(<b>a</b>) The EDX spectra of Sm/La-PMN-PT ceramics in the region. The inset photo shows Sm/La-PMN-PT ceramic disks. (<b>b</b>) Different element mappings of Pb, Mg, Nb, Ti, La, and Sm. Morphologies from SEM images: (<b>c</b>) the Sm/La-PMN-PT powders, (<b>d</b>) the cross-section and (<b>e</b>) the surface of Sm/La-PMN-PT/PDMS composite film with 40 wt.% of BT nanoparticles. The X-ray diffraction spectra of various composite films: (<b>f</b>) Sm/La-PMN-PT/PVDF and (<b>g</b>) Sm/La-PMN-PT/PDMS.</p>
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<p>Stress–strain curve of (<b>a</b>) Sm/La-PMN-PT/PVDF films and (<b>b</b>) Sm/La-PMN-PT/PDMS films with different filler contents. Fracture strength of (<b>c</b>) Sm/La-PMN-PT/PVDF films and (<b>d</b>) Sm/La-PMN-PT/PDMS films with different filler contents. Dielectric properties of (<b>e</b>) Sm/La-PMN-PT/PVDF films and (<b>f</b>) Sm/La-PMN-PT/PDMS films with different filler contents.</p>
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<p>Output performance of PENG with different soft matrices. (<b>a</b>) The output voltage, (<b>b</b>) current, and (<b>c</b>) voltage/current with the external load resistance ranging from 10<sup>2</sup> to 10<sup>9</sup> Ω of 10wt.% Sm/La-PMN-PT/PVDF PENG device. The (<b>d</b>) output voltage, (<b>e</b>) current, and (<b>f</b>) voltage/current with the external load resistance ranging from 10<sup>2</sup> to 10<sup>9</sup> Ω of 40 wt.% Sm/La-PMN-PT/PDMS PENG device.</p>
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<p>(<b>a</b>) The comparison of the output performance of Sm/La-PMN-PT/PVDF and Sm/La-PMN-PT/PDMS PENGs. (<b>b</b>) Output power of 40 wt.% Sm/La-PMN-PT/PDMS and 5wt.% Sm/La-PMN-PT/PVDF PENG devices with the external load resistance ranging from 10<sup>2</sup> to 10<sup>9</sup> Ω. (<b>c</b>) The photo of the measurement system for the durability test. (<b>d</b>) The photo of the measurement system for the LED lighting. (<b>e</b>) The schematic diagram of a diode bridge. The durability test of (<b>f</b>) voltage and (<b>g</b>) current of 40 wt.% Sm/La-PMN-PT/PDMS PENG. The rate is 1 cycle/s. (<b>h</b>,<b>i</b>) The photographs of commercial LEDs connected in series directly lightened by PENG during the pressing/releasing process.</p>
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14 pages, 3205 KiB  
Article
High-Performance Flexible PLA/BTO-Based Pressure Sensor for Motion Monitoring and Human–Computer Interaction
by Xuguang Sui, Qingmiao Mu, Jia Li, Bo Zhao, Hongxi Gu, Han Yu, Juan Du, Lijun Ren and Dengwei Hu
Biosensors 2024, 14(10), 508; https://doi.org/10.3390/bios14100508 - 17 Oct 2024
Cited by 1 | Viewed by 1595
Abstract
Flexible electronics show wide application prospects in electronic skin, health monitoring, and human–machine interfacing. As an essential part of flexible electronics, flexible pressure sensors have become a compelling subject of academic research. There is an urgent need to develop piezoelectric sensors with high [...] Read more.
Flexible electronics show wide application prospects in electronic skin, health monitoring, and human–machine interfacing. As an essential part of flexible electronics, flexible pressure sensors have become a compelling subject of academic research. There is an urgent need to develop piezoelectric sensors with high sensitivity and stability. In this work, the high flexibility of polylactic acid (PLA) film and the excellent ferroelectric properties and high dielectric constant of tetragonal barium titanate (BTO) led to their use as filling materials to fabricate flexible piezoelectric composite films by spinning coating. PLA is used to produce flexible binding substrates, and BTO is added to the composite to enhance its electrical output by improving its piezoelectric performance. The peak output voltage of the PLA/BTO tetragonal piezoelectric film is 22.57 V, and the maximum short-circuit current was 3041 nA. Durability tests showed that during 40,000 s of continuous operation, in the range of 15~120 kPa, the linear relationship between pressure and the film was excellent, the sensitivity for the output voltage is 0.176 V/kPa, and the output current is 27.77 nA/kPa. The piezoelectric pressure sensor (PPS) also enables accurate motion detection, and the extensive capabilities of the PENG highlight its potential in advancing motion sensing and human–computer interactions. Full article
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<p>(<b>a</b>(<b>i</b>)) XRD spectra of BTO cubic and BTO tetragonal; (<b>a</b>(<b>ii</b>)) partial enlargement of the XRD spectrum at 22–24°; (<b>a</b>(<b>iii</b>)) 44–46° partial enlargement of the XRD spectrum; (<b>b</b>) Raman spectrum of BTO cubic and BTO tetragonal; corresponding SEM images of the (<b>c</b>) BTO cubic, (<b>d</b>) BTO tetragonal; (<b>e</b>) production process of piezoelectric composite film; (<b>f</b>) optical images of the flexible film; (<b>f</b>(<b>i</b>)) overhead optical images of both (<b>f</b>(<b>ii</b>,<b>iii</b>))flexure; (<b>g</b>) SEM image of film thickness; (<b>h</b>) structural diagram of PPS; (<b>i</b>) optical diagram of PPS; (<b>j</b>) XRD spectra of the samples; (<b>k</b>) infrared spectra of the samples.</p>
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<p>(<b>a</b>) Schematic diagram of the working principle of flexible PPS; (<b>b</b>) comparison of VOC of PPS prepared by using two different films; (<b>c</b>) comparison of ISC of PPS prepared by using two different films; impact stress and electrical output linear relationship diagram of capacity of (<b>d</b>) PPSBC and (<b>e</b>) PPSBT; (<b>f</b>) open-circuit voltage increment comparison between the two films; (<b>g</b>) comparison of short-circuit current increments of the two films; (<b>h</b>) linear comparison of the pressure and electrical output capacity of the two films.</p>
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<p>(<b>a</b>) Comparison of ferroelectric properties of the two films; (<b>b</b>) Comparison of Relative dielectric constant of the two films (<b>c</b>) HRTEM image of BTO tetragonal; (<b>d</b>) SAED image corresponding to BTO tetragonal; (<b>e</b>) mechanism diagram of BTO tetragonal enhanced piezoelectric output; (<b>f</b>) COMSOL simulation diagram of PPSBC; (<b>g</b>) COMSOL simulation diagram of PPSBT.</p>
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<p>(<b>a</b>) VOC and (<b>b</b>) ISC of PPSBT at BTO concentrations of 0, 2, 4, 6, 8, and 10 ωt%; (<b>c</b>) VOC and (<b>d</b>) ISC of PPSBT (BT content of 6 ωt%) under different pressures; (<b>e</b>) VOCs and (<b>f</b>) ISCs driven by different frequencies; (<b>g</b>) durability tests of PPSBT under different operating frequencies (0~5000 s); (<b>h</b>) enlarged view of partial 100–140 s area data in (<b>g</b>); (<b>i</b>) response time of PPSBT under 75 Kpa; (<b>j</b>) recovery time of PPSBT under 75 Kpa; (<b>k</b>) power output capacity of PPSBT at different temperatures under 75 Kpa; (<b>l</b>) sensitivity of PPSBT.</p>
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<p>(<b>a</b>) Motion monitoring decoration diagram. Place PPSBT (<b>b</b>) at elbow; (<b>c</b>) on soles of the feet; (<b>d</b>) for lifting objects; (<b>e</b>) on the neck; and (<b>f</b>) on the wrist. (<b>g</b>) Optical images and electrical data of the knee joint.</p>
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<p>(<b>a</b>) Electrical signal response of PPSBT after different pressing time; (<b>b</b>) demonstrates the production of the Morse code “HELLO”; (<b>c</b>) demonstrates the generation of the Morse code “YES”; (<b>d</b>) demonstrates the generation of Morse code “THANKS”.</p>
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12 pages, 2353 KiB  
Article
Performance Evaluation of CO2 + SiCl4 Binary Mixture in Recompression Brayton Cycle for Warm Climates
by Muhammad Ehtisham Siddiqui and Khalid H. Almitani
Processes 2024, 12(10), 2155; https://doi.org/10.3390/pr12102155 - 2 Oct 2024
Viewed by 735
Abstract
This work demonstrates the potential of CO2 + SiCl4 binary mixture as a working fluid for power generation cycle. Recompression Brayton cycle configuration is considered due to its proven record of high performance for medium- to high-temperature sources. The objective of [...] Read more.
This work demonstrates the potential of CO2 + SiCl4 binary mixture as a working fluid for power generation cycle. Recompression Brayton cycle configuration is considered due to its proven record of high performance for medium- to high-temperature sources. The objective of this study is to assess the thermodynamic performance of a recompression Brayton cycle using a CO2 + SiCl4 binary mixture as a working fluid, particularly under warm climate conditions. The cycle is simulated using the Peng–Robinson equation of state in Aspen Hysys (v11) software, and the model is validated by comparing VLE data against experimental data from the literature. The analysis involves the assessment of cycle’s thermal efficiency and exergy efficiency under warm climatic conditions, with a minimum cycle temperature of 40 °C. The results demonstrate a notable improvement in the cycle’s thermodynamic performance with CO2 + SiCl4 binary mixture compared to pure CO2. A small concentration (5%) of SiCl4 in CO2 increases the thermal efficiency of the cycle from 41.7% to 43.4%. Moreover, irreversibility losses in the cooler and the heat recovery unit are significantly lower with the CO2 + SiCl4 binary mixture than with pure CO2. This improvement enhances the overall exergy efficiency of the cycle, increasing it from 62.1% to 70.2%. The primary reason for this enhancement is the substantial reduction in irreversibility losses in both the cooler and the HTR. This study reveals that when using a CO2 + SiCl4 mixture, the concentration must be optimized to avoid condensation in the compressor, which can cause physical damage to the compressor blades and other components, as well as increase power input. This issue arises from the higher glide temperature of the mixture at increased SiCl4 concentrations and the limited heat recovery from the cycle. Full article
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<p>(<b>a</b>) Cycle configuration and (<b>b</b>) temperature–entropy diagram of the cycle.</p>
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<p>Vapor–liquid equilibrium diagram depicting the Peng–Robinson model for a CO<sub>2</sub> + SiCl<sub>4</sub> mixture. The dotted points represent experimental data obtained from the work of Doninelli et al. [<a href="#B38-processes-12-02155" class="html-bibr">38</a>].</p>
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<p>Thermal efficiency of the cycle versus (<b>a</b>) flow ratio and (<b>b</b>) turbine inlet pressure.</p>
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<p>Cycle thermal efficiency and compressor inlet vapor fraction for 4% and 6% SiCl<sub>4</sub> mole fractions in the working fluid mixture.</p>
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<p>Saturation pressure and temperature curve of CO<sub>2</sub> + SiCl<sub>4</sub> binary mixture at 5% and 10% molar concentration. The dots represent state points on the bubble and dew lines corresponding to the bubble pressure at cycle minimum temperature, i.e., 40 °C.</p>
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<p>Thermal and exergy efficiency of the cycle versus molar fraction of SiCl<sub>4</sub> in CO<sub>2</sub> + SiCl<sub>4</sub> mixture.</p>
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<p>Exergy loss due to irreversibilities in various components of the cycle for molar concentration of SiCl<sub>4</sub> in CO<sub>2</sub> + SiCl<sub>4</sub> mixture.</p>
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12 pages, 2693 KiB  
Article
Enhanced Flexible Piezoelectric Nanogenerators Using Ethanol-Exfoliated g-C3N4/PVDF Composites via 3D Printing for Self-Powered Applications
by Omkar Y. Pawar, Baoyang Lu and Sooman Lim
Nanomaterials 2024, 14(19), 1578; https://doi.org/10.3390/nano14191578 - 29 Sep 2024
Viewed by 1272
Abstract
This study presents the development of flexible piezoelectric nanogenerators (PENGs) utilizing graphitic carbon nitride (g-C3N4) nanoflakes (CNNFs) and polyvinylidene fluoride (PVDF) composites fabricated via the direct ink writing (DIW) 3D printing method. A novel approach of synthesizing CNNFs using [...] Read more.
This study presents the development of flexible piezoelectric nanogenerators (PENGs) utilizing graphitic carbon nitride (g-C3N4) nanoflakes (CNNFs) and polyvinylidene fluoride (PVDF) composites fabricated via the direct ink writing (DIW) 3D printing method. A novel approach of synthesizing CNNFs using the ethanol exfoliation method was demonstrated, which significantly reduces preparation time and cost compared to traditional acid exfoliation. The CNNFs are incorporated into PVDFs at varying weight percentages (5, 7.5, 10, and 15 wt.%) to optimize the β-phase content and piezoelectric properties. Characterization techniques including XRD, FTIR, and FESEM confirm the successful synthesis and alignment of nanoflakes inside the PVDF matrix. The film with 7.5% CNNF achieves the highest performance, exhibiting a peak output voltage of approximately 6.5 V under a 45 N force. This study also explores the effects of UV light exposure. Under a UV light, the film exhibits an output voltage of 8 V, indicating the device’s durability and potential for practical applications. The fabricated device showed significant voltage outputs during various human motions, confirming its suitability for wearable self-powered IoT applications. This work highlights the efficacy of the ethanol exfoliation method and the DIW printing technique in enhancing the performance of flexible PENGs. Full article
(This article belongs to the Special Issue Advanced Nanomaterials for Flexible and Wearable Electronics)
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<p>(<b>a</b>) Illustration of PVDF/CNNF film fabrication using the DIW method. (<b>b</b>) Image of fabricated film after drying.</p>
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<p>(<b>a</b>) XRD of GCN powder and pure PVDF. (<b>b</b>) FTIR pattern of CNNF (acid-exfoliated and ethanol-exfoliated). (<b>c</b>) FTIR pattern of PVDF/CNNF with different concentrations of CNNF (0, 5, 7.5, 10, and 15 wt.%). (<b>d</b>) β-phase of PVDF/CNNF. (<b>e</b>) FESEM image of bulk GCN. (<b>f</b>) FESEM image of PVDF/CNNF film; inset, magnified FESEM image of fabricated film (PVDF/CNNF). (<b>g</b>) d<sub>33</sub> value of PCDF/CNNF film with GCN 0, 5, 7.5, 10, and 15%. (<b>h</b>) dielectric constant of PVDF/CNNF (GCN 0,5, 7.5, 10 and 15%). (<b>i</b>) Dielectric loss.</p>
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<p>(<b>a</b>) Output voltage of the PVDF/GCN film (GCN 0, 5, 7.5, 10, and 15 wt.%). (<b>b</b>) Voltage produced by the PVDF/GCN 7.5% film with an applied force in Newtons. (<b>c</b>) Frequency output voltage of PVDF/GCN 7.5%. (<b>d</b>) Forward and reverse bias voltage of PVDF/GCN 7.5%. (<b>e</b>) Voltage and current values of PVDF/GCN across a resistance of 10. (<b>f</b>) Power density of PVDF/GCN 7.5 wt.% film. (<b>g</b>) Cyclic stability test.</p>
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<p>(<b>a</b>) Output performance of film fabricated via solution casting. (<b>b</b>) Output performance of film fabricated via DIW.</p>
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<p>(<b>a</b>) Schematic diagram of fabricated device irradiated with UV light. (<b>b</b>) Voltage recorded after different time intervals.</p>
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<p>The fabricated device is attached to different parts of the human body. (<b>a</b>) Output voltage produced via bending pressing movement. (<b>b</b>) Output voltage generated via single finger tapping. (<b>c</b>) Voltage generated via fist strike. (<b>d</b>) Voltage generated via foot tapping.</p>
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21 pages, 19820 KiB  
Article
Evaluation of the Surface Downward Longwave Radiation Estimation Models over Land Surface
by Yingping Chen, Bo Jiang, Jianghai Peng, Xiuwan Yin and Yu Zhao
Remote Sens. 2024, 16(18), 3422; https://doi.org/10.3390/rs16183422 - 14 Sep 2024
Viewed by 1204
Abstract
Surface downward longwave radiation (SDLR) is crucial for maintaining the global radiative budget balance. Due to their ease of practicality, SDLR parameterization models are widely used, making their objective evaluation essential. In this study, against comprehensive ground measurements collected from more than 300 [...] Read more.
Surface downward longwave radiation (SDLR) is crucial for maintaining the global radiative budget balance. Due to their ease of practicality, SDLR parameterization models are widely used, making their objective evaluation essential. In this study, against comprehensive ground measurements collected from more than 300 globally distributed sites, four SDLR parameterization models, including three popular existing ones and a newly proposed model, were evaluated under clear- and cloudy-sky conditions at hourly (daytime and nighttime) and daily scales, respectively. The validation results indicated that the new model, namely the Peng model, originally proposed for SDLR estimation at the sea surface and applied for the first time to the land surface, outperformed all three existing models in nearly all cases, especially under cloudy-sky conditions. Moreover, the Peng model demonstrated robustness across various land cover types, elevation zones, and seasons. All four SDLR models outperformed the Global Land Surface Satellite product from Advanced Very High-Resolution Radiometer Data (GLASS-AVHRR), ERA5, and CERES_SYN1de-g_Ed4A products. The Peng model achieved the highest accuracy, with validated RMSE values of 13.552 and 14.055 W/m2 and biases of −0.25 and −0.025 W/m2 under clear- and cloudy-sky conditions at daily scale, respectively. Its superior performance can be attributed to the inclusion of two cloud parameters, total column cloud liquid water and ice water, besides the cloud fraction. However, the optimal combination of these three parameters may vary depending on specific cases. In addition, all SDLR models require improvements for wetlands, bare soil, ice-covered surfaces, and high-elevation regions. Overall, the Peng model demonstrates significant potential for widespread use in SDLR estimation for both land and sea surfaces. Full article
(This article belongs to the Special Issue Earth Radiation Budget and Earth Energy Imbalance)
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<p>Spatial distribution of the 318 sites in nine surface radiation observing networks. Detailed information about the nine observing networks is provided in <a href="#remotesensing-16-03422-t002" class="html-table">Table 2</a>.</p>
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<p>Validation accuracy of the Prata, Carmona2, and Peng models with the original and calibrated coefficients at daily scales under clear-sky conditions. The color bar indicates the number of samples.</p>
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<p>The same as <a href="#remotesensing-16-03422-f002" class="html-fig">Figure 2</a>, but for the K-C, Carmona2, and Peng models under cloudy-sky conditions.</p>
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<p>Validation accuracies of the four evaluated SDLR models at a daily scale for eight land cover types under clear- and cloudy-sky conditions. The dashed boxes indicate the results under a cloudy sky.</p>
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<p>The same as <a href="#remotesensing-16-03422-f004" class="html-fig">Figure 4</a>, but for six elevation zones (&lt;300 m, 300–1000 m, 1000–1500 m, 1500–2500 m, 2500–3500 m, 3500–4500 m). The results under cloudy-sky conditions are added to the gray background.</p>
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<p>The same as <a href="#remotesensing-16-03422-f005" class="html-fig">Figure 5</a>, but for four seasons: Spring (Mar.–May), Summer (Jun.–Aug.), Autumn (Sep.–Nov.), and Winter (Dec.–Feb.).</p>
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<p>Overall validation accuracy of the four SDLR models and three products (ERA5, CERES4, and GLASS-AVHRR) at daily scales under clear- (<b>a</b>–<b>f</b>) and (<b>g</b>–<b>l</b>) cloudy-sky conditions.</p>
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<p>The spatial distribution of the validated RRMSE at site scale for (<b>a</b>) Peng model and (<b>b</b>–<b>d</b>) three products (GLASS-AVHRR, ERA5, CERES4).</p>
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<p>The time series of the daily SDLR from the Peng model and other three products at two sites (<b>a</b>) SF_GCM (34.25°N, 89.87°W, Grassland) and (<b>b</b>) PM-QAS_M (61.100°N, −46.833°W, ICE).</p>
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<p>Differences in the validated RMSE (ΔRMSE) between the Peng models with different combinations of the five input variables and the original one (all five variables).</p>
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<p>The same as <a href="#remotesensing-16-03422-f010" class="html-fig">Figure 10</a>, but on a daily scale under cloudy-sky conditions for the four seasons. The red box indicates the smallest ΔRMSE. Note that a negative ΔRMSE indicates that the corresponding combination of variables in the Peng model performed better than the original one.</p>
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35 pages, 9916 KiB  
Review
A Comprehensive Review of Strategies toward Efficient Flexible Piezoelectric Polymer Composites Based on BaTiO3 for Next-Generation Energy Harvesting
by Ayda Bouhamed, Sarra Missaoui, Amina Ben Ayed, Ahmed Attaoui, Dalel Missaoui, Khawla Jeder, Nesrine Guesmi, Anouar Njeh, Hamadi Khemakhem and Olfa Kanoun
Energies 2024, 17(16), 4066; https://doi.org/10.3390/en17164066 - 16 Aug 2024
Cited by 3 | Viewed by 2130
Abstract
The increasing need for wearable and portable electronics and the necessity to provide a continuous power supply to these electronics have shifted the focus of scientists toward harvesting energy from ambient sources. Harvesting energy from ambient sources, including solar, wind, and mechanical energies, [...] Read more.
The increasing need for wearable and portable electronics and the necessity to provide a continuous power supply to these electronics have shifted the focus of scientists toward harvesting energy from ambient sources. Harvesting energy from ambient sources, including solar, wind, and mechanical energies, is a solution to meet rising energy demands. Furthermore, adopting lightweight power source technologies is becoming more decisive in choosing renewable energy technologies to power novel electronic devices. In this regard, piezoelectric nanogenerators (PENGs) based on polymer composites that can convert discrete and low-frequency irregular mechanical energy from their surrounding environment into electricity have attracted keen attention and made considerable progress. This review highlights the latest advancements in this technology. First, the working mechanism of piezoelectricity and the different piezoelectric materials will be detailed. In particular, the focus will be on polymer composites filled with lead-free BaTiO3 piezoceramics to provide environmentally friendly technology. The next section will discuss the strategies adopted to enhance the performance of BaTiO3-based polymer composites. Finally, the potential applications of the developed PENGs will be presented, and the novel trends in the direction of the improvement of PENGs will be detailed. Full article
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<p>Illustration of the main piezoelectricity phenomena: (<b>a</b>) tensor direction; (<b>b</b>) direct piezoelectric effect; (<b>c</b>) converse piezoelectric effect.</p>
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<p>Illustration of the energy flow of a piezoelectric generator.</p>
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<p>Different classes of piezoelectric materials.</p>
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<p>Schematic representation of the perovskite structure of BaTiO<sub>3</sub> cubic lattice (above the Curie temperature &gt; 120 °C).</p>
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<p>Diagram of BaTiO<sub>3</sub> preparation process by solid-state reaction.</p>
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<p>Preparation process of BaTiO<sub>3</sub> prepared by the sol–gel method.</p>
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<p>Preparation process of BaTiO<sub>3</sub> prepared by the hydrothermal route.</p>
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<p>Diagram of BaTiO<sub>3</sub> preparation by the co-precipitation process.</p>
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<p>Fabrication process of BaTiO<sub>3</sub> by the polymeric precursor method.</p>
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<p>Impact of BaTiO<sub>3</sub> concentration on the (<b>a</b>) generated voltage and (<b>b</b>) generated power of the polymer composite nanogenerators.</p>
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<p>Main preparation processes of standard nanogenerators based on BaTiO<sub>3</sub> polymer composites.</p>
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<p>Effect of different sonication amplitudes (20%, 30%, and 40%) on the performance of the BCZT/PVD–HFP-based nanogenerator described in Jeder et al. (<b>a</b>) Schematic illustration of the flexible structure of nanogenerator; (<b>b</b>) Young’s modulus as a function of amplitude sonication; and (<b>c</b>) the output voltage response of the various piezoelectric nanogenerators using a simple portable sewing machine [<a href="#B99-energies-17-04066" class="html-bibr">99</a>].</p>
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<p>Effect of different sonication amplitudes (20%, 30%, and 40%) on the performance of the BCZT/PVD–HFP-based nanogenerator described in Jeder et al. (<b>a</b>) Schematic illustration of the flexible structure of nanogenerator; (<b>b</b>) Young’s modulus as a function of amplitude sonication; and (<b>c</b>) the output voltage response of the various piezoelectric nanogenerators using a simple portable sewing machine [<a href="#B99-energies-17-04066" class="html-bibr">99</a>].</p>
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<p>(<b>a</b>) Effect of solvent choice on the piezoelectric performance of the nanogenerator, (<b>b</b>) influence of solvent choice on the output voltage, and (<b>c</b>) impact of dipole moment and solvent evaporation rate on phase transformation of PVDF–HFP [<a href="#B102-energies-17-04066" class="html-bibr">102</a>].</p>
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<p>(<b>a</b>) Effect of solvent choice on the piezoelectric performance of the nanogenerator, (<b>b</b>) influence of solvent choice on the output voltage, and (<b>c</b>) impact of dipole moment and solvent evaporation rate on phase transformation of PVDF–HFP [<a href="#B102-energies-17-04066" class="html-bibr">102</a>].</p>
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<p>(<b>a</b>) Comparative study of the output voltage of BT-, BZT-, and BCZT-based nanogenerators, (<b>b</b>) comparative study of the output power of BT-, BZT-, and BCZT-based nanogenerators, (<b>c</b>) power output vs. various load resistances between different realized NG with BCZT and Zn-BCZT, and (<b>d</b>) stability measurement of the optimal nanogenerator [<a href="#B90-energies-17-04066" class="html-bibr">90</a>,<a href="#B111-energies-17-04066" class="html-bibr">111</a>].</p>
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<p>Illustration showing the positive impact of MWCNTs (<b>a</b>) on the distribution of BaTiO<sub>3</sub> within PDMS polymer and (<b>b</b>) on the performance of the nanogenerator based on Ca-doped BaTiO<sub>3</sub> [<a href="#B91-energies-17-04066" class="html-bibr">91</a>,<a href="#B110-energies-17-04066" class="html-bibr">110</a>].</p>
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<p>10 wt.% Zn-BCZT nanogenerator under different daily human body motions: (<b>a</b>) finger movement; (<b>b</b>) bending and stretching of the elbow; (<b>c</b>) walking; (<b>d</b>) wrist movement [<a href="#B111-energies-17-04066" class="html-bibr">111</a>].</p>
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11 pages, 1385 KiB  
Article
Lateral Femoral Cutaneous Nerve Block or Wound Infiltration Combined with Pericapsular Nerve Group (PENG) Block for Postoperative Analgesia following Total Hip Arthroplasty through Posterior Approach: A Randomized Controlled Trial
by Giuseppe Pascarella, Fabio Costa, Alessandro Strumia, Alessandro Ruggiero, Luigi Maria Remore, Tullio Lanteri, Anton Hazboun, Ferdinando Longo, Francesca Gargano, Lorenzo Schiavoni, Alessia Mattei, Felice Eugenio Agrò, Massimiliano Carassiti and Rita Cataldo
J. Clin. Med. 2024, 13(9), 2674; https://doi.org/10.3390/jcm13092674 - 2 May 2024
Viewed by 1872
Abstract
Background: Pericapsular nerve group (PENG) block, although effective for pain management following total hip arthroplasty (THA), does not cover skin analgesia. In this randomized controlled trial, we compared the effectiveness of PENG block combined with lateral femoral cutaneous nerve (LFCN) block or wound [...] Read more.
Background: Pericapsular nerve group (PENG) block, although effective for pain management following total hip arthroplasty (THA), does not cover skin analgesia. In this randomized controlled trial, we compared the effectiveness of PENG block combined with lateral femoral cutaneous nerve (LFCN) block or wound infiltration (WI) on postoperative analgesia and functional outcomes. Methods: Fifty patients undergoing posterior-approached THA under spinal anesthesia were randomly allocated to receive LFCN block with 10 mL of 0.5% ropivacaine or WI with 20 mL of 0.5% ropivacaine. In both groups, PENG block was performed by injecting 20 mL of 0.5% ropivacaine. Primary outcomes were static and dynamic pain scores (0–10 numeric rating scale) measured in the first 24 h after surgery. Secondary outcomes included postoperative opioid consumption, functional assessment and length of hospital stay. Results: Postoperative static NRS of patients receiving LFCN was higher than that of patients receiving WI at 6 h but lower at 24 h, with a median (IQR) of 3 (2–4) vs. 2 (1–2) (p < 0.001) and 2 (2–3) vs. 3 (3–4) (p = 0.02), respectively. Static pain scores at 12 h did not show significant differences, with an NRS of 3 (2–4) for WI vs. 3 (3–4) for LFCN (p = 0.94). Dynamic pain and range of movement followed a similar trend. No significant differences were detected in other outcomes. Conclusions: LFCN block was not inferior to WI for postoperative analgesia and functional recovery in association with PENG block during the first postoperative day, although it had worse short-term pain scores. Based on these results, it is reasonable to consider LFCN block as a valid alternative to WI or even a complementary technique added to WI to enhance skin analgesia during the first 24 h after THA. Future studies are expected to confirm this hypothesis and find the best combination between PENG block and other techniques to enhance analgesia after THA. Full article
(This article belongs to the Special Issue Clinical Updates on Perioperative Pain Management)
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<p>CONSORT flow diagram. CONSORT indicates Consolidated Standards of Reporting Trials.</p>
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<p><b>Regional Anesthesia Techniques:</b> (<b>A</b>) <b>Lateral femoral cutaneous nerve (LFCN) block.</b> Green dashed line: LFCN; TFLM: tensor fasciae latae muscle; SM: sartorius muscle (<b>B</b>) <b>PENG Block:</b> IPT: iliopsoas tendon; IPE: iliopubic eminence; asterisk (green *): injection target; FA: femoral artery; IPM: iliopsoas muscle; AIIS: anterior inferior iliac spine.</p>
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<p>Static postoperative pain. The box plot shows postoperative pain scores in both study groups. Data include static pain reported at three different postoperative time points (6, 12 and 24 h). Pain severity is expressed using a 0–10 numeric rating scale, with 0 equal to no pain and 10 being the worst imaginable pain. Values are expressed as median (horizontal bars) with 25th–75th (box) and range of minimum to maximum value (whiskers); * denotes statistical significance (<span class="html-italic">p</span> &lt; 0.05). PENG: pericapsular nerve group block; WI: wound infiltration; LFCN: lateral femoral cutaneous nerve block; s-NRS: numeric rating scale at rest (static).</p>
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<p>Dynamic postoperative pain. The box plot shows postoperative pain scores in both study groups. Data include dynamic pain reported at three different postoperative time points (6, 12 and 24 h). Pain severity is expressed using a 0–10 numeric rating scale, with 0 equal to no pain and 10 being the worst imaginable pain. Values are expressed as median (horizontal bars) with 25th–75th (box) and range of minimum to maximum value (whiskers); * denotes statistical significance (<span class="html-italic">p</span> &lt; 0.05). PENG: pericapsular nerve group block; WI: wound infiltration. LFCN: lateral femoral cutaneous nerve block; d-NRS: numeric rating scale on movement (dynamic).</p>
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11 pages, 2288 KiB  
Article
The Effects of the Pericapsular Nerve Group Block on Postoperative Pain in Patients with Hip Fracture: A Multicenter Study
by Carmine Iacovazzo, Rosario Sara, Pasquale Buonanno, Maria Vargas, Antonio Coviello, Roberta Punzo, Vincenzo Maffei and Annachiara Marra
Diagnostics 2024, 14(8), 827; https://doi.org/10.3390/diagnostics14080827 - 17 Apr 2024
Cited by 1 | Viewed by 1798
Abstract
Background: An adequate early mobilization followed by an effective and pain-free rehabilitation are critical for clinical and functional recovery after hip and proximal femur fracture. A multimodal approach is always recommended so as to reduce the administered dose of analgesics, drug interactions, and [...] Read more.
Background: An adequate early mobilization followed by an effective and pain-free rehabilitation are critical for clinical and functional recovery after hip and proximal femur fracture. A multimodal approach is always recommended so as to reduce the administered dose of analgesics, drug interactions, and possible side effects. Peripheral nerve blocks should always be considered in addition to spinal or general anesthesia to prolong postoperative analgesia. The pericapsular nerve group (PENG) block appears to be a less invasive and more effective analgesia technique compared to other methods. Methods: We conducted multicenter retrospective clinical research, including 98 patients with proximal femur fracture undergoing osteosynthesis surgery within 48 h of occurrence of the fracture. Thirty minutes before performing spinal anesthesia, 49 patients underwent a femoral nerve (FN) block plus a lateral femoral cutaneous nerve (LCFN) block, and the other 49 patients received a PENG block. A non-parametric Wilcoxon–Mann–Whitney (α = 0.05) test was performed to evaluate the difference in resting and dynamic numerical rating scale (NRS) at 30 min, 6 h, 12 h, and 24 h. Results: the PENG block administration was more effective in reducing pain intensity compared to the FN block in association with the LFCN block, as seen in the resting and dynamic NRS at thirty minutes and 12 h follow-up. Conclusion: the PENG block was more effective in reducing pain intensity than the femoral nerve block associated with the lateral femoral cutaneous nerve block in patients with proximal femur fracture undergoing to osteosynthesis. Full article
(This article belongs to the Special Issue Updates in Interventional Ultrasonography)
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<p>PENG block with high frequency linear probe. The needle is outlined by a yellow dotted arrow.</p>
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<p>Box plot of the median of dynamic NRS between PENG and FN + LFCN at 30 min. PENG = pericapsular nerve group; NF: Nervous Femoral; LFCN: lateral femoral cutaneous nerve; PE = pertrochanteric fracture; IN = intertrochanteric fracture.</p>
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9 pages, 1223 KiB  
Article
A Randomized Controlled Trial to Evaluate the Analgesic Effectiveness of Periarticular Injections and Pericapsular Nerve Group Block for Patients Undergoing Total Hip Arthroplasty
by Bora Lee, Tae Sung Lee, Jaewon Jang, Hyun Eom Jung, Kwan Kyu Park and Yong Seon Choi
J. Pers. Med. 2024, 14(4), 377; https://doi.org/10.3390/jpm14040377 - 30 Mar 2024
Cited by 1 | Viewed by 1311
Abstract
Pericapsular nerve group (PENG) block and periarticular injection (PAI) provide motor-sparing analgesia following hip surgery. We hypothesized that PAI offers non-inferior pain relief compared with PENG block in patients undergoing primary total hip arthroplasty (THA). In this randomized trial, 66 patients who underwent [...] Read more.
Pericapsular nerve group (PENG) block and periarticular injection (PAI) provide motor-sparing analgesia following hip surgery. We hypothesized that PAI offers non-inferior pain relief compared with PENG block in patients undergoing primary total hip arthroplasty (THA). In this randomized trial, 66 patients who underwent primary THA under spinal anesthesia were assigned to the PENG or PAI groups. The primary endpoint was the resting pain score 24 h postoperatively. The secondary endpoints included pain scores at rest and during movement at 6 and 48 h postoperatively, quadriceps strength at 24 h postoperatively, and opioid consumption at 24 and 48 h postoperatively. The mean difference in pain scores at rest between the two groups was 0.30 (95% confidence interval [CI], −0.78 to 1.39) at 24 h postoperatively. The upper 95% CI was lower than the non-inferiority margin, indicating non-inferior performance. No significant between-group differences were observed in the pain scores at 6 and 48 h postoperatively. Additionally, no significant differences in quadriceps strength and opioid consumption were observed between the two groups. The PAI and PENG blocks provided comparable postoperative analgesia during the first 48 h after primary THA. Further investigation is required to determine the optimal PAI technique and local anesthetic mixture. Full article
(This article belongs to the Special Issue Anesthesiology and Pain Management in Clinical Medicine)
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<p>CONSORT study flow diagram. CONSORT, Consolidated Standards for Reporting Trials; PENG, pericapsular nerve group block; PAI, periarticular injection.</p>
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<p>(<b>A</b>,<b>B</b>) Non-inferiority diagrams show the difference in the numerical rating scale pain score between the PENG and PAI groups 24 h postoperatively. The solid line indicates the non-inferiority margin (δ) of 1.439. Squares indicate mean pain score differences, and error bars indicate 95% confidence intervals of the difference between the groups. PENG, pericapsular nerve group block; PAI, periarticular injection.</p>
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<p>(<b>A</b>,<b>B</b>) Pain scores. Boxplots represent the median with 25th/75th percentiles. The whiskers show the minimum/maximum values, excluding outliers. Points represent outliers. PENG, pericapsular nerve group block; PAI, periarticular injection.</p>
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26 pages, 7011 KiB  
Review
A Review of Polymer-Based Environment-Induced Nanogenerators: Power Generation Performance and Polymer Material Manipulations
by Shuanghong Xie, Huping Yan and Ronghui Qi
Polymers 2024, 16(4), 555; https://doi.org/10.3390/polym16040555 - 18 Feb 2024
Cited by 2 | Viewed by 2698
Abstract
Natural environment hosts a considerable amount of accessible energy, comprising mechanical, thermal, and chemical potentials. Environment-induced nanogenerators are nanomaterial-based electronic chips that capture environmental energy and convert it into electricity in an environmentally friendly way. Polymers, characterized by their superior flexibility, lightweight, and [...] Read more.
Natural environment hosts a considerable amount of accessible energy, comprising mechanical, thermal, and chemical potentials. Environment-induced nanogenerators are nanomaterial-based electronic chips that capture environmental energy and convert it into electricity in an environmentally friendly way. Polymers, characterized by their superior flexibility, lightweight, and ease of processing, are considered viable materials. In this paper, a thorough review and comparison of various polymer-based nanogenerators were provided, focusing on their power generation principles, key materials, power density and stability, and performance modulation methods. The latest developed nanogenerators mainly include triboelectric nanogenerators (TriboENG), piezoelectric nanogenerators (PENG), thermoelectric nanogenerators (ThermoENG), osmotic power nanogenerator (OPNG), and moist-electric generators (MENG). Potential practical applications of polymer-based nanogenerator were also summarized. The review found that polymer nanogenerators can harness a variety of energy sources, with the basic power generation mechanism centered on displacement/conduction currents induced by dipole/ion polarization, due to the non-uniform distribution of physical fields within the polymers. The performance enhancement should mainly start from strengthening the ion mobility and positive/negative ion separation in polymer materials. The development of ionic hydrogel and hydrogel matrix composites is promising for future nanogenerators and can also enable multi-energy collaborative power generation. In addition, enhancing the uneven distribution of temperature, concentration, and pressure induced by surrounding environment within polymer materials can also effectively improve output performance. Finally, the challenges faced by polymer-based nanogenerators and directions for future development were prospected. Full article
(This article belongs to the Special Issue High Performance Polymer Membranes II)
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<p>Different nanogenerators and their applications: using mechanical energy: (<b>a</b>) PENG: for the manufacture of implantable medical devices [<a href="#B25-polymers-16-00555" class="html-bibr">25</a>] and human gait monitoring sensors [<a href="#B26-polymers-16-00555" class="html-bibr">26</a>], (<b>b</b>) TriboENG: for the collection of friction energy between droplets and triboelectric materials [<a href="#B27-polymers-16-00555" class="html-bibr">27</a>] or between different triboelectric materials [<a href="#B28-polymers-16-00555" class="html-bibr">28</a>]. (<b>c</b>) ThermoENG using thermal energy: it is used to manufacture self-powered sensors [<a href="#B29-polymers-16-00555" class="html-bibr">29</a>] and wearable devices [<a href="#B30-polymers-16-00555" class="html-bibr">30</a>]. Using chemical potential energy: (<b>d</b>) OPNG: used to collect energy between different concentrations of liquids [<a href="#B31-polymers-16-00555" class="html-bibr">31</a>] and promote in vitro drug delivery [<a href="#B32-polymers-16-00555" class="html-bibr">32</a>], (<b>e</b>) MENG: used to collect human respiration [<a href="#B33-polymers-16-00555" class="html-bibr">33</a>] and humidity energy in the environment to charge smartphones [<a href="#B34-polymers-16-00555" class="html-bibr">34</a>].</p>
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<p>Power generation principles of different nanogenerators: (<b>a</b>) The power generation principle of PENG with different types of materials: (i) inorganic piezoelectric crystals (ZnO) with asymmetric charge centers [<a href="#B42-polymers-16-00555" class="html-bibr">42</a>], (ii) Piezoelectric polymer with permanent dipole moment [<a href="#B43-polymers-16-00555" class="html-bibr">43</a>], (iii) Ionic hydrogel [<a href="#B44-polymers-16-00555" class="html-bibr">44</a>]. (<b>b</b>) The power generation principle of TriboENG [<a href="#B45-polymers-16-00555" class="html-bibr">45</a>]: (i) Triboelectric effect, (ii) Electrostatic effect. (<b>c</b>) Different types of ThermoENG [<a href="#B46-polymers-16-00555" class="html-bibr">46</a>]: (i) Conductive polymer-based thermal diffusion generator, (ii) Ion hydrogel-based thermal diffusion generator, (iii) Ionic hydrogel-based thermocouple generator. (<b>d</b>) The structure of OPNG [<a href="#B47-polymers-16-00555" class="html-bibr">47</a>]: (i) only one selective cation permeable membrane and (ii) both anion and cation selective permeable membranes: positive and negative ions move from high concentration side to low concentration side through cation selective permeable membrane and anion selective permeable membrane, respectively. (<b>e</b>) The formation method of MENG: (i) the asymmetric distribution of hygroscopic materials [<a href="#B48-polymers-16-00555" class="html-bibr">48</a>], (ii) the gradient distribution of oxygen-containing functional groups.</p>
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<p>Methods and schematic diagrams for improving the piezoelectric performance of PVDF: (<b>a</b>) PVDF with different crystal structures [<a href="#B68-polymers-16-00555" class="html-bibr">68</a>] and (<b>b</b>) PVDF with different conformational structures [<a href="#B68-polymers-16-00555" class="html-bibr">68</a>]: red, cyan, and blue spheres represent F, C, and H atoms. (<b>c</b>) The energy difference between PVDF α and β molecules [<a href="#B69-polymers-16-00555" class="html-bibr">69</a>]: the yellow, white, light blue, and gray balls represent gold, hydrogen, fluoride, and carbon atoms, respectively. (<b>d</b>) Local annealing treatment and changes in Raman spectra of materials before and after annealing treatment [<a href="#B69-polymers-16-00555" class="html-bibr">69</a>], (<b>e</b>) mechanical stretching and images of crystal phase changes before and after stretching [<a href="#B70-polymers-16-00555" class="html-bibr">70</a>], (<b>f</b>) different ways of electrode polarization [<a href="#B71-polymers-16-00555" class="html-bibr">71</a>], (<b>g</b>) the energy difference between the molecular structure of copolymers and those with different phases and isomorphic anti-plane phases with different proportions of TrFE co doping ΔE. Among them, 3/1-helix is the most stable [<a href="#B72-polymers-16-00555" class="html-bibr">72</a>].</p>
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<p>Schematic diagram of PEDOT: PSS structure: (<b>a</b>) Schematic diagram of PSS and PEDOT molecular structure [<a href="#B74-polymers-16-00555" class="html-bibr">74</a>], (<b>b</b>) The structure of PEDOT: PSS before and after treatment with dimethyl sulfone (DMSO<sub>2</sub>) [<a href="#B75-polymers-16-00555" class="html-bibr">75</a>], (<b>c</b>) Trifluoroacetic acid (TFA) [<a href="#B76-polymers-16-00555" class="html-bibr">76</a>] and (<b>d</b>) The effect of the degree of π-π contact between chains on conductivity: (i) The microstructure of intrinsic films of different modified polymers was studied using grazing incidence wide-angle X-ray scattering (GIWAXS) technology. The diffraction signal Qr ≈ 1.5 Å<sup>−1</sup> showed the anisotropic distribution of TBDOPV-T-518 in the layered side chain stacking material, indicating the positive orientation of TBDOPV-T-518 π stacking and the formation of ordered anisotropic arrangements on the molecular side chains. Changes in conductivity of TBDOPV-T-518 when using (ii) N-DMBI and (iii) FeCl<sub>3</sub> as dopants, respectively [<a href="#B77-polymers-16-00555" class="html-bibr">77</a>].</p>
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<p>Ionic hydrogels for different environment-induced power generation and their applications: (<b>a</b>) demonstration of piezoionic neuromodulation in a rodent modelt [<a href="#B44-polymers-16-00555" class="html-bibr">44</a>], (<b>b</b>) injectable and biodegradable PLLA-PENG for osteoarthritis treatment [<a href="#B109-polymers-16-00555" class="html-bibr">109</a>]. (<b>c</b>) PSSA/PAN-MENG made by electrospinning is used as a self-powered respiratory detector [<a href="#B110-polymers-16-00555" class="html-bibr">110</a>].</p>
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<p>Applications of natural polymer nanogenerators: (<b>a</b>) cellulose-based PENG with sponge structure is used as a wearable smart pressure sensor [<a href="#B116-polymers-16-00555" class="html-bibr">116</a>], (<b>b</b>) the self-powered air filter manufactured by CA/Ni-HITP TriboENG and the comparison of the number of submicron particles inside and outside the mask after wearing it for 2 h [<a href="#B117-polymers-16-00555" class="html-bibr">117</a>], (<b>c</b>) the structure of the acidic/alkaline whey protein film, the principle of power generation, and the picture of it powering the wireless position tracker at low humidity [<a href="#B118-polymers-16-00555" class="html-bibr">118</a>], (<b>d</b>) introducing ionic liquids into the internal solvent of the gel [<a href="#B119-polymers-16-00555" class="html-bibr">119</a>].</p>
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<p>Performance enhancement methods of polymer-based nanogenerators: (<b>a</b>) utilizing charged fragments [<a href="#B131-polymers-16-00555" class="html-bibr">131</a>] or (<b>b</b>) utilizing other substances possessing micro-nano pore structures [<a href="#B33-polymers-16-00555" class="html-bibr">33</a>] to creat a single charge channel, (<b>c</b>) utilizing ions with smaller radii as solutes [<a href="#B54-polymers-16-00555" class="html-bibr">54</a>], (<b>d</b>) introducing ionic liquids into the internal solvent of the gel [<a href="#B134-polymers-16-00555" class="html-bibr">134</a>], (<b>e</b>) configuring with a fence-like structure on the sliding surface of TriboENG [<a href="#B135-polymers-16-00555" class="html-bibr">135</a>], (<b>f</b>) increasing contact pressure and accelerate friction frequency to obtain a larger effective contact area [<a href="#B136-polymers-16-00555" class="html-bibr">136</a>], (<b>g</b>) creating an ion rectifier junction akin to a semiconductor [<a href="#B137-polymers-16-00555" class="html-bibr">137</a>].</p>
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