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<article xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">
  <front>
    <journal-meta>
      <journal-id journal-id-type="nlm-ta">Soft Sci.</journal-id>
      <journal-id journal-id-type="publisher-id">SS</journal-id>
      <journal-title-group>
        <journal-title>Soft Science</journal-title>
      </journal-title-group>
      <issn pub-type="epub">2769-5441</issn>
      <publisher>
        <publisher-name>OAE Publishing Inc.</publisher-name>
      </publisher>
    </journal-meta>
    <article-meta>
      <article-id pub-id-type="doi">10.20517/ss.2026.171</article-id>
      <article-categories>
        <subj-group>
          <subject>Review Article</subject>
        </subj-group>
      </article-categories>
      <title-group>
        <article-title>Motion-induced mechano-electric fibers towards wearable electronics with energy and information self-sufficiency</article-title>
      </title-group>
      <contrib-group>
        <contrib contrib-type="author">
          <name>
            <surname>Zhao</surname>
            <given-names>Jizhong</given-names>
          </name>
          <xref ref-type="aff" rid="I1">
            <sup>1</sup>
          </xref>
          <xref ref-type="aff" rid="I2">
            <sup>2</sup>
          </xref>
        </contrib>
        <contrib contrib-type="author">
          <name>
            <surname>Li</surname>
            <given-names>Houyi</given-names>
          </name>
          <xref ref-type="aff" rid="I1">
            <sup>1</sup>
          </xref>
          <xref ref-type="aff" rid="I2">
            <sup>2</sup>
          </xref>
        </contrib>
        <contrib contrib-type="author">
          <name>
            <surname>Fan</surname>
            <given-names>Xiaoxuan</given-names>
          </name>
          <xref ref-type="aff" rid="I1">
            <sup>1</sup>
          </xref>
          <xref ref-type="aff" rid="I2">
            <sup>2</sup>
          </xref>
        </contrib>
        <contrib contrib-type="author">
          <name>
            <surname>Xie</surname>
            <given-names>Hongxiang</given-names>
          </name>
          <xref ref-type="aff" rid="I1">
            <sup>1</sup>
          </xref>
          <xref ref-type="aff" rid="I2">
            <sup>2</sup>
          </xref>
        </contrib>
        <contrib contrib-type="author" corresp="yes">
          <name>
            <surname>Dong</surname>
            <given-names>Kai</given-names>
          </name>
          <xref ref-type="aff" rid="I1">
            <sup>1</sup>
          </xref>
          <xref ref-type="aff" rid="I2">
            <sup>2</sup>
          </xref>
          <xref ref-type="aff" rid="I*">
            <sup>*</sup>
          </xref>
          <xref ref-type="corresp" rid="cor1" />
        </contrib>
      </contrib-group>
      <aff id="I1">
        <sup>1</sup>Beijing Key Laboratory of High-Entropy Energy Materials and Devices, Beijing Institute of Nanoenergy and Nanosystems, Chinese Academy of Sciences, Beijing 101400, China.</aff>
      <aff id="I2">
        <sup>2</sup>School of Nanoscience and Technology, University of Chinese Academy of Sciences, Beijing 100049, China.</aff>
      <author-notes>
        <corresp id="cor1"><sup>*</sup>Correspondence to: Prof. Kai Dong, Beijing Key Laboratory of High-Entropy Energy Materials and Devices, Beijing Institute of Nanoenergy and Nanosystems, Chinese Academy of Sciences, Beijing, 101400, China. E-mail: <email>dongkai@binn.cas.cn</email></corresp>
        <fn fn-type="other">
          <p>
            <bold>Received:</bold> 30 Jun 2026 | <bold>First Decision:</bold> 29 Jul 2026 | <bold>Revised:</bold> 8 Sep 2026 | <bold>Accepted:</bold> 10 Sep 2026 | <bold>Published:</bold> 13 Oct 2026</p>
        </fn>
        <fn fn-type="other">
          <p>
            <bold>Academic Editors:</bold> Jun Chen, Wei Gao | <bold>Copy Editor:</bold> Pei-Yun Wang | <bold>Production Editor:</bold> Pei-Yun Wang</p>
        </fn>
      </author-notes>
      <pub-date pub-type="ppub">
        <year>2026</year>
      </pub-date>
      <pub-date pub-type="epub">
        <day>13</day>
        <month>10</month>
        <year>2026</year>
      </pub-date>
      <volume>6</volume>
	  <issue>4</issue>
      <elocation-id>94</elocation-id>
      <permissions>
        <copyright-statement>© The Author(s) 2026.</copyright-statement>
        <license xlink:href="https://creativecommons.org/licenses/by/4.0/">
          <license-p>© The Author(s) 2026. <bold>Open Access</bold> This article is licensed under a Creative Commons Attribution 4.0 International License (<uri xlink:href="https://creativecommons.org/licenses/by/4.0/">https://creativecommons.org/licenses/by/4.0/</uri>), which permits unrestricted use, sharing, adaptation, distribution and reproduction in any medium or format, for any purpose, even commercially, as long as you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.</license-p>
        </license>
      </permissions>
      <abstract>
        <p>Mechano-electric fibers (MEFs) represent a novel class of smart textiles that offer a robust pathway for comfortable wear and efficient harvesting of human biomechanical energy by integrating with triboelectric nanogenerators (TENGs). MEFs can serve as a sustainable power supply for wearable electronics and function as sensitive and convenient platforms for the acquisition of human motion signals, and the detection of environmental stimuli. This review emphasizes that the triboelectric mechanism, response characteristics, and textile architecture endow MEFs with distinctive advantages, including highly efficient low-frequency bioenergy conversion, progressive multi-stage high-sensitivity responses, and versatile structural designs. Consequently, these features facilitate autonomous and sustainable on-body energy and information supply systems. Furthermore, the emerging functionalities and diverse applications of MEFs demonstrate the substantial potential of human-centric self-powered wearable systems, including motion capture, physiological monitoring, and environmental perception. Finally, we provide a comprehensive discussion on the critical challenges currently impeding the design and practical implementation of MEFs.</p>
      </abstract>
      <kwd-group>
        <kwd>Mechano-electric</kwd>
        <kwd>smart textiles</kwd>
        <kwd>self-powered</kwd>
        <kwd>wearable electronics</kwd>
      </kwd-group>
    </article-meta>
  </front>
  <body>
    <sec id="sec1">
      <title>INTRODUCTION</title>
      <p>Wearable electronics have been widely adopted in daily life<sup>[<xref ref-type="bibr" rid="B1">1</xref>]</sup>. The continuous acquisition of high-fidelity user motion and physiological data has driven an increasing demand for electrical power in wearable devices. However, rigid batteries typically account for a large fraction of the weight and volume of wearable systems, severely compromising device portability, operational longevity, and comfort. The growing disparity between signal-acquisition demands and limited power supply has created an urgent need for integrated solutions capable of simultaneously sensing physiological signals and harvesting biomechanical energy for sustainable power supply. This imperative has catalyzed the emergence of mechano-electric fibers (MEFs)<sup>[<xref ref-type="bibr" rid="B2">2</xref>]</sup>. Biomechanical energy is associated with kinematic states and various physiological parameters<sup>[<xref ref-type="bibr" rid="B3">3</xref>]</sup>. Nevertheless, its highly irregular, rapidly dissipative, and low-density nature has hindered its effective exploitation<sup>[<xref ref-type="bibr" rid="B4">4</xref>]</sup>. Through the integration of triboelectric nanogenerators (TENGs), MEFs can harvest biomechanical energy, track human motion, monitor physiological signals, and interact with the environment. In other words, MEFs refer to fiber- and textile-shaped TENGs, which directly convert mechanical deformation into electrical signals via contact electrification. Consequently, in a self-powered wearable system that contains wearable sensors as electrical loads and MEFs as energy supplements [<xref ref-type="fig" rid="fig1">Figure 1A</xref>], MEFs establish a self-sustaining energy-information closed loop for the wearer<sup>[<xref ref-type="bibr" rid="B5">5</xref>,<xref ref-type="bibr" rid="B6">6</xref>]</sup>, who acts as both the biomechanical energy source<sup>[<xref ref-type="bibr" rid="B7">7</xref>]</sup> and the recipient of diverse physiological information. In such a system, the biomechanical energy conversion in MEFs bridges energy and information flows [<xref ref-type="fig" rid="fig1">Figure 1B</xref>]: it supplies power to operate other wearable devices, while the generated electrical signals can serve as physiological signals for human-state monitoring. MEFs thus provide a novel implementation pathway for wearable intelligent systems [<xref ref-type="fig" rid="fig1">Figure 1C</xref>]. However, current MEFs still face challenges in achieving a fully self-sustaining closed loop, where the harvested energy alone powers all sensing, processing, and communication functions while maintaining stable long-term operation. Accordingly, this review examines operating mechanisms and textile architectures to outline strategies for efficient self-powered applications and summarizes prevailing challenges and potential solutions.</p>
      <fig id="fig1" position="float">
        <label>Figure 1</label>
        <caption>
          <p>The role of MEFs in self-sufficient energy and information systems: (A) Wearable systems include electronic devices and energy harvesters; (B) MEFs serve as a bridge for energy and information exchange; (C) MEFs can undertake various functions. MEFs: Mechano-electric fibers.</p>
        </caption>
        <graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="ss60171.fig.1.jpg" />
      </fig>
    </sec>
    <sec id="sec2">
      <title>MECHANISM</title>
      <p>TENGs utilize the relative motion between two materials with different triboelectric properties to induce contact electrification at their interfaces. Upon electrification, the positive triboelectric material acts as an electron donor and acquires a positive surface charge, whereas the negative triboelectric material acts as an electron acceptor and becomes negatively charged. A greater difference in electron affinity leads to a more pronounced contact electrification effect. The spatial separation of these surface charges generates a localized electric field that drives charge transfer through the external circuit, thereby converting mechanical energy into electrical energy<sup>[<xref ref-type="bibr" rid="B8">8</xref>]</sup>. Periodic contact and separation enable continuous harvesting of biomechanical energy [<xref ref-type="fig" rid="fig2">Figure 2A</xref>]<sup>[<xref ref-type="bibr" rid="B9">9</xref>]</sup>. The generated electrical signals also carry information that reflects the kinematic profiles of the mechanical stimuli, thereby endowing the system with dynamic sensing capabilities.</p>
      <fig id="fig2" position="float">
        <label>Figure 2</label>
        <caption>
          <p>Working principles and structures of MEFs: (A) Mechano-electric conversion process; (B) Electron-cloud potential-well model; (C) Representative designs of the four modes; (D) Multilevel structural design space of textiles. MEFs: Mechano-electric fibers; 1D: one-dimensional; 2D: two-dimensional; 3D: three-dimensional.</p>
        </caption>
        <graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="ss60171.fig.2.jpg" />
      </fig>
      <p>The microscopic mechanism underlying this mechano-electric conversion can be explained by the surface state model and the electron-cloud potential-well model. The surface state model is primarily applicable to materials with well-defined band structures, particularly dielectrics with surface defect states<sup>[<xref ref-type="bibr" rid="B10">10</xref>,<xref ref-type="bibr" rid="B11">11</xref>]</sup>. When two materials come into contact, the energy difference between their surface states drives interfacial electron transfer, resulting in contact electrification. However, for materials whose electronic structures are described by molecular orbitals, such as polymers, the surface state model becomes inadequate. In such scenarios, the electron-cloud potential-well model provides a more broadly applicable theoretical framework [<xref ref-type="fig" rid="fig2">Figure 2B</xref>]<sup>[<xref ref-type="bibr" rid="B12">12</xref>,<xref ref-type="bibr" rid="B13">13</xref>]</sup>. This model emphasizes that the overlap of electron clouds between the two materials in contact is the primary driver of electron transfer. The overlap converts the original single potential wells into an asymmetric double-well structure, thereby lowering the intermolecular potential barrier and establishing an energy gradient that drives electrons from a high-energy state to a low-energy state. Beyond charge generation, charge loss during conversion is an equally critical factor governing MEF output performance. In MEFs, shallow and deep traps store and release charges. Charges in shallow traps can easily escape, while those in deep traps can be retained for a long time. In addition to trap-mediated dissipation, air breakdown constitutes a major pathway for charge loss. When the voltage exceeds a certain threshold, air molecules are ionized, forming conductive channels that cause charges to dissipate rapidly. Environmental conditions, particularly ambient humidity, significantly influence the output performance of MEFs. High humidity can increase the probability of air breakdown, thereby accelerating charge loss. To address these challenges, several optimization strategies can be pursued: (i) material selection and surface modification; (ii) structural design; and (iii) control of operational conditions. Together, these mechanistic insights provide a theoretical basis for the rational design and performance optimization of MEFs.</p>
      <p>Given the precise structural control achievable through advanced design and fabrication processes, the deformation response behavior of fibers can be accurately predicted and rationally tailored. Consequently, the response characteristics of MEFs are highly adjustable by modulating fiber diameter, length, weaving topology, and surface microstructures. Smaller fiber diameters increase specific surface area and strain response, thereby enhancing charge density but potentially limiting mechanical durability; porous or hollow architectures balance these competing effects by providing additional strain dissipation pathways<sup>[<xref ref-type="bibr" rid="B14">14</xref>,<xref ref-type="bibr" rid="B15">15</xref>]</sup>. Yarn twist optimizes inter-bundle packing and conductivity, with optimal twist angles (~30°) maximizing sensitivity and toughness, while excessive twist reduces sensitivity due to fiber obliquity<sup>[<xref ref-type="bibr" rid="B16">16</xref>,<xref ref-type="bibr" rid="B17">17</xref>]</sup>. Fabric topology determines contact mode: knitted structures with three-dimensional (3D) loop configurations exhibit line contact and higher roughness than woven fabrics with point contact, thereby significantly enhancing triboelectric output (up to 240% higher voltage)<sup>[<xref ref-type="bibr" rid="B18">18</xref>,<xref ref-type="bibr" rid="B19">19</xref>]</sup>. Surface microstructures (including wrinkles, cracks, and pores) govern strain localization and conductive network evolution, simultaneously enabling high sensitivity and a broad dynamic range through mechanisms such as crack redistribution (pores delay crack propagation) and hierarchical deformation (wrinkles flatten under large strain)<sup>[<xref ref-type="bibr" rid="B20">20</xref>,<xref ref-type="bibr" rid="B21">21</xref>]</sup>. These structural engineering principles transform textile architectures into tunable platforms for self-powered sensing and energy harvesting. Owing to their hierarchical fibrous or textile substrates, MEFs inherently exhibit abundant surface microstructures. Their response characteristics arise from the progressive contact mechanics of textile architecture, which enhances sensitivity and broadens the dynamic range for pressure sensing. When an MEF and another dielectric medium approach each other, electrostatic induction initially generates limited surface charges. Subsequently, as the surface microfibers progressively contact the opposing medium, the effective contact area expands significantly, yielding electrical signals with exceptionally high sensitivity. Under continuously increasing pressure, the effective contact area gradually approaches saturation. This multi-stage progressive response behavior ensures both high sensitivity and an extended dynamic range, representing an elegant integration of TENG principles with textile architectures. In contrast to conventional capacitive<sup>[<xref ref-type="bibr" rid="B22">22</xref>]</sup> and piezoresistive<sup>[<xref ref-type="bibr" rid="B23">23</xref>]</sup> sensors, self-powered MEFs exhibit superior response speeds and multi-signal output capabilities [<xref ref-type="table" rid="t1">Table 1</xref>]. Thermoelectric<sup>[<xref ref-type="bibr" rid="B31">31</xref>]</sup> and electromagnetic<sup>[<xref ref-type="bibr" rid="B32">32</xref>]</sup> sensors are also self-powered, but their outputs and sensitivities in textile form are typically inferior to those of MEFs. Furthermore, because of the large electronegativity difference between the constituent materials, MEFs generally produce larger signal amplitudes than piezoelectric<sup>[<xref ref-type="bibr" rid="B33">33</xref>]</sup> and ferroelectric<sup>[<xref ref-type="bibr" rid="B34">34</xref>]</sup> transducers under comparable conditions.</p>
      <table-wrap id="t1">
        <label>Table 1</label>
        <caption>
          <p>Comparison of the performance of different sensing mechanisms</p>
        </caption>
        <table frame="hsides" rules="groups">
          <thead>
            <tr>
              <td style="border-bottom:1;">
                <bold>Literature</bold>
              </td>
              <td style="border-bottom:1;">
                <bold>Mechanism</bold>
              </td>
              <td style="border-bottom:1;">
                <bold>Response range</bold>
              </td>
              <td style="border-bottom:1;">
                <bold>Sensitivity</bold>
              </td>
              <td style="border-bottom:1;">
                <bold>Response time</bold>
              </td>
              <td style="border-bottom:1;">
                <bold>Recovery time</bold>
              </td>
            </tr>
          </thead>
          <tbody>
            <tr>
              <td>Cuthbert <italic>et al.</italic><sup>[<xref ref-type="bibr" rid="B24">24</xref>]</sup></td>
              <td>Capacitive</td>
              <td>&lt; 100%</td>
              <td>GF ≈ 4</td>
              <td>N/A</td>
              <td>N/A</td>
            </tr>
            <tr>
              <td>Ji <italic>et al.</italic><sup>[<xref ref-type="bibr" rid="B25">25</xref>]</sup></td>
              <td>Capacitive</td>
              <td>&lt; 1,700 kPa</td>
              <td>0.065 kPa<sup>-1</sup></td>
              <td>100 ms</td>
              <td>100 ms</td>
            </tr>
            <tr>
              <td>Pan <italic>et al.</italic><sup>[<xref ref-type="bibr" rid="B26">26</xref>]</sup></td>
              <td>Piezoresistive</td>
              <td>0.1-30 kPa</td>
              <td>17.73 kPa<sup>-1</sup></td>
              <td>80 ms</td>
              <td>40 ms</td>
            </tr>
            <tr>
              <td>Zhao <italic>et al.</italic><sup>[<xref ref-type="bibr" rid="B27">27</xref>]</sup></td>
              <td>Piezoresistive</td>
              <td>&lt; 10 kPa</td>
              <td>914.97 kPa<sup>-1</sup></td>
              <td>38 ms</td>
              <td>34 ms</td>
            </tr>
            <tr>
              <td>Mokhtari <italic>et al.</italic><sup>[<xref ref-type="bibr" rid="B28">28</xref>]</sup></td>
              <td>Piezoelectric</td>
              <td>50-1,000 Hz</td>
              <td>37 V·Pa<sup>-1</sup></td>
              <td>N/A</td>
              <td>N/A</td>
            </tr>
            <tr>
              <td>Lan <italic>et al.</italic><sup>[<xref ref-type="bibr" rid="B29">29</xref>]</sup></td>
              <td>Triboelectric</td>
              <td>&lt; 20 kPa</td>
              <td>0.94 kPa<sup>-1</sup></td>
              <td>39 ms</td>
              <td>N/A</td>
            </tr>
            <tr>
              <td>Xu <italic>et al.</italic><sup>[<xref ref-type="bibr" rid="B30">30</xref>]</sup></td>
              <td>Triboelectric</td>
              <td>&lt; 16 kPa</td>
              <td>12.33 V·kPa<sup>-1</sup></td>
              <td>70 ms</td>
              <td>60 ms</td>
            </tr>
          </tbody>
        </table>
        <table-wrap-foot>
          <fn>
            <p>GF: Gauge factor; N/A: not applicable.</p>
          </fn>
        </table-wrap-foot>
      </table-wrap>
    </sec>
    <sec id="sec3">
      <title>STRUCTURE</title>
      <p>MEFs combine the characteristics of both TENGs and conventional textiles. MEFs can generate electrical signals inherently linked to mechanical stimuli, thereby enabling the harvesting, conversion, and utilization of diverse forms of biomechanical energy. In addition, owing to their textile nature, MEFs offer exceptional flexibility, hierarchical architecture, and the potential for scalable manufacturing. For wearable applications, multiple TENG configurations can be used to harvest biomechanical energy from various body sites and motion sources. Among the fundamental working modes for wearable applications<sup>[<xref ref-type="bibr" rid="B35">35</xref>]</sup>, the vertical contact-separation mode is specifically designed for mechanical strains perpendicular to the textile surface [<xref ref-type="fig" rid="fig2">Figure 2C(i)</xref>]<sup>[<xref ref-type="bibr" rid="B36">36</xref>]</sup>. A representative example is the dynamic pressure exerted by the plantar surface on an insole during running or jumping. The lateral sliding mode is designed for in-plane sliding, making it highly suitable for monitoring displacement and angular variations [<xref ref-type="fig" rid="fig2">Figure 2C(ii)</xref>]. For instance, it can effectively capture the frictional energy generated between a swinging arm and the torso during running. The single-electrode mode is intended for confined spaces where deploying dual electrodes is impractical [<xref ref-type="fig" rid="fig2">Figure 2C(iii)</xref>]<sup>[<xref ref-type="bibr" rid="B37">37</xref>]</sup>. In this configuration, one electrode is grounded to serve as a reference potential for detecting varying signals on the sensing electrode. The freestanding triboelectric-layer mode allows all electrodes to move freely, and its application scope is similar to that of the lateral sliding mode [<xref ref-type="fig" rid="fig2">Figure 2C(iv)</xref>]<sup>[<xref ref-type="bibr" rid="B38">38</xref>]</sup>.</p>
      <p>From a textile perspective, a wide range of hierarchical structures meet the design requirements of diverse TENG configurations, spanning structural dimensions from fibrils and one-dimensional (1D) yarns to two-dimensional (2D) fabrics and complex 3D structures [<xref ref-type="fig" rid="fig2">Figure 2D</xref>]. Fibrils are the fundamental building blocks of textiles and generally do not directly execute functional roles at the device level. Through various assembly techniques, thousands of individual fibers can be twisted or interlocked to form 1D yarns<sup>[<xref ref-type="bibr" rid="B39">39</xref>]</sup>. A single 1D yarn subjected to mechanical stress can operate in single-electrode mode, generating electrical signals to detect the applied mechanical strains. Alternatively, two 1D yarns twisted around each other can be assembled into a contact-separation-mode TENG. Furthermore, 1D yarns can be seamlessly integrated into 2D or 3D textiles via sewing<sup>[<xref ref-type="bibr" rid="B40">40</xref>]</sup>, weaving<sup>[<xref ref-type="bibr" rid="B41">41</xref>]</sup>, braiding<sup>[<xref ref-type="bibr" rid="B42">42</xref>]</sup>, and other textile manufacturing processes. Specifically, 2D woven structures include plain<sup>[<xref ref-type="bibr" rid="B43">43</xref>,<xref ref-type="bibr" rid="B44">44</xref>]</sup>, twill<sup>[<xref ref-type="bibr" rid="B45">45</xref>]</sup>, and satin weaves, whereas 2D knitted structures include weft<sup>[<xref ref-type="bibr" rid="B46">46</xref>]</sup> knitting and warp knitting. Benefiting from their complex spatial architectures, the fibrous networks can undergo a series of pre-designed deformations in response to dynamic external forces, thereby efficiently converting biomechanical energy into electricity and detecting the deformation process. By introducing additional Z-direction longitudinal yarns into a biaxial structure, a fully interlocked 3D structure can be fabricated<sup>[<xref ref-type="bibr" rid="B47">47</xref>]</sup>. These 3D architectures create additional contact-separation spacing, effectively enhancing the output power density of MEFs. In addition, nonwoven fabrication techniques, such as melt-blowing<sup>[<xref ref-type="bibr" rid="B48">48</xref>]</sup> and electrospinning<sup>[<xref ref-type="bibr" rid="B49">49</xref>,<xref ref-type="bibr" rid="B50">50</xref>]</sup>, are widely used to fabricate MEFs with micro- and nanoscale structures.</p>
      <p>Currently, wearable systems based on MEFs predominantly employ a hybrid architecture consisting of fiber-based sensing/energy harvesting units, flexible interconnects, and conventional electronic modules. The MEFs are responsible for sensing or energy conversion, while signal conditioning, processing, and communication functions are handled by mature, miniaturized electronic modules, with the two subsystems interfaced through flexible interconnections. This approach balances the mechanical compliance and wearability of fibers with the high performance and reliability of conventional electronic modules, representing the most feasible technical pathway. The raw signals generated by MEFs typically exhibit the following characteristics: low current amplitude (mA level or below), high source impedance (MΩ level), and low frequency (0.1 Hz to tens of Hz). Accordingly, the core tasks of front-end signal conditioning include impedance matching, buffering, filtering, amplification, and decoupling. These tasks are typically implemented on a flexible printed circuit (FPC). Subsequently, the data are transmitted to a microcontroller unit (MCU) for conversion and processing, where digital filtering, baseline drift removal, and feature parameter extraction are performed as required by the target application. For computationally demanding tasks, processed data can be transmitted to a mobile device or cloud platform for further processing. Bluetooth Low Energy (BLE) is the most widely adopted wireless solution for wearable devices, offering low power consumption, excellent smartphone compatibility, and suitability for transmitting sensor signals at moderate data rates (tens of kbps). A prevalent approach for establishing electrical interconnects involves exposing the inner conductive layer at the fiber end and using silver paste, carbon paste, or other conductive adhesives to establish low-resistance electrical connections between the fiber electrodes and the FPC. On the FPC, circuit traces interconnect the signal processing chips to communication modules. Owing to their bending durability, FPCs can conform to local fabric curvature and can be either sutured or adhered to the textile surface.</p>
    </sec>
    <sec id="sec4">
      <title>APPLICATIONS</title>
      <sec id="sec4-1">
        <title>Self-sufficient energy systems</title>
        <p>Given the ubiquity of textiles in daily life, MEFs can serve as the energy conversion core of self-sufficient wearable electronic systems on the human body. These systems can convert low-frequency, irregular biomechanical energy, including limb swinging during locomotion<sup>[<xref ref-type="bibr" rid="B51">51</xref>]</sup>, joint flexion-extension, and even subtle respiratory chest excursions, into electricity in real time to power wearable electronics attached to clothing or skin. The harvested electricity directly sustains continuous monitoring of physiological signals, including heart rate, blood oxygen saturation, body temperature, kinematic postures, and biochemical markers in sweat, thereby establishing a closed-loop energy and information system characterized by “harvesting from and feeding back to the human body”.</p>
        <p>To enhance electrical output, two primary strategies are intuitive: improving the contact electrification capability of materials and engineering fabric architectures with superior spatial utilization. Given the stringent safety requirements for wearable electronics, adopting bio-based materials as triboelectric layers is a highly viable approach. For example, Xiong <italic>et al.</italic> developed a scalable core-sheath yarn (CSY) via ring-spinning covering technology, comprising a conductive steel-wire-embedded polyethylene terephthalate (PET) filament core and a wool yarn sheath [<xref ref-type="fig" rid="fig3">Figure 3A</xref>], thereby integrating the antistatic properties of wool with triboelectric energy harvesting<sup>[<xref ref-type="bibr" rid="B52">52</xref>]</sup>. The resulting CSY knitted fabric (CSYF) delivers an open-circuit voltage <italic>V</italic><sub>oc</sub> of ~430 V, a short-circuit current <italic>I</italic><sub>sc</sub> of ~2.7 μA, and a power density of ~740 mW·m<sup>-2</sup> under 2 Hz mechanical excitation, outperforming most yarn-based triboelectric textile devices. In contrast, the surface modification of conventional polymer fibers offers even broader applicability. In a representative work by Park <italic>et al.</italic>, a skin-rubbing single-electrode TENG called a co-weaving triboelectric generator (TEG) was fabricated, featuring a core of silver-plated copper yarn wrapped in polyester yarn, and a porous triboelectric layer formed by dip-coating silicone rubber templated with sugar particles<sup>[<xref ref-type="bibr" rid="B53">53</xref>]</sup>. This fiber was co-woven with a perspiration electric generator (PEG), and this hybrid design mitigates both humidity-induced TEG degradation and the delayed response of PEGs that rely on sweat secretion. Consequently, the device achieves a peak current of ~8.8 μA and a maximum power density of 166 μW·cm<sup>-2</sup>. Sun <italic>et al.</italic> proposed a novel mechanism based on interconnected electron-cloud potential wells (ECPWs) and constructed a TENG employing ethyl cellulose/reduced graphene oxide (EC/rGO) as the positive triboelectric layer and polydimethylsiloxane/reduced graphene oxide (PDMS/rGO) as the negative counterpart<sup>[<xref ref-type="bibr" rid="B54">54</xref>]</sup>. The conductive rGO network activates bulk electrons within the dielectric layers, overcoming the limitation of conventional TENGs where charge transfer is strictly confined to surface electrons. The resulting TENG achieves record-high outputs for contact-separation mode TENGs, including an <italic>I</italic><sub>sc</sub> of 3,180 μA, a current density of <InlineParagraph>~3,533 mA·m<sup>-2</sup>,</InlineParagraph> a charge density of 867 μC·m<sup>-2</sup>, and a maximum output power of 346 mW. To further enhance the triboelectric performance of polymers, high-permittivity inorganic fillers can be incorporated into the polymer matrix<sup>[<xref ref-type="bibr" rid="B55">55</xref>]</sup>. Such fillers typically exhibit superior dielectric constants compared to pristine polymers, thereby effectively enhancing their electron-donating or -accepting capabilities. Chou <italic>et al.</italic> constructed a stretchable, non-contact fabric-based TENG by introducing the topological insulator Bi<sub>2</sub>Se<sub>3</sub> into the triboelectric system<sup>[<xref ref-type="bibr" rid="B56">56</xref>]</sup>. Comprising a Bi<sub>2</sub>Se<sub>3</sub> nanosheet topological insulator/silicone rubber composite layer for triboelectrification and charge trapping/transport, a graphite-like carbonized textile serving as a charge reservoir, and a silver nanowire (AgNW)-decorated Lycra fabric acting as a stretchable electrode, this stretchable textile-based non-contact TENG achieves an ultralong charge retention time of <InlineParagraph>5,000 min</InlineParagraph> alongside efficient non-contact power generation, effectively circumventing the issues of contact friction loss and skin irritation for wearable TENGs.</p>
        <fig id="fig3" position="float">
          <label>Figure 3</label>
          <caption>
            <p>Scale-fabricable high-performance MEFs for energy conversion: (A) Large-scale wrapping spinning process and structure illustration of wool-based CSY. Reprinted with permission from<sup>[<xref ref-type="bibr" rid="B52">52</xref>]</sup>. Copyright 2025, Wiley; (B) 3D fiber formats based on scalable thermal processing of water-resistant thermoplastic elastomers and composites. Reprinted with permission from<sup>[<xref ref-type="bibr" rid="B57">57</xref>]</sup>. Adhering to the CC BY 4.0 agreement. MEFs: Mechano-electric fibers; CSY: core-sheath yarn; 3D: three-dimensional; PET: polyethylene terephthalate; SEBS: styrene-ethylene-butylene-styrene; PTFE: polytetrafluoroethylene.</p>
          </caption>
          <graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="ss60171.fig.3.jpg" />
        </fig>
        <p>Compositional engineering alone cannot fully mitigate the energy dissipation caused by inadequate interfacial contact or interfacial slippage in flexible textiles under real-world wearing conditions. By spatially arranging these materials to achieve ordered and efficient contact-separation cycles, the mechano-electric conversion interfaces can be substantially optimized, and the effective contact area maximized, thereby realizing a holistic synergistic enhancement in device performance. At the single-fiber level, Dong <italic>et al.</italic> designed a fiber-based TENG operating in the contact-separation mode, featuring an inner air gap and a micro-textured surface [<xref ref-type="fig" rid="fig3">Figure 3B</xref>]<sup>[<xref ref-type="bibr" rid="B57">57</xref>]</sup>. Utilizing a stretchable conductive composite of carbon nanotubes (CNTs), high-density polyethylene (HDPE), and styrene-ethylene-butylene-styrene (SEBS), they achieved scalable and controllable thermal drawing from centimeter-scale preforms to kilometer-long continuous fibers. The resulting fiber exhibits exceptional waterproofness, moisture resistance, and high deformability, effectively overcoming the poor environmental adaptability and limited mechanical compliance of conventional fiber-based TENGs. For 2D textiles, Ahmed <italic>et al.</italic> developed a fully weft-faced structured fabric (FWSF) employing silver-plated nylon conductive yarns as the warp and high-density nylon filaments as the weft<sup>[<xref ref-type="bibr" rid="B58">58</xref>]</sup>. The weft yarns completely encapsulate the warp to maximize the effective contact area for triboelectrification. When operating in the contact-separation mode against a BaTiO<sub>3</sub> (BTO) nanoparticle-doped PDMS composite film, it delivers a peak power density of 2,408.70 mW·m<sup>-2</sup>, a <italic>V</italic><sub>oc</sub> of ~621 V, an <italic>I</italic><sub>sc</sub> of ~13.76 μA, and a charge density of 7.5 nC·cm<sup>-2</sup>. The 3D fabrics further elevate the spatial and architectural complexity of the system. So and Xu reported a woven double-cloth TENG (WDC-TENG) that utilizes copper-nickel alloy fabric and BTO-doped PDMS, wherein the double-weave architecture inherently generates multiple triboelectric interfaces<sup>[<xref ref-type="bibr" rid="B59">59</xref>]</sup>. Consequently, the WDC-TENG achieves a remarkable power density of 15 W·m<sup>-2</sup>, an <italic>I</italic><sub>sc</sub> of 0.7 mA, and delivers ~250 V and 602 μA during operation as a smart insole.</p>
      </sec>
      <sec id="sec4-2">
        <title>User behavior and physiological information sensing</title>
        <p>Human motions such as hand clapping, finger tapping, arm touching, walking, running, and jumping are the most readily detectable signals for MEFs. By continuously acquiring kinematic parameters, including joint angles, gait characteristics, and postural variations, these fabrics can provide an objective basis for sports injury risk assessment, rehabilitation training progress tracking, and personalized exercise prescription. Meanwhile, body motion data can serve as an intentional input source for human–machine interaction (HMI), facilitating natural and efficient intelligent control and assisted decision-making<sup>[<xref ref-type="bibr" rid="B60">60</xref>]</sup>. Su <italic>et al.</italic> presented a representative study focusing on health monitoring and rehabilitation training<sup>[<xref ref-type="bibr" rid="B61">61</xref>]</sup>. They employed silica nanofibers and cellulose nanofibers to construct an aerogel skeleton, introducing ZnO@ZIF-8 core–shell heterojunction particles to enhance triboelectric polarity. This design yielded a layer–pillar ordered porous structure that exhibited a pressure sensitivity of 12.1 mV·Pa<sup>-1</sup>, alongside response and recovery times of 100 ms. Furthermore, a four-channel TENG sensing system integrated into a neck shield and coupled with a convolutional neural network (CNN)-based machine-learning algorithm achieved 97% recognition accuracy for eight distinct neck movements. This system enables cervical spine health management, early warning of poor posture, and quantitative evaluation of rehabilitation training. In the realm of personalized sports training, Chen <italic>et al.</italic> prepared a piezoelectric–triboelectric synergistic composite elastic sensing yarn featuring a coaxial three-layer structure of PDMS/poly(vinylidene fluoride) (PVDF)/elastic silver-plated nylon yarn<sup>[<xref ref-type="bibr" rid="B62">62</xref>]</sup>. They further designed a nine-channel E-PT yarn array wrapped around a tennis racket to enable zoned and independent sensing [<xref ref-type="fig" rid="fig4">Figure 4A</xref>]. The pressure sensitivity across different functional zones reached 0.0263, 0.0094, and 0.0018 V·kPa<sup>-1</sup>. By integrating the nine-channel yarn sensing array with a smart elbow brace and CNN machine learning, this system achieved 95% accuracy in recognizing six tennis strokes and 98.3% accuracy in classifying racket-face angles, enabling real-time identification and feedback of hitting postures and ball-impact locations.</p>
        <fig id="fig4" position="float">
          <label>Figure 4</label>
          <caption>
            <p>MEFs have extensive applications in body monitoring and HMI: (A) Schematic diagram of the smart tennis training system. Reprinted with permission from<sup>[<xref ref-type="bibr" rid="B62">62</xref>]</sup>. Copyright 2024, Wiley; (B) The all-textile pressure sensors could monitor pulse and respiratory signals in real time. Reprinted with permission from<sup>[<xref ref-type="bibr" rid="B64">64</xref>]</sup>. Adhering to CC BY-NC 4.0 agreement; (C) The layer-by-layer structure and the flexibility of A­Textile (Scale bar: 2 cm). Reprinted with permission from<sup>[<xref ref-type="bibr" rid="B69">69</xref>]</sup>. Adhering to CC BY-NC 4.0 agreement; (D) The exploded view and the broad applications of the UTE-skin. Reprinted with permission from<sup>[<xref ref-type="bibr" rid="B74">74</xref>]</sup>. Adhering to CC BY 4.0 agreement. MEFs: Mechano-electric fibers; HMI: human–machine interaction; UTE: untethered triboelectric electronic; PDMS: polydimethylsiloxane; PVDF: poly(vinylidene fluoride); E-PT: elastic piezoelectric-triboelectric; NFs-SR: nanoflower–silicone rubber; NFs-GT: nanoflower–decorated graphite-like carbonized textile.</p>
          </caption>
          <graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="ss60171.fig.4.jpg" />
        </fig>
        <p>Notably, among the various wearable configurations for body motion sensing, gesture recognition gloves worn directly on the hands, the most dexterous part of the human body, can capture fine motions such as finger flexion/extension, wrist rotation, and multi-joint coordination with high spatiotemporal resolution. These gloves provide a self-powered, unconstrained natural input interface suitable for both immersive virtual manipulation and silent sign language translation. For example, Xu <italic>et al.</italic> developed a self-powered electrotactile textile haptic (SPETH) glove that realizes passive electrotactile feedback based on TENG-driven gas discharge tube (GDT) breakdown<sup>[<xref ref-type="bibr" rid="B63">63</xref>]</sup>. Tests on 30 subjects revealed that the comfortable perceived energy thresholds were approximately 10 μJ for females and 30 μJ for males. Moreover, the perceived intensity could be precisely regulated by modulating the capacitance, GDT breakdown threshold, and electrode position. Thus, this glove could be used in prosthetics, robotic tactile feedback, and electrostimulation rehabilitation therapy.</p>
        <p>In addition to large-scale body movement perception and fine hand movement decoding, MEFs are also capable of monitoring even weaker physiological signals. The subtle surface deformations induced by pulse waves place higher demands on sensor sensitivity and signal-to-noise ratio (SNR), while they contain a wealth of physiological information. Continuous analysis of parameters including pulse wave morphological features, peak-to-peak intervals, and their variability enables non-invasive assessment of heart rate, blood pressure trends, and arterial stiffness, thereby providing critical data for long-term, unobtrusive dynamic monitoring of cardiovascular system health. Fan <italic>et al.</italic> developed a triboelectric all-textile sensor array (TATSA) to monitor the pulse waves and respiratory waves simultaneously and constructed a wireless mobile health monitoring system (WMHMS) for noninvasive assessment of cardiovascular disease and sleep apnea syndrome [<xref ref-type="fig" rid="fig4">Figure 4B</xref>]<sup>[<xref ref-type="bibr" rid="B64">64</xref>]</sup>. The TATSA used stainless steel as the core, with Terylene yarns twisted onto the surface of a conductive yarn (0.2 mm in diameter). Its pressure sensitivity reached 7.84 mV·Pa<sup>-1</sup> under low-pressure conditions (&lt; 4 kPa) and 0.31 mV·Pa<sup>-1</sup> under high-pressure conditions (&gt; 4 kPa). Liang <italic>et al</italic>. developed wearable self-powered pressure sensors using the natural 3D network fibers of Juncus effusus as a biological template<sup>[<xref ref-type="bibr" rid="B65">65</xref>]</sup>, and Shao <italic>et al.</italic> reported a highly efficient, breathable, and stretchable monolithic hybrid triboelectric-piezoelectric-electromagnetic nanogenerator-based electronic skin (TPEG-skin) based on a topological-insulator-composite<sup>[<xref ref-type="bibr" rid="B66">66</xref>]</sup>. Their sensitivities reach 5.39 V·N<sup>-1</sup> (&lt; 0.2 N) and 111.25 V·kPa<sup>-1</sup> (0-0.8 kPa), respectively, enabling high-fidelity acquisition of arterial pulse waveforms.</p>
        <p>Another monitoring application that also relies on detecting weak mechanical vibrations is acoustic sensing. MEFs can transduce micro/nano-scale deformations induced by laryngeal skin vibrations and environmental acoustic waves into electrical signals, leveraging their highly sensitive contact electrification response<sup>[<xref ref-type="bibr" rid="B67">67</xref>]</sup>. Such acoustic sensing capability exhibits significant application potential in scenarios including high-SNR speech recognition in noisy environments and assistive communication for individuals with speech impairments<sup>[<xref ref-type="bibr" rid="B68">68</xref>]</sup>. For instance, Shao <italic>et al</italic>. presented a triboelectric acoustic perceiving textile (A-Textile), overcoming the limitation of conventional acoustic textiles that rely on rigid cavities [<xref ref-type="fig" rid="fig4">Figure 4C</xref>]<sup>[<xref ref-type="bibr" rid="B69">69</xref>]</sup>. They designed an SnS<sub>2</sub> nanoflower–silicone rubber (SnS<sub>2</sub> NFs-SR) charge trapping and transport layer, and a SnS<sub>2</sub> NFs-decorated graphite-like carbonized textile (SnS<sub>2</sub> NFs-GT) charge storage layer to maximize charge density and retention time. By incorporating a 2D CNN deep learning model, speech recognition based on A-Textile was realized, with direct integration into generative AI (e.g., ChatGPT), IoT, and cloud services.</p>
        <p>Although MEFs have demonstrated highly sensitive responses in body motion tracking and physiological monitoring, their transition to practical wearable textiles imposes stringent requirements beyond conventional safety, breathability, and washability. Specifically, they must effectively suppress dielectric property drift caused by moisture adsorption<sup>[<xref ref-type="bibr" rid="B70">70</xref>]</sup>, sensing baseline shifts induced by repeated mechanical deformations, and electrostatic crosstalk arising from accumulated surface charges. Furthermore, sufficient tensile strength and abrasion resistance are imperative to ensure long-term structural integrity, enabling the stable and reliable extraction of physiological and kinematic data. To isolate moisture interference and improve the stability of mechano-electric conversion output, Qu <italic>et al.</italic> engineered a ZIF-8/polydopamine (PDA)/cotton fabric composite system<sup>[<xref ref-type="bibr" rid="B71">71</xref>]</sup>. By applying a hexadecyltrimethoxysilane (HDTMS) hydrophobic modification, they achieved a superhydrophobic surface with a water contact angle of 154°. This strategy effectively mitigated triboelectric charge dissipation in high-humidity environments, yielding an output attenuation of less than 5% at 80% RH and an ultrafast recovery time of merely 25 s. Adopting an alternative approach based on natural cotton fabrics, Lin <italic>et al.</italic> sequentially modified the fiber surfaces with PDA, MXene, and octadecylamine (ODA) to simultaneously enhance the electron-donating capability, surface potential, dielectric constant, and hydrophobicity<sup>[<xref ref-type="bibr" rid="B72">72</xref>]</sup>. This cotton-textile-based TENG (CT-TENG) achieved a water contact angle of 134.5°, which effectively prevented water penetration and subsequent charge dissipation. At 90% RH, the <italic>V</italic><sub>oc</sub> retention of CT-TENG reached 80.6%, which is far superior to that of unmodified cotton (58.9%). In terms of mechanical stability, Lu <italic>et al.</italic> utilized microphase separation to induce a nanofiber network and a polycrystalline domain-crosslinked architecture<sup>[<xref ref-type="bibr" rid="B73">73</xref>]</sup>. This structure contained a polyvinyl alcohol (PVA) and cellulose nano fibril (CNF) system, and yielded a tensile strength of 42.5 MPa, a fracture toughness of 78.6 MJ·m<sup>-3</sup>, and an elongation at break of 342%. The resulting stable long-term cyclical signals effectively address the chronic issues of stress concentration, signal drift, and premature failure in triboelectric materials. To overcome electrostatic interference and signal crosstalk in large-area multiplexed sensing, Shao <italic>et al.</italic> employed a carbon black-doped Ecoflex composite to construct an omnidirectionally stretchable shielding layer [<xref ref-type="fig" rid="fig4">Figure 4D</xref>]<sup>[<xref ref-type="bibr" rid="B74">74</xref>]</sup>. This configuration realized a fully intrinsically stretchable, large-area TENG electronic skin. Notably, this approach reduced the false recognition rate of a single-electrode mode TENG array to a mere 0.20%, and the line interference voltage dropped to 0.10 V upon grounding the shielding layer.</p>
      </sec>
      <sec id="sec4-3">
        <title>Personal safety protection</title>
        <p>In HMI scenarios, MEFs capture the wearer’s conscious commands. Concurrently, clothing and other textile platforms serve as the primary physical barrier against environmental contaminants and provide thermal insulation against temperature extremes, passively safeguarding the wearer’s health and safety. Filtration is a typical mechanism-driven application. When integrated into a face mask, the high voltage generated by the contact electrification process of MEFs endows the filter media with a robust electrostatic adsorption effect<sup>[<xref ref-type="bibr" rid="B75">75</xref>]</sup>, thereby enhancing the capture efficiency for fine particulate matter<sup>[<xref ref-type="bibr" rid="B76">76</xref>]</sup>. Simultaneously, the waveform and amplitude of the electrical signals produced by the respiration-driven MEFs are directly correlated with breathing depth, respiratory rate, and coughing events, thus enabling self-powered, continuous respiratory monitoring that extends beyond mere filtration protection<sup>[<xref ref-type="bibr" rid="B77">77</xref>]</sup>. Regarding the adsorption of inhalable particulate matter, Yang <italic>et al.</italic> engineered a polyacrylonitrile (PAN) nanofiber/polystyrene (PS) microfiber composite mat<sup>[<xref ref-type="bibr" rid="B78">78</xref>]</sup>. The PS microfibers acted as a supporting skeleton to minimize airflow resistance, while PAN nanofibers served as highly efficient physical interception layers, thereby strengthening filtration performance through two synergistic mechanisms of electrostatic capture and physical interception. For PM<sub>0.3</sub> filtration, the optimal efficiency reached 99.98% at an airflow rate of <InlineParagraph>32 L·min<sup>-1</sup>.</InlineParagraph> Remarkably, efficiency remained above 98% even in an extremely polluted environment (PM<sub>2.5</sub> = 23,000 μg·m<sup>-3</sup>), and it sustained 99.43% efficiency over 48 h under typical daily conditions. Furthermore, the mask exhibited a pressure drop of merely 35 Pa at 32 L·min<sup>-1</sup>, and the filtration efficiency remained at approximately 80% even at 85% RH. Cho <italic>et al.</italic> developed a fully biodegradable poly(butylene adipate-co-terephthalate) (PBAT) and cetyltrimethylammonium bromide (CTAB)-modified montmorillonite (CTAB-MMT) composite fiber as the core component of a face mask<sup>[<xref ref-type="bibr" rid="B79">79</xref>]</sup>. This design simultaneously achieves high-efficiency PM<sub>0.3</sub> filtration, respiration-driven self-powered electrostatic adsorption, broad-spectrum antibacterial and potent antiviral functionalities, and complete biodegradability. The CTAB-MMT decomposed entirely within 6 to 24 months under natural conditions, offering a sustainable alternative to non-degradable polypropylene (PP) melt-blown fabrics. The real-time analysis of electrical outputs generated by respiratory airflow-driven TENGs enables active, self-powered respiratory monitoring. Similarly, Yi <italic>et al.</italic> constructed a respiration-driven TENG air filtration unit composed of Nylon 66 (PA66)/chitosan quaternary ammonium salt (HACC) multiscale nanofibers (PA66/H, as the positive electrode) and poly(vinylidene fluoride-co-hexafluoropropylene) (PVDF-HFP, as the negative electrode) nanofiber membrane<sup>[<xref ref-type="bibr" rid="B80">80</xref>]</sup>. This TENG not only achieves synergistic physical interception and electrostatic adsorption but also distinguishes among normal, rapid, and deep breathing patterns, wirelessly transmitting signals via Bluetooth to facilitate real-time physiological monitoring.</p>
        <p>In addition to monitoring respiratory mechanical parameters, the MEF platform can also detect surface potential variations induced by gas-molecule adsorption via its triboelectric output signals, thereby enabling the concentration monitoring of hazardous gases such as ammonia. Ding <italic>et al.</italic> designed a respiration-driven air filter (RAF) featuring an electron-donating triboelectric layer comprising a CNF aerogel with <italic>in situ</italic> grown MIL-125 (a Ti-based metal-organic framework, MOF), which provides a 3D porous architecture and a high specific surface area<sup>[<xref ref-type="bibr" rid="B81">81</xref>]</sup>. This design integrates air filtration, catalytic ammonia degradation, and respiratory monitoring. It exhibits an ammonia degradation rate exceeding 20%, a sensitive voltage response within the 20-100 ppm concentration range, rapid response and recovery times of 14 and 23 s, respectively, and robust resistance to interfering gases, making it highly applicable to scenarios such as ammonia monitoring and catalytic degradation during seafood spoilage. Furthermore, Kovalska <italic>et al.</italic> developed a surfactant-free, water-based 2D heterostructure preparation process via ultrasonic spraying, enabling green, scalable integration of multilayer graphene/transition metal dichalcogenides (MLG/TMDs) onto textiles<sup>[<xref ref-type="bibr" rid="B82">82</xref>]</sup>. Notably, they realized the first wearable, self-powered styrene gas sensor with a response rate of 126%, effectively overcoming the limitations of traditional volatile organic compound sensors that require external power supplies and lack wearability.</p>
        <p>Beyond chemical and biological hazards, pervasive electromagnetic signals in the environment also pose potential health risks, particularly for vulnerable populations such as pregnant women and infants. MEFs possess an internal conductive network that provides electromagnetic Interference (EMI) shielding via ohmic losses and multiple reflections, independent of the mechano-electric conversion mechanism. Addressing this issue, Zhang <italic>et al.</italic> developed a coaxial wet-spun core–sheath fiber architecture [<xref ref-type="fig" rid="fig5">Figure 5A</xref>]<sup>[<xref ref-type="bibr" rid="B83">83</xref>]</sup>. This strain-insensitive electrode contains liquid metal (LM)/AgNW as the core and a thermoplastic urethane (TPU) as the sheath. AgNWs bridge adjacent LM droplets, and the conductive pathways are rapidly activated under low mechanical stress. The excellent electrical conductivity enables seamless four-function integration of self-powered sensing, kinetic energy harvesting, Joule heating, and EMI shielding. The EMI shielding effectiveness reaches an impressive 51 dB in the 2.17-3.3 GHz frequency range, attenuating approximately 99.99% of incident electromagnetic waves and establishing this fiber as an exceptional electromagnetically protective textile.</p>
        <fig id="fig5" position="float">
          <label>Figure 5</label>
          <caption>
            <p>Representative work for MEFs regarding personal safety protection: (A) Schematic diagram of the coaxial wet-spinning process, structural composition of the multifunctional triboelectric fiber, and potential applications. Reprinted with permission from<sup>[<xref ref-type="bibr" rid="B83">83</xref>]</sup>. Adhering to the CC BY 4.0 agreement; (B) Schematic of the TBT with great flame retardancy and thermal protective performance and the weaving process of the simulated lunar soil basalt textiles (Scale bar: 1 cm). Reprinted with permission from<sup>[<xref ref-type="bibr" rid="B87">87</xref>]</sup>. Copyright 2024, Wiley. MEFs: Mechano-electric fibers; TBT: triboelectric basalt textile; LM: liquid metal; AgNWs: silver nanowires; TPU: thermoplastic urethane; DMF: dimethylformamide; DI: deionized; PI: polyimide; NN-ST: NaNbO<sub>3</sub>–SrTiO<sub>3</sub>.</p>
          </caption>
          <graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="ss60171.fig.5.jpg" />
        </fig>
        <p>As MEFs transition from functional validation toward practical wearable applications, active temperature and humidity regulation capabilities are essential for dynamically maintaining the thermophysiological comfort of the intra-garment microclimate. MEFs can harvest energy to drive Joule heaters for active warming or power micro-thermoelectric devices for cooling, demonstrating the synergistic effect of self-powered operation and thermal management. Zhu <italic>et al.</italic> engineered a bioinspired, spider-web-like, hierarchically structured Janus nanofiber membrane via simultaneous electrospinning and electrospraying<sup>[<xref ref-type="bibr" rid="B84">84</xref>]</sup>. This membrane features a bilayer asymmetric architecture comprising a hydrophobic PVDF-HFP layer and a hydrophilic polyamide 6 (PA6) layer. For thermal and moisture management, a temperature differential of 7.4 °C across the membrane was achieved under 1 kW·m<sup>-2</sup> solar illumination. Furthermore, the electric-field-driven moisture transmission rate increased by 20% compared with passive diffusion. Exhibiting excellent water resistance, breathability, and unidirectional moisture transport, this membrane seamlessly integrates triboelectric energy harvesting, adaptive thermal and moisture regulation, and sterilization functionalities. Focusing on wearable thermal management, Moradi <italic>et al.</italic> reported PAN-MXene composite fibers that demonstrate broad potential for the active heating of smart textiles, flexible heat dissipation in electronic devices, and personal thermoregulation<sup>[<xref ref-type="bibr" rid="B85">85</xref>]</sup>. PAN served as the polymer matrix and Ti<sub>3</sub>C<sub>2</sub>T<sub>x</sub> MXene nanosheets served as the functional filler at a high loading of 50 wt%. The MXene nanosheets were uniformly distributed both on the fiber surfaces and within the interstitial spaces, thereby establishing robust thermally and electrically conductive pathways. Achieving a maximum power density of 432.7 mW·m<sup>-2</sup>, the resulting composite yarns can be directly woven into smart fabrics, offering an optimal combination of flexibility, durability, and industrial manufacturability.</p>
        <p>Concurrently, flame retardancy fundamentally guarantees the thermal safety of the devices under extreme conditions such as high temperatures and open flames<sup>[<xref ref-type="bibr" rid="B86">86</xref>]</sup>. Li <italic>et al.</italic> developed an ultra-wide-temperature-range TENG (triboelectric basalt textile, TBT), effectively overcoming the limited operating-temperature range of conventional TENGs [<xref ref-type="fig" rid="fig5">Figure 5B</xref>]<sup>[<xref ref-type="bibr" rid="B87">87</xref>]</sup>. Utilizing melt-drawn basalt fiber fabric as both the electrode and the thermally insulating flame-retardant layer, paired with a polyimide (PI)/NaNbO<sub>3</sub>–SrTiO<sub>3</sub> (NN-ST) composite nanofiber membrane as the triboelectric counterpart, the resulting TBT retained over 85% of its initial voltage at -196 °C (in liquid nitrogen) and approximately 55% at 520 °C (in an alcohol lamp flame). Remarkably, the limiting oxygen index (LOI) reached an exceptional 90%, and the fabric exhibited neither combustion nor internal structural damage after 180 s of direct flame exposure. To enhance flame retardancy, Qiao <italic>et al.</italic> employed interfacial molecular engineering for the non-destructive sizing modification of poly(p-phenylene-2,6-benzobisoxazole) (PBO) fibers with aminonaphthalimide (NDI-NH<sub>2</sub>), followed by a hot-pressing consolidation process<sup>[<xref ref-type="bibr" rid="B88">88</xref>]</sup>. The assembled single-electrode TENG showed a thermal decomposition index of 303.9 °C, a 5% weight-loss temperature (Td) of 497.3 °C, and an LOI of 36.4%. The material demonstrated excellent self-extinguishing behavior in an open flame without any melt dripping. While flame retardancy inherently arises from the properties of constituent materials, MEFs can add new functional dimensions to flame-retardant protection. For instance, their electrical output signals can be used for early fire warning, thereby converting passive flame retardancy into active protection. In summary, the seamless integration of heat resistance, intrinsic flame retardancy, and robust triboelectric functionality establishes a new paradigm of material–structure–performance synergy for self-powered electronics operating in extreme environments.</p>
      </sec>
    </sec>
    <sec id="sec5">
      <title>OUTLOOK</title>
      <p>By seamlessly integrating TENG technology with textiles, MEFs perform the dual functions of energy harvesting and multimodal information sensing, providing an optimized solution to the challenges of sustainable power supply and enhanced sensing capabilities in wearable systems. These technological features are primarily manifested in two aspects: (1) the unique energy conversion mechanism of TENGs enables the efficient transduction of human motion into quantifiable electrical signals; and (2) textile substrates possess flexibility, physiological compatibility, and scalable manufacturability. In conclusion, MEFs provide new solutions to the long-standing dependence of sensing systems on external power sources and overcome the limitations in information acquisition pathways, ultimately transforming the human body into a unified entity that serves as both the biomechanical energy source and the endpoint for power consumption.</p>
      <p>Looking ahead, fully self-sufficient MEF-based energy systems still face several core challenges that are closely tied to the fiber and textile nature of these devices. Achieving a practical balance among high electrical output, sensing functionality, wear comfort, mechanical durability, and scalable production remains the central bottleneck impeding the translation of self-sufficient MEF systems into real-world applications. For example, the structure–property relationships in woven topologies remain poorly understood. The electrical output of MEF textiles is not simply a linear superposition of individual fiber outputs; factors including warp–weft interlacing patterns, yarn twist, fabric density, and layered architecture strongly influence inter-fiber contact–separation behavior, stress-transfer efficiency, and charge-collection pathways. Drawing on structural design principles from textile engineering can provide systematic approaches to tailoring inter-fiber contact area, contact pressure, and gap distances. In addition, yarn twisting and wrapping techniques can construct helical or spring-like fiber architectures, thereby enhancing stretchability and output stability. At the same time, fiber-scale interconnection has rarely been treated as a dedicated technical module requiring systematic design and evaluation. Critical issues such as electrode routing, low-resistance interconnection reliability, stress concentration and fatigue failure at contact points, and signal crosstalk in multi-fiber integration remain unresolved. Future research must therefore advance fiber-scale micro-interconnection technologies, develop flexible strain-relief structures, and establish standardized interface specifications and reliability testing protocols to enable seamless integration of MEFs with existing electronic systems.</p>
      <p>Another critical issue specific to MEFs is electrical stability and durability under multiaxial deformation. Unlike planar TENGs, which typically operate under relatively simple deformation modes, MEFs in real wearing conditions are subjected to complex multimodal deformations, including bending, torsion, stretching, and shearing, often at amplitudes and frequencies far exceeding those of conventional TENGs. To address these challenges, flexible encapsulation and self-healing strategies are particularly promising. Ultra-thin flexible encapsulation layers and self-healing dielectric or electrode materials based on dynamic covalent bonds or supramolecular interactions can significantly improve durability under multiaxial deformation and over repeated washing cycles.</p>
      <p>Alongside these structural and material innovations, user behavior perception and physiological signal monitoring still suffer from insufficient linearity and limited resistance to interference. Future advancements in user behavior perception will focus on multimodal interaction innovations and fine motion capture. This involves integrating multiple sensing modalities, such as pressure and bending, to enrich the interaction experience. Besides, developing non-contact MEF sensors also extends device lifetimes and expands applicable scenarios. With the aid of intelligent diagnostic algorithms such as deep learning, multi-source and longitudinal physiological data can be fused and analyzed to enable automated disease diagnosis and risk assessment, thereby advancing personalized medicine and remote health management.</p>
      <p>For environmental safety and personal protection, MEF development trends focus on improving selectivity toward hazardous factors and supporting emergency rescue operations. The development of nanofibrous materials with high specific surface areas and tailored adsorption properties, alongside multilayer composite filter media, will strengthen particulate matter capture capabilities. Furthermore, functional group modification and sensitive material screening can significantly enhance the selective detection of specific toxic gases. Their integration into a smart healthcare system triggers automatic responses, ensuring environmental health and safety.</p>
      <p>Addressing these critical issues will open a new chapter for the development of MEFs. Ultimately, this will enable MEFs to deliver higher-quality services, safeguard physical and mental well-being, facilitate intelligent interactions, and ensure robust protection.</p>
    </sec>
  </body>
  <back>
    <sec>
      <title>DECLARATIONS</title>
      <sec>
        <title>Authors’ contributions</title>
        <p>Conceptualization: Zhao, J.; Dong, K.</p>
        <p>Investigation: Zhao, J.; Li, H.; Fan, X.; Xie, H.</p>
        <p>Writing - original draft: Zhao, J.</p>
        <p>Writing - review and editing: Dong, K.</p>
        <p>Project administration: Dong, K.</p>
        <p>Funding acquisition: Zhao, J.; Dong, K.</p>
      </sec>
      <sec>
        <title>Availability of data and materials</title>
        <p>Not applicable.</p>
      </sec>
      <sec>
        <title>AI and AI-assisted tools statement</title>
        <p>Not applicable.</p>
      </sec>
      <sec>
        <title>Financial support and sponsorship</title>
        <p>This work was supported by the National Natural Science Foundation of China (Grant No. 22109012), China Postdoctoral Science Foundation (Grant No. 2024M753175), Changchun-CAS Science and Technology Innovation Joint Program (Grant No. 24SH06), Fundamental Research Funds for the Central Universities (Grant No. E1E46805), Natural Science Foundation of the Beijing Municipality (Grant No. L222037 and 2212052), Postdoctoral Fellowship Program of CPSF (Grant No. GZC20232612).</p>
      </sec>
      <sec>
        <title>Conflicts of interest</title>
        <p>Dong, K. is a Guest Editor of the special topic “Smart Fibers and Self-Powered Wearable Devices” of the journal <italic>Soft Science</italic>, but was not involved in any stage of editorial processing, including reviewer selection, manuscript handling, and decision-making, while the other authors have declared that they have no conflicts of interest.</p>
      </sec>
      <sec>
        <title>Ethical approval and consent to participate</title>
        <p>Not applicable.</p>
      </sec>
      <sec>
        <title>Consent for publication</title>
        <p>Not applicable.</p>
      </sec>
      <sec>
        <title>Copyright</title>
        <p>© The Author(s) 2026.</p>
      </sec>
    </sec>
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