Scalable nanomanufacturing of inkjet-printed wearable energy storage devices

Tao-Tse Huang a and Wenzhuo Wu *ab
aSchool of Industrial Engineering, Purdue University, West Lafayette, Indiana 47907, USA. E-mail: wenzhuowu@purdue.edu
bFlex Laboratory, Purdue University, West Lafayette, Indiana 47907, USA

Received 17th May 2019 , Accepted 26th June 2019

First published on 27th June 2019


Abstract

The economic production and integration of nanomaterial-based wearable energy storage devices with mechanically-compliable form factors and reliable performance will usher in exciting opportunities in emerging technologies such as consumer electronics, pervasive computing, human–machine interface, robotics, and the Internet of Things. Despite the increased interests and efforts in nanotechnology-enabled flexible energy storage devices, reducing the manufacturing and integration costs while continuously improving the performance at the device and system level remains a major technological challenge. The inkjet printing process has emerged as a potential economic method for nanomanufacturing printed electronics, sensors, and energy devices. Nevertheless, there have been few reports reviewing the scalable nanomanufacturing of inkjet printed wearable energy storage devices. To fill this gap, here we review the recent advances in inkjet printed flexible energy storage technologies. We will provide an in-depth discussion focusing on the materials, manufacturing process integration, and performance issues in designing and implementing the inkjet printing of wearable energy storage devices. We have also compiled a comprehensive list of the reported device technologies with the corresponding processing factors and performance metrics. Finally, we will discuss the challenges and opportunities associated with related topics. The rapid and exciting progress achieved in many emerging and traditional disciplines is expected to lead to more theoretical and experimental advances that would ultimately enable the scalable nanomanufacturing of inkjet printed wearable energy storage devices.


image file: c9ta05239a-p1.tif

Wenzhuo Wu

Dr Wenzhuo Wu is the Ravi and Eleanor Talwar Rising Star Assistant Professor in School of Industrial Engineering at Purdue University. He received his BS in Electronic Information Science and Technology in 2005 from the University of Science and Technology of China (USTC), Hefei and his ME in Electrical and Computer Engineering from the National University of Singapore (NUS) in 2008. Dr Wu received his PhD from Georgia Institute of Technology in Materials Science and Engineering in 2013. Dr Wu's research interests include design, manufacturing, and integration of 1D and 2D nanomaterials for applications in energy, electronics, optoelectronics, and wearable devices. He was a recipient of the Oak Ridge Associated Universities (ORAU) Ralph E. Powe Junior Faculty Enhancement Award in 2016, the IOP Semiconductor Science and Technology Best Early Career Research in 2017, and the Society of Manufacturing Engineers (SME) Barbara M. Fossum Outstanding Young Manufacturing Engineer Award in 2019.


1. Introduction

The economic production and integration of nanomaterials-based wearable energy storage devices with mechanically-compliable form factors and reliable performance will provide exciting opportunities in emerging technologies such as consumer electronics, pervasive computing, human–machine interface, robotics, and the Internet of Things (IoT).1–10 Lithium-ion batteries (LIBs) are the most widely used commercial portable energy storage devices, with a projected global market value at 26 billion USD by 2023. Meanwhile, the supercapacitors market was estimated to be around 948.63 million USD in 2018 and is projected to have an annual growth of 18.69% from 2019 to 2024. Prototypes of flexible energy storage devices that exhibit lightweight and mechanical deformability have been recently developed in technology sectors with huge market needs, such as smart textiles, biomedical electronics, and implementable systems.8,11,12 Several commercial electronic devices with folding and rolling capability, such as the Samsung Galaxy Fold and the LG flexible TV, were also introduced recently.

Despite the increased interests and efforts in nanotechnology-enabled flexible energy storage devices, reducing the manufacturing and integration costs while continuously improving the performance at the device and system level remains a major technological challenge. The inkjet printing process has emerged as a potential economic method for nanomanufacturing printed electronics, sensors, and energy devices, due to advantages such as full digital mask-less printability, versatile ink formulation, cost-effectiveness, low working temperature, and feasibility for scale-up production.13–15 Many efforts have been devoted to developing the related technology, and several review articles provided good coverage discussing the material and process aspects of inkjet printed devices.16,17 Nevertheless, to our best knowledge, there have been few reports reviewing the scalable nanomanufacturing of inkjet printed wearable energy storage devices. To fill this gap, here we review the recent advances in inkjet printed flexible energy storage technologies. The recent rapid increase in the research interests and efforts in related areas can be seen in Fig. 1, which was generated by conducting a bibliometric analysis using the keywords of “nanomaterial” “inkjet printing” “flexible” and “energy storage device”. We will provide an in-depth discussion focusing on the materials and process integration. Finally, we will discuss the challenges and opportunities associated with the scalable nanomanufacturing of inkjet-printed wearable energy storage devices.


image file: c9ta05239a-f1.tif
Fig. 1 The increased interests of the research topic on the inkjet printing of flexible nanomaterials based energy storage devices in recent years.

2. State-of-the-art flexible energy storage devices

The most commonly used electrochemical energy storage (EES) devices are batteries and supercapacitors (SCs). Various types of flexible batteries were reported in the literature, such as the lithium-ion battery,18–26 zinc–air battery,27–33 lithium–sulfur battery,34–38 lithium–air battery,39,40 sodium ion battery,41–46 and aluminum–air battery,39,47 among which flexible LIBs are the most widely researched and utilized. A detailed discussion of the recent developments in flexible batteries can be found in previous review papers.8,23,48–51 The three types of supercapacitors are the electrochemical double layer capacitor, pseudocapacitor, and hybrid capacitor, which is the combination of the previous two.52–54 The major difference between batteries and SCs is that batteries can store large amounts of energy while with relatively low power density, which leads to longer charge periods. Supercapacitors, on the other hand, possess high power densities with lower energy densities than those typical for batteries. A detailed review of the general principles and recent progress in flexible supercapacitors could be found in ref. 12 and 55. Flexible EES usually consist of several components, including an anode, cathode, divider, electrolyte, and a current collector, which should all have bending capability and shape compatibility to achieve the overall flexibility of the device. Nanomaterials with high electrochemical performance are usually utilized as active materials, such as metal oxides,52,54,56–60 conductive polymers,61–69 carbon-based materials,70–80 and other emerging materials, such as titanium carbide.81–84 Various configurations of flexible EES have been provided in a review by Dubal et al.55 which are cable-type (Fig. 2a), sandwich (Fig. 2b), planar, wire-type (Fig. 2c),85 and fiber-shaped (Fig. 2d) structure.86 This review primarily focuses on the inkjet printing of planar and sandwich-structured devices.
image file: c9ta05239a-f2.tif
Fig. 2 (a) Structure of a cable-type sodium-ion battery.41 Reproduced with permission. Copyright 2017, Elsevier; (b) structure of a sandwich type sodium-ion battery. Reproduced with permission.41 Copyright 2017, Elsevier; (c) structure of a wire-shaped lithium-ion battery.85 Reproduced with permission. Copyright 2013, Wiley-VCH; (d) structure of fiber-shaped supercapacitor.86 Reproduced with permission. Copyright 2019, American Chemical Society.

3. Process elements in inkjet printing for nanomanufacturing wearable energy devices

A recent review on advances in flexible EES devices by Wang et al. discussed numerous techniques for fabricating flexible EES. Conventional techniques such as spray deposition, chemical vapor deposition (CVD), electrochemical deposition, and sputtering have been widely employed for fabricating flexible EES devices.87–92 However, the lack of process scalability and the convoluted processing conditions make these techniques unfavorable for large-scale manufacturing. Compared to the conventional fabrication methods, printing techniques, especially inkjet printing, presents a facile and effective process for manufacturing flexible EES due to the feasibility and flexibility of printing various individual components as well as the integrated systems at large-scale.

Dozens of manufacturing methods have been developed for printing EES devices.93 The commonly utilized printing techniques for depositing nanomaterials include screen-printing, transfer printing, 3D printing, and inkjet printing.94–96 The screen-printing technique deposits ink onto a substrate with the use of a pre-patterned mask. The transfer printing technique starts by patterning a material on a substrate, followed by transferring the printed materials to another substrate. 3D printing extrudes material out of the nozzle and deposits the material onto the substrate, where multi-layer printing is utilized for stacking the patterns into three-dimensional structures. The inkjet printing process hinges on an extrusion-based ink deposition, which ejects the suspension from the nozzle and deposits it onto the substrates (Fig. 3). The inkjet printing process can be categorized into continuous inkjet (CIJ) (Fig. 3a)97 and drop-on-demand (DOD) (Fig. 3b)97 methods. The CIJ method deposits a continuous stream of ink onto the substrates and recycles the excess ink, while the DOD method deposits discrete ink droplets at the predesigned locations which offer less contamination and cost-effective printing of precious materials. The two main types of inkjet printheads are thermal and piezoelectric, as shown in Fig. 3b. Thermal print heads contain a resistive heater inside the ink chamber for superheating the ink so that it can flow through the printhead. Piezoelectric printheads contain a mechanism that osculates due to electrical excitation and purges the ink through the chamber by forming a pressure wave. Other than the thermal and piezoelectric printheads, an electrohydrodynamic printing technique was also discussed in the literature.98–100 In all the inkjet printing processes, the droplet ejection is highly dependent on the viscosity, surface tension, and density of the ink. Benefits possessed by the inkjet printing process, specifically, the DOD method includes maskless, rapid deposition, scalability from small droplet to large area fabrication, less contamination, good material compatibility, less wastage, and low cost.


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Fig. 3 Schematic of (a) continuous inkjet (CIJ) printer.97 Reproduced with permission. Copyright 2010, Annual Review of Materials Research; (b) drop on demand (DOD) inkjet printer with thermal (left) and piezoelectric (right) printheads.97 Reproduced with permission. Copyright 2010, Annual Review of Materials Research.

Some key processing elements for the inkjet printing include the dimensions of the nanomaterial, material agglomeration, ink concentration, droplet travel distances, ink viscosity, the surface tension of the ink, etc. The size of the material should be at least 50 times less than the printing nozzle to avoid clogging the nozzles,94–96 which could be achieved through co-designing and controlling the synthesis and preparation of nanomaterials. The agglomeration of materials could be resolved by incorporating surfactants or dispersing agents, such as dimethylformamide (DMF),83,101–104N-methyl pyrrolidone (NMP),82,105,106 or propylene glycol.13,107 The concentration of the ink is also critical for the inkjet printing process, where a too high concentration can clog the nozzle and too low value can significantly increase the printing time for desired feature dimensions.93,108,109 A small droplet traveled distance is ideal for the inkjet printing process with improved control of the feature dimensions and spatial locations. The idea ink viscosity should be around 1 to 20 cP,82,93,109 which is significantly lower than that for screen-printing or 3D printing, and surface tension value should be below 80 N m−1 for efficient printing onto versatile substrates.93,109

In addition to the above guidelines for inkjet printing in general, there are some specific requirements that need to be taken into consideration for inkjet printing of wearable EES. To ensure the quality of the printing process, the ink should meet the required viscosity and surface tension. The dimension of the nanomaterial should also be in an acceptable range, which is generally 50 times smaller than the size of the printhead, to avoid the clogging of the nozzles. To ensure the quality of the printed film and the device performance, annealing or film compression are usually utilized after the inkjet printing process. These post-printing processes need to be compatible with the printed materials, e.g., not causing material degradation, and should be well controlled to ensure the desired mechanical flexibility and robustness that are needed in the wearable EES applications. The long-term stability of the printed devices is critical for practical applications. Cyclic aging characterization is usually required for probing the material and device stability/reliability when the devices are subject to bending, deformation, elevated temperature, and humidity. Consequently, the selection of active materials, substrates, electrolyte, and current collector should all be put into consideration since these components need to have properties that are capable of creating devices that have not only good electrical performance but also desired mechanical robustness.

Current inkjet printing technology is capable of printing nanoparticles (NP) dispersions, conducting polymers, biological molecules, 1D and 2D nanostructures. Nanomaterials offer advantages over bulk material for enhanced electrochemical performance due to the lightweight, superior mechanical properties, high porosity, and large surface area. The performance of flexible batteries and flexible SCs is primarily determined by their electrode materials,93,109 which makes the selection of active material critical. Most of the materials utilized require incorporating other materials for the enhancement of physical durability and energy capacity.11 In the following sections, we will review recent advances in inkjet printing flexible batteries and supercapacitors.

4. Inkjet printing of nanomaterials for wearable batteries

4.1. Inkjet printed flexible zinc–air battery

Hilder et al.110 demonstrated the fabrication of a flexible zinc–air battery using both the inkjet printing and screen-printing process. The anode was created utilizing screen-printing with a combination of zinc/carbon/polymer composite. The poly(3,4-ethylene dioxythiophene) (PEDOT) cathode was prepared with inkjet printing a pattern of iron(III) p-toluenesulfonate ((FepTS)3) as a solution in 1-butanol onto a paper. A solution of lithium chloride (LiCl)/lithium hydroxide (LiOH) was prepared as an electrolyte and inkjet printed onto the paper substrate. The authors compared the device performance with different processing conditions, such as different electrolytes, various Zn contents, the utilization of polyethylene naphthalate (PEN), and paper substrates. The result concluded that an 8 M LiCl electrolyte contributes to higher efficiency than the 1 M NaCl does since the absences of water in the LiCl system leads to the reduction of aqueous zinc corrosion. Also, the devices with 1 M NaCl electrolyte showed no significant difference in efficiency when different Zn contents were used; while a significant enhancement in efficiency was observed under high Zn content for devices printed with 8 M LiCl electrolyte. The comparison between the substrates suggested that paper substrates led to less superior performance, possibly due to the highly porous substrate structure. The study provided important processing knowledge for inkjet printing flexible zinc–air batteries, particularly on the selection of proper electrolyte and substrate, which suggests the utilization of high-molarity electrolytes and less-porous substrates can lead to improved device performance. Such fundamental knowledge can be applied in future studies for further optimization of the inkjet printed devices.

4.2 Inkjet printed flexible zinc-silver battery

Ho et al.98 reported an alkaline zinc–silver micro-battery with 3D pillar electrodes utilizing a super inkjet printing (SIJP) technique. Silver (Ag) nanopaste was mixed with n-tetradecane as the ink for printing the current collectors for both electrodes. The Ag current collector also served as the backbone structure for depositing the electroplated zinc onto the negative electrode and silver oxide on the positive electrode. An aqueous electrolyte solution of KOH with dissolved ZnO was used for the battery operation. The study suggested that the conductivity and the porosity of the printed structures were influenced by the temperature and duration of the post-printing sintering process. Moreover, the performance characterization showed that the 3D pillar electrodes possess an up to 60% increase in capacity compared to a planar electrode with the same footprint. The device was printed using an electrohydrodynamic actuator, which also significantly reduced the droplet volume and hence enabled better printing resolutions compared to that can be achieved by commercial printers with piezoelectric or thermal printheads. The electrohydrodynamic printing technique is capable of printing smaller feature size, can be utilized not only printing batteries but also for other electronic devices. The 3D pillar geometry can also be applied to other EES devices for performance enhancement.

4.3 Inkjet printed flexible lithium–sulfur battery

Sulfur as a cathode material has characteristics such as high specific capacity, non-toxic, and low cost, which are beneficial for producing cost-effective batteries. However, sulfur has poor cyclic performance and conductivity,111 which necessitates the incorporation of conductive materials for improved battery performance. To address this issue, Milroy et al.34 reported the inkjet printing of a lithium–sulfur (Li–S) battery which utilized single-wall carbon nanotubes (SWNT) infused with electronically conductive sulfur straight-chain (S@SWNT) as the integrated current-collector/active-material composite. A post-printing annealing process was implemented to remove the excess solvent, where the printed structures were annealed on a hot plate with a gradual increase of 4 °C per minute from 25 to 150 °C, followed by heating at 150 °C for 10 to 15 minutes. The printed devices show a capacitance of 800 mA h g−1 initially and 700 mA h g−1 after 100 cycles, which is promising for potential applications in supplying power to thin-film devices. The study suggested that the gradual increase of annealing temperature at a suitable rate (e.g., 4 °C per minute) is essential for preserving the shape conformality. On the contrary, an increased rate below 2 °C per minute can lead to an inhomogeneous electrode due to the undesired Marangoni effect (Fig. 4a). Few studies have been performed on flexible Li–S batteries as well as the inkjet printing of such devices, likely due to the lack of understandings in the corresponding electrochemical processes. Further research is necessary to understand better the printing process and how it could engineer and affect the properties of the printed materials and structures in future wearable Li–S batteries with enhanced performance.
image file: c9ta05239a-f4.tif
Fig. 4 (a) Schematic of the evaporation of the droplet (Marangoni effect).107 Reproduced with permission. Copyright 2018, Elsevier; (b) schematic of the inkjet printing process for ionogel.116 Reproduced with permission. Copyright 2015, Elsevier.

4.4 Inkjet printed flexible lithium-ion battery

Lithium iron phosphate (LiFePO4, LFP), one of the commonly used cathode materials for EES, offers unique characteristics such as high capacity, low cost, and is environmental benign.111 Gu and colleagues19 utilized the DOD inkjet printing method and water-soluble LFP for fabricating LIB cathodes, with aluminum (Al) foil and CNT micro-paper as the current collector. The authors found that the binding and interaction between the printed active materials and CNT paper leads to better electrochemical performance than the devices with Al current collectors. The study also provided interesting and important manufacturing knowledge regarding the effects of ink impurity and oxygen content in the LFP on the performance of the printed devices. The authors revealed that the impurities in the suspension would lower the electrical conductivity of LiFePO4 and hence lead to higher resistance and significant energy loss. Moreover, the removal of oxygen content from water could prevent the oxidation of LiFePO4 to Fe2O3 and Fe3O4. Similar studies by Ben-Barak et al.20 and Delannoy et al.112 also demonstrated inkjet-printed LFP cathode for flexible LIBs using DOD printing method. LiCoO2 is another cathode material with a high specific capacitance that has been utilized for printing LIBs. Huang et al.113 fabricated a thin-film LiCoO2 electrode for LIB via inkjet printing and observed a 95% retention rate after 100 charge–discharge cycles. Their study also suggested that the device can be charged at various current densities, e.g., even as high as 384 μA cm−1, without compromising the charge and discharge efficiency. It should be noted, though, LiCoO2 suffers from the poor conductivity and high cost, which limit its manufacturing potential for printing cost-effective, flexible LIBs at large scale.

There have also been a few studies reporting the inkjet printing of anodes for LIBs using nanomaterials. Zhao et al.114 demonstrated the fabrication of tin oxide (SnO2) thin-film anode for rechargeable LIBs with a high discharge capacitance of 812.7 mA h g−1 through inkjet printing. For the preparation of the SnO2 ink, wet ball-milling was used for stabilizing the SnO2 NP and acetylene black (AB) with two polymeric hyperdispersants (CH10B and CH12B). The thickness of the SnO2 thin film can be controlled by repeating the printing procedure on the Cu foil substrate, followed by direct compression of the printed-film for the subsequent electrochemical characterization. Zhao et al.115 presented a printed Li4Ti5O12 (LTO) thin films on a gold (Au) substrate as the anode for LIBs. The excellent electrochemical properties of the device suggested the promise of ink-jet printing for manufacturing future flexible LIBs. In a separate study, Delannoy and colleagues116 focused on the inkjet printing of sol–gel silica-based ionogel (Fig. 4b) as the solid electrolyte for LIBs, with LFP and LTO being the electrodes. This study is interesting and unique in the sense that most other reported work focused on the inkjet printing of electrodes. A list of the reported inkjet-printed flexible battery devices is compiled in Table 1, and the performance of those devices is summarized in Table 2. The corresponding Ragone plots of the devices are shown in Fig. 7a, and b.

Table 1 Various components fabricated via inkjet printing in the literaturea
Devices Apparatus Additives Material Component Ref.
a Multi-wall carbon nanotubes (MWCNT); single-walled carbon nanotube (SWNT); graphene oxide (GO); nano graphene platelets (NGP); polyaniline (PANI); deionized water (DI water); sodium dodecyl sulfate (SDS); sodium dodecylbenzene sulfonate (SDBS); isopropylalcohol (IPA); ionic liquid (IL); polytetrafluoroethylene (PTFE); carboxymethyl cellulose (CMC); tetrahydrofuran (THF); ethylene glycol (EG); acetylene black (AB); carbon black (CB); activated carbon (AC); carbon nanofiber (CNF); LiFePO4 (LFP); Li4Ti5O12 (LTO); cumene hydroperoxide (CHP); N-methylpyrolidone (NMP); tetrabutylammonium hydroxide (TBA·OH); manganese dioxide (MnO2); 1-butyl-3-methylimidazolium tetrafluoroborate ([BMIM][BF4]); poly(3,4-ethlyenedioxythiophene) (PEDOT); cellulose nanofibers (CeNF); tin oxide (SnO2); lithium chloride (LiCl); lithium hydroxide (LiOH); polyethylene glycol (PEG), poly-acrylic-co-maleic acid (PAMA), N-methyl-N-propylpyrro-lidinium bis(trifluoromethane) suflonylimide ionic liquid (PYR13-TFSI); lithium bis(trifluoro-methane)sulfonylimide salt (Li-TFSI); ethoxylated trimethylolpropane triacrylate (ETPTA); dimethylsulfoxid (DMSO), (S)-(+)-10-camphorsulfonic acid (CSA). The table was recompiled based on the review paper by Zhang et al.136 with additional information.
Zinc–air battery DMP 2811, Dimatrix Pyridine, polyurethane diol PEDOT Cathode 110
PEG LiCl/LiOH Electrolyte
Zinc–silver battery Customized super inkjet printing n-Tetradecane Silver nanopaste Electrode 98
Manganese battery Lexmark 3200 25 wt% PVDF-HFP, THF, 2 M NH4Cl 75 wt% MnO2 Electrode 117
Li–S battery DMP 2800, Dimatix CHP Sulfur infused SWNT-MET Cathode 34
LIB Canon BJC-1000sp printer Lomar D, carbon black, monoethanolamine, NaCMC LiCoO2 Cathode 113
LIB DMP 2800, Dimatix Triton X-100, glycerin LFP, carbon black, SCMC at 8[thin space (1/6-em)]:[thin space (1/6-em)]1[thin space (1/6-em)]:[thin space (1/6-em)]1 Cathode 19
LIB PICO Pμlse DI water, Triton X-100, NaCMC LFP, carbon black Cathode 20
LIB Canon BJC-1000sp AB, hyperdispersant (CH10B, CH12B), DI water/absolute ethanol/diethylene glycol/triethanolamine/IPA 56[thin space (1/6-em)]:[thin space (1/6-em)]18[thin space (1/6-em)]:[thin space (1/6-em)]5[thin space (1/6-em)]:[thin space (1/6-em)]1[thin space (1/6-em)]:[thin space (1/6-em)]1 by mass SnO2 Anode 114
LIB Canon BJC-1000sp AB, hyperdispersant (CH10B, CH12B), DI water/absolute ethanol/diethylene glycol/triethanolamine/IPA 56[thin space (1/6-em)]:[thin space (1/6-em)]18[thin space (1/6-em)]:[thin space (1/6-em)]5[thin space (1/6-em)]:[thin space (1/6-em)]1[thin space (1/6-em)]:[thin space (1/6-em)]1 by mass LTO Anode 115
LIB Piezoelectric printer Triton X 100, CMC, PAMA LFP, carbon black Electrode 112
LIB DMP 2800, Dimatix N/A PYR13-Li-TFSI Electrolyte 116
SC HP Deskjet 1010 inkjet printer 200 mg SDBS, 40 ml DI water MnO2, 200 mg MWCNT, 160 mg Ag Anode 108
200 mg SDBS, 40 ml DI water 200 mg MWCNT, 160 mg Ag Conductive pattern
SC DMP 2800, Dimatix N/A 2 mg ml−1 GO Electrode 118
SC DMP 2800, Dimatix N/A 2 mg ml−1 GO Electrode 119
MSC DMP 3000, Dimatrix Dispersant: ethanol Ag ink Current collector 120
K2Co3(P2O7)2·2H2O nanocrystal Anode
Graphene nanosheet Cathode
SC Epson Artisan 50 piezoelectric printer 1 wt% aqueous SDS in DI water 0.2 mg ml−1 SWNTs Electrode 121
MSC N/A 5% EG, PTFE, Triton-X 100 AC Electrode 122
SC Piezoelectric printer 200 mg SDBS and 100 ml water 200 mg NGP, 200 mg PANI Electrode 123
SC HP Deskjet 1010 1.0 wt% SDBS AC powder, SWNT Electrode 124
Water/IPA in 1[thin space (1/6-em)]:[thin space (1/6-em)]1 (v/v) Ag NW Current collector
N/A CNF suspension Substrate
ETPTA, ethanol or water IL: ([BMIM][BF4]) Electrolyte
MSC DMP 2800, Dimatix TBA·OH, H2O2, Triton X-100, EG, propylene glycol/water in 1[thin space (1/6-em)]:[thin space (1/6-em)]10 (M/M) δ-MnO2 nanosheet, 3–4% PEDOT Electrode 107
SC DMP 2800, Dimatix N/A GO 10 mg ml−1 Electrode 125
Ammonia, H2SO4, water/ethanol in 1[thin space (1/6-em)]:[thin space (1/6-em)]1 GH-PANI nanocomposite Electrode
SC EPSON L130 EG, NMP AC Cathode 56
NMP GO Substrate
NMP GO–MnO2 Anode
EG, NMP MnO2 Electrode
All-solid-state MSC N/A EG/PH1000, IPA Graphene, PEDOT:PSS Electrode 126
Transparent SC DMP 3000, Dimatrix Triton X-100, EG PEDOT:PSS, Ag grid Electrode 127
Negative SC Piezoelectric printer DMSO, CSA, TFMS PANI Tracks 128
MSC DMP 2800, Dimatrix Toluene, ethyl cellulose, DMF, ethanol, terpineol Graphene Electrode 101
Transparent MSC DMP 2800, Dimatrix Ethyl cellulose, terpineol/ethanol in 3[thin space (1/6-em)]:[thin space (1/6-em)]1 (v/v) Graphene nanosheet Electrode 129
SC HP Deskjet D2360 IPA, ethanol, DMF, ODCB, chloroform, water MWCNT Electrode 130
MSC MJ-AT-01, MicroFab EC, ethanol, NaCl, EG Graphene Electrode 70
PS-PMMA-PS, n-butyl acetate IL: [EMIM][TFSI] Electrolyte
SC N/A DI water rGO Electrode 131
MSC DMP 2800, Dimatrix EG GO/commercial pen ink 49[thin space (1/6-em)]:[thin space (1/6-em)]1 (v/v) Electrode 132
MSC Ceradrop X-Serie, DMC-11610 Cyclohexanone, terpineol, di(ethylene glycol)methyl ether 80[thin space (1/6-em)]:[thin space (1/6-em)]15[thin space (1/6-em)]:[thin space (1/6-em)]5 v/v Graphene, ethyl cellulose Electrode 133
MSC DMP 2800, Dimatrix N/A PEDOT:PSS – CNT/Ag Electrode 134
MSC DMP 2800, Dimatrix NMP, DMSO Ti3C2Tx MXene ink Electrode 82
MSC DMP 2800, Dimatrix DMF, EC, toluene[thin space (1/6-em)]:[thin space (1/6-em)]ethanol 80[thin space (1/6-em)]:[thin space (1/6-em)]20 Graphene Electrode 135
Poly(4-styrenesulfonic acid), EG, phosphoric acid PSSH Electrolyte


Table 2 Performance of various devices fabricated via inkjet printing
Devices Mechanical stability Cycle stability Max power density Max energy density Capacitance Potential window Ref.
Zinc–air battery N/A N/A N/A N/A Polyethylene naphthalate substrate 1.4 mA h cm−2 0–0.8 V 110
Paper-based 0.5 mA h cm−2
(Sandwich)
(Dimension N/A)
Zinc–silver battery N/A N/A 70 W h kg−1 3.95 mW h cm−2 N/A 1.1–2.0 V 98
(3D)
(9 mm2)
Manganese battery N/A N/A N/A N/A 270 mA h g−1 at 4.01 A g−1 −0.5–0.65 V 117
(N/A)
(0.5 cm × 0.7 cm)
Li–S battery N/A 100 cycle N/A N/A 800 mA h g−1 at C/2 1.6–2.8 V 34
87.5% retention (Sandwich)
(2 mm × 2 mm, 5 mm × 5 mm)
LIB N/A 100 cycles N/A N/A 120 mA h g−1 at 180 μA cm−2 3.0–4.2 V 113
95% retention 132 mA h g−1 at 64 μA cm−2
115 mA h g−1 at 192 μA cm−2
105 mA h g−1 at 394 μA cm−2
(Configuration N/A)
(0.5 cm2)
LIB N/A 30 cycle N/A N/A Al current collector 2.0–4.0 V 19
∼100% retention 129.9 mA h g−1 at 0.1C
CNT current collector
151.3 mA h g−1 at 0.1C
(Coin-type with thin film electrodes)
(Dimension N/A)
LIB N/A 100 cycle N/A N/A 140 mA h g−1 at 0.1C 0–1.0 V 20
98.2% retention 80 mA h g−1 at 6C
(Coin-type with thin film electrodes)
(12 mm diameter)
LIB N/A 50 cycle N/A N/A 812.7 mA h g−1 at 33 μA cm−2 0.05–1.2 V 114
30.78% (Coin-type with thin film electrodes)
(1.5 cm2)
LIB N/A 300 cycle N/A N/A 174 mA h g−1 at 10.4 μA cm−2 1.0–2.0 V 115
88% retention (Configuration N/A; thin film electrode)
(Dimension N/A)
LIB N/A 100 cycle N/A N/A 150 mA h g−1 at 1C 2.5–4.0 V 112
∼100% retention 125 mA h g−1 at 9C
∼90 mA h g−1 at 18C
<30 mA h g−1 at 45C
∼30 mA h g−1 at 90C
(Configuration N/A)
(Dimension N/A)
LIB N/A 100 cycle N/A N/A 60 mA h g−1 at C/10 2.0–4.1 V 116
∼100% retention (3D)
(10 mm diameter, 1 mm thick)
SC Bending to curvature of 10, 20, 30, and 40%, with a maximum change in electrical resistance of 25% 3000 cycles 512.1 mW cm−3 1.28 mW h cm−3 Overall device N/A 0–1.8 V 108
Bending at 20% curvature over 2000 cycles with less than 10% change in electrical resistance 96.9% retention MnO2–Ag-MWCNT anode 30.5 F cm−3 at 10 mV s−1
MnO2–Ag-MWCNT anode 4.1 F cm−3 at 1 V s−1
Filtrated MWCNT cathode 5.3 F cm−3 at 10 mV s−1
(Sandwich)
(1.5 cm × 1 cm)
SC Bending 350 cycles led to less than 5% capacitance 500 cycle 5.8 kW kg−1 2.6 W h kg−1 0.5 M H2SO4 electrolyte 124 F g−1 at 20 mV s−1 0–1 V 118
∼65% retention 10 kW kg−1 5 W h kg−1 1 M H2SO4 electrolyte 192 F g−1 at 20 mV s−1 0–1 V
19 kW kg−1 5.5 W h kg−1 BMIM BF4 electrolyte 73 F g−1 at 20 mV s−1 0–3 V
(Sandwich)
(3 cm × 3 cm)
SC N/A 1000 cycle 2.19 kW kg−1 6.74 W h kg−1 Device 125 F g−1 at 50 mV s−1 −0.6–0.4 V 119
96.8% retention Device 132 F g−1 at 0.01 V s−1
Device 48 F g−1 at 0.5 V s−1
(Configuration N/A)
(Dimension N/A)
MSC Bending from 0–180° with negligible change in performance 5000 cycle 54.5 mW cm−3 0.96 mW h cm−3 6.0 F cm−3 at 10 mA cm−3 0–0.6 V 120
94.4% retention (Planar)
(Dimension N/A)
SC N/A 1000 cycle 96 kW kg−1 18.8 W h kg−1 Overall 138 F g−1 0–1.0 V 121
∼100% retention 4.5 kW kg−1 8.2 W h kg−1 SWNT-PET electrode 65 F g−1
3.0 kW kg−1 6.1 W h kg−1 SWNT-fabric electrode 60 F g−1
(Sandwich)
(6 cm2)
MSC N/A N/A 44.9 mW cm−2 N/A 2.1 mF cm−2 0–2.5 V 122
(Planar)
(1.5 mm × 1 mm)
SC N/A 1000 cycle 124 kW kg−1 2.4 W h kg−1 NGP/PANI 82 F g−1 0–1.0 V 123
85.7% retention 132 kW kg−1 0.3 W h kg−1 NGP 10 F g−1
1000 cycle (Sandwich)
100% retention (Dimension N/A)
SC Bending hundreds of cycles at radius 1, 3, and 5 mm with negligible change in performance 10[thin space (1/6-em)]000 cycle N/A N/A 100 mF cm−2 0–2.0 V 124
∼100% retention (Planar)
(2 cm × 3 cm)
Solid-state MSC Bending at 120° (radius 1 cm) for 250 cycles, small crack occurs 3600 cycle 0.018 W cm−3 1.8 × 10−4 W h cm−3 2.4 F cm−3 at 0.05 A cm−3 0–0.8 V 107
88% retention (Planar)
(Dimension N/A)
SC Bending at 45, 90, and 180° with 1% decrease in capacitance, less than 2% decrease in capacitance after 100 bending cycle at 180° 1000 cycle 3202.4 W kg−1 24.02 W h kg−1 864 F g−1 at 1A g−1 0–0.8 V 125
96% retention (3D)
(Dimension N/A)
SC Bending from 0–360° with negligible change in performance, 98.4% retention rate after bending at radius 6 mm over 1000 cycles 9000 cycle 0.4 W cm−3 22 mW h cm−3 1023 F g−1 at 4 mA cm−2 0–2.0 V 56
89.6% retention (Sandwich)
(Dimension N/A)
All-solid-state MSC Bending over 1000 cycles with negligible change in performance 5000 cycle N/A N/A 5.4 mF cm−2 at 1 mV s−1 0–1.0 V 126
90% retention 2 mF cm−2 at 5 mV s−1
(Planar)
(2 cm × 3 cm)
Transparent SC Bending from 0, 60, 120, and 180° with negligible change in performance, however, electrical resistance increases as repeated deformation is present 5000 cycle 0.036 W cm−2 0.38 mW h cm−2 PEDOT:PSS SC 1.18 mF cm−2 0–0.8 V 127
83.7% retention 0.036 W cm−2 0.59 mW h cm−2 PEDOT:PSS electrode 4.72 mF cm−2
PEDOT:PSS/Ag SC 1.84 mF cm−2
PEDOT:PSS/Ag electrode 7.36 mF cm−2
(Sandwich)
(2 cm × 2 cm)
Negative SC N/A N/A N/A N/A −799 F g−1 N/A 128
(Configuration N/A)
(Dimension N/A)
MSC N/A N/A 8.8 mW cm−2 N/A 0.82 mF cm−2 at 10 mV s−1 −0.4–0.4 V 101
0.19 mF cm−2 at 100 mV s−1
(Planar)
(Dimension N/A)
Transparent MSC Bending at radius 7.5 and 5 cm with negligible change in performance, a 93.1 retention rate at the bending radius of 2.75 cm 10[thin space (1/6-em)]000 cycle N/A N/A 71% light transmittance 99 μF cm−2 0–1.0 V 129
91.3% retention 90% light transmittance 16 μF cm−2
(Planar)
(2 cm × 3.5 cm)
SC N/A 1000 cycle 2 ± 0.09 kW kg−1 4.5 ± 0.2 W h kg−1 ACN + TBAP 268 ± 12 F g−1 −0.5–1.5 V 130
90% retention
1000 cycle 1.1 ± 0.05 kW g−1 29.7 ± 1.2 W h kg−1 H2SO4 240 ± 10 F g−1 0–1.0 V
92% retention
1000 cycle 1.2 ± 0.05 kW kg−1 6.2 ± 0.2 W h kg−1 Na2SO4 233 ± 9 F g−1 −0.2–1.0 V
87% retention
1000 cycle 0.3 ± 0.03 kW kg−1 0.22 ± 0.02 W h kg−1 KOH 120 ± 11 F g−1 0–0.5 V
85% retention (Configuration N/A)
(Dimension N/A)
MSC Bending at radius of 1 cm over 1000 cycles with negligible change in performance 1000 cycle N/A N/A 268 μF cm−2 at 10 mV s−1 0–1.0 V 70
97% retention (Planar)
(2.22 mm × 0.46 mm)
SC Bending from 0–180° with negligible change in performance N/A 0.408 W cm−3, 25.5 kW kg−1 1.06 mW h cm−3, 63 W h kg−1 EMIMBF4 0.63 F cm−3, 39 F g−1 0–3.5 V 131
0.259 W cm−3, 16.2 kW kg−1 0.87 mW h cm−3, 54.2 W h kg−1 TEABF4 0.82 F cm−3, 51 F g−1 0–2.75 V
0.089 W cm−3, 5.6 kW kg−1 0.09 mW h cm−3, 6 W h kg−1 H2SO4 0.70 F cm−3, 43 F g−1 0–1 V
(Planar)
(1.75 mm × 1.89 mm)
MSC Bending at 90° for 500 cycles with negligible change in performance 10[thin space (1/6-em)]000 cycles 100% retention N/A N/A 19 μF cm−2 0–0.8 V 132
(Planar)
(1 cm × 1 cm)
MSC Bending at radius 2.5 mm for 5000 cycles with negligible change in performance, bending strain of 2.5% 10[thin space (1/6-em)]000 cycles 40.3 W cm−3 2.47 mW h cm−3 Full device 17.8 F cm−3 at 0.25 A cm−3 0–1.0 V 133
100% retention Electrode 71.2 F cm−3 at 0.5 A cm−3
(Sandwich)
(2.6 cm × 0.9 cm)
MSC Bending from 0–90° with negligible change in performance 10[thin space (1/6-em)]000 cycles 89.1 mW cm−3 42.1 mW h cm−3 23.6 F cm−3 0–0.9 V 134
92% retention (Planar)
(1.2 cm2)
MSC Bending for 0–150° over 1000 cycles with negligible change in performance, slight decrease in conductivity at 150° 10[thin space (1/6-em)]000 cycles 158 μW cm−2 0.32 μW h cm−2 562 F cm−3 0–0.5 V 82
100% retention (Planar)
(4 mm × 8 mm)
MSC N/A 11[thin space (1/6-em)]000 cycles 0.1 W cm−3 1 mW h cm−3 0.7 mF cm−2 0–1.0 V 135
77% retention (Planar)
(4 mm × 8 mm)


5. Inkjet printing of nanomaterials for flexible supercapacitors

Due to the unique characteristics such as low cost, high conductivity, porous structure, and excellent electrochemical stability, carbon-based materials, such as activated carbons (ACs), carbon nanotubes (CNTs), and graphene are the typical electrode materials for EDLCs.11,19 It should be noted that specific surfactants are needed for printing carbon-based material since most of these materials are not hydrophilic. For CNTs, sodium dodecyl sulfate (SDS) and sodium dodecyl benzene sulfonate (SDBS) is the typically dispersing agents.136 Metal oxides and conductive polymers are the primary materials for printing pseudocapacitors. For instance, manganese dioxide (MnO2), which has remarkable theoretical specific capacitance, natural abundance, low cost, and environment-friendliness, is one of the most investigated metal oxides for EES.56,107,117,130 Besides MnO2, ruthenium dioxide (RuO2) has also been primarily investigated for SCs.121 Characteristics such as excellent energy storage capability make polyaniline (PANI) and polypyrrole (PPy) the two typical conducting polymers for SCs. PEDOT is the most studied conducting polymer for flexible SCs due to its high conductivity and solution processability.11 However, these conductive polymer fibers lack mechanical strength and long-term stability, necessitating the integration of these polymers with other more stable conductive materials.

5.1 Inkjet printed flexible electric double layer capacitor (EDLC)

Le et al.119 demonstrated the fabrication of a graphene supercapacitor electrode via DOD method, using a piezoelectric printhead with the utilization of thermal reduction of graphene oxide (GO). In a separate study, Ervin and colleagues118 also reported the inkjet-printed flexible graphene-based SCs, where the electrodes were fabricated by inkjet printing GO ink onto the Kapton current collector. The authors identified the effects of the electrolytes, e.g., types and concentration, on the performance of printed SC devices. They revealed that printed devices using 1 M K2SO4 showed the highest capacitance, and the devices using ionic liquid BMIM BF4 exhibited the highest energy and power density. Ervin and colleagues also investigated the impacts of the annealing temperature on the device performance and found that a high annealing temperature could lead to enhanced capacitance in the printed devices. This study further provided valuable manufacturing knowledge for improving the performance of printed SC devices. Hyun et al.70 presented a unique fabrication technique that deposited graphene ink onto a UV-curable polymer molding, followed by a photonic annealing process utilizing an intense pulsed lamp (IPL) (Fig. 5a). The authors studied the effects of the various widths of the printed interdigital electrodes on the SC performance and concluded that the increased finger width would lead to improved performance. Hyun and colleagues further evaluated the manufacturability of their process by investigating the operation of 44 printed devices, which showed little variation in the device performance. Li and colleagues133 demonstrated a high-performance inkjet printed micro supercapacitor (MSC) using graphene ink. Various electrode thicknesses ranging from 30 to 2000 nm were investigated, and the result suggested that a printed electrode thickness of 40 nm led to the highest device performance. In another study, Pei et al.132 fabricated a hybrid ink by mixing GO ink and commercial pen ink for inkjet printing a solid-state MSC. Interestingly, the hybrid ink gave rise to a significant enhancement in the areal capacitance of the printed devices compared to the ones printed with pure GO ink. The study suggested that such improvement is likely due to the reduced ink agglomeration with the small amount addition of commercial pen ink.
image file: c9ta05239a-f5.tif
Fig. 5 (a) Illustration of an entire fabrication process demonstrated by Hyun et al. for graphene MSC.70 Reproduced with permission. Copyright 2017, Wiley-VCH; (b) schematic of an interdigital micro-supercapacitor.122 Reproduced with permission. Copyright 2010, Elsevier; (c) schematic illustration of a fully inkjet-printed SCs.124 Reproduced with permission. Copyright 2016, The Royal Society of Chemistry; (d) CV curve of the MSC under different bending angles at a scan rate of 20 mV s−1. Reproduced with permission.107 Copyright 2018, Elsevier; (e) illustration of a fully inkjet-printed GH-PANI supercapacitor. Reproduced with permission.125 Copyright 2014, American Chemical Society.

Besides graphene, activated carbon (AC) is also widely used for inkjet printing EDLCs. Pech et al.122 developed a carbon-based micro SC for a self-powered module by inkjet printing AC ink onto a silicon substrate with an Au current collector (Fig. 5b). The ink consists of a mixture of AC powder, PTFE polymer binder, ethylene glycol (EG), and surfactant. A 1 M Et4NBF4 propylene carbonate serves as the electrolyte, giving rise to a wide potential range of 0–2.5 V with a cell capacitance of 2.1 mF cm−2 for the printed device. Choi et al.124 demonstrated a fully printed device with multiple inkjet-printed components, including SWNT/AC as the active electrode materials, Ag nanowire ink for the current collector, cellulose nanofibril (CeNF) suspension as the primer layer on the paper substrate, and solid-state [BMIM][BF4]/ETPTA electrolyte (Fig. 5c). The incorporation of Ag nanowire (NW) into the SWNT network led to a significant improvement in the electrical conductivity of the inkjet-printed electrode. The printed device also showed excellent mechanical flexibility, with no significant degradation in the structural integrity or electrochemical performance after 1000 bending cycles. Ujjain et al.130 demonstrated the inkjet printing of highly conductive aromatic functionalized MWCNT for SC on flexible PET substrates. The authors performed a comprehensive investigation of various electrolytes and identified that ACN + TBAP electrolyte led to the largest capacitance and power density while H2SO4 electrolyte gave rise to the highest energy density of the printed devices. These findings are significant since the ACN + TBAP electrolyte could provide an alternative option to the highly acidic electrolyte. Jung et al.131 presented a printed electrode using rGO ink and found that the ionic liquid EMIMBF4 electrolyte led to the highest energy and power density, while the TEABF4 electrolyte induced the highest capacitance.

5.2 Inkjet printed flexible pseudocapacitor

Pseudocapacitive materials, e.g., metal oxides, metal sulfides and conducting polymers, are promising electrode materials since their capacitance generally far exceeds the double-layer capacitance achievable with carbon materials.137 The exploration of inkjet printed pseudocapacitor is still at its infancy. Wang et al.107 demonstrated a flexible solid-state MSC by inkjet printing δ-MnO2 nanosheets and PEDOT:PSS on a polyimide substrate. The authors explored the mitigation of the coffee-ring effect, a major issue occurring during the inkjet printing process, with the addition of propylene glycol. The printed pseudocapacitor device showed excellent mechanical flexibility with little degradation in the electrochemical performance after cyclic bending (Fig. 5d). The relationship between the thickness of the printed layer and the device performance was also examined. The result suggested that an optimal thickness existed for the device performance. Cheng et al.127 inkjet printed a transparent MSC using PEDOT:PSS/Ag grid as the active materials and compared the performance of the PEDOT:PSS/Ag and PEDOT:PSS electrodes. They found that the incorporation of Ag grid gave rise to the improved energy density, electrode capacitance, and overall device capacitance. Moreover, the flexible and transparent nature of the device also enhances the aesthetic appearance for better wearable experience with diversified functionality.

5.3 Inkjet printed flexible hybrid supercapacitor

A hybrid supercapacitor hybridizes the EDLCs and pseudocapacitors with the integration of carbon materials, conductive polymers, and metal oxides.54,138,139 Hybrid capacitors can be further grouped into three subcategories, i.e., asymmetric capacitors, battery-type capacitors, and composite capacitors. Pang et al.120 reported a high performance flexible solid-state asymmetric micro-supercapacitor, which has the potential to be integrated into roll-up display panels and power-on-chip systems. The device was fabricated through inkjet printing the graphene nanosheet and lamellar K2Co3(P2O7)2·2H2O nanocrystal whiskers, which are eco-friendly materials and synthesized under mild hydrothermal conditions. The device showed a high specific capacitance 6.0 F cm−3 with a high retention rate of 94.4% after 5000 cycles. The mechanical flexibility of the device was also evaluated, showing excellent deformability with large degree bending. Xu and colleagues123 demonstrate the inkjet-printed electrodes using the graphene/polyaniline (PANI) ink, with 1 M H2SO4 as the electrolyte. The graphene/PANI electrode showed excellent electrochemical performance and long cycle life. The authors also conducted a comparison between graphene/PANI and graphene electrodes, revealing that the presence of PANI led to a significantly improved energy density (2.4 W h kg−1) compared to the devices with only graphene electrodes (0.3 W h kg−1). It should be noted, though, the graphene/PANI electrode resulted in a slightly decreased power density (124 kW kg−1) compared to the case with graphene electrode (132 kW kg−1). In a separate study, Chi et al.125 demonstrated a fully inkjet-printed device using 3D porous graphene hydrogel/PANI nanocomposite with a gel electrolyte supported on graphene papers (Fig. 5e).

The inkjet printing of metal oxide nanomaterials has also been explored for fabricating flexible hybrid capacitors. Chen et al.121 employed an inkjet-printed SWNT/RuO2 nanowire (NW) thin-film electrode for flexible SCs, where the RuO2 NWs were synthesized through a chemical vapor deposition (CVD) method. The authors found that the SWNT/PET devices had a superior performance in terms of the capacitance, energy density, and power density. Such findings have important implications for future industrial manufacturing of flexible SC devices. The results of this study also suggested that the incorporation of RuO2 NW led to improved specific capacitance, power density, and energy density. Such understanding provides fundamental yet essential manufacturing knowledge such as the process–structure–property–performance relation for engineering the preparation of the materials and optimizing the inkjet printing process. Wang et al.108 presented an asymmetric capacitor through inkjet printing MnO2–Ag–MWCNT composites into the anode. A filtrated MWCNT cathode was fabricated using a vacuum filtration method with the addition of SDBD surfactant. The fabricated devices exhibited high capacitance, energy density, power density, and retention rate. The incorporation of the highly conductive nanomaterials here, i.e., Ag nanoparticles and MWCNT, helps mitigate the poor electrical conductivity of MnO2. Meanwhile, the integration of MnO2 helps enhance the capacitance and current density with better electron transfer of the Ag–MWCNT conductive network. The authors further evaluated the effects of the printed layer numbers on the device performance and revealed a negative correlation between the electrical resistance and the number of printed-layers (Fig. 6a). Sundriyal and Bhattacharya56 presented asymmetric SC electrodes on A4 papers through inkjet printing 40 layers of conducting GO ink on the paper surface. The anode was fabricated through depositing GO–MnO2 nanocomposite on the substrate; the cathode was made with deposited AC ink. Polyvinyl alcohol (PVA)–LiCl gel was used as the electrolyte. The devices showed outstanding mechanical flexibility and electrochemical performance, holding promise for future low-cost, flexible energy storage applications. The authors found that with the increased layer numbers, the electric charge density would increase for both GO–MnO2 and AC electrodes (Fig. 6b). A comparison between GO–MnO2 and MnO2 electrodes were provided, and the incorporation of the GO enhanced the capacitance of the nanocomposite, compare to MnO2 alone, as shown in Fig. 6c.


image file: c9ta05239a-f6.tif
Fig. 6 (a) The effect of the number printed layers on the electrical resistance of the devices. Reproduced with permission.108 Copyright 2015, The Royal Society of Chemistry; (b) the effect of the number printed layers on the electric of the charge density of the devices. Reproduced with permission.56 Copyright 2017, American Chemical Society; (c) incorporation of GO into MnO2 leads to higher capacitance. Reproduced with permission.56 Copyright 2017, American Chemical Society; (d) illustration of inkjet printing and extrusion printing of titanium carbide as a supercapacitor fabrication method. Reproduced with permission.82 Copyright 2019, Nature; (e) large-scale of fully inkjet printed MSC.135 Reproduced with permission. Copyright 2017, American Chemical Society; (f) intense pulse lighting setup for annealing graphene inkjet-printed film. Reproduced with permission.150 Copyright 2015, Wiley-VCH.

image file: c9ta05239a-f7.tif
Fig. 7 (a) Ragone plot of flexible energy storage devices fabricated via inkjet printing (per unit mass). Data is compiled from ref. 118, 119, 121, 123, 125, 130 and 131; (b) Ragone plot of flexible energy storage devices fabricated via inkjet printing (per unit volume). Data is compiled from ref. 56, 61, 108, 120, 127, 131 and 133–135.

6. Challenges and opportunities

Inkjet printing is a customizable, scalable, waste-free, and lean additive manufacturing process, which can enable seamless device fabrication and integration. Inkjet printing holds promises for scalable manufacturing of integrated, flexible electronic systems that consist of electronic components, sensors, energy units, and interconnects. However, the scientific nature of inkjet printing for nanomanufacturing wearable EES remains elusive, particularly on the ink formulation, substrate effect, spatial resolution, and sintering, which directly impact the productivity, yield, performance uniformity, and batch-to-batch reproducibility. More efforts are required to address the knowledge and technology gaps, at the material, device, and process levels, in the R&D status quo for inkjet printing of wearable EES. These challenges could be tackled through exploring and understanding the related process–structure–property–functionality relations. Such knowledge will enable the modeling, design, manufacturing, integration, and optimization of the inkjet printing process as an economically-viable option for future scalable nanomanufacturing of wearable EES and various other societally-pervasive technologies.

At the material level, the performance of EES largely depends on the electrode and electrolyte materials, which should be future explored particularly for the inkjet printing process since the performance of these printed devices is still less superior compared to traditional EES. More efforts are needed for exploring non-traditional active materials that are compatible with the inkjet printing, such as V2O5 and MoO2 for SCs, as well as LiNiMnCoO2 and lithium manganese (LiMn) for LIBs. The emerging materials such as PV2Mo10, PMo12, Cu-CAT, Ti3C2Tx, VN, Fe2N, and TiN, also provide new opportunities for research.55 Among the list of these emerging materials, Ti3C2Tx has been mostly investigated due to its high metallic conductivity, ion intercalation capability, and the surface hydrophilicity.81,83,140,141 A very recent study by Zhang et al. developed an additive-free 2D titanium carbide (Ti3C2Tx) MXene ink for MSC via inkjet printing and extrusion printing82 (Fig. 6d). The printed Ti3C2Tx MSC devices showed excellent performance metrics such as excellent retention rate (100% after 10[thin space (1/6-em)]000 cycles and 97% after 14[thin space (1/6-em)]000 cycles, respectively). Active materials should be carefully chosen, and the integration of different active materials could be effective in enhancing the electrical performance of the electrodes. The concentration of the electrolyte also impacts the device performance.118 The incorporation of solvents and surfactant can avoid particle agglomeration and mitigate the coffee-ring effect.107 The safety issues of the relevant electrolyte and active materials during the device operation should also be considered particularly for future wearable applications such as smart textile, biomedical, and implantable electronics.11 For instance, acidic electrolyte materials have been widely used for printing flexible EES devices, and they could cause significant issues if there is a leakage in the packaging. Many studies had explored alternative electrolyte materials for SCs, such as organic electrolyte or ionic liquid electrolyte, which not only give rise to superior device performance but also offer reduced toxicity compared to the traditional acidic electrolyte. Besides electrolyte, many widely used surfactants, e.g., DMF and NMP, for dispersing the nanomaterials during inkjet printing are also toxic.94 More efforts are required to explore and identify appropriate surfactant alternatives that are less or even non-toxic. Last but not least, active materials and electrolytes with inherent flexibility or even stretchability are of significant interests for the wearable EES applications.142–144

At the device level, the reported inkjet-printed flexible EES were dominant with the planar and sandwiched device configurations. More intriguing EES configurations such as 3D convoluted structures should be considered and implemented particularly for applications, e.g., smart textile. The self-cleaning and anti-fouling capability of the printed EES is another desired characteristics for the smart textile and implantable applications. Also, it would be desirable to integrate the advantages of both batteries and SCs for implementing flexible EES that possess simultaneously high energy and power densities with other characteristics such as fast charging rate, lightweight, excellent cycling stability, and long lifetime. New device concepts for EES could bring in unprecedented capabilities that transform the energy storage devices into other functional products, e.g., piezoelectric SCs, photo-SCs, shape-memory SCs, microbial SCs, electrochromic SCs, and self-healing SCs.55 Cai et al. also presented a study on the multifunctional smart window, where the anode and the cathode were fabricated via inkjet printing, and the device can be used as an electrochromic window and an energy storage unit.145

At the process level, a holistic process flow that integrates the unit processing modules, e.g., ink formulation, inkjet printing process, annealing, quality evaluation, and packaging, should be designed and standardized for specific EES applications. Standardization of the process can be challenging for inkjet printing of nanomaterial. Hyun et al. carried out efforts to explore the feasibility of inkjet printing for scalable manufacturing of EES with high yield and good uniformity (Fig. 6e).70 The preparation and formulation of the designer functional inks can be potentially scale-up given the versatility in materials synthesis. During the printing, additional energy input such as laser and UV light could be integrated in-line to provide new functionalities of the printed structures.146 The post-printing annealing of the print film can also be scaled up with the utilization of larger heating plates or other annealing techniques, such as chemical or photonic annealing process16 (Fig. 6f). Compared to the traditional annealing methods, photonic annealing using light sources ranging from infrared,147 UV,148 laser,16,149 and intense pulsed light70,150 could mitigate substrate damage due to excessive heating in the traditional methods, and makes possible the processing of flexible substrates that usually could not withstand the high temperature seen in the traditional annealing process. Further, photonic annealing enables rapid processing and treatment of the defects in the inkjet-printed films for improved electrical performance. More efforts are required, though, to better understand the light–matter interaction during the photonic annealing and its impacts on the active materials in the EES. Processing modules for in-line inspection should be designed and integrated so that real-time structural quality control is possible.151 Cracking of the printed film with mechanical deformation poses a significant failure mode for flexible EES applications. The incorporation of self-healing materials and structures into the EES presents a promising solution to address the cracking issue. Huang et al.152 demonstrated a self-healing SC capable of stretching over 3700% without the occurrence of a crack in the printed film. The material utilized was VSNPs–PAA, which is vinyl hybrid silica nanoparticles crosslinking into PAA chain. In another study, Wang et al.153 reported a manufacturing process for printing shape-memory polymer (SMP) composite using spray deposition followed by a hot-pressing process, which serves as both the annealing and compressing for the printed film to mitigate potential cracking. Last but not least, most reported studies only adopted the inkjet printing process for fabricating one of the device components, primarily the electrodes. To make possible future integrated manufacturing of fully printed flexible EES, more efforts are required for the material and process innovations.124,125

At the application level, the primary concerns are the mechanical stability, package leakage, and cycle stability. Wearable devices tend to be subjected to constant bending and deformation, which demands excellent mechanical stability of the devices. Another potential issue when implementing these devices is the leakage of the packaging since many devices utilized acidic solution as the electrolyte. However, this issue could be potentially addressed with organic electrolyte and ionic liquid electrolyte as replacements.

7. Summary and outlook

The flexible EES has emerged as not only a research topic of interests but also an area of far-reaching societal impacts. The economical manufacturing and integration of flexible EES with controlled properties and desired performance will provide significant opportunities in implementing novel wearable technologies that can operate sustainably. Among all the demonstrated approaches to fabricating EES, as have been reviewed in the previous sections, inkjet printing emerges as a potential economic method for nanomanufacturing wearable EES, due to its energy saving, cost-effectiveness, low working temperature, feasibility for scale-up production, and the potential for printing multifunctional materials into structures with controlled dimensions at designed locations. In order to realize the manufacturing and production potential of inkjet printed flexible EES, more efforts are required to reveal and identify the scientific nature of inkjet printing process for the hierarchical levels of materials, structures, and components in flexible EES, particularly on the ink formulation, ink–substrate interaction, spatial resolution of the printed pattern, post-printing annealing process, and process integration, which directly impact the production rate, yield, performance uniformity, and batch-to-batch reproducibility for future practical production and application of wearable EES. Further, the holistic hybridization of next-generation flexible EES with energy harvesting technologies154–157 is expected to usher in exciting opportunities in self-powered micro-/nano-systems that can scavenge and store the environmental energy through sustainable pathways. The rapid and exciting progress achieved in many emerging and “traditional” disciplines, e.g., nanomanufacturing, data science, material science, solid-state chemistry, and etc., are expected to excite a confluence of collective efforts from the research community and lead to more theoretical and experimental advances that would ultimately enable the scalable nanomanufacturing of inkjet printed wearable EES (Fig. 8).
image file: c9ta05239a-f8.tif
Fig. 8 The prospect and research opportunities of inkjet printing for the scalable nanomanufacturing of future wearable energy storage devices. Cited in a counterclockwise order taken from Credit: Islam Mosa/University of Connecticut and Maher El-Kady/UCLA; http://www.iot-now.com; http://www.flexenable.com; ref. 141 and 158; http://www.sackel.com; http://www.fujifilmusa.com; ref. 70, 125 and 159.

Conflicts of interest

The authors declare no competing financial interests.

Acknowledgements

W. Z. W. acknowledges the College of Engineering and School of Industrial Engineering at Purdue University for the startup support and the Ravi and Eleanor Talwar Rising Star Assistant Professorship. W. Z. W. was partially supported by the National Science Foundation under grant CMMI-1762698.

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