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12 pages, 5627 KiB  
Article
Robust Brewed Tea Waste/Reduced Graphene Oxide Hydrogel for High Performance Flexible Supercapacitors
by Dan Wu, Jiajia Zhou, Wuqiang Deng, Guowen He and Zheng Liu
Polymers 2024, 16(22), 3170; https://doi.org/10.3390/polym16223170 - 14 Nov 2024
Viewed by 113
Abstract
Tea waste contains various substances with phenolic hydroxyl groups, including lignin, tannins, tea polyphenols, etc., which are rarely utilized. In this study, tea waste was directly dispersed with graphene oxide to prepare tea waste/reduced graphene oxide (TW/rGO) hydrogel through a one-step hydrothermal method. [...] Read more.
Tea waste contains various substances with phenolic hydroxyl groups, including lignin, tannins, tea polyphenols, etc., which are rarely utilized. In this study, tea waste was directly dispersed with graphene oxide to prepare tea waste/reduced graphene oxide (TW/rGO) hydrogel through a one-step hydrothermal method. The prepared hydrogel presented a continuous three-dimensional porous structure and exhibited good mechanical properties with a compressive strength of 53.4 ± 4.0 kPa. It also showed excellent electrochemical performance as an electrode material. Its specific capacitance reached 434.7 F g−1 at a current density of 1 A g−1, and its capacitance retention was 55.8% when the current density was increased to 100 A g−1. In addition, an TW/rGO assembled all-solid-state supercapacitor demonstrated a superior specific capacitance of 372.8 F g−1 and a competitive energy density of 12.9 Wh kg−1 at 1 A g−1. Full article
(This article belongs to the Section Polymer Applications)
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<p>Schematic illustration of the preparation process for TW/rGO.</p>
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<p>SEM images of (<b>a</b>,<b>b</b>) rGO and (<b>c</b>,<b>d</b>) TW/rGO.</p>
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<p>(<b>a</b>) Adsorption–desorption isotherm curves (the inset displays pore size distribution curves obtained using the Barrett–Joyner–Halenda method), (<b>b</b>) Raman spectra, (<b>c</b>) XRD patterns, (<b>d</b>) XPS survey, and C1s core-level spectra of (<b>e</b>) rGO and (<b>f</b>) TW/rGO.</p>
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<p>Electrochemical performances of rGO and TW/rGO hydrogels: (<b>a</b>) CV curves at a scan rate of 5 mV s<sup>−1</sup>, (<b>b</b>) GCD profiles at a current density of 1 A g<sup>−1</sup>, (<b>c</b>) plots of C<sub>m</sub> versus current density, and (<b>d</b>) Nyquist plots.</p>
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<p>Electrochemical performances of rGO and TW/rGO hydrogels: (<b>a</b>) CV curves at a scan rate of 5 mV s<sup>−1</sup>, (<b>b</b>) GCD profiles at a current density of 1 A g<sup>−1</sup>, (<b>c</b>) plots of C<sub>m</sub> versus current density, and (<b>d</b>) Nyquist plots.</p>
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<p>Electrochemical performance and flexibility tests of TW/rGO-based all-solid-state supercapacitor: (<b>a</b>) CV curves at different scan rates (2–500 mV s<sup>−1</sup>); (<b>b</b>) plots of C<sub>s</sub> versus current density (inset shows GCD curves at 1–30 A g<sup>−1</sup>); (<b>c</b>) Ragone plot of energy density versus power density; (<b>d</b>) cycling stability at current density of 20 A g<sup>−1</sup>; (<b>e</b>) CV curves at 10 mV s<sup>−1</sup> for different bending angles; and (<b>f</b>) capacitance retention of supercapacitor after mechanical folding cycles.</p>
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18 pages, 5203 KiB  
Review
Conductive Hydrogel Materials for Flexible Supercapacitor Electrodes
by Kun Zhang, Zhizhou Chen, Jinling Li, Gaoqiang Feng, Chang Xu, Jizhi Yang and Wanwan Li
Crystals 2024, 14(11), 971; https://doi.org/10.3390/cryst14110971 - 9 Nov 2024
Viewed by 428
Abstract
Flexible supercapacitors (SCs), as promising energy storage devices, have shown great potential for both next-generation wearable electronics and addressing the global energy crisis. Conductive hydrogels (CHs) are suitable electrode materials for flexible SCs on account of their intrinsic characteristics and functional advantages, such [...] Read more.
Flexible supercapacitors (SCs), as promising energy storage devices, have shown great potential for both next-generation wearable electronics and addressing the global energy crisis. Conductive hydrogels (CHs) are suitable electrode materials for flexible SCs on account of their intrinsic characteristics and functional advantages, such as a unique 3D porous structure, remarkable conductivity, tunable chemical and physical properties, and outstanding mechanical properties. Herein, an overview of the fabrication strategies for CHs as electrode materials in flexible SCs, as well as their advantages and disadvantages, and perspectives on CH-based SCs is provided. First, the fabrication strategies for CHs are systematically introduced. Second, various multifunctional CH-based SCs are presented and discussed. Finally, this review concludes with insights into the challenges and opportunities related to CHs or CH-based SCs, indicating future research prospects and application orientations in this field. Full article
(This article belongs to the Special Issue Research on Energy Storage and Conversion Materials)
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<p>Preparation strategies for electronically CHs (<b>a</b>–<b>c</b>) and ionically CHs (<b>d</b>,<b>e</b>) [<a href="#B27-crystals-14-00971" class="html-bibr">27</a>]: (<b>a</b>) the formation of CHs in a conductive filler suspension; (<b>b</b>) polymerization in a preformed hydrogel matrix; (<b>c)</b> single-component CHs; (<b>d</b>) zwitterionic hydrogel (introducing ionizable functional groups into the polymer network); (<b>e</b>) introducing conductive ions into a hydrogel precursor solution or as-fabricated hydrogel.</p>
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<p>(<b>a</b>) The molecular structure of polyaniline containing boric acid groups and a SEM image of PPH [<a href="#B47-crystals-14-00971" class="html-bibr">47</a>]. (<b>b</b>) The preparation process of TiO<sub>2</sub>-PEDOT:PSS-CNT hydrogel [<a href="#B48-crystals-14-00971" class="html-bibr">48</a>]. (<b>c</b>) The preparation process of PDA-rGO-PAM hydrogel [<a href="#B49-crystals-14-00971" class="html-bibr">49</a>]. (<b>a</b>) Reproduced with permission from Reference [<a href="#B47-crystals-14-00971" class="html-bibr">47</a>], copyright © Wiley 2016; (<b>b</b>) reproduced with permission from Reference [<a href="#B48-crystals-14-00971" class="html-bibr">48</a>], copyright © Wiley 2014; (<b>c</b>) reproduced with permission from Reference [<a href="#B49-crystals-14-00971" class="html-bibr">49</a>], copyright © Wiley 2016.</p>
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<p>(<b>a</b>) Synthesis steps of Hep-MA/PANI hydrogels [<a href="#B56-crystals-14-00971" class="html-bibr">56</a>]. (<b>b</b>) Process for preparing C-IPN hydrogels [<a href="#B57-crystals-14-00971" class="html-bibr">57</a>]. (<b>c</b>) The formation of a microelectrode array via the electrochemical polymerization of PEDOT within molten agar [<a href="#B58-crystals-14-00971" class="html-bibr">58</a>]. (<b>d</b>) Preparation of TOCNF/PAA-PPy composite gels [<a href="#B59-crystals-14-00971" class="html-bibr">59</a>]. (<b>a</b>) Reproduced with permission from Reference [<a href="#B56-crystals-14-00971" class="html-bibr">56</a>], copyright © American Chemical Society 2014; (<b>b</b>) reproduced with permission from Reference [<a href="#B57-crystals-14-00971" class="html-bibr">57</a>], copyright © Nature 2018; (<b>c</b>) reproduced with permission from Reference, copyright © American Chemical Society 2010 [<a href="#B58-crystals-14-00971" class="html-bibr">58</a>]; (<b>d</b>) reproduced with permission from Reference [<a href="#B59-crystals-14-00971" class="html-bibr">59</a>], copyright © Multidisciplinary Digital Publishing Institute 2019.</p>
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<p>(<b>a</b>) Chemical structure and morphology of phytic-acid-gelated and -doped polyaniline hydrogel with a 3D hierarchical microstructure. Reproduced with permission [<a href="#B60-crystals-14-00971" class="html-bibr">60</a>]. Copyright 2012, National Academy of Sciences. (<b>b</b>) Digital images and cross-sectional SEM images of PEDOT:PSS hydrogels before and after freeze-drying, showing various geometric forms. Reproduced with permission. Copyright 2017, Wiley [<a href="#B76-crystals-14-00971" class="html-bibr">76</a>]. (<b>c</b>) Schematic diagrams of the synthesis and polymerization mechanism of elastic polypyrrole hydrogel, detailing the step-by-step process and structural changes. Reproduced with permission. Copyright 2010, American Chemical Society [<a href="#B70-crystals-14-00971" class="html-bibr">70</a>].</p>
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<p>(<b>a</b>) Schematic illustration of the stable network structure for the integrated all-hydrogel supercapacitor. (<b>b</b>) Capacitance retention under different deformations [<a href="#B101-crystals-14-00971" class="html-bibr">101</a>]. (<b>c</b>) Schematic illustration of the formation of MPGP-Fe conductive hydrogels. (<b>d</b>) Optical image of the assembled all-gel MPGP-Fe-0.3M SC. The enlarged area indicates the strongly bound electrode/electrolyte interface. (<b>e</b>) The corresponding capacitance retention with respect to that at 20 °C and compared with that of other temperature-tolerant supercapacitors [<a href="#B102-crystals-14-00971" class="html-bibr">102</a>]. (<b>f</b>) Optical images demonstrate the flexibility of the capacitor, fluorescent images show the electrode/electrolyte interface with the electrolyte dyed by Rhodamine B, and scanning electron microscopy (SEM) images reveal the microstructure of the interface. (<b>g</b>) Repeated lighting of an LED bulb by the capacitor via cut/healing operations [<a href="#B103-crystals-14-00971" class="html-bibr">103</a>]. (<b>a</b>,<b>b</b>) Reproduced with permission from Reference [<a href="#B101-crystals-14-00971" class="html-bibr">101</a>], copyright © Elsevier 2019; (<b>c</b>–<b>e</b>) reproduced with permission from Reference [<a href="#B102-crystals-14-00971" class="html-bibr">102</a>], copyright © Elsevier 2024; (<b>f</b>,<b>g</b>) reproduced with permission from Reference [<a href="#B103-crystals-14-00971" class="html-bibr">103</a>], copyright © Wiley 2017.</p>
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11 pages, 2651 KiB  
Communication
Synthesis of Needle-like CoO Nanowires Decorated with Electrospun Carbon Nanofibers for High-Performance Flexible Supercapacitors
by Xiang Zhang
Nanomaterials 2024, 14(21), 1770; https://doi.org/10.3390/nano14211770 - 4 Nov 2024
Viewed by 582
Abstract
Needle-like CoO nanowires have been successfully synthesized by a facile hydrothermal process on an electrospun carbon nanofibers substrate. The as-prepared sample mesoporous CoO nanowires aligned vertically on the surface of carbon nanofibers and cross-linked with each other, producing loosely porous nanostructures. These hybrid [...] Read more.
Needle-like CoO nanowires have been successfully synthesized by a facile hydrothermal process on an electrospun carbon nanofibers substrate. The as-prepared sample mesoporous CoO nanowires aligned vertically on the surface of carbon nanofibers and cross-linked with each other, producing loosely porous nanostructures. These hybrid composite electrodes exhibit a high specific capacitance of 1068.3 F g−1 at a scan rate of 5 mV s−1 and a good rate capability of 613.7 F g−1 at a scan rate of 60 mV s−1 in a three-electrode cell. The CoO NWs@CNF//CNT@CNF asymmetric device exhibits remarkable cycling stability and delivers a capacitance of 79.3 F/g with a capacitance retention of 92.1 % after 10,000 cycles. The asymmetric device delivers a high energy density of 37 Wh kg−1 with a power density of 0.8 kW kg−1 and a high power density of 16 kW kg−1 with an energy density of 23 Wh kg−1. This study demonstrated a promising strategy to enhance the electrochemical performance of flexible supercapacitors. Full article
(This article belongs to the Special Issue Advanced Nanocomposites for Batteries and Supercapacitors)
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<p>Schematic representation of the procedure used to fabricate needle-like CoO NWs@CNF.</p>
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<p>(<b>a</b>) X-ray diffraction pattern of CoO NWs@CNF. (<b>b</b>) Raman spectra of CoO NWs@CNF. (<b>c</b>) N<sub>2</sub> adsorption and desorption isotherm of CoO NWs@CNF. (<b>d</b>) Pore size distribution of CoO NWs@CNF.</p>
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<p>(<b>a</b>) SEM image of CoO nanowires on carbon nanofibers membrane. (<b>b</b>) SEM image of CoO Nanowires on one single carbon nanofiber. (<b>c</b>) High magnification SEM images of CoO nanowires. (<b>d</b>) SEM image of CoO NWs@CNF with elements mapping; (<b>e</b>–<b>g</b>) element mappings of cobalt (red), oxygen (blue) and carbon (green), respectively. (<b>h</b>,<b>i</b>) XPS of CoO NWs@CNF.</p>
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<p>(<b>a</b>) Cyclic voltammetry measurement of CoO NWs@CNF at various scan rates ranging from 5 to 60 mV s<sup>−1</sup>. (<b>b</b>) Specific capacitance derived from the CV measurements. (<b>c</b>) The galvanostatic charge and discharge voltage profiles of CoO NWs@CNF at various current densities ranging from 1 to 20 A g<sup>−1</sup> and (<b>d</b>) the corresponding specific capacitance as a function of current density.</p>
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<p>(<b>a</b>) Cycling performance for 10,000 cycles. The inset is galvanostatic charge–discharge curves at 1st and 10,000th cycles. (<b>b</b>). The Ragone plot of CoO NWs@CNF//CNT@CNF asymmetric supercapacitors and other asymmetric supercapacitors reported in the literature.</p>
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27 pages, 6977 KiB  
Review
Comparison of Advanced Flexible Alternating Current Transmission System (FACTS) Devices with Conventional Technologies for Power System Stability Enhancement: An Updated Review
by Andrea Carbonara, Sebastian Dambone Sessa, Angelo L’Abbate, Francesco Sanniti and Riccardo Chiumeo
Electronics 2024, 13(21), 4262; https://doi.org/10.3390/electronics13214262 - 30 Oct 2024
Viewed by 468
Abstract
The continuously growing penetration of renewable energy sources (RESs) in electrical networks provides increasing challenges and critical situations to be managed by worldwide system operators. Due to their features and variability, non-programmable RES power plants, whose increasing penetration reduces the inertia level of [...] Read more.
The continuously growing penetration of renewable energy sources (RESs) in electrical networks provides increasing challenges and critical situations to be managed by worldwide system operators. Due to their features and variability, non-programmable RES power plants, whose increasing penetration reduces the inertia level of the power system, may determine the instability effects on the grids, especially from the frequency and voltage regulation standpoints. The present study focuses on the support that advanced FACTS (Flexible Alternating Current Transmission System) devices, such as STATCOMs (Static Synchronous Compensators), can provide to the power system operation in terms of system inertia improvement, frequency stability, and voltage stability. In particular, a review of the scientific literature and practice is performed, with the aim of benchmarking the ongoing evolution of these technologies, also comparing them with different options based on synchronous condensers, synchronous condensers integrated with flywheels, and STATCOMs with supercapacitors. The outcome of the analysis consists of an updated evaluation of the state-of-the-art technological development in the field and of a comparison between different FACTSs with the purpose of identifying the most suitable solutions for different practical situations, also taking account of synergies across various options. This study includes an updated overview regarding the status of STATCOM installation in the Italian power grid. Full article
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<p>Power system structure evolution, from the past to the future.</p>
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<p>Frequency response with high and low inertia [<a href="#B10-electronics-13-04262" class="html-bibr">10</a>].</p>
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<p>Schematic diagram of the frequency regulation as a function of the intervention time [<a href="#B11-electronics-13-04262" class="html-bibr">11</a>].</p>
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<p><b>A</b> 3D Cad representation of the SCF layout [<a href="#B12-electronics-13-04262" class="html-bibr">12</a>].</p>
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<p>Frequency in the Sardinia network for single-phase fault in the 150 kV grid of central Sardinia. (<b>a</b>) All SCFSs and SCs are in normal operation; (<b>b</b>) SCFs are out of service [<a href="#B12-electronics-13-04262" class="html-bibr">12</a>].</p>
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<p>An overall representation of a VSM.</p>
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<p>VSM control structure and grid integration.</p>
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<p>Circuit diagram of a simple STATCOM.</p>
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<p>Cascade converter basic topology.</p>
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<p>Diagram of an E-STATCOM.</p>
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<p>Schematic diagram of an E-STATCOM.</p>
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<p>Scheme of the E-STATCOM topology with MMC power modules.</p>
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<p>Typical station layout of an E-STATCOM. Reprinted with permission from [<a href="#B26-electronics-13-04262" class="html-bibr">26</a>].</p>
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<p>Impact of different solutions to improve the system inertia following a frequency imbalance. Reprinted with permission from [<a href="#B26-electronics-13-04262" class="html-bibr">26</a>].</p>
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<p>Basic scheme of an LCC-HVDC inverter-side system.</p>
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<p>DC voltage waveforms shapes and valve conduction periods of an LCC-HVDC inverter system-station, with commutation failures highlighted in red.</p>
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<p>CFII improvement for an LCC-HVDC system equipped with a STATCOM. Reprinted with permission from [<a href="#B35-electronics-13-04262" class="html-bibr">35</a>].</p>
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<p>Schematization of the LCC-HVDC model used for the CFII study and based on CIGRE Benchmark [<a href="#B35-electronics-13-04262" class="html-bibr">35</a>].</p>
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<p>Map of SC/SCF installations in Italian transmission network [<a href="#B37-electronics-13-04262" class="html-bibr">37</a>,<a href="#B38-electronics-13-04262" class="html-bibr">38</a>].</p>
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<p>Localization of the five STATCOMs in the Italian transmission grid [<a href="#B38-electronics-13-04262" class="html-bibr">38</a>].</p>
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<p>Schematic single-line diagram of an H-SC setup (reprinted with permission from [<a href="#B51-electronics-13-04262" class="html-bibr">51</a>]).</p>
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<p>Comparison of costs and responsiveness for different technologies (modified/updated from [<a href="#B42-electronics-13-04262" class="html-bibr">42</a>]).</p>
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16 pages, 5009 KiB  
Article
Conductive-Polymer-Based Double-Network Hydrogels for Wearable Supercapacitors
by Bu Quan, Linjie Du, Zixuan Zhou, Xin Sun, Jadranka Travas-Sejdic and Bicheng Zhu
Gels 2024, 10(11), 688; https://doi.org/10.3390/gels10110688 - 24 Oct 2024
Viewed by 575
Abstract
In the field of contemporary epidermal bioelectronics, there is a demand for energy supplies that are safe, lightweight, flexible and robust. In this work, double-network polymer hydrogels were synthesized by polymerization of 3,4-ethylenedioxythiophene (EDOT) into a poly(vinyl alcohol)/poly(ethylene glycol diacrylate) (PVA/PEGDA) double-network hydrogel [...] Read more.
In the field of contemporary epidermal bioelectronics, there is a demand for energy supplies that are safe, lightweight, flexible and robust. In this work, double-network polymer hydrogels were synthesized by polymerization of 3,4-ethylenedioxythiophene (EDOT) into a poly(vinyl alcohol)/poly(ethylene glycol diacrylate) (PVA/PEGDA) double-network hydrogel matrix. The PEDOT-PVA/PEGDA double-network hydrogel shows both excellent mechanical and electrochemical performance, having a strain up to 498%, electrical conductivity as high as 5 S m−1 and specific capacitance of 84.1 ± 3.6 mF cm⁻2. After assembling two PEDOT-PVA/PEGDA double-network hydrogel electrodes with the free-standing boron cross-linked PVA/KCl hydrogel electrolyte, the formed supercapacitor device exhibits a specific capacitance of 54.5 mF cm⁻2 at 10 mV s−1, with an energy density of 4.7 μWh cm−2. The device exhibits excellent electrochemical stability with 97.6% capacitance retention after 3000 charging–discharging cycles. In addition, the hydrogel also exhibits great sensitivity to strains and excellent antifouling properties. It was also found that the abovementioned hydrogel can achieve stable signals under both small and large deformations as a flexible sensor. The flexible and antifouling PEDOT-PVA/PEGDA double-network hydrogel-based supercapacitor is a promising power storage device with potential applications in wearable electronics. Full article
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<p>(<b>A</b>) The “sandwich” structure of the PEDOT-PVA/PEGDA DN hydrogel-based supercapacitor. (<b>B</b>) The double-network structure of the PEDOT-PVA/PEGDA DN hydrogels. (<b>C</b>) Chemical polymerization of EDOT and chemical structures of PEGDA and PVA. (<b>D</b>) Optical photographs showing PEDOT-PVA/PEGDA DN hydrogels under compression, bending, stretching, twisting and torsional stretching.</p>
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<p>(<b>A</b>) CVs at different scan rates and (<b>B</b>) areal specific capacitances of PEDOT-PVA/PEGDA DN hydrogel electrodes with PEGDA content from 0 wt.% to 50 wt.% in 1 M KCl solution at a scan rate of 100 mV s<sup>−1</sup>. (<b>C</b>) CVs at different scan rates and (<b>D</b>) areal specific capacitances of PEDOT−PVA/PEGDA DN hydrogel electrodes with EDOT content from 10 wt.% to 28 wt.% in 1 M KCl solution at a scan rate of 100 mV s<sup>−1</sup>.</p>
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<p>(<b>A</b>) FTIR spectra of the dried PVA, PVA/PEGDA and PEDOT-PVA/PEGDA DN hydrogels. (<b>B</b>) Raman spectra of dried PEDOT-PVA/PEGDA DN hydrogel. (<b>C</b>) SEM morphologies of the fracture surfaces of the freeze-dried PEDOT-PVA/PEGDA DN hydrogels. (<b>D</b>) EDX elemental mapping images of freeze-dried PEDOT-PVA/PEGDA DN hydrogel: C element, O element and S element.</p>
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<p>Characterization of PEDOT-PVA/PEGDA DN hydrogel as supercapacitor electrode material. (<b>A</b>) CV curves at various scan rates in the potential window of 0–0.8 V. (<b>B</b>) Specific capacitance of the PEDOT-PVA/PEGDA DN hydrogel electrode at different scan rates. The error bars represent a standard deviation from 3 measurements. (<b>C</b>) GCD curves at a current density from 0.2 mA·cm<sup>−2</sup> to 1 mA cm<sup>−2</sup> in a potential window of 0–0.8 V. (<b>D</b>) Nyquist plot of PEDOT-PVA/PEGDA DN hydrogel in the frequency range of 0.1–100 kHz.</p>
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<p>(<b>A</b>) Tensile stress–strain curves of PEDOT-PVA/PEGDA DN hydrogel and PVA/PEGDA DN hydrogel. (<b>B</b>) Cyclic tensile test of PEDOT-PVA/PEGDA DN hydrogel up to 75% strain. (<b>C</b>) The change in the relative resistance (∆<span class="html-italic">R/R</span><sub>0</sub>) of PEDOT-PVA/PEGDA DN hydrogel at different strains (25%, 50%, 75%, 100%). (<b>D</b>) <span class="html-italic">GF</span> of PEDOT-PVA/PEGDA DN hydrogel at different tensile strain stages.</p>
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<p>Characterizations of PEDOT-PVA/PEGDA DN hydrogel-based supercapacitor device. (<b>A</b>) CV plots at different scan rates in the voltage window of 0–0.8 V. (<b>B</b>) Specific capacitance plot of PEDOT-PVA/PEGDA DN hydrogel-based supercapacitors at different scan rates. The error bars represent a standard deviation from 3 measurements. (<b>C</b>) GCD curves at a current density from 0.1 mA·cm<sup>−2</sup> to 0.5 mA cm<sup>−2</sup> in voltage windows of 0–0.8 V. (<b>D</b>) GCD curves at a current density of 1 mA cm<sup>−2</sup> in various voltage windows. (<b>E</b>) CV plots of the PEDOT-PVA/PEGDA DN hydrogel-based supercapacitor at different bending angles. (<b>F</b>) GCD curves of a single PEDOT-PVA/PEGDA DN hydrogel-based supercapacitor, two PEDOT-PVA/PEGDA DN hydrogel-based supercapacitors connected in parallel and two PEDOT-PVA/PEGDA DN hydrogel-based supercapacitors connected in series. (<b>G</b>) Capacitance retention (%) during GCD cyclic test at a current density of 3 mA cm<sup>−2</sup>. (<b>H</b>) Ragone plots of comparison with various PEDOT-based supercapacitors.</p>
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8 pages, 4392 KiB  
Article
Flexible All-Carbon Nanoarchitecture Built from In Situ Formation of Nanoporous Graphene Within “Skeletal-Capillary” Carbon Nanotube Networks for Supercapacitors
by Tao Chen, Hongyan Li, Jiaziyi Wang and Xilai Jia
Nanomaterials 2024, 14(20), 1683; https://doi.org/10.3390/nano14201683 - 21 Oct 2024
Viewed by 497
Abstract
It is difficult for carbonaceous materials to combine a large specific surface area with flexibility. Here, a flexible all-carbon nanoarchitecture based on the in situ growth of nanoporous graphene within “skeletal-capillary” carbon nanotube (CNT) networks has been achieved by a chemical vapor deposition [...] Read more.
It is difficult for carbonaceous materials to combine a large specific surface area with flexibility. Here, a flexible all-carbon nanoarchitecture based on the in situ growth of nanoporous graphene within “skeletal-capillary” carbon nanotube (CNT) networks has been achieved by a chemical vapor deposition (CVD) process. Multi-path long-range conductivity is established, and the porous graphene provides a large specific surface area for charge storage. The flexibility of the films allows them to be directly used as binder-free electrodes for supercapacitors. Since the polymeric binders are saved, the supercapacitors exhibit a higher overall storage density. Full article
(This article belongs to the Section 2D and Carbon Nanomaterials)
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<p>(<b>a</b>) Schematic fabrication of skeletal–capillary CNT/graphene composite. (<b>b</b>) SEM morphology of Mg(OH)<sub>2</sub> in skeletal–capillary CNT networks. (<b>c</b>) XRD spectra of skeletal–capillary CNTs before and after in situ growth of porous graphene. (<b>d</b>) Stress–strain curve (inset showing a digital photograph of the flexible film) and (<b>e</b>) electrical conductivity of the electrode film.</p>
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<p>(<b>a</b>,<b>b</b>) SEM and (<b>c</b>–<b>e</b>) TEM images of the skeletal–capillary CNT/graphene composite. (<b>f</b>) Schematic of the charge transport in the skeletal–capillary CNT/graphene composite.</p>
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<p>(<b>a</b>) CV plots. (<b>b</b>) Charge–discharge curves. (<b>c</b>) Cycling stability. (<b>d</b>) TEM image of the film electrode after 2000 cycles (inset: digital photograph).</p>
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13 pages, 2832 KiB  
Article
High-Performance Dual-Redox-Mediator Supercapacitors Based on Buckypaper Electrodes and Hydrogel Polymer Electrolytes
by Garbas A. Santos Junior, Kélrie H. A. Mendes, Sarah G. G. de Oliveira, Gabriel J. P. Tonon, Neide P. G. Lopes, Thiago H. R. da Cunha, Mario Guimarães Junior, Rodrigo L. Lavall and Paulo F. R. Ortega
Polymers 2024, 16(20), 2903; https://doi.org/10.3390/polym16202903 - 15 Oct 2024
Viewed by 846
Abstract
In recent years, the demand for solid, thin, and flexible energy storage devices has surged in modern consumer electronics, which require autonomy and long duration. In this context, hybrid supercapacitors have become strategic, and significant efforts are being made to develop cells with [...] Read more.
In recent years, the demand for solid, thin, and flexible energy storage devices has surged in modern consumer electronics, which require autonomy and long duration. In this context, hybrid supercapacitors have become strategic, and significant efforts are being made to develop cells with higher energy densities while preserving the power density of conventional supercapacitors. Motivated by these requirements, we report the development of a new high-performance dual-redox-mediator supercapacitor. In this study, cells were constructed using fully moldable buckypapers (BPs), composed of carbon nanotubes and cellulose nanofibers, as electrodes. We evaluated the compatibility of BPs with hydrogel polymer electrolytes, based on 1 mol L−1 H2SO4 and polyvinyl alcohol (PVA), supplemented with different redox species: methylene blue, indigo carmine, and hydroquinone. Solid cells were constructed containing two active redox species to maximize the specific capacity of each electrode. Considering the main results, the dual-redox-mediator supercapacitor exhibits high energy density of 32.0 Wh kg−1 (at 0.8 kW kg−1) and is capable of delivering 25.9 Wh kg−1 at high power demand (4.0 kW kg−1). Stability studies conducted over 10,000 galvanostatic cycles revealed that the PVA polymer matrix benefits the system by inhibiting the crossover of redox species within the cell. Full article
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<p>(<b>a</b>) Schematic representation and (<b>b</b>) image of the obtained CNT/CNF buckypaper. (<b>c</b>) Schematic of the HGPE buckypaper preparation process and (<b>d</b>) photography of the HGPE buckypaper. (<b>e</b>) Schematic representation of the cell configuration and (<b>f</b>) photography of the flexible solid-state supercapacitor device. Schematic representation of the fabricated symmetric SC device assembled using 0.8-HGPE buckypaper and redox mediator: (<b>g</b>) carmine indigo, (<b>h</b>) methylene blue, (<b>i</b>) hydroquinone.</p>
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<p>(<b>a</b>) Nyquist plot—inset shows the equivalent circuit; (<b>b</b>) GCD curves at J = 1 A g<sup>−1</sup>; (<b>c</b>) specific capacity of SCs based on HGPE electrolyte compared to the liquid electrolyte system at 1 A g<sup>−1</sup> (3.54 mA cm<sup>−2</sup>).</p>
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<p>Cyclic voltammetry for cells constructed with (<b>a</b>) 0.8-HGPE—the inset shows the magnified cyclic voltammetry—and 0.8-HGPE containing (<b>b</b>) methylene blue, (<b>c</b>) hydroquinone, and (<b>d</b>) indigo carmine. The inset also shows the dependence of peak currents on the square root of the scan rate for both anodic and cathodic potentials. The anodic peak current is represented by empty squares, while the cathodic peak current is represented by filled squares.</p>
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<p>Dual-redox-mediator solid-state SC: (<b>a</b>) schematic configuration; (<b>b</b>) GCD curves at different current densities, inset compares the system with 0.8-HGPE SC, at 1 A g<sup>−1</sup>; (<b>c</b>) cyclic voltammetry at different scan rates, inset compares the system with 0.8-HGPE SC, at 100 mV s<sup>−1</sup>; (<b>d</b>) specific capacity compared to 0.8-HGPE SC.</p>
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<p>Dual-redox-mediator solid-state SC: (<b>a</b>) evolution of the potential of the electrodes at different current densities (red line, positive electrode (methylene blue redox mediator); blue line, negative electrode (indigo carmine redox mediator)); (<b>b</b>) cycling stability for 10,000 cycles at 2.5 A g<sup>−1</sup> (8.84 mA cm<sup>−2</sup>) and coulombic efficiency; (<b>c</b>) comparison of the potential evolution of the electrodes at the 1st and the 10,000th cycle. (<b>d</b>) Ragone plot of the dual-redox-mediator solid-state SC, compared with some previously published systems [<a href="#B19-polymers-16-02903" class="html-bibr">19</a>,<a href="#B25-polymers-16-02903" class="html-bibr">25</a>,<a href="#B26-polymers-16-02903" class="html-bibr">26</a>,<a href="#B27-polymers-16-02903" class="html-bibr">27</a>,<a href="#B28-polymers-16-02903" class="html-bibr">28</a>,<a href="#B29-polymers-16-02903" class="html-bibr">29</a>,<a href="#B30-polymers-16-02903" class="html-bibr">30</a>,<a href="#B31-polymers-16-02903" class="html-bibr">31</a>].</p>
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29 pages, 5705 KiB  
Review
A Review of Green Aerogel- and Xerogel-Based Electrodes for Supercapacitors
by Ngo Tran, Hyung Wook Choi and Quang Nhat Tran
Polymers 2024, 16(19), 2848; https://doi.org/10.3390/polym16192848 - 9 Oct 2024
Viewed by 903
Abstract
The decline in fossil fuels on the earth has become a primary global concern which has urged mankind to explore other viable alternatives. The exorbitant use of fuels by an ever-increasing global population demands a huge production of energy from renewable sources. Renewable [...] Read more.
The decline in fossil fuels on the earth has become a primary global concern which has urged mankind to explore other viable alternatives. The exorbitant use of fuels by an ever-increasing global population demands a huge production of energy from renewable sources. Renewable energy sources like the sun, wind, and tides have been established as promising substitutes for fossil fuels. However, the availability of these renewable energy sources is dependent on weather and climatic conditions. Thus, this goal can only be achieved if the rate of energy production from renewable sources is enhanced under favorable weather conditions and can be stored using high energy storing devices for future utilization. The energy from renewable sources is principally stored in hydropower plants, superconducting magnetic energy storage systems, and batteries. Full article
(This article belongs to the Special Issue Advances in Multifunctional Polymer-Based Nanocomposites, 2nd Edition)
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<p>Relation between the pH and the amount of catalyst [<a href="#B41-polymers-16-02848" class="html-bibr">41</a>].</p>
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<p>Schematic of the synthesis of the aerogels [<a href="#B42-polymers-16-02848" class="html-bibr">42</a>].</p>
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<p>SEM image of the carbon aerogel.</p>
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<p>Schematic of the fabrication process of CNF aerosol/rGO/CNT electrodes [<a href="#B79-polymers-16-02848" class="html-bibr">79</a>].</p>
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<p>Synthesis of carbon fiber aerogel from natural cotton.</p>
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<p>Schematic representation of the preparation of aerogels from wood [<a href="#B85-polymers-16-02848" class="html-bibr">85</a>].</p>
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<p>Schematic representation of the synthesis of cattail aerogels [<a href="#B93-polymers-16-02848" class="html-bibr">93</a>].</p>
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<p>Process of synthesis of aerogel from jackfruit and durian [<a href="#B94-polymers-16-02848" class="html-bibr">94</a>].</p>
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<p>Schematic representation of xerogels derived from MOF [<a href="#B110-polymers-16-02848" class="html-bibr">110</a>].</p>
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<p>Schematic representation of the synthesis procedure of aerogel and xerogel [<a href="#B117-polymers-16-02848" class="html-bibr">117</a>].</p>
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33 pages, 2403 KiB  
Review
Hydrothermal Carbonization of Biomass for Electrochemical Energy Storage: Parameters, Mechanisms, Electrochemical Performance, and the Incorporation of Transition Metal Dichalcogenide Nanoparticles
by Manuel Prieto, Hangbo Yue, Nicolas Brun, Gary J. Ellis, Mohammed Naffakh and Peter S. Shuttleworth
Polymers 2024, 16(18), 2633; https://doi.org/10.3390/polym16182633 - 18 Sep 2024
Cited by 1 | Viewed by 1268
Abstract
Given the pressing climate and sustainability challenges, shifting industrial processes towards environmentally friendly practices is imperative. Among various strategies, the generation of green, flexible materials combined with efficient reutilization of biomass stands out. This review provides a comprehensive analysis of the hydrothermal carbonization [...] Read more.
Given the pressing climate and sustainability challenges, shifting industrial processes towards environmentally friendly practices is imperative. Among various strategies, the generation of green, flexible materials combined with efficient reutilization of biomass stands out. This review provides a comprehensive analysis of the hydrothermal carbonization (HTC) process as a sustainable approach for developing carbonaceous materials from biomass. Key parameters influencing hydrochar preparation are examined, along with the mechanisms governing hydrochar formation and pore development. Then, this review explores the application of hydrochars in supercapacitors, offering a novel comparative analysis of the electrochemical performance of various biomass-based electrodes, considering parameters such as capacitance, stability, and textural properties. Biomass-based hydrochars emerge as a promising alternative to traditional carbonaceous materials, with potential for further enhancement through the incorporation of extrinsic nanoparticles like graphene, carbon nanotubes, nanodiamonds and metal oxides. Of particular interest is the relatively unexplored use of transition metal dichalcogenides (TMDCs), with preliminary findings demonstrating highly competitive capacitances of up to 360 F/g when combined with hydrochars. This exceptional electrochemical performance, coupled with unique material properties, positions these biomass-based hydrochars interesting candidates to advance the energy industry towards a greener and more sustainable future. Full article
(This article belongs to the Special Issue Carbonized Polymers and Their Functional Applications)
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<p>Temperature variation scenarios for the next 100 years [<a href="#B7-polymers-16-02633" class="html-bibr">7</a>], where RCP is ‘Representative Concentration Pathway’. (<b>a</b>) represents CO<sub>2</sub> concentration scenarios and (<b>b</b>) represents global temperature increase scenarios. The dashed line indicates pre-industrial CO<sub>2</sub> concentration.</p>
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<p>Schematic on hydrothermal carbonization precursors, products, and applications.</p>
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<p>Mechanistic routes of cellulose and hemicellulose breakdown under hydrothermal conditions. Scheme constructed from information in references [<a href="#B76-polymers-16-02633" class="html-bibr">76</a>,<a href="#B77-polymers-16-02633" class="html-bibr">77</a>,<a href="#B80-polymers-16-02633" class="html-bibr">80</a>].</p>
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<p>Lignin hydrothermal mechanism. Adapted from [<a href="#B19-polymers-16-02633" class="html-bibr">19</a>] with permission from Elsevier.</p>
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<p>Energy storage mechanisms in a supercapacitor (adapted from [<a href="#B159-polymers-16-02633" class="html-bibr">159</a>]).</p>
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21 pages, 4561 KiB  
Article
Optimizing EV Powertrain Performance and Sustainability through Constraint Prioritization in Nonlinear Model Predictive Control of Semi-Active Bidirectional DC-DC Converter with HESS
by P. S. Praveena Krishna, Jayalakshmi N. Sabhahit, Vidya S. Rao, Amit Saraswat, Hannah Chaplin Laugaland and Pramod Bhat Nempu
Sustainability 2024, 16(18), 8123; https://doi.org/10.3390/su16188123 - 18 Sep 2024
Cited by 1 | Viewed by 794
Abstract
The global transportation sector is rapidly shifting towards electrification, aiming to create more sustainable environments. As a result, there is a significant focus on optimizing performance and increasing the lifespan of batteries in electric vehicles (EVs). To achieve this, the battery pack must [...] Read more.
The global transportation sector is rapidly shifting towards electrification, aiming to create more sustainable environments. As a result, there is a significant focus on optimizing performance and increasing the lifespan of batteries in electric vehicles (EVs). To achieve this, the battery pack must operate with constant current charging and discharging modes of operation. Further, in an EV powertrain, maintaining a constant DC link voltage at the input stage of the inverter is crucial for driving the motor load. To satisfy these two conditions simultaneously during the energy transfer, a hybrid energy storage system (HESS) consisting of a lithium–ion battery and a supercapacitor (SC) connected to the semi-active topology of the bidirectional DC–DC converter (SAT-BDC) in this research work. However, generating the duty cycle for the switches to regulate the operation of SAT-BDC is complex due to the simultaneous interaction of the two mentioned constraints: regulating the DC link voltage by tracking the reference and maintaining the battery current at a constant value. Therefore, this research aims to efficiently resolve the issue by incorporating a highly flexible nonlinear model predictive control (NMPC) to control the switches of SAT-BDC. Furthermore, the converter system design is tested for operational performance using MATLAB 2022B with the battery current and the DC link voltage with different priorities. In the NMPC approach, these constraints are carefully evaluated with varying prioritizations, representing a crucial trade-off in optimizing EV powertrain operation. The results demonstrate that battery current prioritization yields better performance than DC link voltage prioritization, extending the lifespan and efficiency of batteries. Thus, this research work further aligns with the conceptual realization of the sustainability goals by minimizing the environmental impact associated with battery production and disposal. Full article
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<p>Ragone plot to demonstrate the importance of lithium–ion battery/SC HESS. Red dashed box shows that it is the HESS which is selected for the research work.</p>
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<p>The different battery/SC configuration approaches for EV powertrain (<b>a</b>–<b>d</b>).</p>
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<p>Electrical equivalent cell model of lithium–ion battery.</p>
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<p>(<b>a</b>) Structure; (<b>b</b>) Electrical equivalent of the model of the supercapacitor.</p>
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<p>Generated variable current sequence at the DC link.</p>
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<p>Semi-active topology of bidirectional DC–DC converter for HESS operation.</p>
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<p>Schematic representation of the proposed system configuration.</p>
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<p>Optimal open-loop solution with initial conditions A, B, and C, and corresponding waveforms (<b>a</b>) current waveforms; (<b>b</b>) output DC-link voltage waveforms; (<b>c</b>) duty cycle; and (<b>d</b>) Epsilon, the slack variable.</p>
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<p>Optimal closed-loop operation with the lithium–ion battery without supercapacitor integration: (<b>a</b>) Current waveforms and (<b>b</b>) output DC-link voltage waveforms; (<b>c</b>) duty cycle of SAT-BDC switches; and (<b>d</b>) Epsilon, the slack variable.</p>
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<p>Closed-loop operation of SAT-BDC with HESS with the integration of supercapacitor: (<b>a)</b> Current waveforms obtained; (<b>b</b>) DC-link voltage waveform; (<b>c</b>) obtained duty cycle of the SAT-BDC switches; and (<b>d</b>) Slack variable and its variation.</p>
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<p>Closed-loop operation of SAT-BDC with HESS using voltage prioritization throughout the time horizon: (<b>a</b>) Inductor current and variable output current waveforms; (<b>b</b>) DC-link voltage waveform tracking reference; (<b>c</b>) duty cycle for SAT-BDC switch control; (<b>d</b>) Slack variable and its variation.</p>
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<p>Closed-loop operation of SAT-BDC with HESS using current prioritization: (<b>a</b>) Inductor current and variable output current waveforms; (<b>b</b>) DC-link voltage waveform tracking reference; (<b>c</b>) duty cycle for SAT-BDC switch control; (<b>d</b>) Slack variable and its variation.</p>
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24 pages, 5937 KiB  
Review
Recent Advances in Wearable Textile-Based Triboelectric Nanogenerators
by Sivasubramaniyan Neelakandan, S. R. Srither, N. R. Dhineshbabu, Suman Maloji, Oscar Dahlsten, Ramachandran Balaji and Ragini Singh
Nanomaterials 2024, 14(18), 1500; https://doi.org/10.3390/nano14181500 - 15 Sep 2024
Viewed by 1271
Abstract
We review recent results on textile triboelectric nanogenerators (T-TENGs), which function both as harvesters of mechanical energy and self-powered motion sensors. T-TENGs can be flexible, breathable, and lightweight. With a combination of traditional and novel manufacturing methods, including nanofibers, T-TENGs can deliver promising [...] Read more.
We review recent results on textile triboelectric nanogenerators (T-TENGs), which function both as harvesters of mechanical energy and self-powered motion sensors. T-TENGs can be flexible, breathable, and lightweight. With a combination of traditional and novel manufacturing methods, including nanofibers, T-TENGs can deliver promising power output. We review the evolution of T-TENG device structures based on various textile material configurations and fabrication methods, along with demonstrations of self-powered systems. We also provide a detailed analysis of different textile materials and approaches used to enhance output. Additionally, we discuss integration capabilities with supercapacitors and potential applications across various fields such as health monitoring, human activity monitoring, human–machine interaction applications, etc. This review concludes by addressing the challenges and key research questions that remain for developing viable T-TENG technology. Full article
(This article belongs to the Section Nanofabrication and Nanomanufacturing)
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<p>Four basic operation modes of TENGs. (<b>a</b>) Contact Separation. (<b>b</b>) Single Electrode. (<b>c</b>) Lateral Sliding. (<b>d</b>) Freestanding Triboelectric mode. Loads are depicted as resistors, connected to electrodes (or ground). The electrodes are coated on tribo-positive and tribo-negative materials, which move relative to each other.</p>
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<p>Demonstration of TS-TENG sewn on clothes for mechanical energy harvesting. (<b>a</b>) The output voltage and (<b>b</b>) current of TS-TENG device (10 cm × 12 cm). (<b>c</b>) TS-TENG was connected to a wearable night-time running light. (<b>d</b>) Night running light was illuminated by the TS-TENG as the person swinging his arm. (<b>e</b>) Digital watch was connected to the TS-TENG without batteries. (<b>f</b>) TS-TENG powered a digital watch [<a href="#B45-nanomaterials-14-01500" class="html-bibr">45</a>]. Reproduced with permission from [<a href="#B45-nanomaterials-14-01500" class="html-bibr">45</a>] (Copyright 2018, Royal Society of Chemistry).</p>
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<p>(<b>a</b>) Schematic image of a cloth-based TENG device with a grating structure. (<b>b</b>) SEM image of the surface of nylon cloth microstructure. (<b>c</b>) photographic image of the grid structure of cloth TENG. (<b>d</b>) Fabrication process of the T-TENG. Reproduced with permission from [<a href="#B48-nanomaterials-14-01500" class="html-bibr">48</a>] (Copyright 2015, American Chemical Society).</p>
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<p>Structure design of fully cloth-based T-TENGs harvesting mechanical energy from human movements (<b>a</b>) schematic representative of T-TENG sewn on cloth, inset: photographic image of wearable T-TENG. (<b>b</b>) Schematic illustration of the fabrication process. (<b>c</b>,<b>d</b>) are the SEM images of nylon and polyester fabrics; the insets in (<b>c</b>,<b>d</b>) are the corresponding partial enlargements of the respective nylon and polyester fabrics. Reproduced with permission from [<a href="#B50-nanomaterials-14-01500" class="html-bibr">50</a>] (Copyright 2020, American Chemical Society).</p>
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<p>SE mode of fiber/yarn-TENG. (<b>a</b>) Fiber-TENG based on silicone-coated stainless steel yarns, reproduced with permission from [<a href="#B58-nanomaterials-14-01500" class="html-bibr">58</a>] (Copyright 2017, Wiley); (<b>b</b>) core–shell-yarn-based triboelectric nanogenerator by spinning PU fiber with stainless steel fibers, reproduced with permission from [<a href="#B59-nanomaterials-14-01500" class="html-bibr">59</a>] (Copyright 2017, American Chemical Society).</p>
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<p>CS mode of fiber/yarn-TENG: (<b>a</b>) fiber-TENG prepared by the coating of CNT/PMMA/PDMS on silicone rubber tube, reproduced with permission from [<a href="#B60-nanomaterials-14-01500" class="html-bibr">60</a>] (Copyright 2017, Royal Society of Chemistry); (<b>b</b>) the fabrication process of the woven-structured TENG, reproduced with permission from [<a href="#B61-nanomaterials-14-01500" class="html-bibr">61</a>] (Copyright 2021, Elsevier).</p>
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<p>Fabrication of the 2DW-WTNG core shell structure. (<b>a</b>) The schematic diagram of the weaving process. Scanning electron microscope images of nylon (<b>b</b>) and polyester (<b>c</b>) fabrics, respectively. (<b>d</b>,<b>e</b>) Optical image of nylon coated copper wire and polyester coated steel wire. (<b>f</b>) 2DW-WTNG optical image. Reproduced with permission from [<a href="#B64-nanomaterials-14-01500" class="html-bibr">64</a>] (Copyright 2019, Springer Nature).</p>
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<p>Fabrication of the 2DW-WTNG core shell structure. (<b>a</b>) The schematic diagram of the weaving process. Scanning electron microscope images of nylon (<b>b</b>) and polyester (<b>c</b>) fabrics, respectively. (<b>d</b>,<b>e</b>) Optical image of nylon coated copper wire and polyester coated steel wire. (<b>f</b>) 2DW-WTNG optical image. Reproduced with permission from [<a href="#B64-nanomaterials-14-01500" class="html-bibr">64</a>] (Copyright 2019, Springer Nature).</p>
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<p>Power generation characteristics of 2DW-WTNG. (<b>a</b>) Illustrating the process of generating electricity. (<b>b</b>,<b>c</b>) 2DW-WTNG output voltage and current. (<b>d</b>) Power density at different load resistances [<a href="#B64-nanomaterials-14-01500" class="html-bibr">64</a>]. Reproduced with permission from [<a href="#B64-nanomaterials-14-01500" class="html-bibr">64</a>] (Copyright 2019, Springer Nature).</p>
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<p>(<b>a</b>) Schematic structure of laminated fabrics and TENG textiles. (<b>b</b>) Optical image of TENG textile and freestanding laminate fabric is sewn on cloth for energy harvesting from human motion. Reproduced with permission from [<a href="#B65-nanomaterials-14-01500" class="html-bibr">65</a>] (Copyright 2019, Elsevier).</p>
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<p>Schematic illustration and fabrication procedure of T-TENG. (<b>a</b>) Fabrication process of the liquid metal/polymer core/shell fiber (LCF) structure. (<b>b</b>–<b>e</b>) Digital photograph (<b>b</b>) original ultra-fine hollow fiber polymer; (<b>c</b>) hollow fiber polymer after pumping process, (<b>d</b>) T-TENG weaving and (<b>e</b>) tri-color PTFE fibers. Reproduced with permission [<a href="#B68-nanomaterials-14-01500" class="html-bibr">68</a>] (Copyright 2020, Elsevier).</p>
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<p>Working principle and electrical output of the T-TENG structure. (<b>a</b>) operation of the device in a contact separation mode. (<b>b</b>–<b>d</b>) electrical outputs, including V<sub>oc</sub>, I<sub>sc</sub> and power density at different load resistances. Reproduced with permission from [<a href="#B68-nanomaterials-14-01500" class="html-bibr">68</a>] (Copyright 2020, Elsevier).</p>
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<p>Illustration of the fabrication process of PVDF/GQD composite NFs by the ES method and diagram of the TENG device structure. Structure of N-doped GQDs and their luminescence images under UV excitation (λ ~266 nm). The inset shows high-resolution TEM images of GQDs. Reproduced with permission from [<a href="#B82-nanomaterials-14-01500" class="html-bibr">82</a>] (Copyright 2019, Elsevier).</p>
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<p>Schematic representation and electrochemical characterization of the yarn SC. (<b>a</b>) Schematic view of the structure of the yarn SC. (<b>b</b>) The optical image of the fabric SC woven by the PA yarn and the yarn SC. (<b>c</b>) An optical image showing the fabric SC hanging on a pencil. (<b>d</b>) CV curves of the yarn SC at different scan rates. (<b>e</b>) Charge–discharge profiles at different current loads. (<b>f</b>) Charge–discharge curve data bending from 0−180° degrees. (<b>g</b>) Stability cycles of the yarn SC. (<b>h</b>) CV curves in series connection. (<b>i</b>) Charge–discharge profiles in series connection. Reproduced with permission from [<a href="#B84-nanomaterials-14-01500" class="html-bibr">84</a>] (Copyright 2020, American Chemical Society).</p>
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<p>(<b>a</b>) The application scenarios of HITWS. (<b>b</b>) The structure and working principle of HITWS. Reproduced with permission from [<a href="#B92-nanomaterials-14-01500" class="html-bibr">92</a>] (Copyright 2024, Elsevier).</p>
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64 pages, 16567 KiB  
Review
Composite Track-Etched Membranes: Synthesis and Multifaced Applications
by Anastassiya A. Mashentseva, Duygu S. Sutekin, Saniya R. Rakisheva and Murat Barsbay
Polymers 2024, 16(18), 2616; https://doi.org/10.3390/polym16182616 - 15 Sep 2024
Cited by 1 | Viewed by 1035
Abstract
Composite track-etched membranes (CTeMs) emerged as a versatile and high-performance class of materials, combining the precise pore structures of traditional track-etched membranes (TeMs) with the enhanced functionalities of integrated nanomaterials. This review provides a comprehensive overview of the synthesis, functionalization, and applications of [...] Read more.
Composite track-etched membranes (CTeMs) emerged as a versatile and high-performance class of materials, combining the precise pore structures of traditional track-etched membranes (TeMs) with the enhanced functionalities of integrated nanomaterials. This review provides a comprehensive overview of the synthesis, functionalization, and applications of CTeMs. By incorporating functional phases such as metal nanoparticles and conductive nanostructures, CTeMs exhibit improved performance in various domains. In environmental remediation, CTeMs effectively capture and decompose pollutants, offering both separation and detoxification. In sensor technology, they have the potential to provide high sensitivity and selectivity, essential for accurate detection in medical and environmental applications. For energy storage, CTeMs may be promising in enhancing ion transport, flexibility, and mechanical stability, addressing key issues in battery and supercapacitor performance. Biomedical applications may benefit from the versality of CTeMs, potentially supporting advanced drug delivery systems and tissue engineering scaffolds. Despite their numerous advantages, challenges remain in the fabrication and scalability of CTeMs, requiring sophisticated techniques and meticulous optimization. Future research directions include the development of cost-effective production methods and the exploration of new materials to further enhance the capabilities of CTeMs. This review underscores the transformative potential of CTeMs across various applications and highlights the need for continued innovation to fully realize their benefits. Full article
(This article belongs to the Section Polymer Composites and Nanocomposites)
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<p>Symmetric and asymmetric polymeric nanochannels fabricated using the track etching technique (adapted with permission from ref. [<a href="#B72-polymers-16-02616" class="html-bibr">72</a>]. Copyright 2021 American Chemical Society).</p>
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<p>General synthesis routes for the preparation of CTeMs.</p>
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<p>The scheme of chitosan ECD in the pores of PC TeM (adapted with permission from ref. [<a href="#B100-polymers-16-02616" class="html-bibr">100</a>]. Copyright 2005 Royal Society of Chemistry).</p>
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<p>SEM images of the surface of CTeM with copper NTs obtained using various types of reducing agents (adapted with permission from ref. [<a href="#B122-polymers-16-02616" class="html-bibr">122</a>]. Copyright 2023 MDPI with license under CC BY 4.0).</p>
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<p>Scheme of Cu<sub>2</sub>O/ZnO@PET CTeM formation by galvanic substitution and SEM images of the studied composites (adapted with permission from ref. [<a href="#B124-polymers-16-02616" class="html-bibr">124</a>]. Copyright 2022 MDPI with license under CC BY 4.0).</p>
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<p>(<b>a</b>) Diagram showing the effects of different radiation dose rates on metal nanoparticle size (top panel). Diagram illustrating how the reduction rate affects the synthesis of bimetallic nanoparticles (bottom panel). Schematic representation of metal ion reduction in solution through ionizing radiation in the presence of a stabilizer (left panel). The blue cloudy shell around the ions or nanoparticles represents the capping/stabilizing organic phase, such as grafted polymer chains in a functionalized TeM. (<b>b</b>) Production methodology including grafting, sorption, and radiolysis for the synthesis of copper nanostructure-containing CTeMs using e-beam and gamma rays. The digital pictures and SEM images of the composite membranes are shown on the right ((<b>b</b>) is adapted with permission from ref. [<a href="#B128-polymers-16-02616" class="html-bibr">128</a>]. Copyright 2023 MDPI with license under CC BY 4.0).</p>
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<p>SEM images of Ar ion beam-etched PET TeMs with embedded Au microtubes (<b>a</b>), Ni dendrite structures on the unetched surface (<b>b</b>). SEM images (<b>c</b>), EDS spectra and mapping (<b>d</b>,<b>e</b>), and XRD patterns (<b>f</b>) of the core-shell Au/Ni microtubesand elemental composition (<b>j</b>). Ni@Au with gold needles: SEM (<b>g</b>), TEM (<b>h</b>), EDX-mapping (<b>i</b>), and elemental composition (<b>k</b>). Digital photographs and SEM images of the composite membranes are also shown on the right (adapted with permission from ref. [<a href="#B104-polymers-16-02616" class="html-bibr">104</a>] Copyright 2022 MDPI with license under CC BY 4.0).</p>
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<p>(<b>a</b>) UV spectra for reaction mixture, (<b>b</b>) calculated apparent rate constants for Ag and Au CTeMs (adapted with permission from ref. [<a href="#B116-polymers-16-02616" class="html-bibr">116</a>]. Copyright 1990 IOP Publishing Ltd.).</p>
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<p>(<b>a</b>) The UV vis spectra of reduction of <span class="html-italic">p</span>-NP by Pd-based CTeMs synthesized by green approach, (<b>b</b>) graph of ln(a/a<sub>0</sub>) vs. time for the reduction in <span class="html-italic">p</span>-NP in the presence of Pd-based CTeMs (adapted with permission from ref. [<a href="#B156-polymers-16-02616" class="html-bibr">156</a>]. Copyright 1999 Royal Society of Chemistry).</p>
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<p>Mechanistic pathway of <span class="html-italic">p</span>-nitrophenol reduction on copper-based CTeM in the presence of NaBH<sub>4</sub>: Steps of the Langmuir–Hinshelwood mechanism, including adsorption, intermediate formation, and product desorption, involved in the catalytic reduction of <span class="html-italic">p</span>-nitrophenol on nanocatalyst surface (adapted with permission from ref. [<a href="#B32-polymers-16-02616" class="html-bibr">32</a>]. Copyright 2020 MDPI with license under CC BY 4.0).</p>
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<p>The mechanism of Congo red decomposition in the presence of NaBH<sub>4</sub> (adapted with permission from ref. [<a href="#B30-polymers-16-02616" class="html-bibr">30</a>]. Copyright 2016 Elsevier).</p>
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<p>The change in color from blue to colorless was visually noted as a sign of MB (0.1 mg/L) degradation by the composite catalyst over various periods (adapted with permission from ref. [<a href="#B143-polymers-16-02616" class="html-bibr">143</a>] Copyright 2021 MDPI with license under CC BY 4.0).</p>
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<p>The mechanism for the photocatalytic decomposition of MB dye under UV irradiation in the presence of Cu@PET-<span class="html-italic">g</span>-PAA CTeMs (adapted with permission from ref. [<a href="#B128-polymers-16-02616" class="html-bibr">128</a>] Copyright 2023 MDPI with license under CC BY 4.0).</p>
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<p>The reusability of the Pd_Asc@PVP-<span class="html-italic">g</span>-PET catalyst: change in the degradation degree (D, %) of MTZ in repeated use (adapted with permission from ref. [<a href="#B66-polymers-16-02616" class="html-bibr">66</a>] Copyright 2023 from the Royal Society of Chemistry).</p>
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<p>Schematic representation of installation (adapted with permission from ref [<a href="#B185-polymers-16-02616" class="html-bibr">185</a>]. Copyright 2021 Springer Nature).</p>
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<p>(<b>a</b>) Impact of contact time on the sorption of As (III) (50 ppm) by the composite TeMs, (<b>b</b>) dependence of As (III) removal (%) to pH during 420 min (<b>c</b>) (adapted with permission from ref. [<a href="#B119-polymers-16-02616" class="html-bibr">119</a>] Copyright 2021 MDPI with license under CC BY 4.0).</p>
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<p>Sorption of Pb(II) as a function of solution pH (Pb(II) concentration: 50 ppm; contact time: 120 min) (<b>a</b>); pH point zero charge (pH<sub>PZC</sub>) plot (<b>b</b>); effect of contact time on the sorption of Pb(II) ions (<b>c</b>) and equilibrium sorption capacity (<b>d</b>) (adapted with permission from ref. [<a href="#B122-polymers-16-02616" class="html-bibr">122</a>] Copyright 2023 MDPI with license under CC BY 4.0).</p>
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<p>SEM of a nanoparticle composite membrane (nominal pore diameter 1000 nm; nanoparticle diameter 200–230 nm): filled pores before coupling reaction over-night (<b>a</b>), cross-section after coupling reaction and complete washing (<b>b</b>), cross-section detail demonstrating the distance between neighbored bound nanoparticles (<b>c</b>) and and depiction of the mass transfer and catalytic reaction behavior for the conventional enzyme membrane (<b>above</b>) and the nanoparticle composite enzyme membrane (<b>below</b>) (adapted with permission from ref. [<a href="#B204-polymers-16-02616" class="html-bibr">204</a>] Copyright 2006 Elsevier).</p>
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<p>SEM images of the polycarbonate porous membranes without PNIPAM grafts (<b>a</b>,<b>b</b>), with PNIPAM grafts (<b>c</b>,<b>d</b>), without PNIPAM grafts after silver nanoparticles synthesized in situ (<b>e</b>), grafted with PNIPAM and after silver nanoparticles synthesized in situ (<b>f</b>–<b>h</b>) (adapted with permission from ref. [<a href="#B206-polymers-16-02616" class="html-bibr">206</a>]. Copyright 2014 Wiley with license under CC BY 3.0).</p>
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<p>The preparation of arrays of copper ultramicrowires (CuUWs) by using porous membranes as templates track-etched polycarbonate (PC) and anodized aluminum oxide (AAO) for efficient substrates for surface enhanced Raman spectroscopy (SERS) (adapted with permission from ref. [<a href="#B208-polymers-16-02616" class="html-bibr">208</a>]. Copyright 2021 MDPI with license under CC BY 4.0).</p>
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<p>SEM image of metallized TMs surface elongated to deformation of 5% (<b>a</b>) and 15% (<b>b</b>), SERS spectra of malachite green molecules adsorbed on a surface metallized with a silver (<b>c</b>), and gold (<b>d</b>) (adapted with permission from ref. [<a href="#B209-polymers-16-02616" class="html-bibr">209</a>]. Copyright 2022 AIP Publishing).</p>
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<p>(<b>a</b>) SEM top view of the TeM, (<b>b</b>) Ag-NWs bundles array (Ag-NWs diameter of 100 nm and their length of 12 µm), and (<b>c</b>) mechanism of action for surface-enhanced Raman scattering (SERS) with metal nanowires (NWs) grown in pores of polymer TeMs and enhancement of Raman signal for 4-Mercaptophenylboronic acid (4-MPBA) adsorbed on the “wet” (green line) and “dry” (red line) substrates) (adapted with permission from ref. [<a href="#B87-polymers-16-02616" class="html-bibr">87</a>]. Copyright 2021 MDPI with license under CC BY 4.0).</p>
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<p>The SEM images illustrating metasurfaces featuring vertically standing nanowires (NWs) with varying diameters and surface pore densities: the substrate surface with NWs of 200 (<b>a</b>,<b>b</b>), 100 (<b>c</b>,<b>d</b>), and 60 nm (<b>e</b>,<b>f</b>) diameter and 10 µm length. (adapted with permission from ref. [<a href="#B137-polymers-16-02616" class="html-bibr">137</a>]. Copyright 2022 MDPI with license under CC BY 4.0).</p>
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<p>(<b>a</b>) Scheme of SERS experiment, (<b>b</b>) SERS spectra for various concentrations of MB, and (<b>c</b>) SERS intensity depending on the concentration of the 1624 cm<sup>−1</sup> shift (adapted with permission from ref. [<a href="#B130-polymers-16-02616" class="html-bibr">130</a>]. Copyright 2021 Elsevier).</p>
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<p>SEM images and SEM-EDX results of Ni-Au nanotubes (<b>a</b>) and their SERS spectra for different concentrations of R6G (<b>b</b>) (adapted with permission from ref. [<a href="#B214-polymers-16-02616" class="html-bibr">214</a>] Copyright 2022 Elsevier).</p>
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<p>Top view of the NTNW before surface etching (<b>a</b>), SEM top view image of NiCo-LDH@Ni-NTNWs after 120 sec of hydroxide electrodeposition (<b>b</b>) and schematic representation of the NTNW electrode fabrication (<b>c</b>) (adapted with permission from ref. [<a href="#B216-polymers-16-02616" class="html-bibr">216</a>]. Copyright 2021 Elsevier).</p>
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<p>(<b>a</b>) Construction of PI/PEO/LiTFSI composite, (<b>b</b>) cross-sectional SEM image with zoomed-in aligned nanopores, (<b>c</b>) SEM image of PI/PEO/LiTFSI composite, (<b>d</b>) cross-sectional SEM image of the PI membrane (adapted with permission from ref. [<a href="#B219-polymers-16-02616" class="html-bibr">219</a>]. Copyright 2019 Springer Nature).</p>
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<p>(<b>a</b>) SEM image of an SK Innovation separator, (<b>b</b>) surface of a PET TeM with an average pore diameter of approximately 100 nm and a pore density of 2.5 × 10<sup>9</sup> cm<sup>−2</sup>, and (<b>c</b>) cross-section of the PET TeM (adapted with permission from ref. [<a href="#B227-polymers-16-02616" class="html-bibr">227</a>]. Copyright 2021 IOP Publishing Ltd. with license under CC 4.0).</p>
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<p>The cycling performance of lithium-sulfur coin cells utilizing PET etched ion track membranes, placed between two separators from SK Innovation, was assessed under a constant pore density (10<sup>9</sup> cm<sup>−2</sup>) while varying the pore diameter. (<b>a</b>) Solid symbols represent charge capacities, and empty symbols indicate discharge capacities; (<b>b</b>) Coulombic efficiency as a function of pore size (adapted with permission from ref. [<a href="#B227-polymers-16-02616" class="html-bibr">227</a>]. Copyright 2021 IOP Publishing Ltd. with license under CC 4.0).</p>
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<p>Schematic representation of the PI/hBN separator fabrication process (adapted with permission from ref. [<a href="#B236-polymers-16-02616" class="html-bibr">236</a>]. Copyright 2022 American Chemical Society).</p>
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<p>Images of various separators after the addition of electrolyte on the surfaces: (<b>a</b>) PP, (<b>b</b>) PI TeM, and (<b>c</b>) PI/hBN. Contact angle experiments between separators and electrolytes: (<b>d</b>) PP, (<b>e</b>) PI TeM, and (<b>f</b>) PI/hBN separator (adapted with permission from ref. [<a href="#B236-polymers-16-02616" class="html-bibr">236</a>]. Copyright 2022 American Chemical Society).</p>
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<p>Gas separation mechanism of PdPt BNP decorated track-etched polymer membranes and gas separation performance of the UV functionalized PdPt BNP dipped PET membrane series (adapted with permission from ref. [<a href="#B241-polymers-16-02616" class="html-bibr">241</a>]. Copyright 2024 Royal Society of Chemistry with license under CC BY-NC 3.0).</p>
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<p>(<b>a</b>) schematic of AuNTs synthesis and (<b>b</b>) DNA biosensor setup using AuNTs electrodes. Biosensor includes working electrode (WE), reference electrode (RE), and counter electrode (CE). AuNTs array electrodes showed improved electron transfer compared to bare Au electrodes. Biosensor detected DNA in linear range of 0.01 ng/µL to 100 ng/µL, with a limit of detection of 0.05 ng/µL (adapted with permission from ref. [<a href="#B33-polymers-16-02616" class="html-bibr">33</a>]. Copyright 2016 Elsevier).</p>
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<p>Measures for the further development and adaptation of CTeMs. The figure summarizes critical steps to advance CTeM technology, including enhanced fabrication techniques, material optimization, integration of smart materials, scaling up production, focus on promising applications, sensor technology improvements, ensuring safety and regulatory compliance, fostering interdisciplinary collaboration, and exploring technological integration.</p>
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12 pages, 5090 KiB  
Article
Controllable Synthesis of Manganese Organic Phosphate with Different Morphologies and Their Derivatives for Supercapacitors
by Jingwen Zhao, Qingling Jing, Ting Zhou, Xinhuan Zhang, Wenting Li and Huan Pang
Molecules 2024, 29(17), 4186; https://doi.org/10.3390/molecules29174186 - 4 Sep 2024
Viewed by 571
Abstract
Morphological control of metal-organic frameworks (MOFs) at the micro/nanoscopic scale is critical for optimizing the electrochemical properties of them and their derivatives. In this study, manganese organic phosphate (Mn-MOP) with three distinct two-dimensional (2D) morphologies was synthesized by varying the molar ratio of [...] Read more.
Morphological control of metal-organic frameworks (MOFs) at the micro/nanoscopic scale is critical for optimizing the electrochemical properties of them and their derivatives. In this study, manganese organic phosphate (Mn-MOP) with three distinct two-dimensional (2D) morphologies was synthesized by varying the molar ratio of Mn2+ to phenyl phosphonic acid, and one of the morphologies is a unique palm leaf shape. In addition, a series of 2D Mn-MOP derivatives were obtained by calcination in air at different temperatures. Electrochemical studies showed that 2D Mn-MOP derivative calcined at 550 °C and exhibited a superior specific capacitance of 230.9 F g−1 at 0.5 A g−1 in 3 M KOH electrolyte. The aqueous asymmetric supercapacitor and the constructed flexible solid-state device demonstrated excellent rate performance. This performance reveals the promising application of 2D Mn-MOP materials for energy storage. Full article
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<p>(<b>a</b>) Schematic synthesis of Mn-MOP; (<b>b</b>) Mn-MOP precursors’ calcination route.</p>
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<p>(<b>a</b>–<b>h</b>) SEM and TEM images of Mn-0.05-x (x = 150, 250, 350 and 550 °C); (<b>i</b>,<b>j</b>) HRTEM image (inset: SAED); (<b>k</b>) EDX mapping results of Mn-0.05-550.</p>
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<p>(<b>a</b>) XRD patterns of Mn-0.05-x; (<b>b</b>) FT-IR spectra of Mn-0.05-x; (<b>c</b>) full XPS spectrum of Mn-0.05-x; (<b>d</b>–<b>f</b>) Mn 2p, P 2p, and O 1s XPS spectra of Mn-0.05-x.</p>
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<p>(<b>a</b>) Rate capability of Mn-0.05-x; (<b>b</b>) CV profiles of Mn-0.05-550 at various scan rates; (<b>c</b>) GCD profiles of Mn-0.05-550; (<b>d</b>) log(<span class="html-italic">i</span>) versus log(<span class="html-italic">v</span>) plots of Mn-0.05-550; (<b>e</b>) capacitive contribution of Mn-0.05-550 at 100 mV s<sup>−1</sup>; (<b>f</b>) percentages of capacitive contributions of Mn-0.05-550; (<b>g</b>) cyclic performance of Mn-0.05-550 at 4 A g<sup>−1</sup>.</p>
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<p>Electrochemical performance of the Mn-0.05-550//AC aqueous device. (<b>a</b>) CV profiles at varied voltages; (<b>b</b>) CV curves at varied scan rates; (<b>c</b>) GCD profiles at different current densities; (<b>d</b>) bar chart of specific capacitance and capacitance retention; (<b>e</b>) cyclic performance at 4 A g<sup>−1</sup>.</p>
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<p>Electrochemical performance of the Mn-0.05-550//AC flexible solid-state device. (<b>a</b>) CV profiles at various scan rates; (<b>b</b>) GCD profiles; (<b>c</b>) CV profiles under various bending conditions; (<b>d</b>) cyclic stability under different bending conditions; (<b>e</b>) cyclic performance at 3 mF cm<sup>−2</sup>.</p>
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32 pages, 11676 KiB  
Review
Hydrogels and Aerogels for Versatile Photo-/Electro-Chemical and Energy-Related Applications
by Jiana Sun, Taigang Luo, Mengmeng Zhao, Lin Zhang, Zhengping Zhao, Tao Yu and Yibo Yan
Molecules 2024, 29(16), 3883; https://doi.org/10.3390/molecules29163883 - 16 Aug 2024
Viewed by 910
Abstract
The development of photo-/electro-chemical and flexible electronics has stimulated research in catalysis, informatics, biomedicine, energy conversion, and storage applications. Gels (e.g., aerogel, hydrogel) comprise a range of polymers with three-dimensional (3D) network structures, where hydrophilic polyacrylamide, polyvinyl alcohol, copolymers, and hydroxides are the [...] Read more.
The development of photo-/electro-chemical and flexible electronics has stimulated research in catalysis, informatics, biomedicine, energy conversion, and storage applications. Gels (e.g., aerogel, hydrogel) comprise a range of polymers with three-dimensional (3D) network structures, where hydrophilic polyacrylamide, polyvinyl alcohol, copolymers, and hydroxides are the most widely studied for hydrogels, whereas 3D graphene, carbon, organic, and inorganic networks are widely studied for aerogels. Encapsulation of functional species with hydrogel building blocks can modify the optoelectronic, physicochemical, and mechanical properties. In addition, aerogels are a set of nanoporous or microporous 3D networks that bridge the macro- and nano-world. Different architectures modulate properties and have been adopted as a backbone substrate, enriching active sites and surface areas for photo-/electro-chemical energy conversion and storage applications. Fabrication via sol–gel processes, module assembly, and template routes have responded to professionalized features and enhanced performance. This review presents the most studied hydrogel materials, the classification of aerogel materials, and their applications in flexible sensors, batteries, supercapacitors, catalysis, biomedical, thermal insulation, etc. Full article
(This article belongs to the Special Issue New Sights in Nanomaterials for Photoelectrochemistry)
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<p>Scheme of hydrogel applications, reprinted with permission [<a href="#B1-molecules-29-03883" class="html-bibr">1</a>,<a href="#B2-molecules-29-03883" class="html-bibr">2</a>,<a href="#B6-molecules-29-03883" class="html-bibr">6</a>,<a href="#B8-molecules-29-03883" class="html-bibr">8</a>,<a href="#B9-molecules-29-03883" class="html-bibr">9</a>,<a href="#B12-molecules-29-03883" class="html-bibr">12</a>], copyright © 2023 John Wiley &amp; Sons, © 2021−2024 Springer Nature and © 2022 Elsevier B.V.</p>
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<p>Scheme of aerogel applications, reprinted with permission [<a href="#B3-molecules-29-03883" class="html-bibr">3</a>,<a href="#B4-molecules-29-03883" class="html-bibr">4</a>,<a href="#B10-molecules-29-03883" class="html-bibr">10</a>,<a href="#B11-molecules-29-03883" class="html-bibr">11</a>,<a href="#B13-molecules-29-03883" class="html-bibr">13</a>,<a href="#B14-molecules-29-03883" class="html-bibr">14</a>], copyright © 2019–2023 American Chemical Society, © 2023 Springer Nature, and © 2023 Elsevier B.V.</p>
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<p>SEM images of (<b>a</b>) PAAm/CS hydrogel, (<b>b</b>) microgel@PAAm/CS hydrogel, (<b>c</b>) S−PAAm hydrogel, (<b>e</b>) IPN PAAm−PAAc hydrogel (after freeze−drying), and (<b>h</b>) AG/T−PAAm DN hydrogel. Scheme for (<b>d</b>) production of S−PAAm hydrogel, (<b>f</b>) synthesis process of C−PAAm IPN hydrogels, (<b>g</b>) preparation of AG/T−PAAm DN hydrogel, (<b>i</b>) structure of PCTN organo−hydrogel. (<b>j</b>) Adhesion mechanism of the PCTN used as ionic skin. (<b>k</b>) The relative resistance of organo-hydrogel thermistors varied from 25 °C to 90 °C, reprinted with permission [<a href="#B33-molecules-29-03883" class="html-bibr">33</a>,<a href="#B34-molecules-29-03883" class="html-bibr">34</a>,<a href="#B36-molecules-29-03883" class="html-bibr">36</a>,<a href="#B37-molecules-29-03883" class="html-bibr">37</a>,<a href="#B41-molecules-29-03883" class="html-bibr">41</a>,<a href="#B42-molecules-29-03883" class="html-bibr">42</a>], copyright © 2021−2023 American Chemical Society, © 2023 John Wiley &amp; Sons, © 2018 Royal Society of Chemistry, © 2019 Springer Nature, and © 2022 Elsevier B.V., respectively.</p>
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<p>(<b>a</b>) Scheme of PVA-COOH/PDA hydrogel structure. (<b>b</b>) Adhesion strength diagram of PVA-COOH/PDA hydrogels with different carboxyl group contents on different materials. (<b>c</b>) Scheme of fabrication procedure for HA-PVA hydrogels. (<b>d</b>) Scheme of the fabrication of xylan/PVA/B DN hydrogel. (<b>e</b>) Diagram of bond-breaking changes of xylan/PVA/B DN hydrogel under tension. (<b>f</b>) Scheme of the structure of biocompatible hydrogel sensor. (<b>g</b>) The mechanism of copper and lead ion detection and removal, reprinted with permission [<a href="#B21-molecules-29-03883" class="html-bibr">21</a>,<a href="#B43-molecules-29-03883" class="html-bibr">43</a>,<a href="#B44-molecules-29-03883" class="html-bibr">44</a>,<a href="#B45-molecules-29-03883" class="html-bibr">45</a>,<a href="#B47-molecules-29-03883" class="html-bibr">47</a>], copyright © 2020–2021 Elsevier B.V., © 2021 Springer Nature, and © 2020 John Wiley &amp; Sons., respectively.</p>
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<p>(<b>a</b>) Scheme of the production process and structure of the hybrid hydrogel. (<b>b</b>) Stress–stretch curves of hybrid hydrogels of various weight percentages of acrylamide as labeled. (<b>c</b>) Chart for fracture energy versus elastic modulus compared with various soft materials. (<b>d</b>) Scheme of the synthetic process and structure of the Ag@rGO/PVA−PAAm hydrogel. (<b>e</b>) Self-healing and (<b>f</b>) anti-freezing properties of Ag@rGO/PVA−PAAm hydrogel contrasted with hydrogel at 25 and −30 °C. (<b>g</b>) Schematic diagram of fabrication of GPPD-hydrogel. (<b>h</b>) Strain sensing performance for different tensile strain GPPD−hydrogel. (<b>i</b>) The output performance of GPPD−TENG at different temperatures at frequency of 2 Hz, reprinted with permission [<a href="#B48-molecules-29-03883" class="html-bibr">48</a>,<a href="#B49-molecules-29-03883" class="html-bibr">49</a>,<a href="#B50-molecules-29-03883" class="html-bibr">50</a>], copyright © 2014 Royal Society of Chemistry, © 2022 John Wiley &amp; Sons, and © 2022 Springer Nature, respectively.</p>
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<p>(<b>a</b>) Scheme of the C/CA composite production using RF aerogel as precursor. (<b>b</b>) SEM image of the C/CA<sub>RF</sub> at carbonized state. (<b>c</b>) Schematic of the crosslinked RF aerogel structure. (<b>d</b>) Schematic illustration of the fabrication process of a NiMR-H aerogel. (<b>e</b>) Scheme for SWCNT/TA and Mg<sup>2+</sup>/SWCNT/TA aerogel production. (<b>f</b>) Scheme of the fabrication process of O− and N−doped CNT aerogel film. SEM images of (<b>g</b>) SWCNT/TA, (<b>h</b>) Mg<sup>2+</sup>/SWCNT/TA, and (<b>i</b>) N−doped carbon aerogels, with permissions [<a href="#B16-molecules-29-03883" class="html-bibr">16</a>,<a href="#B60-molecules-29-03883" class="html-bibr">60</a>,<a href="#B61-molecules-29-03883" class="html-bibr">61</a>,<a href="#B67-molecules-29-03883" class="html-bibr">67</a>,<a href="#B68-molecules-29-03883" class="html-bibr">68</a>,<a href="#B69-molecules-29-03883" class="html-bibr">69</a>], copyright © 2015−2023 Elsevier B.V., © 2019 John Wiley &amp; Sons, and © 2021–2023 American Chemical Society, respectively.</p>
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<p>(<b>a</b>) Scheme of the fabrication process of PVA/CNC/GNS composite aerogel. (<b>b</b>) Thermal insulation scheme of fiber-reinforced SiO<sub>2</sub> aerogel thermal insulation pads. (<b>c</b>) Fabrication of polyaniline/silver/cellulose nanofibril aerogel supercapacitors. SEM images of (<b>d</b>) PVA/CNC/GNS composite aerogel and (<b>e</b>) ZrO<sub>2</sub>–Al<sub>2</sub>O<sub>3</sub> composite aerogel coating. (<b>f</b>) Electrospinning fabrication processes of SiO<sub>2</sub>/SnO<sub>2</sub> nanofibers, reprinted with permissions [<a href="#B71-molecules-29-03883" class="html-bibr">71</a>,<a href="#B72-molecules-29-03883" class="html-bibr">72</a>,<a href="#B74-molecules-29-03883" class="html-bibr">74</a>,<a href="#B75-molecules-29-03883" class="html-bibr">75</a>,<a href="#B76-molecules-29-03883" class="html-bibr">76</a>], copyright © 2014–2022 Elsevier B.V., © 2023 Springer Nature, and © 2019 The American Ceramic Society, respectively.</p>
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<p>(<b>a</b>) The strain response curves of the PCCG organo−hydrogel. (<b>b</b>) The conductive network change procedure in the PCCG organo−hydrogel upon stretching. (<b>c</b>) Schematic diagram of GelMA hydrogel−based pressure sensor structure. (<b>d</b>) The variation in pressure sensitivity as a function of GelMA concentrations. (<b>e</b>) The fabrication procedure of the FGA/FGA@PDMS pressure sensor. (<b>f</b>) The mechanism of FGA/FGA@PDMS flexible pressure sensor, reprinted with permission [<a href="#B86-molecules-29-03883" class="html-bibr">86</a>,<a href="#B88-molecules-29-03883" class="html-bibr">88</a>,<a href="#B90-molecules-29-03883" class="html-bibr">90</a>], copyright © 2022 Springer Nature, © 2020 John Wiley &amp; Sons, and © 2023 American Chemical Society, respectively.</p>
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<p>(<b>a</b>) Structure of MXene/PANI/BC aerogel for the applications of e-skins and gas sensors. (<b>b</b>) Response of the MXene/PANI/BC composite aerogel-based gas sensor of NH<sub>3</sub> gas. (<b>c</b>) Scheme of PDMS-encapsulated ionic hydrogel and PDMS-encapsulated PVA-G-FeCl<sub>3</sub> and PVA-G hydrogel. (<b>d</b>) The PVA-G-FeCl<sub>3</sub>/PDMS hybrid hydrogel for human motion monitoring, reprinted with permission [<a href="#B92-molecules-29-03883" class="html-bibr">92</a>,<a href="#B93-molecules-29-03883" class="html-bibr">93</a>], copyright © American Chemical Society and © MDPI, respectively.</p>
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<p>(<b>a</b>) Schematic diagram of elastomer−hydrogel integration as skin sensor and flexible electrode for detecting physiological health signal. (<b>b</b>) Application of hydrogel electrodes in sustained attention evaluation. (<b>c</b>) Interfacial contact impedance of different electrodes under real EEG signals. (<b>d</b>) Schematic diagram of the mechanism and evaluation of EEG acquisition system for wireless transmission, reprinted with permission [<a href="#B103-molecules-29-03883" class="html-bibr">103</a>,<a href="#B106-molecules-29-03883" class="html-bibr">106</a>], copyright © 2022 Elsevier B.V. and © 2023 John Wiley &amp; Sons, respectively.</p>
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<p>(<b>a</b>) Schematic diagram of the dynamic network of healable and recyclable PDMS-based elastomers (H-PDMS-Pym). (<b>b</b>) Stress–strain curves of cyclic loading–unloading for H-PDMS-Py0.25 at 500%. (<b>c</b>) Schematic diagram cyclic stretching/releasing for sacrificial bond rupture and reshuffling. (<b>d</b>) Schematic diagram of self-healing procedure of PDMS@MXene. (<b>e</b>) Digital photograph of the SCNC-CNT/PDMS elastomer and schematic illustration of the application of SCNC-CNT/PDMS-based as sensor. (<b>f</b>) Stress–strain curves for PDMS@MXene conductive elastomers of modified-MXene with different mass ratios. (<b>g</b>) Fabrication of a wireless micro-heater device. (<b>h</b>) The relationship of current in SnO<sub>2</sub> nanowires and CO gas levels in the absence of a heater (black line) and in the presence of a heater (red line), reprinted with permission [<a href="#B111-molecules-29-03883" class="html-bibr">111</a>,<a href="#B112-molecules-29-03883" class="html-bibr">112</a>,<a href="#B113-molecules-29-03883" class="html-bibr">113</a>,<a href="#B115-molecules-29-03883" class="html-bibr">115</a>], copyright © 2022 John Wiley &amp; Sons, © 2021 American Chemical Society, © 2022 Elsevier B.V., © 2022 MDPI, respectively.</p>
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<p>(<b>a</b>) Illustration for the structure of flexible zinc−air battery. (<b>b</b>) The antifreeze mechanism of OHE. (<b>c</b>) Charge/discharge curves of OHE−based flexible ZABs at different temperature. (<b>d</b>) Schematic structure of flexible zinc-ion battery with the ZSC−gel electrolyte under an external electric field. (<b>e</b>) The curve of ionic conductivity and bending angle of the ZSC−gel electrolyte. (<b>f</b>) Cycling performances at different C−rates of the Zn−MnO<sub>2</sub> coin cells with the ZSC−gel electrolyte. (<b>g</b>) Photographs of the self−healing process for Zn<sup>2+</sup>-CS/PAAM hydrogel, reprinted with permission [<a href="#B116-molecules-29-03883" class="html-bibr">116</a>,<a href="#B118-molecules-29-03883" class="html-bibr">118</a>,<a href="#B119-molecules-29-03883" class="html-bibr">119</a>], copyright © 2020–2022 John Wiley &amp; Sons and © 2023 Elsevier B.V., respectively.</p>
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<p>(<b>a</b>) Schematic diagram of the fabrication process of NGCA. (<b>b</b>) Schematic structure of Li−CO<sub>2</sub> battery with NGCA cathode. (<b>c</b>) Illustration for the structure of liquid flow rechargeable ZAB structure. (<b>d</b>) Polarization curves and corresponding power density curves, and (<b>e</b>) specific capacity curves of Pt/C + RuO<sub>2</sub> and NSCA/FeCo. (<b>f</b>) Schematic diagram of the synthesis process of MGA material. (<b>g</b>) Rate performance of the coin cells with different anode materials, reprinted with permission [<a href="#B121-molecules-29-03883" class="html-bibr">121</a>,<a href="#B122-molecules-29-03883" class="html-bibr">122</a>,<a href="#B124-molecules-29-03883" class="html-bibr">124</a>], copyright © 2023 Elsevier B.V., © 2023 Springer Nature, and © 2022 John Wiley &amp; Sons, respectively.</p>
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<p>(<b>a</b>) Scheme of cellulose/GO/PANI aerogel production process. (<b>b</b>) CV curves of the device at different degree bending deformations. (<b>c</b>) Ragone plots and comparisons with other reported solid−state supercapacitors. (<b>d</b>) Structure of aqueous supercapacitor. (<b>e</b>) Cross−sectional SEM image of the three−layered hydrogel. (<b>f</b>) Galvanostatic charge–discharge (GCD) curves of aqueous supercapacitor at different current densities. (<b>g</b>) Scheme of the synthesis process and operation mechanism of the H−ZHS. (<b>h</b>) Cycling performance of H−ZHS at 5 A·g<sup>−1</sup>, inset as the lighting of green LED (start−up voltage 2 V) powered by H−ZHS, with permission [<a href="#B127-molecules-29-03883" class="html-bibr">127</a>,<a href="#B133-molecules-29-03883" class="html-bibr">133</a>,<a href="#B139-molecules-29-03883" class="html-bibr">139</a>], copyright © 2020 MDPI, © 2022 Springer Nature, and © 2020 Elsevier B.V., respectively.</p>
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<p>(<b>a</b>) Scheme of the photocatalytic HER process using floatable and sunken aerogel nanocomposites. (<b>b</b>) H<sub>2</sub> evolution rate of the floatable and sunken aerogel nanocomposites. (<b>c</b>) Scheme of the 3D Rh/G−(CN) electrocatalyst structure and cyclic voltammogram (CV) profiles of the different electrodes in 1 mol L<sup>–1</sup> KOH with 1 mol L<sup>–1</sup> CH<sub>3</sub>OH mixed solution. (<b>d</b>) The methanol oxidation mass activities of various electrodes before and after cycling tests. (<b>e</b>) CV curves of the Rh/G<sub>3</sub>−(CN)<sub>7</sub> electrode before and after 500 cycles. (<b>f</b>) SEM image of the Janus ZIF−8@wood aerogel. (<b>g</b>) The conversion of benzaldehyde using ZIF−8@wood aerogel and Janus ZIF−8@wood aerogel as catalysts. (<b>h</b>) Schematic illustration for the synthesis process of Janus MOFs@wood aerogel, reprinted with permission [<a href="#B141-molecules-29-03883" class="html-bibr">141</a>,<a href="#B143-molecules-29-03883" class="html-bibr">143</a>,<a href="#B144-molecules-29-03883" class="html-bibr">144</a>], copyright © 2023 Springer Nature and © 2021 American Chemical Society, respectively.</p>
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<p>(<b>a</b>) Antibacterial effect of different concentrations of PHMG hydrogels on <span class="html-italic">E. coli</span> (i) and <span class="html-italic">S. aureus</span> (ii). From left to right, the concentration of PHMG increases, 0%, 0.005%, 0.01%, 0.05%, 0.1%, and 0.5%, respectively. (<b>b</b>) Cell counting kit−8 (CCK−8) assays of the PVA/PAAm IPN hydrogel against human embryonic kidney cells. (<b>c</b>) Schematic illustration of the synthetic process of PCV hydrogel. (<b>d</b>) Simulation model of antibacterial experiment in vitro. The in vitro antibacterial experiment of (<b>e</b>) the distribution of <span class="html-italic">S. aureus</span> colony in culture dish after coating for 24 h and (<b>f</b>) the relative activity of L929 cells and <span class="html-italic">S. aureus</span>. (<b>g</b>) The in vitro cytocompatibility experiment of PVA−based hydrogels examined against L929 cells after incubation for 1, 3, and 5 days via MTT assay. * <span class="html-italic">p</span> &lt; 0.05, ** <span class="html-italic">p</span> &lt; 0.01, *** <span class="html-italic">p</span> &lt; 0.001. (<b>h</b>) SEM images of (i) <span class="html-italic">E. coli</span> and (ii) <span class="html-italic">S. aureus</span> captured after irradiation with NIR light at 808 nm for 15 min, reprinted with permission [<a href="#B145-molecules-29-03883" class="html-bibr">145</a>,<a href="#B146-molecules-29-03883" class="html-bibr">146</a>,<a href="#B147-molecules-29-03883" class="html-bibr">147</a>], copyright © 2021−2022 Elsevier B.V. and © 2021 John Wiley &amp; Sons, respectively.</p>
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<p>(<b>a</b>) Scheme of GA/HEC-SiO<sub>2</sub> aerogels’ production process. (<b>b</b>) The heat transfer process of composite aerogels. (<b>c</b>) Thermal conductivity comparison of GA/HEC-SiO<sub>2</sub> aerogel with other aerogels. (<b>d</b>) The pseudo-color thermal images of different aerogels settled on continuous heating at 100 °C platform. (<b>e</b>) Thermal insulation and stability tests of the GA/HEC-SiO<sub>2</sub> aerogel. (<b>f</b>) Scheme of the SCAB fabrication process. (<b>g</b>) Forward-looking infrared (FLIR) images of the putty block without and with SCABs heating bottom plates at different temperatures. (The unit of temperature scale bar on right is °C). (<b>h</b>,<b>i</b>) Thermal stability characterization of SCABs using the thermogravimetric analysis profile, reprinted with permission [<a href="#B28-molecules-29-03883" class="html-bibr">28</a>,<a href="#B155-molecules-29-03883" class="html-bibr">155</a>], copyright © 2022 MDPI and © 2021 John Wiley &amp; Sons, respectively.</p>
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17 pages, 10250 KiB  
Article
Planar Micro-Supercapacitors with High Power Density Screen-Printed by Aqueous Graphene Conductive Ink
by Youchang Wang, Xiaojing Zhang, Yuwei Zhu, Xiaolu Li and Zhigang Shen
Materials 2024, 17(16), 4021; https://doi.org/10.3390/ma17164021 - 13 Aug 2024
Viewed by 803
Abstract
Simple and scalable production of micro-supercapacitors (MSCs) is crucial to address the energy requirements of miniature electronics. Although significant advancements have been achieved in fabricating MSCs through solution-based printing techniques, the realization of high-performance MSCs remains a challenge. In this paper, graphene-based MSCs [...] Read more.
Simple and scalable production of micro-supercapacitors (MSCs) is crucial to address the energy requirements of miniature electronics. Although significant advancements have been achieved in fabricating MSCs through solution-based printing techniques, the realization of high-performance MSCs remains a challenge. In this paper, graphene-based MSCs with a high power density were prepared through screen printing of aqueous conductive inks with appropriate rheological properties. High electrical conductivity (2.04 × 104 S∙m−1) and low equivalent series resistance (46.7 Ω) benefiting from the dense conductive network consisting of the mesoporous structure formed by graphene with carbon black dispersed as linkers, as well as the narrow finger width and interspace (200 µm) originating from the excellent printability, prompted the fully printed MSCs to deliver high capacitance (9.15 mF∙cm−2), energy density (1.30 µWh∙cm−2) and ultrahigh power density (89.9 mW∙cm−2). Notably, the resulting MSCs can effectively operate at scan rates up to 200 V∙s−1, which surpasses conventional supercapacitors by two orders of magnitude. In addition, the MSCs demonstrate excellent cycling stability (91.6% capacity retention and ~100% Coulombic efficiency after 10,000 cycles) and extraordinary mechanical properties (92.2% capacity retention after 5000 bending cycles), indicating their broad application prospects in flexible wearable/portable electronic systems. Full article
(This article belongs to the Section Carbon Materials)
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Graphical abstract

Graphical abstract
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<p>Schematic synthesis of aqueous graphene conductive ink and screen-printed preparation of MSCs.</p>
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<p>(<b>a</b>) SEM image of pristine graphite before exfoliation. (<b>b</b>) TEM image of several stacked graphene nanosheets. (<b>c</b>) A typical AFM image of graphene. (<b>d</b>) SEM image of graphene after exfoliation. (<b>e</b>) HRTEM image of the rectangle region in (<b>b</b>). Histograms of the (<b>f</b>) thickness distribution and (<b>g</b>) area distribution of graphene.</p>
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<p>(<b>a</b>) Raman spectra and (<b>b</b>) C1s XPS of pristine graphite and graphene.</p>
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<p>(<b>a</b>) Viscosity of ink as a function of shear rate; (<b>b</b>) thixotropy of ink; (<b>c</b>) percentage recovery of ink viscosity; (<b>d</b>) variation of storage modulus (G′), and loss modulus (G″) with shear stress, where the solid and hollow symbols stand for G′ and G″, respectively; (<b>e</b>) loss coefficient tan δ as a function of shear stress; (<b>f</b>) optical microscope images of thin lines of ink printed on PET substrate by passing through the opening of a 100 μm optical microscope images of fine lines printed by ink through screen openings on PET substrates, from top to bottom corresponding to Ink–0.25, Ink–0.67, Ink–1.5, and Ink–4, respectively; (<b>g</b>) electrical conductivity of the printed patterns before and after hot pressing; (<b>h</b>) change in the relative electrical resistance of the printed patterns during 1000 repetitive bending cycles at a bending angle of 120°; (<b>i</b>) top-view SEM image of the fine line printed with Ink–1.5.</p>
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<p>(<b>a</b>) A representative cross-sectional SEM image of MSC. (<b>b</b>) A digital photograph of MSC<sub>1000</sub>, MSC<sub>500</sub>, and MSC<sub>200</sub>.</p>
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<p>(<b>a</b>–<b>f</b>) CV curves of MSC<sub>200</sub> at different scan rates of 0.01, 0.1, 1, 10, 100, and 200 V∙s<sup>−1</sup>. (<b>g</b>) The relationship of discharge current density varies with the scan rate for MSC<sub>200</sub>. (<b>h</b>) Nyquist plot of MSC<sub>200</sub>, MSC<sub>500</sub>, and MSC<sub>1000</sub>. (<b>i</b>) The relationship of impedance phase angle varies with frequency for the three MSCs.</p>
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<p>GCD curves at varying current densities of (<b>a</b>) 0.05–0.4 mA∙cm<sup>−2</sup> and (<b>b</b>) 0.5–1.0 mA∙cm<sup>−2</sup>. (<b>c</b>) Area capacitance of the three MSCs varying current density of 0.05–1.0 mA∙cm<sup>−2</sup>. (<b>d</b>) Comparison of area-specific capacitance of this study and other reported printed MSCs. (<b>e</b>) Cycling performance of MSC<sub>200</sub> at the current density of 0.5 mA∙cm<sup>−2</sup>. (<b>f</b>) Ragone plot on energy density and power density. (<b>g</b>) Photographs of MSC<sub>200</sub> at various bending angles. (<b>h</b>) Capacitance retention of MSC<sub>200</sub> during 5000 bending cycles. Inset: CV curves obtained at various bending angles using a scan rate of 200 mV∙s<sup>−1</sup> [<a href="#B15-materials-17-04021" class="html-bibr">15</a>,<a href="#B17-materials-17-04021" class="html-bibr">17</a>,<a href="#B18-materials-17-04021" class="html-bibr">18</a>,<a href="#B20-materials-17-04021" class="html-bibr">20</a>,<a href="#B22-materials-17-04021" class="html-bibr">22</a>,<a href="#B52-materials-17-04021" class="html-bibr">52</a>,<a href="#B56-materials-17-04021" class="html-bibr">56</a>,<a href="#B58-materials-17-04021" class="html-bibr">58</a>,<a href="#B59-materials-17-04021" class="html-bibr">59</a>,<a href="#B61-materials-17-04021" class="html-bibr">61</a>,<a href="#B62-materials-17-04021" class="html-bibr">62</a>].</p>
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