High-voltage applications of the triboelectric nanogenerator— … · can be produced by...

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MRS Energy & Sustainability: A Review Journal page 1 of 23 © Materials Research Society, 2020 doi:10.1557/mre.2020.2 Introduction Triboelectric nanogenerators (TENGs), invented by Prof. Z.L. Wang in 2012, 1 are now becoming an emerging technol- ogy, which can scavenge ambient environmental mechanical energy stemming from winds, 7,159 vibrations, 156,158 water flows, 8,9 body motions, and so on, 2–6 to provide electricity to smart electronic devices. Through the combination of triboe- lectrification and electrostatic induction effects, the electricity can be produced by TENGs. 10–12 TENGs are not only an excel- lent energy harvester but also a self-powered active sensor since the detailed mechanical motion profiled can be revealed by the output electrical signals. 2 Employing TENGs, wind speed, 16 heart rate, 14 sound, 28,160 displacement, 15 and tactile touching 13 can be effectively and accurately sensed, where sleeping ABSTRACT Self-powered smart systems utilizing the high voltages generated by triboelectric nanogenerators (TENGs) have been systematically reviewed, with several featured applications highlighted, including electrospray, optical device, microplasma, and microfluidic. To provide a sustainable power solution for electronics, triboelectric nanogenerator (TENG) has been developed since 2012 for high-efficiency mechanical energy harvesting from the ambient environment. TENG has very unique output characteristics including high voltage and limited current density. Thus, it is challenging to directly power most of the commercial electronics in high efficiency. However, these features also bring opportunities for high-voltage applications. Here, we will review the efforts for developing TENG as a controllable high-voltage power source for various applications. The review article will start from fundamental studies about how the high-voltage output was generated, and then, several representative research in recent years will be reviewed, including electrospray, optical devices, microplasma, field emission, and electrically responsive materials. These studies will drive the further development of TENG technology for broad applications and industriali- zations toward high-efficiency self-powered systems. Keywords: energy generation; sensor; energetic material DISCUSSION POINTS • More approaches are expected to further enhance the electrical output performance of TENGs, for instance, eliminating or alleviating the air breakdown effect. • More innovative smart actuators employing electrically responsive materials should be developed to be driven by TENGs, considering the fact that TENGs have ultralow current and extremely high output voltage. • Innovative conjunction principle between TENGs and smart actuators can be anticipated, for example, wireless power transmission. High-voltage applications of the triboelectric nanogenerator— Opportunities brought by the unique energy technology Jiaqi Wang and Yunlong Zi , Department of Mechanical and Automation Engineering, The Chinese University of Hong Kong, Hong Kong, China; and Shun Hing Institute of Advanced Engineering, The Chinese University of Hong Kong, Hong Kong, China Shuyao Li and Xiangyu Chen, CAS Center for Excellence in Nanoscience, Beijing Key Laboratory of Micro-nano Energy and Sensor, Beijing Institute of Nanoenergy and Nanosystems, Chinese Academy of Sciences, Beijing 100083, People’s Republic of China; and School of Nanoscience and Technology, University of Chinese Academy of Sciences, Beijing 100049, People’s Republic of China Address all correspondence to Xiangyu Chen at [email protected] and Yunlong Zi at [email protected] (Received 9 November 2019; accepted 10 January 2020) REVIEW https://doi.org/10.1557/mre.2020.2 Downloaded from https://www.cambridge.org/core. IP address: 54.39.106.173, on 28 Dec 2020 at 02:19:51, subject to the Cambridge Core terms of use, available at https://www.cambridge.org/core/terms.

Transcript of High-voltage applications of the triboelectric nanogenerator— … · can be produced by...

Page 1: High-voltage applications of the triboelectric nanogenerator— … · can be produced by TENGs.10–12 TENGs are not only an excel-lent energy harvester but also a self-powered active

MRS Energy & Sustainability: A Review Journalpage 1 of 23© Materials Research Society, 2020doi:10.1557/mre.2020.2

IntroductionTriboelectric nanogenerators (TENGs), invented by Prof.

Z.L. Wang in 2012,1 are now becoming an emerging technol-ogy, which can scavenge ambient environmental mechanical energy stemming from winds,7,159 vibrations,156,158 water flows,8,9 body motions, and so on,2–6 to provide electricity to smart electronic devices. Through the combination of triboe-lectrification and electrostatic induction effects, the electricity can be produced by TENGs.10–12 TENGs are not only an excel-lent energy harvester but also a self-powered active sensor since the detailed mechanical motion profiled can be revealed by the output electrical signals.2 Employing TENGs, wind speed,16 heart rate,14 sound,28,160 displacement,15 and tactile touching13 can be effectively and accurately sensed, where sleeping

ABSTRACT

Self-powered smart systems utilizing the high voltages generated by triboelectric nanogenerators (TENGs) have been systematically reviewed, with several featured applications highlighted, including electrospray, optical device, microplasma, and microfluidic.

To provide a sustainable power solution for electronics, triboelectric nanogenerator (TENG) has been developed since 2012 for high-efficiency

mechanical energy harvesting from the ambient environment. TENG has very unique output characteristics including high voltage and limited

current density. Thus, it is challenging to directly power most of the commercial electronics in high efficiency. However, these features also

bring opportunities for high-voltage applications. Here, we will review the efforts for developing TENG as a controllable high-voltage power

source for various applications. The review article will start from fundamental studies about how the high-voltage output was generated, and

then, several representative research in recent years will be reviewed, including electrospray, optical devices, microplasma, field emission, and

electrically responsive materials. These studies will drive the further development of TENG technology for broad applications and industriali-

zations toward high-efficiency self-powered systems.

Keywords: energy generation; sensor; energetic material

DISCUSSION POINTS• Moreapproachesareexpectedtofurtherenhancetheelectrical

outputperformanceofTENGs,forinstance,eliminatingoralleviatingtheairbreakdowneffect.

• MoreinnovativesmartactuatorsemployingelectricallyresponsivematerialsshouldbedevelopedtobedrivenbyTENGs,consideringthefactthatTENGshaveultralowcurrentandextremelyhighoutputvoltage.

• InnovativeconjunctionprinciplebetweenTENGsandsmartactuatorscanbeanticipated,forexample,wirelesspowertransmission.

High-voltage applications of the triboelectric nanogenerator—Opportunities brought by the unique energy technology

Jiaqi Wang and Yunlong Zi , Department of Mechanical and Automation Engineering, The Chinese University of Hong Kong, Hong Kong, China; and Shun Hing Institute of Advanced Engineering, The Chinese University of Hong Kong, Hong Kong, China

Shuyao Li and Xiangyu Chen, CAS Center for Excellence in Nanoscience, Beijing Key Laboratory of Micro-nano Energy and Sensor, Beijing Institute of Nanoenergy and Nanosystems, Chinese Academy of Sciences, Beijing 100083, People’s Republic of China; and School of Nanoscience and Technology, University of Chinese Academy of Sciences, Beijing 100049, People’s Republic of China

Address all correspondence to Xiangyu Chen at [email protected] and Yunlong Zi at [email protected]

(Received 9 November 2019; accepted 10 January 2020)

RevIew

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monitoring 162 and human–machine interfacing161,163 greatly benefit. TENGs are born to have ability to provide high volt-ages. Compared with other energy harvesters such as solar cells and pyroelectric and piezoelectric devices, TENGs can achieve much higher output voltages owing to their ultralow capaci-tance.17,18 Several kilovolts open circuit voltage can be obtained using TENGs. Compared with traditional high-voltage sources, which are usually very bulky and difficult to be integrated in smart systems, TENGs can be fabricated extremely thin, attach-able, and flexible to be combined with other electronic or mechanical components. Besides, the traditional high-voltage sources can be dangerous during the operations because of the unexpected current leakage issues. In contrast, TENGs can be very safe since their output currents are usually in microampere level, which is not harmful to human beings.

As a high-voltage source, TENGs can be used to drive elec-trically responsible materials and devices, making them self- powered and well-integrated.19,164 Electrically, TENGs can be treated as a serial connection of a capacitor and an ideal volt-age source. The output of TENG is usually in the form of alter-nating current (AC).11 If direct current (DC) output is desired, a bridge rectifier is usually required. Over the past years, great efforts have been paid to manage the electrical power gener-ated by TENGs in circuit level. For instance, the output volt-age can be lowered by connecting an external capacitor, which shares transferred charges, and can be greatly enhanced via voltage multiplier circuits.20,21 In the TENG device, the out-put voltage can be greatly enhanced with improved triboelec-tric charges or alleviated breakdown effects.22–24 To improve the triboelectric charges, the surface of triboelectric layers can be patterned to enhance the contact areas 25 and the break-down effect can be alleviated or eliminated by the use of high-pressure gases or vacuum atmospheres.24 Until now, a vast variation of output voltages can be attained by TENGs, ranging from a few volts to several kilovolts, which meets the driving requirements of the majority of electrically responsi-ble materials and devices.

The electrically responsible materials which can be driven by TENGs include solids such as dielectric elastomers and piezoe-lectric films, liquids including liquid metals (LMs) and water droplets, and gases, for instance, rare gases etc. Driven by the electric field generated by the TENGs, smart devices can also be actuated, including micro-motors68,73,165 and electroadhesive patches (EAPs).116 By combining the high-voltage TENGs and responsible materials or devices, a great number of self- powered smart systems can be achieved. In this review, the latest developments of high-voltage applications of TENGs have been revealed, which provides in-depth understanding of TENG-driven smart systems. Figure 1 illustrates the theme of this review paper with several important examples featured, highlighting the conjunction principles. To the best of our knowledge, the self-powered smart systems with a conjunction of high-voltage TENGs and corresponding actuating materials and devices will be reviewed in detail, including the characteri-zation of high-voltage sources and actuators, driving requirements of materials and devices and the potential application fields.

Finally, the perspective future research directions have been expected to conclude this review.

TeNg as a high-voltage sourceTENGs are able to harvest various kinds of mechanical ener-

gies in ambient environments, where the operation mecha-nisms of TENGs are different. Over the past years, great efforts have been paid to improve the output voltage of TENGs, which greatly extends the applications of TENG-driven self-powered systems.

Mechanical motions to trigger TENGs

There are generally four basic operation modes of TENGs, involving vertical contact-separation (CS), lateral-sliding (LS), single-electrode (SE), and freestanding triboelectric-layer (FT) modes, as indicated in Fig. 2.2 For all these four operation modes, at least a pair of two different materials should be con-tacted for the triboelectrification and separated for the electro-static induction. The CS mode TENG is mainly used to harvest mechanical energies stemming from pressing and releasing, for instance, compression and touching.26,27 Besides, acoustic energy can also be scavenged by the CS mode TENGs, where the contact and separation of membranes can be triggered by sound.28,29 Different from the CS mode TENG, the LS mode TENG generates electricity by sliding, where two triboelectric layers will keep contacting, even though the contact area varies during the sliding process. One advantage of the LS mode TENG over the CS mode TENG is that the current output per-formance can be greatly improved when the striped triboelec-tric surfaces are used. 30,31

The disadvantages of both the CS and LS mode TENGs come from the wire connection of the moving triboelectric, which greatly hinders the flexibility of the mechanical motions. The SE and FT mode TENGs provide effective solutions to the wire connection issues, where one triboelectric layer can move freely without connected wires in these two TENGs.30,32–34 Besides, in the FT mode TENGs, the mechanical structure can be much more robust and the output voltage is usually much higher than that of the CS and SL mode TENGs. The SE mode TENGs have been mainly used to harvest the mechanical energy of vertical free-moving motions, such as stepping and raindrop collisions. Oppositely, the FT mode TENG can be used to scavenge ener-gies of free-sliding mechanical motions. Owing to their high output voltage, the FT-TENGs have been widely applied for the self-powered systems with high-voltage requirements.

Approaches for triboelectrification performance enhancement

Beside the structural design to harvest various kinds of mechanical energies, great efforts were made to enhance the triboelectrification performance. The selection of two triboe-lectric materials with larger affinity difference can also result in improved electrification performance. The material choosing priority should be given to two materials with larger distance in the series of triboelectrification.35,36 For given two materi-als for triboelectrification, the electrification performance is

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affected by the contact surface area.25,37,38 Patterning on the two triboelectric surfaces can improve the contact area for elec-trification, thus the output voltage can be greatly improved. Figures 3(a)–3(c) illustrate the structural characterization of the patterned polydimethylsiloxane (PDMS) thin film using the scanning electron microscope (SEM), the morphologies of which includes lines, cubes, and pyramids.25 Figure 3(d) indi-cates a comparison of output voltages of the CS mode TENGs using a polyethylene terephthalate (PET) film and PDMS films with various surface patterns. It can observed that the patterned surface can achieve at least 2-fold of the output voltage compared with the surface without patterning, and the TENG with the pyra-mid microstructure presents the highest output voltage.

In addition to the contact area enhancement, ionized air injection can also contribute to the high output performance of TENGs.22 Figures 4(a) and 4(b) illustrate the schematic diagram of the ionized air injection for the achievement of high-performance TENGs, and Fig. 4(c) shows a comparison of the transferred charge number before and after the ionized air injection. It can be observed that the ionized air injection approach can greatly facilitate the electrification and following

charge transferring process. However, it should be noted that the boosted electrification will be limited by the air breakdown effect, which is governed by Paschen’s law.23,24

Dielectric elastomers driven by TeNgsDielectric elastomers can be actuated by the high voltage

generated by the TENGs, from which self-powered optical mod-ulation can benefit. Among various optical modulators, tunable optical gratings (TOGs) is the core element of various optical splitting and light-connecting devices.39–42 The development of nanofabrication techniques has led to the creation of many new materials, such as various stretchable electrode materials, which have facilitated the improvement of dielectric elastomer actuator (DEA) devices. Besides, it also brings more possibili-ties to modify the TOGs systems on the basis of DEA.43–46 The DEA’s driving requirements for high voltage just match the TENG electrical output performance, and the breakdown effect in a TOG system can be eliminated or greatly alleviated because of the limited amount of transferred charge.47,48 Chen et al.49 proposed several different TOG systems that can adapt to the

Figure 1. Overview of high voltage applications of TENGs. Press-based TENG: Reproduced with permission.50 Copyright 2017, John Wiley and Sons. Rotating-based TENG, Electrospinning: Reproduced with permission.139 Copyright 2017, American Chemical Society. Rotating motor, optical scanning: Reproduced with permission.107 Copyright 2019, Springer Nature. Electroadhesive patch, electro-adhesion: Reproduced with permission.116 Copyright 2018, American Chemical Society. Argon, plasma display: Reproduced with permission.104 Copyright 2018, Springer Nature. Solid elastomer, tunable grating: Reproduced with permission.49 Copyright 2017, Elsevier. Droplet, mini-vehicle: Reproduced with permission.73 Copyright 2018, American Chemical Society.

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high voltage output of TENG [Fig. 5(a)]. The driving element for this kind of TENG–DEA conjunction system is an SE TENG using contact–separation motion to generate high-voltage con-trol signal, which means that an efficient and reliable operation of DEA device can be achieved. In the triboelectric course of two electrode materials, aluminum (Al) tends to be positively charged and Kapton is the opposite. Three specific TOG models for this structure are proposed, which can greatly improve the self-powered effect. The compression mode TOG [Figs. 5(b) and 5(c)] is consisted of two DEA elements and a grating array, which is made by aggregated metallic nanoparticles. The elasto-mer film is constrained by the boundary frames, so that the induced strain concentrated in the middle part can help DEA to smoothly deform. In a self-driven system, the two elastomers dilate due to the base of TENG, while also have an opposite deformation in the non-driven TENG location. Figures 5(d) and 5(e) (expansion mode 1) show that the conductive Ag nanopar-ticle is used for fabricating the grating array, as one electrode and the other electrode is a transparent hydrogel film. The expansion of grating arrays leads to the increase of the grating period and the expansion strain of the device may not be high enough to realize an effective operation of the device. In this case, Chen et al. further demonstrate the design of expansion mode 2 in Figs. 5(f) and 5(g). Both hydrogel electrodes are glued to the top and bottom sides of the grating array sealed in a PDMS membrane, and this new design of TOG can fully utilize the transparency and stretch ability of hydrogel electrodes. To ensure an effective modulation of TOG, the grating array is directly printed on the surface of elastomer film due to the sticky characteristics of the elastomer itself. Figures 6(a)–6(f) show the details for percentage of light transmission by the spe-cial samples. This grating structure of Ag nanoparticles, which

are used as conductive grating arrays specifically for extended mode 1, is the best candidates to work with TENG, and this Ag nanoparticles-based printing method greatly simplifies the manufacturing process of the TOG system. After the self- powered system is upgraded, the cycle of the grating can be reduced and the operation efficiency of the whole device can be greatly improved, thereby having broad prospects in tracking system and internet of things (IoTs). In addition to the optical grating, TENG–DEA system, which uses the silver nanowires as the electrode materials, can also work as a smart optical modu-lator (SOM)50 to modify the transparency, as shown in Fig. 7(a). Under the SE mode of the TENG, the movement of the Kapton film can control the mechanical strain of the elastomer film when the Kapton film is separated from the aluminum foil, which can not only provide energy supply but also show the signal for the elastomer to deform. To further improve the out-put performance of the TENG, an inductively coupled plasma (ICP) reaction [Fig. 7(b)] is applied to modify the contact charged material to increase its surface charge density. Under the activation of the TENG, the nanowire electrode can squeeze the elastomer in the micrometer scale and a great number of tiny wrinkles appear on the surface of elastomer, which block the observations. Therefore, this can be called a privacy protection device that controls the image through the film by TENG controlling the light transmittance through the

Figure 2. Four basic operation modes for TENG. (a) CS mode, (b) LS mode, (c) SE mode, and (d) FT mode. Reproduced with permission.2 Copyright 2015, Elsevier.

Figure 3. Structural and electrical characterizations of thin film–based PDMS with various patterns. (a) SEM image of the patterned PDMS thin film with line features. The inset is a 75° tilted high-magnification image showing the size and cross section structure of the features. (b) SEM image of the patterned PDMS thin film with cubic features. The inset is a 45° tilted high-magnification image showing the height of the cubes. (c) SEM image of the patterned PDMS thin film with pyramids features. The inset is a 45° tilted high-magnification image showing the pyramid structure of the features. (d) Output current of the TENG using PDMS thin film with flat surface and various patterned features. Reproduced with permission.25 Copyright 2012, American Chemical Society.

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Figure 4. (a) Obtaining surface charges through the triboelectrification process. (b) Gaining static charges through the employment of ionized air. (c) Measured short-circuit charge density (ΔσSC) produced by the TENG with ions injected in different times. Reproduced with permission.22 Copyright 2014, John Wiley and Sons.

Figure 5. (a) The basic structure and the operation principle of TENG-DEA conjunction system, where a single-electrode TENG using contact-separation motion mode was employed as the driving element for the conjunction system. (b) The structure design of the compression mode TOGs, (c) the working principle of the compression mode TOGs, (d) the structure design of the TOGs with expansion mode 1, (e) the working principle of the TOGs with expansion mode 1, (f) the structure design of the TOGs with expansion mode 2, (g) the working principle of the TOGs with expansion mode 2. Reproduced with permission.49 Copyright 2017, Elsevier.

Figure 6. The SEM image of the (a) master grating, (b) Fe nanoparticles, and (c) Ag nanoparticles. (d) Percentage of light transmission by different samples compared with the initial state: the transparency and the photo (inset) for (d) the master grating; (e) Fe nanoparticles, as shown higher brightness than (d); (f) Ag nanoparticles, as shown the highest brightness. Reproduced with permission.49 Copyright 2017, Elsevier.

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elastomer [Fig. 7(c)]. The SOM system and the specialized operation method proposed here are the typical study of TENG technique for the field of micro-electro-mechanical system (MEMS) and human–robots interaction,52–55 which can finally enrich the applications of TENG in optical communication, light capture, and other optical application.56–58,166

Self-powered microfluidic based mini-vehiclesNot only solid-state dielectric material can be actuated by

TENGs but also liquid droplets can be driven by the triboelectri-fication induced electric field. Microfluidics targets at the pre-cise control and manipulation of fluids with small volumes,59–62 while the high-voltage source and the control circuits increase the complexity of the microfluidic system.63–67 To achieve the effective control of position and velocity of fluids in the micro-channels, Nie et al.68 developed a fully self-powered microflu-idic system that eliminates the need for the power source and the control circuits. By integrating a TENG and a simple circuit board, the motion of water droplets can be controlled by the output of the TENG.69 The method based on the electrostatic induction theory constructs a physical model, which can pre-cisely simulate the detailed motion behavior of the droplet under driving of TENG, and it can also reveal the influences of surface hydrophobicity on the motion of the droplet. The model structure in Fig. 8 can provide us key parameters of the

microfluidic system. The sliding motion of Kapton on the grat-ing electrode can precisely control the stepping movement of the droplet. To reach the electrostatic balance, the amount of negative charges on the Kapton film is the total amount of the positive charges on two Al foils. Because of the large amount of negative charges on the Kapton film, the potential on the two electrodes will drop strongly. Hence, a strong Coulomb force can be established between the water droplet and the negatively charged electrode. When the Kapton film slides from the left foil to the right foil, the droplet is moved from the left-hand electrode to the right-hand electrode due to the Coulomb force. The force analysis of the droplet in this microfluidic system is systematically studied, as shown in Fig. 8(b). To simplify the experimental model, the droplet is considered as a rigid body and the tribo-induced positive charge distributes homogene-ously on the surface of the droplet. As shown in Figs. 8(c) and 8(d), the fluorinated ethylene propylene (FEP) film is subjected to some treatments to achieve a superhydrophobic state. The superhydrophobic surface can be achieved [Figs. 8(e) and 8(f)], which can help to further clarify the effect of surface properties on the droplet movement. The superhydrophobic surface can reduce the resistance on the movement of the drop and facili-tate the acceleration of the droplet in the electric field. This kind of theoretical analysis provides an in-depth understanding of both the advantages and the limitations of this integrated sys-tem, which can guide further optimization of this self-powered microfluidic system.70–72 A self-powered microfluidic transport system, which can carry some tiny objects to realize a micro transport system in the millimeter scale size, was designed by Nie et al.73 The mini-vehicle was driven by the Coulomb force generated by the free-standing TENG. These “wheels” can be moved freely in the horizontal direction or moved up the steps under the driving of TENG.74–77 The motion of the independent mode TENG not only powers the motion of the micro-vehicle but also controls the signal of this micro-transmission system [Figs. 9(a) and 9(b)]. Based on a single droplet that can be driven by TENG, it is also possible to drive multiple droplet move-ments, which in turn act as a power source or a control signal to direct the droplets. This freestanding mode TENG with multi-ple grating electrodes, which can increase the tribo-induced charges, effectively regulates the motion of the droplet in the microfluidic system with high efficiency and fast response speed. Meanwhile, it can realize manual control without any detector or control circuit. Bu et al.78 proposed that the TENG is used as a medium to first drive and accurately con-trol LMs 79,80 by external mechanical force, which enriches the self-powered microfluidic systems. More applications can be anticipated benefiting from the TENG-based self-powered microfluidic systems.

Self-powered wireless sensing based on tribo-induced liquid lens

Liquids actuated by TENGs not only can be used to carry objects serving as motion-controlled mini-vehicles but also ena-ble the self-powered wireless sensing.87 Basically, TENGs are

Figure 7. (a) On the basis of SOM for the self-powered system. (b) The microscale structure of the etched Kapton film (SEM image). (c) During the movement of TENG, the logo placed 3 cm behind the SOM film changed from transparent to opaque. Reproduced with permission.50 Copyright 2017, John Wiley and Sons.

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born self-powered mechanical sensors, where the output volt-age signal corresponds to the mechanical motions. Since their invention in 2012, TENGs have been widely applied as a self-powered active sensor, including but not limited to pres-sure measurements, displacement detections, and vibration characterizations.88–90 Ultrahigh signal-to-noise ratio can be achieved by the TENG-driven sensor because of the high-voltage output of TENGs. In addition, compared with conventional battery-powered sensor nodes, the size of TENG-based sensors can be greatly shrunk down and the manufacturing cost can be very low.91 Such a mechanical-to-electrical sensor needs wires for electrical connections, where the sensed electrical signal should be processed by the preamplifier since TENGs feature high voltages and ultralow currents. However, in some specific applications such as turbulence detections, sensing in severe environments, and infrastructure health monitoring, cables are usually not allowed. Therefore, TENG-based wireless sensing is needed. Light is an excellent candidate for wireless communica-tion, where the sensed information can be loaded by switching on and off.92–96 If the TENG-generated voltage signal can be

converted into the optical signal, self-powered wireless sensing is enabled. As shown in Fig. 10, a self-powered electrowetting optical switch (EOS) triggered by a TENG was proposed by Wang et al. for wireless sensing applications.87 The demon-strated EOS consists of an FS-TENG and an electrically tunable liquid lens (ETULL) made of 10% NaCl solution and purified olive oil. In the ETULL, the NaCl solution and olive oil serve as conducting and insulating liquids, respectively. Two liquids are both optically transparent. As shown in Figs. 10(a) and 10(b), when the FS-TENG was triggered by the mechanical motions, the triboelectrification-induced high-voltage electric field will drive the interface between two liquids to be curved according to the electrowetting effect.97 The curved interface results in an olive oil–based concave lens, considering the fact that the refractive indices (RIs) of 10% NaCl solution and olive oil are 1.46 and 1.34 at 650 nm wave length, respectively. When light is emitted into the high voltage–driven ETULL, the beam will be diverged by the concave lens and the remotely detected radi-ant power will be greatly reduced. When the FS-TENG is not triggered, the interface between two liquids is flat, where light

Figure 8. (a) The schematic diagram of mini-vehicles driven by TENG. (b) Theoretical analysis of the force on droplets at different locations of the electric field. (c) SEM image of the FEP film before superhydrophobic treatment; inset: zoomed-in image. (d) Contact angle for the FEP film before superhydrophobic treatment. (e) SEM image of the FEP film after superhydrophobic treatment; inset: zoomed-in SEM image; (f) Contact angle for the FEP film after superhydro-phobic treatment. Reproduced with permission.68 Copyright 2018, AIP Publishing.

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propagation will not be affected by the ETULL and the remotely detected radiant power nearly remains the same. The ETULL operations with and without FS-TENG charging are defined as the off and on states, respectively, which can be indicated by the remotely detected radiant powers. Therefore, the mechanical motions on the FS-TENG can be revealed by the remotely detected radiant powers. The electrowetting effect contributes to the detection of the mechanical motion appearance, and the other important issue to be solved is to effectively detect the motion termination. In their studies, it is interesting to notice that a discharging channel was formed upon loading high volt-age, which means that if the mechanical motion stopped, the electric field quickly disappeared and the liquid recovered to its original morphology very soon. Wireless sensing applications were performed to verify the effectiveness of their proposed EOS, and a system for remotely sensing the stepping motions was constructed as shown in Fig. 10(c). As illustrated in Figs. 10(d) and 10(e), the siren was activated when the stepping was loaded, demonstrating the sensing capability of the proposed EOS.

TeNg-stimulated microplasmaIn addition to the solid- and liquid-based actuation systems,

gas can also be used to be stimulated by the high voltage gener-ated by the TENGs. One typical gas-based application using the high voltage generated by TENGs is the generation of microplas-mas. Plasmas have been considered as the forth state of matters, widely applied in various fields such as surface treatments,98,99

displays,100,101 and biomedicines.102,103 The plasma can be achieved by the breakdown of gases, which is named as atmos-pheric pressure plasma. In terms of the discharging mechanism, the atmospheric pressure plasma can be classified into dielectric barrier discharge (DBD), atmospheric pressure non-equilibrium plasma jets (APNP-J), corona discharge, microspark discharge, etc. To initiate breakdown in the gases, the voltage applied should be at least above 1000 V. The born character of TENGs is high voltage become of their ultralow capacitance; thus, TENG is an excellent candidate to provide high voltages for generating plasmas.

As shown in Fig. 11, Cheng et al. proposed a triboelectric microplasma generation system powered by the mechanical stimuli.104 The structure of the TENG used in the study is illus-trated in Fig. 11(a). Two triboelectric materials in the TENG are FEP and copper, where the FEP film serves as the rotator and the copper substrate plays a role as the stator. The FEP film was bended to contact the underneath copper layer instead of directly pressing the FEP film to the electrode, where the wear could be minimized to benefit long-term operation. An argon microplasma capillary was connected with the TENG in series. Illumination can be achieved by the capillary upon loading high voltage, as shown in Fig. 11(b). The operation mechanism of the TENG-driven plasma is illustrated in Fig. 11(c), which includes four stages in total. There are two stages where the plasma can be triggered by the TENG where the voltage drop on the plasma capillary is above the breakdown threshold voltage. The voltage measurement setup is shown in Fig. 11(d), where a

Figure 9. The working principle of the self-powered microfluidic transport system (a) with two electrodes and (b) with four electrodes. Reproduced with permission.73 Copyright 2018, American Chemical Society.

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high-voltage probe was used to measure the high voltage gener-ated by the TENG. The measured output voltages of the TENG are shown in Fig. 11(e), where we can find that the output volt-age reaches its maximal value when the rotating speed is around 460 rpm. If the rotating speed is too high, the FEP will be floated driven by the air pressure difference, and thus, the con-tact area for triboelectrification will be reduced, lowering the output voltage. The achieved triboelectrification-induced plasma can be used for the surface treatment and the display, as shown in Fig. 12. When the plasma is pumped to the surface of the FEP film, the hydrophobicity was affected, which can be indi-cated by the contact angle, as indicated in Figs. 12(a) and 12(b). Figures 12(c)–12(f) indicate a plasma-based display powered by the TENG, where the breakdown area was patterned.

Microactuators triggered by TeNgsIn addition to several electrically responsible materials that

can be actuated by the high-voltage TENGs, over past years, great efforts have been made to develop smart devices intentionally to

be driven by TENGs. In those studies, high-voltage electric field can be generated by TENGs, which induces electrostatic force and can drive some microactuators. Such devices achieve con-versions from mechanical to electrical and then to mechanical energies. The mechanical-to-electrical energy conversion can be achieved by the TENGs, where high electric field can be formed. Situated in the high-voltage electric field and driven by the elec-trostatic force, the actuators will achieve mechanical responses, such as deformation, rotation, and vibration, serving as an electrical–mechanical energy converter. Various applications such as light scanning and beam steering can benefit from the actuations.105 Compared with the traditional battery-powered actuators, beside the advantage of being energy-saving and environmentally friendly, TENG-triggered actuators can be fab-ricated to be extremely thin, which will not occupy large spaces. Besides, since TENG itself can generate extremely high voltage, voltage-boosting circuit is not needed in the TENG triggered actuators, which simplifies the integration difficulties. Figure 13 illustrates a self-powered beam steering system, which consists of a TENG and a piezoelectric bimorph.106 Al and polytetrafluo-roethylene (PTFE) are two triboelectric materials in the TENG. Two Al electrodes, as two conducting and triboelectrification layers, function as a stator, between which the PTFE-based slider sweeps. There are basically two Al-FEP TENGs located at bottom and top, respectively, as shown in Fig. 13(a). The elec-trode alignment of the top Al electrode is perpendicular to that of the bottom electrode, which means that either sliding in X or Y direction can generate high voltages through the triboelec-trification effect. The PTFE film surface was nano-patterned by the ICP to enhance the triboelectrification effect, and the SEM image of which is shown in Fig. 13(b). When the PTFE film was situated in different locations between two aluminum elec-trodes, the output voltage varies.

As shown in Fig. 13(d), both bottom and top TENGs were connected with piezoelectric bimorphs, serving as actuation systems. For each actuation system, a 47 nF external capacitor was connected with the piezoelectric bimorph in parallel to tune the voltage applied on the bimorph. The voltage drop on the bimorph will be reduced when an external capacitor was con-nected in parallel. The piezoelectric bimorph will be deformed on loading the voltage. Even though the deformation of the bimorph driven by high voltage is very small, it is capable to tune the optical path through the mirror reflection. As shown in Fig. 13(c), two piezoelectric bimorphs were perpendicularly ori-ented, which are driven by the two TENGs, respectively. For each piezoelectric bimorph, one terminal was fixed and the other end is free. The piezoelectric bimorph will be bended upon charged by the TENG, where the optical path can be greatly changed after the two continuous reflections by the bimorphs. After the reflec-tion by the top bimorph, the light beam will be projected on the screen for visualization. The light-spot moving distance driven by such a self-powered device can be above 15 mm, which is greatly beneficial to the optical modulation.

Another smart actuator that can be triggered by the TENG is the self-powered triboelectric motor (TM), which can con-vert the ultralow frequency sliding mechanical motion into

Figure 10. Schematic diagram of the switching mechanism of the TENG-driven self-powered EOS and its application demos for the wireless stepping detection. (a) EOS without mechanical motion. (b) EOS with mechanical motion loaded. (c) Photograph of the wireless sensing system for stepping motions. (d) Photograph of the wireless sensing system when no stepping was loaded. (e) Photograph of the wireless sensing system when stepping was loaded. Reproduced with permission.87 Copyright 2019, Elsevier.

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the high-frequency rotations.107 As shown in Fig. 14(a), the whole actuation system consists of an FT-TENG and an electrostatic-force-driven rotating motor. The triboelectrifica-tion of the PTFE and the copper layer on the FT-TENG can gen-erate high voltage. The rotating motor consists of a rotor with four uniformly distributed copper fins in the center and two bar-shaped copper electrodes, each of which was attached with a carbon fiber. The carbon fiber performs good electrical conduc-tivity. The FT-TENG was electrically connected with the two bar-shaped copper electrodes of the rotating motor through a bridge rectifier. The two copper electrodes of the rotating motor will be charged by the TENG in DC mode. As shown in Fig. 14(b), owing to the electrostatic induction effect, the rotor moved, where the fin approached to the carbon fiber. Upon the fin was contacted with the carbon fiber, the charge of the fiber was transferred to the copper fin, resulting in a repulsive force. The charged fin was attracted by another copper bar electrode until being neutralized. Such operation mechanism ensures the rotor to keep rotating since both repulsive and attractive forces

are kept in the same direction. Using this principle, the ultralow mechanical stimuli can be converted to the high-frequency rota-tion, as shown in Fig. 14(c). Using their proposed self-powered rotating actuation system, a rotating mirror for scanning rays can be achieved, which can be applied for the bar code recogni-tion, as shown in Figs. 14(d) and 14(e). The proposed paradigm enables the optical MEMS systems to be fully self-powered, where a large potential market size can be expected.108,109

Self-powered electroadhesion driven by TeNgsAnother featured smart device enabled by high-voltage

TENGs is self-powered electrosdhesion systems. Electroad-hesion technology driven by an external power source can be applied in the field of robotics and material processing.110–115 Xu et al.116 proposed a self-powered electroadhesion system that uses a high-voltage signal of improved modified multilayer TENGs to provide a stable output voltage of 4750 V. In the case of different surface charge densities and device configurations,

Figure 11. (a) Schematic illustration of a TENG-driven atmospheric pressure non-equilibrium plasma jets (APNP-J). (b) The employment of the APNP-J for biomedicine usage. (c) Four-stage scheme of the TENG-powered DBD device. (d) Electrical characterization setup for the TENG triggered plasma emitter. (e) Open-circuit voltage characterization of the TENG rotating in various speeds. Reproduced with permission.104 Copyright 2018, Springer Nature.

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the highest open circuit voltage can be achieved by optimal charge distribution, which is related to the multilayer TENG structure and charge replenishment channel.117,118 The struc-tural illustration of the TENG-triggered electroadhesion sys-tem is shown in Fig. 15(a) and the photograph of the system is shown in Fig. 15(d), which includes three contact–separation TENGs and an EAP. This TENG electrification mode is the same as the process of conventional EAP attachment and release, and the contact and separation between the TENG electrodes facili-tate control of the entire system. The SEM images of the nanos-tructures of PTFE are shown in Fig. 15(b), where the surface of the friction layer after etching can enhance the triboelectrifica-tion effect. The basic working principle of this multilayer TENG is stated below [Fig. 15(c)]: generally, PTFE presents a higher electron affinity than Al, and as a result, a low potential is

generated on one side of the Al electrode. By the periodic contact–separation movement of the tribo-layers, positive charges are transferred from the top Al electrode to the back Al electrode, which causes the alternating electrical signal of the TENG output. Afterward, researchers demonstrated self- powered electrical adhesion systems for various applications, as can be seen in Fig. 16(a). Based on the combination of TENG and the supplementary capacitor, the attenuation of high volt-age on the EAP, which consists of a set of electrodes and an insu-lating layer, can be slowed down and adhesion can be stabilized at a certain value for a long time. Electroadhesive force was ena-bled by the high-voltage polarization through the electro-static induction effect. With the enhancement of the charge supplement channel (CSC), the voltage of the TENG unit is capable of working effectively on the EAP with a much lower

Figure 12. Demonstrated applications of the tribo-induced plasma. (a), (b) Surface treatment via the tribo-induced plasma processing and contact angle variation of the FEP film. (c), (d) Tribo-induced plasma-based display (e) A plasma disk driven by the TENG. (f) Photographs of the triboelectric plasma-based display exposed in different time. Reproduced with permission.104 Copyright 2018, Springer Nature.

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capacitance [Fig. 16(b)]. When no capacitor is added, as shown in Fig. 16(c), the voltage of the EAP in the circuit can quickly reach a high voltage state and the corresponding adhesion force also shows a tendency to increase rapidly. Integration of a 2.5 nF capacitor in the circuit slows down the rise of voltage and adhesion force, where the output voltage and adhesion are essentially in the previous state [Fig. 16(d)]. The humidity may strongly influence the performance of the adhesion system, and as shown in Fig. 16(e), the increase in the humidity results in the fast decrease in the established voltage. However, with the help of supplementary capacitor, the system can maintain high voltage for a longer period [see Fig. 16(f)], which can provide a much larger flexibility for manipulating target object. Through the demonstrations of the utility of an integrated self-powered electrical adhesion system by picking up, manipulating, and transporting different materials (conductive, semiconductive, and nonconductive materials), it is clear that the implementation of the CSC in TENGs can effectively generate power adhesion force in the EAP for practical applications [Figs. 16(g)–16(k)]. This TENG-based self-powered adhesion system is cost-effective, highly efficient, and convenient to manufacture that can be worked without further processing. Based on the previously mentioned form of charge replenishment, the CSC can achieve the highest voltage output in the corresponding configuration [Fig. 16(l)]. As for TENGs without charge replenishment chan-nels, their charge allocation is not stabilized, which causes the charge to dissipate rapidly, yielding a low-voltage performance. This research proposed a self-powered electric adhesive system based on ascending voltage of TENG, which can provide a sim-ple operation process and high adhesion force. The proposed

adhesive system can manipulate conductive, semiconductive, and nonconductive material objects with various configura-tions, showing great potential in material handling, and the similar TENG device can also meet the need of high-voltage power supply for all kinds of application scenarios.119–121

Triboelectrification-induced electrospinning and mass spectrometer applications

High-voltage TENGs not only contributes to the develop-ment of self-powered actuation systems but also greatly facili-tate the advanced fabrication and material characterization technologies. In recent years, the development of flexible wearable electronic products has been accompanied by the production of various printing technologies,122–126 such as screen printing and inkjet printing. Electrospinning, which is the charged fluid produced by high-voltage atomization sepa-ration of polymers, has been widely used in medical, sensor, and other fields.127–131 Under the high electric field, polymer filaments with nanoscale diameters can be produced since the droplet at the needle changes from a sphere to a cone (known as a “Taylor cone”),132 extending from the tip of the cone to form filaments. Another powerful technique is the inkjet printing, which belongs to electrohydrodynamic jet (e-jet), a high-resolution printing electronics technology that uses a high electric field to produce droplets.133–136 As a kind of spe-cial power source, TENG has the characteristic of high voltage and low current, which leads to a better safety for both equip-ment and human body compared with conventional high- voltage power supplies.137,138 In 2017, Li et al.139 designed a self-powered electrostatic spinning system based on a rotating FT-TENG, as shown in Fig. 17(a), consisting of a rotating disc TENG, a pressure doubling rectifier circuit (VDRC), and a simple spinneret head. R-TENG [Fig. 17(b)] is composed of two triboelectric materials and one electrode layer, wherein the triboelectric material consists of a copper strip and an FEP film. Photograph of FT-TENG rotor (copper strip as friction material, left) and stator (copper strip as electrode layer, right) is shown in Fig. 17(c), and the assembled hand-cranked R-TENG is shown in Fig. 17(d). Thanks to the R-TENG drive; this self-powered electrospinning system is simpler to operate than commercial electrospinning machines on the market, with lower production costs, more efficient production, and energy savings. This self-driven electrospinning technology will bring major changes in the development of electric spin-ning machines, making it possible to implement electrospin-ning machines for on-site or remote areas without power. At the same time, Li et al. systematically studied the VDRC which demonstrated TENG’s capabilities for high-voltage applications to obtain the best configuration that the system can output the maximum constant DC voltage of 8.0 kV at the magnification factor of 22 and the capacitance value of 1 × 104 pF. Subsequently, Wu et al. proposed a printed elec-tronic circuit based on e-jet printing of TENG [Fig. 17(e)].136 A RF-TENG, which consists of two parts, one stator and one rotator, is connected to the printing nozzle and the substrate

Figure 13. TENG-driven self-powered optical modulator. (a) Schematic diagram of the designed three-layer sliding TENG. (b) SEM photograph of the nanostructured PTFE film. (c) A sketch of the structure of a 2D modulator driven by the three-layer sliding TENG. (d) Schematic diagram of an active optical attenuator with two channels. Reproduced with permission.106 Copyright 2014, John Wiley and Sons.

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through a voltage boost circuit. The nozzle is slowly moved by the machine, and the ink can be stabilized by air pressure control. The triboelectrifcation between the nylon films and the PTFE films induces positive charges on nylon and negative

charges on PTFE shows the basic working principle of TENG [Fig. 17(f)]. Under electrostatic induction, when the nylon in the interdigital electrode sweeps across the PTFE film, electrons move between the two electrodes and ensure

Figure 14. (a) Structural illustration of TM and the PTFE film surface photograph. (b) Operation mechanism of the TM rotation. (c) Snapshot photograph of the rotated motor. (d) Photograph of the scanned light. (e) Schematic diagram of the self-powered scanner for the bar code recognition. Reproduced with permission.107 Copyright 2019, Springer Nature.

Figure 15. (a) The structure of the self-powered electroadhesion system: three TENGs and one EAP. (b) SEM image of PTFE surface through the ICP method. (c) Basic working principle of the TENG. (d) Photograph of the fabricated system. Inlets show the EAP and the stacked TENGs, respectively. The above diagrams are not given to scale. Reproduced with permission.116 Copyright 2018, American Chemical Society.

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continuous AC. A boost circuit was used to amplify the output voltage of FT-TENGs, which enables smooth and accurate printing. Figures 18(a)–18(c) show the different graphics printed by Wu et al.140 TENG drives include a pair of printed gears, two printed s-shaped conductive interconnections, and four conductive arrow patterns. Depending on the printing setup, the printed graphics can be used for a variety of different scenarios such as sensor array and electrical components print-ing. Due to their safety, stability, low cost, and high efficiency,

this work provides an alternative to high-resolution e-jet print-ing and extends the range of applications for TENG.141–144

Mass spectrometry (MS) is one of the most powerful tools for the identification of pure substances, which has high sen-sitivity and important applications in many fields such as drug metabolism, clinical, food chemistry, and national defense.145 Dedicated high-voltage switches and transformers can be used to drive finer electrospray ionization (ESI) modes through high-voltage pulses, dielectric barrier polarization,

Figure 16. (a) Schematic diagram for the application circuit of self-powered electroadhesion system. (b) High-voltage state of different capacitors. (c) Test the adhesion and voltage of the Al plate at different points in time removing the capacitor. (d) Test two values above when adding capacitor. (e) The Voc of electroadhesion from dry to wet conditions. (f) Test the Voc in the same environment as E in the case of a capacitor. (g)–(k) The implementation of the CSC in TENGs can effectively power adhesion force generation in the EAP for practical applications. (l) The schematic of the EAP-TENG system. Reproduced with permission.116 Copyright 2018, American Chemical Society.

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or capacitive induction.146–150 Based on the fine and accurate characteristics of the charge pulse, the ionization process that triggers the more durable ESI device can be repetitive and sim-ple to operate.151 Nano-ESI due to the high voltage of TENG can bring higher sensitivity under the charge of lower ion pulse, so as to maximize the utilization of the sample; this is a matter of improving efficiency on both sides. TENG-based MS has now

studied small organic molecules and large biomolecules, including various compounds, chemical explosives, and mili-tary mimics. The CS and FT TENGs, which are composed of two electrodes and at least one pair of triboelectric layers, are used in the work of Li et al.,152 and their coupling to a nano-ESI emit-ter. The mechanical movement of these layers can disturb the electrostatic balance. Therefore, the charge movement is redis-tributed by the connection with the external circuit, and the balance of the charge is achieved by this process, which is called as electrostatic balance. The CS-TENG shown in Fig. 19(a) is used to generate a unipolar charging pulse, and the FT-TENG [Fig. 19(b)] is used to generate charging pulses of alternating polarity. Both TENG-generated charges – TENGs are used for plasma discharge by providing charges to the nano ESI emitter [Fig. 19(c)] or the needle electrode. As shown in Fig. 19(d), the ion source can be electrically treated as a capacitor, indicating that air leaks through the switch S when the voltage of the ion source is greater than the initial value. Therefore, the air leakage during each cycle, which is called an ionization pulse, can be measured by the two mass spectrometers described above. In the absence of fragment ions, the low-voltage CS-TENG can gener-ate a detection signal similarly to the high-voltage FT-TENG nano-ESI under the similar concentration level; in other words, the result is the increase in sensitivity of FT-TENG (Fig. 20). Figure 20(c) shows that the detection frequency of fragment ions decreases with respect to the abundance. As for m/z 182.118 fragment ions, when the detectable probability is 50%, the cocaine concentration is 8 pg/mL, as shown in Fig. 20(d), which further proves the nano-ESI function. The defocusing effect shown in Fig. 21(f), depositing a square via mask aper-tures [Figs. 21(g) and 21(h)], is opposite to effect of reversed

Figure 17. (a) The working process of the rotary FT-TENG. (b) Schematic diagram of the rotary freestanding-TENG. (c) Picture of the device part of the rotary FT-TENG. (d) The actual picture of the rotary FT-TENG. Reproduced with permission.139 Copyright 2017, American Chemical Society. (e) E-jet motion process of TENG-based equipment. (f) The working situation of TENG is a sliding mode. (g) Analog circuit diagram of TENG boosting voltage process. Reproduced with permission.136 Copyright 2019, John Wiley and Sons.

Figure 18. The process of fluid-driven injection. (a) Two gear shapes photos. (b) The pattern to be printed connect to the LED. (c) Sensor distribution of the entire device. Reproduced with permission.136 Copyright 2019, John Wiley and Sons.

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and is similar to the expansion effect. TENG-driven ionization method is a convenient way to provide ESI and plasma discharge ionization and opens a new direction for efficient ionization with accurate numbers of total charges.153–156 These new fea-tures have enormous potential applications in medical chemis-try, medicinal chemistry, and defense chemistry.

Summary and perspectivesIn recent years, with the rapid development of TENG tech-

nologies, more and more self-powered high-voltage applica-tions have been proposed by many researchers worldwide. The conjunction of the high-voltage TENGs and electrically respon-sible materials and devices has been systematically reviewed in this paper. Various types of TENGs that can harvest mechanical energy in different modes from ambient environments were firstly reviewed including CS, SL, SE, and FT mode TENGs, followed by recent efforts to enhance the output performance of TENGs. Afterward, self-powered smart systems have been reviewed at material and device levels, respectively. Gases, liquids, and solids can serve as the electrically responsible materials for the TENG-triggered high-voltage applications.

For applications usng gases, rare gases such argon can have breakdowns upon loading high voltages generated by the TENGs, resulting in the emission of microplasmas, which can be widely applied for the surface treatment and plasma-based displays. For liquids, the actuation of liquids situated at the high electric field can be achieved based on the electrowetting mechanism. The electrostatic-driven morphology variation of the liquids can be used for the self-powered wireless sensing, and the droplet which can move upon high-voltage loading can serve as a mini-vehicle, which is greatly beneficial to the chemi-cal reactions. In addition, the electrospinning can also be achieved, where a great number of droplets can be created when the liquid was compressed and split by the strong electric field provided by the TENG, which can be used for the additive man-ufacturing and mass spectrometers. Solid can also be actuated by the high-voltage TENGs, and a typical application is the self-powered elastomer. Upon loading, the TENG generated high voltage on the elastomer and the deformation of the elasto-mer can be achieved, where the surface area will be enlarged and the thickness will be decreased, attributed to the electro-static force. Besides responsible materials, several smart mechanical structures can also be driven by the TENGs.

Figure 19. Ionization by TENGs. Two different TENGs work in (a) separation of electrodes by contact; (b) electrode connected by sliding. Yellow, copper electrode layers; blue, FEP layers; red, move directions of the TENG electrodes; and pulse, the corresponding charge flow (e−, I) to the ion source. The vertical rectangle represents a steel plate collecting the ion current. (c) Dark-field images of a nanoelectrospray emitter. (d) An equivalent electronic circuit. The TENG, a capacitor (C1), and the part of the dotted line on the left; NanoESI emitter, C2, and the part of the dotted line on the right; Leak (S), after reaching an onset charge value; A, picoamperemeter; y, generated ions; Rair, air gap; switch SC, the CS-TENG electrodes (a) are extended on the side to reset the electrostatic status at the contact position. Reproduced with permission.152 Copyright 2017, Springer Nature.

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Micro-motors in this review such as piezoelectric bimorph-based mirror system and electrostatic-driven rotating motor can be actuated by the high-voltage TENGs, which can be used for the optical modulations and optical scanning.

Beside the reviewed high-voltage applications, it can be anticipated that more and more new paradigms can be pro-posed based on the reach of existing technologies. The fol-lowing research should be considered and more works should be done in future to facilitate the high-voltage applications of TENGs.

(i) More efforts should be made to improve the both electri-

cal output capability and reliability of TENGs. The voltage generated by the TENGs is limited by the break-

down effect, which is governed by Paschen’s law. If the TENG generated output voltage is too high, the breakdown will occur and the output power will be greatly affected. Gases will be more

easily to have a breakdown than the dielectric materials. Thus, structural optimization can be made on the TENGs to ensure that the high voltage is loaded on the dielectric material instead of the gas. Besides, according to Paschen’s law, the breakdown voltage limit under high pressure or vacuum atmosphere is much higher than that under normal pressures. Therefore, high-pressure or vacuum-packaged TENGs are desired to achieve the breakdown-free TENGs. Besides material selection, energy management circuit can also be used to minimize the power loss owing to the breakdown effect. If the breakdown effect in TENGs can be eliminated or alleviated, not only the output voltage can be further improved but also the reliabilities of TENGs can be strengthened, where a more stable power out-put can be ensured. Another issue to be considered with TENGs is the wear issue. After long time use, the triboelectrification degradation should be considered while designing the TENGs, which is an important factor for the commercialization.

Figure 20. Enhanced sensitivity under transient TENG high voltage. Test methods for cocaine solution: (a) in the main mode, specific ions can be detected by FT-TENG; (b) in the sub-mode, higher levels of ions can be detected. (c) The method of quality inspection in the main mode. (d) The detection limit can be calculated by the red line. Reproduced with permission.152 Copyright 2017, Springer Nature.

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Figure 21. Ion deposition on various types of surface using the FT-TENG. (a) Components in the deposition apparatus. (b) A positive charge will be concentrated at the tip of the needle at the transmitting end. (c) Increased surface potential causes spray deposition to stop. (d) An opposite electric gradient which triggering a spray pulse of the opposite polarity. (e) The process of stop and recycle for the emitter. (f) Scheme of the process of the FT-TENG. (g) The microscopic image of Alexa Fluor 488 fluorescent squares k. (h) The deposited patterned crystal violet spots. (i) The shape in the figure can be obtained by a specific solution during the movement of the target object. Inset: The dark-field image of the decreasing spot sizes. Reproduced with permission.152 Copyright 2017, Springer Nature.

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(ii) The energy management circuit for the boost of frequency for high-power TENGs is desired in future. The majority of natural mechanical energy is usually with slow oscilla-tions, which results in ultralow-frequency electrical out-puts of TENGs. However, in some applications such as liquid crystal–based smart windows and focal length tuna-ble lens, high-frequency electrical inputs are necessary. If the low-frequency electrical output generated by the TENG can be boosted through an energy management circuit with high-frequency oscillation, the application of high-voltage TENGs can be greatly enriched.

(iii) The majority of the reviewed high-voltage actuations trig-gered by TENGs are powered by wire-connected TENGs. However, wireless power transmissions are desired in some specific applications, which makes the powering process more flexible. It is possible that the harvested electrical power can be transformed into other energy forms such as ultrasound energy for the wireless transmis-sion. However, minimizing the power loss during the power conversion process is the most important issue to be considered.

(iv) The triboelectrification-induced soft-robotics can be expected in future. The aforementioned electrically responsible materials can be mechanically integrated to achieve targeted continuing mechanical motions upon charging by the TENG in AC mode. And if the aforemen-tioned high-frequency electrical outputs and wireless power transmission can be achieved, many applications achieved by self-powered triboelectrification-induced robotics can be anticipated.

(v) The reviewed self-powered smart systems with a combina-tion of TENGs and actuators illustrate great application potentials. However, to facilitate the commercialization of these TENG-driven smart system, it is necessary to undertake the techno-economic analysis of the conjunc-tion systems. The techno-economic life cycle assessment of TENGs as energy harvesters has been undertaken by Ahmed et al.157 In their study, a grating structured and a rotation FT-TENGs were used for evaluation, where the capital expenditure, material processing and fabrica-tion, operation expense, and lifetime were taken into account. Their results show that the predicted levelized cost of the grating structured and rotation FT-TENGs can be as low as US 2.681 cents per kWh and US 9.43 cents per kWh, respectively. However, until now, few people have ever made the techno-economic life cycle assessment of the self-powered system consisting of a TENG and an actuator. Beside the economic assessment of actuators, the lifetime influenced by the conjunction and the integration expense should also be considered.

AcknowledgmentsJiaqi Wang and Shuyao Li contribute equally to this

work. This work was funded by HKSAR, the Research Grants Council Early Career Scheme (Grant No. 24206919), HKSAR

Innovation and Technology Support Programme Tier 3 (Grant No. ITS/085/18), the Chinese University of Hong Kong Direct Grant (Grant No. 4055086), Shun Hing Institute of Advanced Engineering (Grant No. RNE-p5-18), the National Key R&D Project from Minister of Science and Technology (2016YFA0202704), the National Natural Science Founda-tion of China (Grant Nos. 51775049, 51432005, 11674215, 5151101243, and 51561145021), Beijing Natural Science Foundation (4192069), the Beijing Municipal Science & Tech-nology Commission (Z171100000317001), and Young Top-Notch Talents Program of Beijing Excellent Talents Funding (2017000021223ZK03).

ReFeReNCeS:

1. Fan F-R., Tian Z-Q., and Wang Z.L.: Flexible triboelectric generator. Nano energy 1(2), 328–334 (2012).

2. Wang S., Lin L., and Wang Z.L.: Triboelectric nanogenerators as self- powered active sensors. Nano Energy 11, 436–462 (2015).

3. Pu X., Li L., Liu M., Jiang C., Du C., Zhao Z., Hu W., and Wang Z.L.: Wearable self-charging power textile based on flexible yarn supercapacitors and fabric nanogenerators. Adv. Mater. 28(1), 98–105 (2016).

4. Niu S., Wang X., Yi F., Zhou Y.S., and Wang Z.L.: A universal self-charging system driven by random biomechanical energy for sustainable operation of mobile electronics. Nat. Commun. 6, 1–8 (2015).

5. Zhu G., Chen J., Zhang T., Jing Q., and Wang Z.L.: Radial-arrayed rotary electrification for high performance triboelectric generator. Nat. Commun. 5, 3426 (2014).

6. Yang W., Chen J., Jing Q., Yang J., Wen X., Su Y., Zhu G., Bai P., and Wang Z.L.: 3D stack integrated triboelectric nanogenerator for harvesting vibration energy. Adv. Funct. Mater. 24(26), 4090–4096 (2014).

7. Wang S., Mu X., Wang X., Gu A.Y., Wang Z.L., and Yang Y.: Elasto-aerodynamics-driven triboelectric nanogenerator for scavenging air-flow energy. ACS Nano 9(10), 9554–9563 (2015).

8. Yang X., Xu L., Lin P., Zhong W., Bai Y., Luo J., Chen J., and Wang Z.L.: Macroscopic self-assembly network of encapsulated high-performance triboelectric nanogenerators for water wave energy harvesting. Nano Energy 60, 404–412 (2019).

9. Xu M., Zhao T., Wang C., Zhang S.L., Li Z., Pan X., and Wang Z.L.: High power density tower-like triboelectric nanogenerator for harvesting arbitrary directional water wave energy. ACS Nano 13(2), 1932–1939 (2019).

10. Wang Z.L.: On maxwell’s displacement current for energy and sensors: The origin of nanogenerators. Mater. Today 20(2), 74–82 (2017).

11. Niu S. and Wang Z.L.: Theoretical systems of triboelectric nanogenerators. Nano Energy 14, 161–192 (2015).

12. Zhu G., Peng B., Chen J., Jing Q., and Wang Z.L.: Triboelectric nanogenerators as a new energy technology: From fundamentals, devices, to applications. Nano Energy 14, 126–138 (2015).

13. Zhu G., Yang W.Q., Zhang T., Jing Q., Chen J., Zhou Y.S., Bai P., and Wang Z.L.: Self-powered, ultrasensitive, flexible tactile sensors based on contact electrification. Nano Lett. 14(6), 3208–3213 (2014).

14. Lin Z., Chen J., Li X., Zhou Z., Meng K., Wei W., Yang J., and Wang Z.L.: Triboelectric nanogenerator enabled body sensor network for self-powered human heart-rate monitoring. ACS Nano 11(9), 8830–8837 (2017).

15. Yu H., He X., Ding W., Hu Y., Yang D., Lu S., Wu C., Zou Y., Liu R., Lu C., and Wang Z.L.: A self-powered dynamic displacement monitoring system based on triboelectric accelerometer. Adv. Energy Mater. 7(19), 1700565 (2017).

16. Su Y., Xie G., Xie T., Zhang H., Ye Z., Jing Q., Tai H., Du X., and Jiang Y.: Wind energy harvesting and self-powered f low rate sensor enabled by contact electrification. J. Phys. D: Appl. Phys. 49(21), 215601 (2016).

17. Zi Y. and Wang Z.L.: Nanogenerators: An emerging technology towards nanoenergy. APL Mater. 5(7), 074103 (2017).

https://doi.org/10.1557/mre.2020.2Downloaded from https://www.cambridge.org/core. IP address: 54.39.106.173, on 28 Dec 2020 at 02:19:51, subject to the Cambridge Core terms of use, available at https://www.cambridge.org/core/terms.

Page 20: High-voltage applications of the triboelectric nanogenerator— … · can be produced by TENGs.10–12 TENGs are not only an excel-lent energy harvester but also a self-powered active

20 n MRS eNeRgy & SUSTAINABIlITy // V O L U M E 6 // e 1 7 // www.mrs.org/energy-sustainability-journal

18. Wang Z.L., Lin L., Chen J., Niu S., and Zi Y.: Triboelectric Nanogenerators (Springer International Publishing, Berlin, Germany, 2016).

19. Nie J., Chen X., and Wang Z.L.: Electrically responsive materials and devices directly driven by the high voltage of triboelectric nanogenerators. Adv. Funct. Mater. 29(4) 1806351 (2018).

20. Ghaffarinejad A., Hasani J.Y., Hinchet R., Lu Y., Zhang H., Karami A., Galayko D., Kim S., and Basset P.: A conditioning circuit with exponential enhancement of output energy for triboelectric nanogenerator. Nano Energy 51, 173–184 (2018).

21. Zhang H., Lu Y., Ghaffarinejad A., and Basset P.: Progressive contact-separate triboelectric nanogenerator based on conductive polyurethane foam regulated with a Bennet doubler conditioning circuit. Nano energy 51, 10–18 (2018).

22. Wang S., Xie Y., Niu S., Lin L., Liu C., Zhou Y.S., and Wang Z.L.: Maximum surface charge density for triboelectric nanogenerators achieved by ionized-air injection: Methodology and theoretical understanding. Adv. Mater. 26(39), 6720–6728 (2014).

23. Zi Y., Wu C., Ding W., and Wang Z.L.: Maximized effective energy output of contact-separation-triggered triboelectric nanogenerators as limited by air breakdown. Adv. Funct. Mater. 27(24), 1700049 (2017).

24. Wang J., Wu C., Dai Y., Zhao Z., Wang A., Zhang T., and Wang Z.L.: Achieving ultrahigh triboelectric charge density for efficient energy harvesting. Nat. Commun. 8(1), 88 (2017).

25. Fan F.R., Lin L., Zhu G., Wu W., Zhang R., and Wang Z.L.: Transparent triboelectric nanogenerators and self-powered pressure sensors based on micropatterned plastic films. Nano Lett. 12(6), 3109–3114 (2012).

26. Yang P.K., Lin Z.H., Pradel K.C., Lin L., Li X., Wen X., He Jr., and Wang Z.L.: Based origami triboelectric nanogenerators and self-powered pressure sensors. ACS Nano 9(1), 901–907 (2015).

27. Lee K.Y., Yoon H.J., Jiang T., Wen X., Seung W., Kim S.W., and Wang Z.L.: Fully packaged self-powered triboelectric pressure sensor using hemispheres-array. Adv. Energy Mater. 6(11), 1502566 (2016).

28. Fan X., Chen J., Yang J., Bai P., Li Z., and Wang Z.L.: Ultrathin, rollable, paper-based triboelectric nanogenerator for acoustic energy harvesting and self-powered sound recording. ACS Nano 9(4), 4236–4243 (2015).

29. Cui N., Gu L., Liu J., Bai S., Qiu J., Fu J., Kou X., Liu H., Qin Y., and Wang Z.L.: High performance sound driven triboelectric nanogenerator for harvesting noise energy. Nano Energy 15, 321–328 (2015).

30. Xie Y., Wang S., Niu S., Lin L., Jing Q., Yang J., Wu Z., and Wang Z.L.: Grating-structured freestanding triboelectric-layer nanogenerator for harvesting mechanical energy at 85% total conversion efficiency. Adv. Mater. 26(38), 6599–6607 (2014).

31. Niu S., Wang S., Liu Y., Zhou Y.S., Lin L., Hu Y., Pradel K.C., and Wang Z.L.: A theoretical study of grating structured triboelectric nanogenerators. Energy Environ. Sci. 7(7), 2339–2349 (2014).

32. Wang M., Zhang N., Tang Y., Zhang H., Ning C., Tian L., Li W., Zhang J., Mao Y., and Liang E.: Single-electrode triboelectric nanogenerators based on sponge-like porous PTFE thin films for mechanical energy harvesting and self-powered electronics. J. Mater. Chem. A 5(24), 12252–12257 (2017).

33. Mao Y., Geng D., Liang E., and Wang X.: Single-electrode triboelectric nanogenerator for scavenging friction energy from rolling tires. Nano Energy 15, 227–234 (2015).

34. Wang S., Xie Y., Niu S., Lin L., and Wang Z.L.: Freestanding triboelectric-layer-based nanogenerators for harvesting energy from a moving object or human motion in contact and non-contact modes. Adv. Mater. 26(18), 2818–2824 (2014).

35. Zou H., Zhang Y., Guo L., Wang P., He X., Dai G., Zheng H., Chen C., Wang A.C., Xu C., and Wang Z.L.: Quantifying the triboelectric series. Nat. Commun. 10(1), 1–9 (2019).

36. Clint J.H. and Dunstan T.S.: Acid-base components of solid surfaces and the triboelectric series. Europhys. Lett. 54(3), 320 (2001).

37. Tang W., Jiang T., Fan F.R., Yu A.F., Zhang C., Cao X., and Wang Z.L.: Liquid-metal electrode for high-performance triboelectric nanogenerator at an instantaneous energy conversion efficiency of 70.6%. Adv. Funct. Mater. 25(24), 3718–3725 (2015).

38. Park S.J., Seol M.L., Jeon S.B., Kim D., Lee D., and Choi Y.K.: Surface engineering of triboelectric nanogenerator with an electrodeposited gold nanoflower structure. Sci. Rep. 5, 1–7 (2015).

39. Truxal S.C., Kurabayashi K., and Tung Y-C.: Design of a MEMS tunable polymer grating for single detector spectroscopy. Int. J. Optomechatronics 2(2), 75–87 (2008).

40. Paloczi G.T., Huang Y., Yariv A., Luo J., and Jen A.K.Y.: Replica-molded electro-optic polymer Mach–Zehnder modulator. Appl. Phys. Lett. 85(10), 1662–1664 (2004).

41. Huang G., Shin J.S., Lee W.J., Park T.H., Chu W.S., and Oh M.C.: Surface relief apodized grating tunable filters produced by using a shadow mask. Optic Express 23(16), 21090–21096 (2015).

42. Kollosche M., Döring S., Stumpe J., and Kofod G.: Voltage-controlled compression for period tuning of optical surface relief gratings. Optic Lett. 36(8), 1389–1391 (2011).

43. Aschwanden M. and Stemmer A.: Polymeric, electrically tunable diffraction grating based on artificial muscles. Optic Lett. 31(17), 2610–2612 (2006).

44. Kofod G. et al.: Electroelastic optical fiber positioning with submicrometer accuracy: Model and experiment. Appl. Phys. Lett. 94(20), 202901 (2009).

45. Hajiesmaili E. and Clarke D.R.: Reconfigurable shape-morphing dielectric elastomers using spatially varying electric fields. Nat. Commun. 10(1), 183 (2019).

46. Maffli L., Rosset S., Ghilardi M., Carpi F., and Shea H.: Ultrafast all-polymer electrically tunable silicone lenses. Adv. Funct. Mater. 25(11), 1656–1665 (2015).

47. Anderson I.A., Hale T., Gisby T., Inamura T., McKay T., O’Brien B., Walbran S., and Calius E.P.: A thin membrane artificial muscle rotary motor. Appl. Phys. A: Mater. Sci. Process. 98(1), 75 (2010).

48. Keplinger C., Sun J.Y., Foo C.C., Rothemund P., Whitesides G.M., and Suo Z.: Stretchable, transparent, ionic conductors. Science 341(6149), 984–987 (2013).

49. Chen X., Wu Y., Yu A., Xu L., Zheng L., Liu Y., Li H., and Wang Z.L.: Self-powered modulation of elastomeric optical grating by using triboelectric nanogenerator. Nano Energy 38, 91–100 (2017).

50. Chen X., Pu X., Jiang T., Yu A., Xu L., and Wang Z.L.: Tunable optical modulator by coupling a triboelectric nanogenerator and a dielectric elastomer. Adv. Funct. Mater. 27(1), 1603788 (2017).

51. Niu S., Liu Y., Wang S., Lin L., Zhou Y.S., Hu Y., and Wang Z.L.: Theoretical investigation and structural optimization of single-electrode triboelectric nanogenerators. Adv. Funct. Mater. 24(22), 3332–3340 (2014).

52. Xu S., Qin Y., Xu C., Wei Y., Yang R., and Wang Z.L.: Self-powered nanowire devices. Nat. Nanotechnol. 5(5), 366–373 (2010).

53. Hwang G.T., Park H., Lee J.H., Oh S., Park K.I., Byun M., Park H., Ahn G., Jeong C.K., No K., Kwon H., Lee S-G., Joung B., and Kwon H.: Nanogenerators: Self-powered cardiac pacemaker enabled by f lexible single crystalline PMN-PT piezoelectric energy harvester (Adv. Mater. 28/2014). Adv. Mater. 26(28), 4754–4754 (2014).

54. Lee J.H., Lee K.Y., Gupta M.K., Kim T.Y., Lee D.Y., Oh J., Ryu C., Yoo W.J., Kang C.Y., Yoon S., Yoo J.B., and Kim S.: Highly stretchable piezoelectric-pyroelectric hybrid nanogenerator. Adv. Mater. 26(5), 765–769 (2014).

55. Ding W., Wu C., Zi Y., Zou H., Wang J., Cheng J., Wang A.C., and Wang Z.L.: Self-powered wireless optical transmission of mechanical agitation signals. Nano Energy 47, 566–572 (2018).

56. Yang C.H., Chen B., Zhou J., Chen Y.M., and Suo Z.: Electroluminescence of giant stretchability. Adv. Mater. 28(22), 4480–4484 (2016).

57. Shian S. and Clarke D.R.: Electrically tunable window device. Opt. Lett. 41(6), 1289 (2016).

58. Shian S., Bertoldi K., and Clarke D.R.: Dielectric elastomer based grippers for soft robotics. Adv. Mater. 27(43), 6814–6819 (2016).

59. Conrad H., Schenk H., Kaiser B., Langa S., Gaudet M., Schimmanz K., Stolz M., and Lenz M.: A small-gap electrostatic micro-actuator for large deflections. Nat. Commun. 6, 1–7 (2015).

60. Zhang W.M., Yan H., Peng Z.K., and Meng G.: Electrostatic pull-in instability in MEMS/NEMS: A review. Sens. Actuators, A 214(4), 187–218 (2014).

https://doi.org/10.1557/mre.2020.2Downloaded from https://www.cambridge.org/core. IP address: 54.39.106.173, on 28 Dec 2020 at 02:19:51, subject to the Cambridge Core terms of use, available at https://www.cambridge.org/core/terms.

Page 21: High-voltage applications of the triboelectric nanogenerator— … · can be produced by TENGs.10–12 TENGs are not only an excel-lent energy harvester but also a self-powered active

MRS eNeRgy & SUSTAINABIlITy // V O L U M E 6 // e 1 7 // www.mrs.org/energy-sustainability-journal n 21

61. Prins M.W., Welters W.J., and Weekamp J.W.: Fluid control in multichannel structures by electrocapillary pressure. Science 291(5502), 277–280 (2001).

62. Moon H., Cho S.K., Garrell R.L., and Kim C.J.C.: Low voltage electrowetting-on-dielectric. J. Appl. Phys. 92(7), 4080–4087 (2002).

63. Eow J.S. and Ghadiri M.: Motion, deformation and break-up of aqueous drops in oils under high electric field strengths. Chem. Eng. Process. 42(4), 259–272 (2003).

64. Nazemi M.H. and Hinrichsen V.: Experimental investigations on water droplet oscillation and partial discharge inception voltage on polymeric insulating surfaces under the influence of AC electric field stress. IEEE Trans. Dielectr. Electr. Insul. 20(2), 443–453 (2013).

65. Li J., Wei Y., Huang Z., Wang F., Yan X., and Wu Z.: Electrohydrodynamic behavior of water droplets on a horizontal super hydrophobic surface and its self-cleaning application. Appl. Surf. Sci. 403, 133–140 (2017).

66. Chen X., Iwamoto M., Shi Z., Zhang L., and Wang Z.L.: Self-powered trace memorization by conjunction of contact-electrification and ferroelectricity. Adv. Funct. Mater. 25(5), 739–747 (2015).

67. Jeong C.K., Kim I., Park K.I., Oh M.H., Paik H., Hwang G.T., No K., Nam Y.S., and Lee K.J.: Virus-directed design of a flexible BaTiO3 nanogenerator. ACS Nano 7(12), 11016–11025 (2013).

68. Nie J., Jiang T., Shao J., Ren Z., Bai Y., Iwamoto M., Chen X., and Wang Z.L.: Motion behavior of water droplets driven by triboelectric nanogenerator. Appl. Phys. Lett. 112(18), 183701 (2018).

69. Hayes R.A. and Johan Feenstra B.: Video-speed electronic paper based on electrowetting. Nature 425(6956), 383 (2003).

70. Chen X., Wu Y., Shao J., Jiang T., Yu A., Xu L., and Wang Z.L.: On-skin triboelectric nanogenerator and self-powered sensor with ultrathin thickness and high stretchability. Small 13(47), 1702929 (2017).

71. Chen X., Taguchi D., Manaka T., and Iwamoto M.: Study of blocking effect of Cu-phthalocyanine layer in zinc oxide/pentacene/CuPc/C60/Al organic solar cells by electric field-induced optical second harmonic generation measurement. Org. Electron. 14(1), 320–325 (2013).

72. Zheng L., Wu Y., Chen X., Yu A., Xu L., Liu Y., Li H., and Wang Z.L.: Self-powered electrostatic actuation systems for manipulating the movement of both microfluid and solid objects by using triboelectric nanogenerator. Adv. Funct. Mater. 27(16), 1606408 (2017).

73. Nie J., Ren Z., Shao J., Deng C., Xu L., Chen X., Li M., and Wang Z.L.: Self-powered microfluidic transport system based on triboelectric nanogenerator and electrowetting technique. ACS Nano 12(2), 1491–1499 (2018).

74. Zhong J., Zhong Q., Fan F., Zhang Y., Wang S., Hu B., Wang Z.L., and Zhou J.: Finger typing driven triboelectric nanogenerator and its use for instantaneously lighting up LEDs. Nano Energy 2(4), 491–497 (2013).

75. Wang X., Yin Y., Yi F., Dai K., Niu S., Han Y., Zhang Y., and You Z.: Bioinspired stretchable triboelectric nanogenerator as energy-harvesting skin for self-powered electronics. Nano Energy 39, 429–436 (2017).

76. Hinchet R. and Kim S-W.: Wearable and implantable mechanical energy harvesters for self-powered biomedical systems. ACS Nano 9(8), 7742–7745 (2015).

77. Han H-V., Lu A-Y, Lu L-S, Huang J-K, Li H, Hsu C-L, Lin Y-C, Chiu M-H, Suenaga K, Chu C-W, Kuo H-C, Chang W-H, Li L-J, and Shi Y.: Photoluminescence enhancement and structure repairing of monolayer MoSe2 by hydrohalic acid treatment. ACS Nano 10(1), 1454–1461 (2016).

78. Bu T. et al.: Triboelectric effect-driven liquid metal actuators. Soft Robot. 6(5), 664–670 (2019).

79. Wang Q., Yang Y., and Liu J.: Preparations, characteristics and applications of the functional liquid metal materials. Adv. Eng. Mater. 20(5), 1700781 (2018).

80. Daeneke T., Khoshmanesh K., Mahmood N., De Castro I.A., Esrafilzadeh D., Barrow S.J., Dickey M.D., and Kalantar-Zadeh K.: Liquid metals: Fundamentals and applications in chemistry. Chem. Soc. Rev. 47(11), 4073–4111 (2018).

81. Monat C., Domachuk P., and Eggleton B.J.: Integrated optofluidics: A new river of light. Nat. Photon. 1(2), 106 (2007).

82. Atencia J. and Beebe D.J.: Controlled microfluidic interfaces. Nature 437(7059) 648–655 (2005).

83. Sheng L., Zhang J., and Liu J.: Diverse transformations of liquid metals between different morphologies. Adv. Mater. 26(34), 6036–6042 (2014).

84. Zhang J., Sheng L., and Liu J.: Synthetically chemical-electrical mechanism for controlling large scale reversible deformation of liquid metal objects. Sci. Rep. 4, 7116 (2014).

85. Zhang J., Yao Y., Sheng L., and Liu J.: Self-fueled biomimetic liquid metal mollusk. Adv. Mater. 27(16), 2648–2655 (2015).

86. Hu L., Wang L., Ding Y., Zhan S., and Liu J.: Manipulation of liquid metals on a graphite surface. Adv. Mater. 28(41), 9210–9217 (2016).

87. Wang J., Wang H., Li X., and Zi Y.: Self-powered electrowetting optical switch driven by a triboelectric nanogenerator for wireless sensing. Nano Energy 66, 104140 (2019).

88. Bai P., Zhu G., Jing Q., Yang J., Chen J., Su Y., Ma J., Zhang G., and Wang Z.L.: Membrane-based self-powered triboelectric sensors for pressure change detection and its uses in security surveillance and healthcare monitoring. Adv. Funct. Mater. 24(37), 5807–5813 (2014).

89. Xu M., Wang S., Zhang S.L., Ding W., Kien P.T., Wang C., Li Z., Pan X., and Wang Z.L.: A highly-sensitive wave sensor based on liquid-solid interfacing triboelectric nanogenerator for smart marine equipment. Nano Energy 57, 574–580 (2019).

90. Luo J., Fan F.R., Zhou T., Tang W., Xue F., and Wang Z.L.: Ultrasensitive self-powered pressure sensing system. Extreme. Mech. Lett. 2, 28–36 (2015).

91. Chen Y., Zhang Y., Zhan T., Lin Z., Zhang S.L., Zou H., Zhang G., Zou C., and Wang Z.L.: An elastic triboelectric nanogenerator for harvesting random mechanical energy with multiple working modes. Adv. Mater. Technol. 4(7), 1900075 (2019).

92. Chan V.W.S.: Free-space optical communications. J. Lightwave Technol. 24(12), 4750–4762 (2006).

93. Kiasaleh K.: Performance of APD-based, PPM free-space optical communication systems in atmospheric turbulence. IEEE Trans. Commun. 53, 1455–1461 (2005).

94. Boucouvalas A., Chatzimisios P., Ghassemlooy Z., Uysal M., and Yiannopoulos K.: Standards for indoor optical wireless communications. IEEE Commun. Mag. 53, 24–31 (2015).

95. Moss B.R., Orcutt J.S., and Stojanovic V.M.: Devices and techniques for integrated optical data communication. U.S. Patent Application No. 16/150,965 (2018).

96. Silberberg Y., Perlmutter P., and Baran J.: Digital optical switch. Appl. Phys. Lett. 51, 1230–1232 (1987).

97. Mugele F. and Baret J.: Electrowetting: From basics to applications. J. Phys.: Condens. Matter 17, R705 (2005).

98. Roh H.S., Lee C.M., Hwang Y.H., Kook M.S., Yang S.W., Lee D., and Kim B.H.: Addition of MgO nanoparticles and plasma surface treatment of three-dimensional printed polycaprolactone/hydroxyapatite scaffolds for improving bone regeneration. Mater. Sci. Eng., C 74, 525–535 (2017).

99. Zhang C., Lin H., Zhang S., Xie Q., Ren C., and Shao T.: Plasma surface treatment to improve surface charge accumulation and dissipation of epoxy resin exposed to DC and nanosecond-pulse voltages. J. Phys. D: Appl. Phys. 50, 405203 (2017).

100. Kim T.H., Lee S.M., Lee C.H., Bae J.O., Yeom G.Y., and Kim K.N.: Characteristics of pulsed internal inductively coupled plasma for next generation display processing. J. Nanosci. Nanotechnol. 14, 9614–9618 (2014).

101. Lee S.M., Kim D., Jeon D.Y., and Choi K.C.: Nanoplasmon-enhanced transparent plasma display devices. Small 8, 1350–1354 (2012).

102. Haertel B., von Woedtke T., Weltmann K.D., and Lindequist U.: Non-thermal atmospheric-pressure plasma possible application in wound healing. Biomol. Ther. 22, 477–490 (2014).

103. Graves D.B.: The emerging role of reactive oxygen and nitrogen species in redox biology and some implications for plasma applications to medicine and biology. J. Phys. D: Appl. Phys. 45, 263001 (2012).

104. Cheng J., Ding W., Zi Y., Lu Y., Ji L., Liu F., Wu C., and Wang Z.L.: Triboelectric microplasma powered by mechanical stimuli. Nat. Commun. 9(1), 1–11 (2018).

105. Liu C., Wang Q-H., and Wang M-H.: Mirror reflector actuated by liquid droplet. IEEE Photonics Technol. Lett. 26(11), 1077–1080 (2014).

https://doi.org/10.1557/mre.2020.2Downloaded from https://www.cambridge.org/core. IP address: 54.39.106.173, on 28 Dec 2020 at 02:19:51, subject to the Cambridge Core terms of use, available at https://www.cambridge.org/core/terms.

Page 22: High-voltage applications of the triboelectric nanogenerator— … · can be produced by TENGs.10–12 TENGs are not only an excel-lent energy harvester but also a self-powered active

22 n MRS eNeRgy & SUSTAINABIlITy // V O L U M E 6 // e 1 7 // www.mrs.org/energy-sustainability-journal

106. Zhang C., Tang W., Pang Y., Han C., and Wang Z.L.: Active micro-actuators for optical modulation based on a planar sliding triboelectric nanogenerator. Adv. Mater. 27(4), 719–726 (2015).

107. Yang H., Pang Y., Bu T., Liu W., Luo J., Jiang D., Zhang C., and Wang Z.L.: Triboelectric micromotors actuated by ultralow frequency mechanical stimuli. Nat. Commun. 10(1), 1–7 (2019).

108. Solgaard O., Godil A.A., Howe R.T., Lee L.P., Peter Y.A., and Zappe H.: Optical MEMS: From micromirrors to complex systems. J. Microelectromech. Syst. 23(3), 517–538 (2014).

109. Xie Z., Jiao S., Zhang H.F., and Puliafito C.A.: Laser-scanning optical-resolution photoacoustic microscopy. Optic Lett. 34(12), 1771–1773 (2009).

110. Monkman G.J.: An analysis of astrictive prehension. Int. J. Robot Res. 16(1), 1–10 (1997).

111. Graule M.A., Chirarattananon P., Fuller S.B., Jafferis N.T., Ma K.Y., Spenko M., Kornbluh R., and Wood R.J.: Perching and takeoff of a robotic insect on overhangs using switchable electrostatic adhesion. Science 352(6288), 978–982 (2016).

112. Shintake J., Rosset S., Schubert B., Floreano D., and Shea H.: Versatile soft grippers with intrinsic electroadhesion based on multifunctional polymer actuators. Adv. Mater. 28(2), 231–238 (2016).

113. Guo J., Bamber T., Chamberlain M., Justham L., and Jackson M.: Optimization and experimental verification of coplanar interdigital electroadhesives. J. Phys. D: Appl. Phys. 49(41), 415304 (2016).

114. Ruffatto D. III, Parness A., and Spenko M.: Improving controllable adhesion on both rough and smooth surfaces with a hybrid electrostatic/gecko-like adhesive. J. R. Soc. Interface 11(93), 20131089 (2014).

115. Asano K., Hatakeyama F., and Yatsuzuka K.: Fundamental study of an electrostatic chuck for silicon wafer handling. IEEE Trans. Ind. Appl. 38(3), 840–845 (2002).

116. Xu L., Wu H., Yao G., Chen L., Yang X., Chen B., Huang X., Zhong W., Chen X., Yin Z., and Wang Z.L.: Giant voltage enhancement via triboelectric charge supplement channel for self-powered electroadhesion. ACS Nano 12(10), 10262–10271 (2018).

117. Guo J., Bamber T., Singh J., Manby D., Bingham P.A., Justham L., Petzing J., Penders J., and Jackson M.: Experimental study of a flexible and environmentally stable electroadhesive device. Appl. Phys. Lett. 111(25), 251603 (2017).

118. Rus D. and Tolley M.T.: Design, fabrication and control of soft robots. Nature 521(7553), 467–475 (2015).

119. Wang Z.L.: ACS Nano 7, 9533 (2013); Z.L. Wang: Faraday Discuss 176, 447 (2014).

120. Wang Z.L., Chen J., and Lin L.: Progress in triboelectric nanogenerators as a new energy technology and self-powered sensors. Energy Environ. Sci. 8(8), 2250–2282 (2015).

121. Yang C., Yang G., Ouyang Q., Kuang S., Song P., Xu G., Poenar D.P., Zhu G., Yong K.T., and Wang Z.L.: Nanowire-array-based gene electro-transfection system driven by human-motion operated triboelectric nanogenerator. Nano Energy 64, 103901 (2019).

122. Bellan L.M. and Craighead H.G.: Nanomanufacturing using electrospinning. J. Manuf. Sci. Eng. 131(3), 034001 (2009).

123. Li D. and Xia Y.: Electrospinning of nanofibers: Reinventing the wheel? Adv. Mater. 16(14), 1151–1170 (2010).

124. Bhardwaj N. and Kundu S.C.: Electrospinning: A fascinating fiber fabrication technique. Biotechnol. Adv. 28(3), 325–347 (2010).

125. Huang Z.M., Zhang Y.Z., Kotaki M., and Ramakrishna S.: A review on polymer nanofibers by electrospinning and their applications in nanocomposites. Compos. Sci. Technol. 63(15), 2223–2253 (2003).

126. Deitzel J.M., Kleinmeyer J., Harris D.E.A., and Tan N.B.: The effect of processing variables on the morphology of electrospun nanofibers and textiles. Polymer 42(1), 261–272 (2001).

127. Cho J.S., Young J.H., and Kang Y.C.: Design and synthesis of bubble-nanorod-structured Fe2O3–carbon nanofibers as advanced anode material for Li-ion batteries. ACS Nano 9(4), 4026–4035 (2015).

128. Sridhar R., Lakshminarayanan R., Madhaiyan K., Barathi V.A., Lim K.H.C., and Ramakrishna S.: Electrosprayed nanoparticles and electrospun nanofibers based on natural materials: Applications in

tissue regeneration, drug delivery and pharmaceuticals. Chem. Soc. Rev. 44(3), 790–814 (2015).

129. Hu X., Liu S., Zhou G., Huang Y., Xie Z., and Jing X.: Electrospinning of polymeric nanofibers for drug delivery applications. J. Contr. Release 185, 12–21 (2014).

130. Strain I.N., Wu Q., Pourrahimi A.M., Hedenqvist M.S., Olsson R.T., and Andersson R.L.: Electrospinning of recycled PET to generate tough mesomorphic fibre membranes for smoke filtration. J. Mater. Chem. A 3(4), 1632–1640 (2015).

131. Li W., Ma S., Li Y., Yang G., Mao Y., Luo J., Gengzang D., Xu X., and Yan S.: Enhanced ethanol sensing performance of hollow ZnO–SnO2 core–shell nanofibers. Sens. Actuators, B 211, 392–402 (2015).

132. Taylor G.I.: Disintegration of water drops in an electric field. Proc. R. Soc. London, Ser. A 280(1382), 383–397 (1964).

133. Secor E.B.: Principles of aerosol jet printing. Flexible Printed Electron. 3(3), 035002 (2018).

134. Chang Y.H., Wang K., Wu C., Chen Y., Zhang C., and Wang B.: A facile method for integrating direct-write devices into three-dimensional printed parts. Smart Mater. Struct. 24(6), 065008 (2015).

135. Park J.U., Hardy M., Kang S.J., Barton K., Adair K., Kishore Mukhopadhyay D., Lee C.Y., Strano M.S., Alleyne A.G., Georgiadis J.G., Ferreira P.M., and Rogers J.A.: High-resolution electrohydrodynamic jet printing. Nat. Mater. 6(10), 782–789 (2007).

136. Wu C., Tetik H., Cheng J., Ding W., Guo H., Tao X., Zhou N., Zi Y., Wu Z., Wu Z., Lin D., and Wang Z.L.: Electrohydrodynamic jet printing driven by a triboelectric nanogenerator. Adv. Funct. Mater. 29(22), 1901102 (2019).

137. Wang H.S., Jeong C.K., Seo M.H., Joe D.J., Han J.H., Yoon J.B., and Lee K.J.: Performance-enhanced triboelectric nanogenerator enabled by wafer-scale nanogrates of multistep pattern downscaling. Nano Energy 35, 415–423 (2017).

138. Seol M.L., Han J.W., Park S.J., Jeon S.B., and Choi Y.K.: Hybrid energy harvester with simultaneous triboelectric and electromagnetic generation from an embedded floating oscillator in a single package. Nano Energy 23, 50–59 (2016).

139. Li C., Yin Y., Wang B., Zhou T., Wang J., Luo J., Tang W., Cao R., Yuan Z., Li N., Du X., Wang C., Zhao S., Liu Y., and Wang Z.L.: Self-powered electrospinning system driven by a triboelectric nanogenerator. ACS Nano 11(10), 10439–10445 (2017).

140. Huo H., Liu F., Luo Y., Gu Q., Liu Y., Wang Z., Chen R., Ji L., Lu Y., Yao R., and Cheng J.: Triboelectric nanogenerators for electro-assisted cell printing. Nano Energy 67, 104150 (2019).

141. Wang K., Paine M.D., and Stark J.P.W.: Fully voltage-controlled electrohydrodynamic jet printing of conductive silver tracks with a sub-100 μm linewidth. J. Appl. Phys. 106(2), 024907 (2009).

142. Park J.U., Lee J.H., Paik U., Lu Y., and Rogers J.A.: Nanoscale patterns of oligonucleotides formed by electrohydrodynamic jet printing with applications in biosensing and nanomaterials assembly. Nano Lett. 8(12), 4210–4216 (2008).

143. Kim B.H., Onses M.S., Lim J.B., Nam S., Oh N., Kim H., Yu K.J., Lee J.W, Kim J., Kang S., Lee C.H., Lee J., Shin J.H., Kim N.H., Leal C., Shim M., and Rogers J.A.: High-resolution patterns of quantum dots formed by electrohydrodynamic jet printing for light-emitting diodes. Nano Lett. 15(2), 969–973 (2015).

144. Kim K., Kim G., Lee B.R., Ji S., Kim S.Y., An B.W., Song M.H., and Park J.U.: High-resolution electrohydrodynamic jet printing of small-molecule organic light-emitting diodes. Nanoscale 7(32), 13410–13415 (2015).

145. Maher S., Jjunju F.P.M., and Taylor S.: Colloquium: 100 years of mass spectrometry: Perspectives and future trends. Rev. Mod. Phys. 87(1), 113 (2015).

146. Liang X., Han H., Xia Y., and McLuckey S.A.: A pulsed triple ionization source for sequential ion/ion reactions in an electrodynamic ion trap. J. Am. Soc. Mass Spectrom. 18(3), 369–376 (2007).

147. Bushey J.M., Kaplan D.A., Danell R.M., and Glish G.L.: Pulsed nano-electrospray ionization: Characterization of temporal response and implementation with a flared inlet capillary. Instrum. Sci. Technol. 37(3), 257–273 (2009).

https://doi.org/10.1557/mre.2020.2Downloaded from https://www.cambridge.org/core. IP address: 54.39.106.173, on 28 Dec 2020 at 02:19:51, subject to the Cambridge Core terms of use, available at https://www.cambridge.org/core/terms.

Page 23: High-voltage applications of the triboelectric nanogenerator— … · can be produced by TENGs.10–12 TENGs are not only an excel-lent energy harvester but also a self-powered active

MRS eNeRgy & SUSTAINABIlITy // V O L U M E 6 // e 1 7 // www.mrs.org/energy-sustainability-journal n 23

148. Xu W., Charipar N., Kirleis M.A., Xia Y., and Ouyang Z.: Study of discontinuous atmospheric pressure interfaces for mass spectrometry instrumentation development. Anal. Chem. 82(15), 6584–6592 (2010).

149. Schilling M., Janasek D., and Franzke J.: Electrospray-ionization driven by dielectric polarization. Anal. Bioanal. Chem. 391(2), 555–561 (2008).

150. Huang G., Li G., and Graham Cooks R.: Induced nanoelectrospray ionization for matrix-tolerant and high-throughput mass spectrometry. Angew. Chem., Int. Ed. 50(42), 9907–9910 (2011).

151. Shekhar M., Wang J., Lee W.S., Williams W.D., Kim S.M., Stach E.A., Miller J.T., Deglass W.N., and Ribeiro F.H.: Size and support effects for the water–gas shift catalysis over gold nanoparticles supported on model Al2O3 and TiO2. J. Am. Chem. Soc. 134(10), 4700–4708 (2012).

152. Li A., Zi Y., Guo H., Wang Z.L., and Fernández F.M.: Triboelectric nanogenerators for sensitive nano-coulomb molecular mass spectrometry. Nat. Nanotechnol. 12(5), 481–487 (2017).

153. Tang W., Tian J., Zheng Q., Yan L., Wang J., Li Z., and Wang Z.L.: Implantable self-powered low-level laser cure system for mouse embryonic osteoblasts’ proliferation and differentiation. ACS Nano 9(8), 7867–7873 (2015).

154. Wang S., Zi Y., Zhou Y.S., Li S., Fan F., Lin L., and Wang Z.L.: Molecular surface functionalization to enhance the power output of triboelectric nanogenerators. J. Mater. Chem. A 4(10), 3728–3734 (2016).

155. Bernier M.C., Li A., Winalski L., Zi Y., Li Y., Caillet C., Newton P., Wang Z.L., and Fernández F.M.: Triboelectric nanogenerator (TENG) mass spectrometry of falsified antimalarials. Rapid Commun. Mass Spectrom. 32(18), 1585–1590 (2018).

156. Chen J., Zhu G., Yang W., Jing Q., Bai P., Yang Y., Hou T., and Wang Z.L.: Harmonic-resonator-based triboelectric nanogenerator as a sustainable power source and a self-powered active vibration sensor. Adv. Mater. 25(42), 6094–6099 (2013).

157. Ahmed A., Hassan I., Ibn-Mohammed T., Mostafa H., Reaney I.M., Koh L.S., Zu J., and Wang Z.L.: Environmental life cycle assessment and

techno-economic analysis of triboelectric nanogenerators. Energy Environ. Sci. 10(3), 653–671 (2017).

158. Yang W., Chen J., Zhu G., Wen X., Bai P., Su Y., Lin Y., and Wang Z.: Harvesting vibration energy by a triple-cantilever based triboelectric nanogenerator. Nano Res. 6(12), 880–886 (2013).

159. Chen B., Yang Y., and Wang Z.L.: Scavenging wind energy by triboelectric nanogenerators. Adv. Energy Mater. 8(10), 1702649 (2018).

160. Yang J., Chen J., Liu Y., Yang W., Su Y., and Wang Z.L.: Triboelectrification- based organic film nanogenerator for acoustic energy harvesting and self-powered active acoustic sensing. ACS Nano 8(3), 2649–2657 (2014).

161. Yi F., Lin L., Niu S., Yang P.K., Wang Z., Chen J., Zhou Y., Zi Y., Wang J., Liao Q., Zhang Y., and Wang Z.L.: Stretchable-rubber-based triboelectric nanogenerator and its application as self-powered body motion sensors. Adv. Funct. Mater. 25(24), 3688–3696 (2015).

162. Lin Z., Yang J., Li X., Wu Y., Wei W., Liu J., Chen J., and Yang J.: Large-scale and washable smart textiles based on triboelectric nanogenerator arrays for self-powered sleeping monitoring. Adv. Funct. Mater. 28(1), 1704112 (2018).

163. Chen J., Zhu G., Yang J., Jing Q., Bai P., Yang W., Qi X., Su Y., and Wang Z.L.: Personalized keystroke dynamics for self-powered human–machine interfacing. ACS Nano 9(1), 105–116 (2015).

164. Li S., Fan Y., Chen H., Nie J., Liang Y., Tao X., Zhang J., Chen X., Fu E., and Wang Z.: Manipulating the triboelectric surface charge density of polymers by low-energy Helium irradiation/implantation. Energy Environ. Sci. (2019).

165. Nie J., Ren Z., Xu L., Lin S., Zhan F., Chen X., and Wang Z.L.: Probing contact-electrification-induced electron and ion transfers at a liquid–solid interface. Adv. Mater. 32(2), 1905696 (2020).

166. Wang J., Lo J.C., Lee S.R., Tao M., Zou H., and Yun F.: A novel approach to characterize phosphor particles for the color tuning of WLEDs. IEEE Photonics Technol. Lett. 30(6), 513–516 (2017).

https://doi.org/10.1557/mre.2020.2Downloaded from https://www.cambridge.org/core. IP address: 54.39.106.173, on 28 Dec 2020 at 02:19:51, subject to the Cambridge Core terms of use, available at https://www.cambridge.org/core/terms.