Enhancing electrochemical performance of graphene fiber-based

Mar 30, 2018 - The plasma treated GFSCs also exhibit ultrahigh rate capability (69.13% for 40 s plasma-treated ones) and superior cycle stability (96...
3 downloads 4 Views 6MB Size
Subscriber access provided by - Access paid by the | UCSB Libraries

Energy, Environmental, and Catalysis Applications

Enhancing electrochemical performance of graphene fiber-based supercapacitors by plasma treatment Jie Meng, Wenqi Nie, Kun Zhang, Fujun Xu, Xin Ding, Shiren Wang, and Yiping Qiu ACS Appl. Mater. Interfaces, Just Accepted Manuscript • DOI: 10.1021/acsami.8b04438 • Publication Date (Web): 30 Mar 2018 Downloaded from http://pubs.acs.org on March 30, 2018

Just Accepted “Just Accepted” manuscripts have been peer-reviewed and accepted for publication. They are posted online prior to technical editing, formatting for publication and author proofing. The American Chemical Society provides “Just Accepted” as a service to the research community to expedite the dissemination of scientific material as soon as possible after acceptance. “Just Accepted” manuscripts appear in full in PDF format accompanied by an HTML abstract. “Just Accepted” manuscripts have been fully peer reviewed, but should not be considered the official version of record. They are citable by the Digital Object Identifier (DOI®). “Just Accepted” is an optional service offered to authors. Therefore, the “Just Accepted” Web site may not include all articles that will be published in the journal. After a manuscript is technically edited and formatted, it will be removed from the “Just Accepted” Web site and published as an ASAP article. Note that technical editing may introduce minor changes to the manuscript text and/or graphics which could affect content, and all legal disclaimers and ethical guidelines that apply to the journal pertain. ACS cannot be held responsible for errors or consequences arising from the use of information contained in these “Just Accepted” manuscripts.

is published by the American Chemical Society. 1155 Sixteenth Street N.W., Washington, DC 20036 Published by American Chemical Society. Copyright © American Chemical Society. However, no copyright claim is made to original U.S. Government works, or works produced by employees of any Commonwealth realm Crown government in the course of their duties.

Page 1 of 36 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

ACS Applied Materials & Interfaces

Enhancing

electrochemical

performance

of

graphene

fiber-based

supercapacitors by plasma treatment Jie Meng1,2, Wenqi Nie1,2, Kun Zhang1,2*, Fujun Xu1,2, Xin Ding1,2, Shiren Wang3, Yiping Qiu1,2,4 1

Key Laboratory of Textile Science & Technology (Donghua University), Ministry of Education,

Shanghai 201620, PR China 2

3

College of Textiles, Donghua University, Shanghai 201620, PR China Department of Industrial and Systems Engineering, Texas A&M University, College Station, TX

77843, United States 4

College of Textiles and Apparel, Quanzhou Normal University, Fujian 362000, PR China

*Corresponding author. E-mail: [email protected]

Abstract Graphene fiber-based supercapacitors (GFSCs) hold high power density, fast charge/discharge rate, ultralong cycling life, exceptional mechanical/electrical properties and safe operation conditions, making them very promising to power small wearable electronics. However, the electrochemical performance is still limited by the severe stacking of graphene sheets, hydrophobicity of graphene fiber and complex preparation process. In this work, we develop a facile but robust strategy to easily enhance electrochemical properties of all-solid-state GFSCs by simple plasma treatment. We find that one-minute plasma treatment under ambient condition result in 33.1% enhancement of areal specific capacitance (36.25 mF/cm2) in comparison to the as-prepared GFSC. The energy density reaches 0.80 µWh/cm2 in PVA/H2SO4 gel 1

ACS Paragon Plus Environment

ACS Applied Materials & Interfaces 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

electrolyte and 18.12 µWh/cm2 in PVDF/EMIMBF4 electrolyte which is 22 times of that of as-prepared ones. The plasma treated GFSCs also exhibit ultrahigh rate capability (69.13% for 40 s plasma-treated ones) and superior cycle stability (96.14% capacitance retention after 20000 cycles for 1 min plasma-treated ones). This plasma strategy can be extended to mass-manufacture high-performance carbonaceous FSCs, such as graphene and carbon nanotube-based ones. Keywords: plasma, graphene fiber, supercapacitor, energy density, cycle stability Introduction In recent years, wearable energy conversion, storage devices and systems have attracted more and more attentions.1 Great efforts have been made in supercapacitors,2 solar cells,3 thermoelectric devices4-6 and rechargeable batteries.7 Among them, fiber-based supercapacitors (FSCs) are very promising due to their tiny volume, high power density, long cycle life, short charge/discharge time and safe operation conditions.8-11 In comparison to pseudocapacitors, carbonaceous FSCs (i.e. graphene based FSCs) possess high rate capability and ultralong cycle life thanks to the typical electrical double layer capacitive (EDLC) behavior. The ion transport and storage in FSCs are strongly associated with the specific surface area (SSA), accessible pore size distribution and the wettability of electrodes in electrolyte.12-13 Because of its extraordinary mechanical/electrical properties and high theoretical SSA (~2620 m2/g).14-15 graphene offers great potentials for FSCs. However, practical applications are still suffered from the ultralow specific capacitance and energy density. This is 2

ACS Paragon Plus Environment

Page 2 of 36

Page 3 of 36 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

ACS Applied Materials & Interfaces

assigned to the low SSA and improper pore size distribution. Very limited amount of graphene layers in graphene fibers contributes to the ion transport and storage. Due to graphene stacking, the lamellar structure along radical direction makes ions inaccessible and results in ultralong ion transport path. The ion transport is further reduced as graphene fiber gets thicker. Moreover, the hydrophobicity of graphene fiber makes it unfavorable for electrolyte penetration and adsorption, greatly limiting the interface between active materials and solvent.16 Therefore, fabricating porous graphene fibers with good wettability can provide sufficient ion transport channels and improve the active interfacial area for enhanced electrochemical (EC) performance.17 Many efforts have been made toward high-EC-performance GFSCs. A type of sheath-core graphene sponge@graphene fiber was prepared by electrochemically electrolyzing graphene oxide (GO) on graphene fiber in aqueous GO suspension. The GFSC demonstrates areal specific capacitance up to 1.2-1.7 mF/cm2, with the areal energy and power density of 0.04–0.17 µWh/cm2 and 6–100 µW/cm2, respectively.18 Hydrothermally reduced graphene oxide (rGO) nanosheets based FSC using Na2MoO4/polymer gel electrolyte shows a areal capacitance of 38.2 mF/cm2 and areal energy density of 5.3 µWh/cm2, respectively.19 Graphene/active carbon based FSCs show volumetric specific capacitance of 27.6 F/cm3, good cyclability with 90.4% retention after 10,000 cycles and good bendability with 96.8% retention after bending 1,000 times.20 A conformal Ni layer and rGO film were successively coated on the surface of common polyester yarns, the resultant symmetric yarn supercapacitor 3

ACS Paragon Plus Environment

ACS Applied Materials & Interfaces 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

achieved the areal specific capacitance of 72.1 mF/cm2 and stable cycling performances (96% for 10 000 cycles).21 Hierarchically mesoporous structured MnO2 nanowire(40 wt%)graphene hybrid fibers were fabricated,the FSC exhibits a volumetric capacitance of 66.1 F/cm3,excellent cycling stability of 96% capacitance retention after 10,000 cycles, high energy and power density at 5.8 mWh/cm3 and 0.51 W/cm3, respectively.22 Although significant progress has been made, facile and strategy for mass production of FSCs are still highly in need. Herein, we develop a scalable, fast and green but robust plasma method to fabricate graphene fibers with high SSA, tunable pore size distribution and high hydrophilicity without deteriorating their tensile properties (similar tensile strength but large elongation). Plasma can tune the intrinsic properties of carbon materials by rapidly and uniformly modifying the surface energy and morphology of graphene layers under physical and chemical interactions,23-24 including CNTs,25-26 graphite27 and graphene.28-32 The plasma treatment can not only change the surface roughness,33-38 but also introduce additional oxygen-contained groups which should be favorable for better wettability.23, 39 In this work, we report that one-minute air plasma treatment on graphene fibers leads to enhanced areal specific capacitance (36.25 mF/cm2) and energy density (18.12 µWh/cm2) of graphene fiber based supercapacitors, which is 22 times of that of GFSCs based on as-prepared graphene fibers. Experimental Graphite was purchased from Nanjing Xianfeng Nano, China. Potassium 4

ACS Paragon Plus Environment

Page 4 of 36

Page 5 of 36 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

ACS Applied Materials & Interfaces

permanganate (KMnO4), anhydrous ethanol, polyvinyl alcohol 1788 (PVA), hydrogen peroxide (H2O2) and calcium chloride (CaCl2) were purchased from Shanghai Lingfeng Chemical reagent Co., Ltd., China. Sulfuric acid (H2SO4, 98 wt%) and hydrochloric acid (HCl, 38 wt%) were purchased from Kunshan Jingke Microelectronics Material Co., Ltd., China. Phosphoric acid (H3PO4, 85 wt%), DMF (N,N-Dimethylformamide) were purchased from Sinopharm Chemical Reagent Co., Ltd., China. Polyvinylidene fluoride-co-hexafluoropropylene (PVDF) was purchased from Sigma-Aldrich. 1-ethyl-3-methylimidazolium tetrafluoroborate (EMIMBF4) was purchased from Titan. The materials were used as received without further purification. Deionized (DI) water was made with Master-Q15 (Resistivity ~ 18.3 MΩ*cm). Preparation of graphene oxide and graphene fiber Graphene oxide was made according to the reported literature.40-41 Graphene oxide dispersion was injected into the coagulation bath by syringe with an inner diameter of 260 µm. The coagulation bath contains 5 wt% CaCl2 in ethanol (volume ratio of ethanol to water is 1:3). Then continuous GO fibers were drawn out from the coagulation with roller under the infrared drying condition, then washed by DI water and ethanol, and winded onto a PTFE winder. The obtained graphene oxide fibers were dried in tension, followed by drying at 60 oC for 4 h in a vacuum oven. Graphene oxide fibers were reduced by the thermal annealing method at the temperature of 800 oC. Graphene oxide fibers were heated from room temperature to 300 oC at a rate of 10 oC/min and kept at the temperature for 30 minutes to reduce the 5

ACS Paragon Plus Environment

ACS Applied Materials & Interfaces 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

graphene oxide fibers partly. The partly reduced graphene oxide fibers were heated up to 800 oC at a rate of 4 oC/min and maintained at this temperature for 3 h. It is noted that the thermal annealing process was under the protection of high-purity nitrogen. The reduced graphene oxide fibers were washed by DI water and dried at room temperature. Plasma treated with reduced graphene fiber The graphene fibers were straightened on a self-made glass support, which was placed in the middle of the plasma chamber (Harrick plasma, Ithaca, NY) at 20W RF power, so that the fibers can be treated comprehensively with the plasma. Graphene fibers were treated with air plasma in ambient condition for a series of duration times (10 s, 20 s, 40 s, 1 min, 2 min, 3 min and 5 min). Preparation of all-solid-state GFSCs The PVA/H2SO4 gel electrolyte was prepared with the following method. Briefly, 1 g of PVA powder was added to mixture of 10 mL of deionized water. Subsequently, the mixture was heated to 90 oC under vigorous stirring for 30 min until the solution clarified. After cooling down to room temperature, 1 g of H2SO4 solution was added and stirred thoroughly. The organic electrolyte was prepared with the following steps: 189 mg polyvinylidene fluoride-co-hexafluoropropylene (PVDF) was added into 10 ml DMF and stirred for 1 hour, then 1.98 g 1-ethyl-3-methylimidazolium tetrafluoroborate (EMIMBF4) was added in. The assembled GFSC on flexible PET substrate consists of two parallel graphene fiber electrodes and electrolyte in between. Characterizations 6

ACS Paragon Plus Environment

Page 6 of 36

Page 7 of 36 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

ACS Applied Materials & Interfaces

Scanning electron microscope (SEM) of graphene fibers were obtained with low-/high-resolution scanning electron microscope (SEM, HITACHI, TM3000 and SU5000). Fourier transform infrared spectroscopy (FTIR) was tested with a Nicolet NEXUS-670. The wettability and contact angles of graphene fibers were conducted with a video-based optical contact angle measurement system (OCA 40 Micro, DataPhysics, Germany). The mechanical properties were recorded using the single fiber tension tester (XQ-2, Shanghai New Fiber Instrument). The electrical conductivities were measured with Keithley 2400 source-meter. The plasma treatment was performed on a Harrick cleaner (PDC-32G-2, Ithaca, NY). Raman spectra were collected with a Raman spectrometer using an excitation wavelength of 532 nm (inVia-Reflex). Electrochemistry test and BET results were calculated according to the paper as our group published before.42 Results and discussion

7

ACS Paragon Plus Environment

ACS Applied Materials & Interfaces 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

Figure 1. Schematic illustration exhibits the preparation method of graphene fiber and plasma treatment.

Figure 1 shows the roadmap of fabricating plasma-treated graphene fibers. The graphene oxide fiber (GOF) was wet-spun with the large graphene oxide (LGO) dispersion, and subsequently reduced by thermal annealing at high temperature. The resultant graphene fibers (GF) were straightened and placed on a glass support for further plasma treatment. Finally, two plasma treated graphene fibers (PGF) were placed in parallel and the PVA/H2SO4 gel electrolyte was casted between the fiber electrodes to form the GFSC.

8

ACS Paragon Plus Environment

Page 8 of 36

Page 9 of 36 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

ACS Applied Materials & Interfaces

Figure 2. SEM images of graphene fiber and plasma-treated graphene fiber. (a) The cross-sectional image of as-prepared graphene fiber. (b) The surface image of as-prepared graphene fiber. (c) The cross-sectional image of plasma-treated graphene fiber (1 min). (d) The surface image of plasma-treated graphene fiber. The as-prepared graphene fiber and plasma-treated graphene fiber were first characterized by scanning electron microscopy (SEM). Figure 2a and 2c are typical cross-sectional images of as-prepared and 1 min plasma-treated graphene fiber, respectively. The fiber is formed with graphene layers closely wrapped and stacked together with a diameter of ~31 µm. Figure 2b and 2d exhibit the surface image of control and plasma-treated graphene fibers, respectively. Typical rough and winkled surface in graphene fiber can be seen in both types, which may contribute to the SSA 9

ACS Paragon Plus Environment

ACS Applied Materials & Interfaces 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

of graphene fibers. Moreover, it is hard to detect significant differences of their surface morphology between as-prepared and plasma-treated graphene fibers.

Figure 3. Electrochemical performance of as-prepared graphene fiber and plasma-treated graphene fibers with different treated time. (a) CV curves at a scan rate of 5 mV/s. (b) The GCD curves at a current density of 0.1 mA/cm2. (c) Specific capacitance of as-prepared graphene fiber and plasma-treated graphene fiber at different current densities obtained from GCD tests. (d) Ragone plot of GFSCs under different plasma treatments. The electrochemical properties of resultant GFSCs are summarized in Figure 3. As shown in Figure 3a, all the CV curves demonstrate rectangular-like shape and a rapid current response to voltage reversal at each end potential, indicating the typical behavior of electrical double layer capacitor.43 Among them, the plasma-treated

10

ACS Paragon Plus Environment

Page 10 of 36

Page 11 of 36 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

ACS Applied Materials & Interfaces

graphene fibers with 40 s and 1 min show the largest CV areas compared with other graphene fibers (10 s, 20 s, 2 min, 3 min and 5 min), confirming the fiber electrode has better charge storage capability. Figure 3b shows the galvanostatic charge-discharge (GCD) behaviors of all samples at current density 0.1 mA/cm2. It is obvious that all curves show triangular shape with negligible electrode-potential drop (IR drop) for as-prepared graphene fiber (37.7 mV) and plasma-treated graphene fiber electrodes (9.2 mV, 10.2 mV, 8.1 mV, 18.8 mV, 17.5 mV, 33.8 mV, 27.6 mV for 10 s, 20 s, 40 s, 1 min, 2 min, 3 min and 5 min, respectively). This is probably owing to the low ion-transport resistance and short diffusion distance, which is beneficial to the charge storage capability for FSCs.44 The discharge time for as-prepared graphene fiber and plasma-treated graphene fibers are 106 s, 114.6 s, 119.6 s, 143.1 s, 144.9 s, 73.8 s, 49.3 s and 32.5 s for 10 s, 20 s, 40 s, 1 min, 2 min, 3 min and 5 min treatment, respectively. It is noteworthy that 1 min-plasma-treated graphene fiber possesses excellent symmetry and the longest discharge time which may result in higher CA than others. In addition, the charge curves of plasma-treated graphene fibers are symmetric to their corresponding discharge counterparts, demonstrating the high reversibility of GFSCs and the rapid charge transport between fiber electrodes. Figure 3c shows the areal specific capacitance CA based on GCD curves relative to the current density from 0.1 to 1 mA/cm2. The as-prepared graphene fiber based supercapacitors exhibit 26.55 mF/cm2 at 0.1 mA/cm2 which is comparable to reported values in literature.21, 45-46 Plasma treatment leads to higher CA up to 36.25 mF/cm2 for 11

ACS Paragon Plus Environment

ACS Applied Materials & Interfaces 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

1 min plasma treatment. This areal CA is 21 folds of that of sheath-core graphene sponge@graphene fiber (1.2-1.7 mF/cm2),18 41.8% higher than the as-prepared graphene fiber (21.1 mF/cm2),42 10.1% higher than that of hybrid GFSC based on MnO2/graphene core–sheath fiber and CNT/graphene fiber (32.6 mF/cm2),45 22 folds of that of FSC based on ZnO nanowires and graphene (1.6 mF/cm2),47 82 times of CVD graphene fiber (443 µF/cm2).15 However, longstanding plasma treatment can deteriorate the electrochemical performance of graphene fiber. For instance, 5 min plasma-treated graphene fiber-based supercapacitors shows the lowest specific capacitance of 8.13 mF/cm2, which is even much lower than that of as-prepared graphene fiber based ones. Moreover, it can be found that the plasma treatment can also enhance the rate capability of graphene fiber based supercapacitors. The 40 s plasma-treated sample holds the highest the capacitance retention of 69.18%, while further increasing the plasma treatment time dramatically deteriorates the capacitance retention. Figure 3d displays the Ragone plots for all GFSCs. The areal energy density increases to 0.80 µWh/cm2 for 1 min plasma-treated graphene fiber-based supercapacitor in PVA/H2SO4 gel electrolyte, which is 29% higher than that of as-prepared graphene fiber based supercapacitor (0.62 µWh/cm2). The energy density of all GFSCs follows a downtrend with respect to the power density. Interestingly, the 40 s plasma-treated GFSCs shows relatively flat EA-PA curve with the best energy density retention of 69.18%, while the rate capability of as-prepared GFSC (21.70%) is much worse than it. 12

ACS Paragon Plus Environment

Page 12 of 36

Page 13 of 36 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

ACS Applied Materials & Interfaces

Figure 4. (a) Nitrogen adsorption–desorption isotherm and (b) pore-size distribution of as-prepared graphene fiber and 1 min plasma-treated graphene fiber. (c) Different pore volume percentages of as-prepared graphene fiber and 1 min plasma-treated graphene fiber. (d) Optical microscopic images of water droplet on graphene fibers to determine contact angles. (left) the as-prepared graphene fiber; (right) plasma-treated graphene fiber. (e) Electrical conductivities of graphene fiber with different plasma treated times. (f) Nyquist plots from the EIS test for graphene fiber and plasma-treated graphene fiber. 13

ACS Paragon Plus Environment

ACS Applied Materials & Interfaces 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

To uncover the effect of plasma on the electrochemical enhancement of graphene fiber based supercapacitors, we conducted a series of characterizations, including BET, contact angle, electrical conductivity measurements and EIS test. The pore characteristics of plasma-treated graphene fibers were characterized by N2 absorption/desorption isotherm test. Figure 4a shows typical Type IV isotherms and mesoporous structures. The specific surface area (SSA) of 1 min plasma-treated graphene fiber is 253.32 m2/g, which is higher than that of as-prepared graphene fiber (221.05 m2/g). It should be notified that the 1 min plasma-treated graphene fibers are from the same batch as as-prepared graphene fibers. So, it suggests that the 1 min plasma treatment indeed increases the SSA of graphene fibers. Further analysis by plotting the pore size distribution (Figure 4b) and pore volume percentages (Figure 4c) provides more detailed information. As shown in Figure 4b, the 1 min plasma-treated graphene fiber shows a pore size distribution with 20.75% micropores, 70.66% mesopores and 10.84% macropores, while the as-prepared graphene fiber consists of 13% micropores, 86.14% mesopores and 3.1% macropores. It is clearly that the micro-porosity (20.75%) in 1 min plasma-treated graphene fiber is significantly improved as compared to as-prepared graphene fibers (13%). As we know, nanoporous carbons including micropores (0-2 nm) to mesopores (2-50 nm) are essential to the ion storage in carbonaceous materials.13 Micropores enhance the ion storage while mesoporous walls shorten ion pathways.48-49 More importantly, subnanometer pores (1 min) further increases, the electrochemical 15

ACS Paragon Plus Environment

ACS Applied Materials & Interfaces 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

performance of GFSCs (Figure 3) decreases dramatically, this should be related with the impropriate pore size distribution and suppressed electrical conductivity of graphene fiber electrodes probably due to the destruction of graphene fibers. Long plasma exposure will damage the graphitization of graphene layers, leading to reduced electrical conductivity and mechanical properties (Figure S1a). In Figure 4e, as the plasma treatment time is less than 1 min, the electrical conductivity slightly decreases from 35 S/cm (as-prepared graphene fiber) to ~25-30 S/cm for 1 min plasma treated graphene fiber. As the plasma treatment time further increases, the electrical conductivity is severely reduced to ~5-10 S/cm. Additionally, the mechanical properties of plasma treated graphene fibers (Figure S1a) are well retained after 40 s and 1 min plasma exposure, however, overlong exposure damages the tensile properties of graphene fibers. Figure S1e shows the Raman spectra of graphene fiber as control and 1 min plasma treated graphene fiber. Two obvious peaks at 1350 cm-1 and 1582 cm-1 characteristic of D and G bands coming from carbon materials clearly appear for both control graphene fiber and 1 min plasma treated graphene fiber. The D band intensity demonstrates the defect of the crystalline region. The G band stands for the regular sp2 carbon networks. The intensity ratio ID/IG is widely used for characterizing the defect quantity in graphitic materials.51-52 The intensity ratio ID/IG was increased from 1.013 to 1.203 after plasma treatment, demonstrating that the graphene fiber was effectively etched by plasma. Consequently, it can be stated that the plasma treatment has a synergistic effect on improving the electrochemical properties of graphene fiber-based supercapacitors 16

ACS Paragon Plus Environment

Page 16 of 36

Page 17 of 36 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

ACS Applied Materials & Interfaces

by tuning the pore size distribution with higher micro-porosity and enhancing the wettability in PVA/H2SO4 gel electrolyte.

Figure 5. Comparison of the areal (a) and volumetric (b) Ragone plots of our GFSCs with other fiber-based supercapacitors. Figure 5a shows the comparison of the areal energy densities and power densities of GFSCs in our work with other fiber-based supercapacitors based on SWCNTs/PANi, GF/3D-G and SWCNTs. 1 min plasma-treated GFSC exhibits the energy density of 0.80 µWh/cm2 in PVA/H2SO4 gel electrolyte as the areal power density is 0.02 mW/cm2. It is 9 times of that of SWCNTs yarn based FSC (0.09 µWh/cm2), 2 folds of SWCNTs/PANi based FSC (0.4 µWh/cm2),53 80 times of CVD-grown graphene fiber (0.0039 to 0.010 µWh/cm2),15 4 times of GF@3D-G supercapacitor

(0.04-0.17

µWh/cm2).18

We

further

applied

1

M

1-ethyl-3-methylimidazolium tetrafluoroborate (EMIMBF4)/polyvinylidene fluoride (PVDF)/N, N-dimethylformamide (DMF) gel electrolyte) to further increase the energy density by enlarging the working voltage.42 It shows high energy density (18.12 µWh/cm2) in organic gel electrolyte at a scanning rate of 5 mV/s, which is 22

17

ACS Paragon Plus Environment

ACS Applied Materials & Interfaces 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

Page 18 of 36

times higher than that in PVA/H2SO4 electrolyte. In figure 5b, the volumetric energy density was 0.895 mWh/cm3 in PVA/H2SO4 electrolyte, which is even comparable to RGO/MnO2/PPy

yarn

based

supercapacitor

(1.1

mWh/cm3),54

similar

to

PPy/RGO/MWCNT fiber based supercapacitor (0.94 mWh/cm3),55 lower than rGO/CNC hybrid fiber based supercapacitor (5.1 mWh/cm3),56 194 folds of wire shaped supercapacitor with CVD growth of graphene (0.0046 mWh/cm3).15 Specifically, it is worthy noted that the 1 min plasma treated GFSC exhibits extraordinary volumetric energy density of 10.296 mWh/cm3 in organic electrolyte.

Figure 6. (a) CV curves of the 1 min plasma-treated GFSC under bending. (b) GCD curves of the 1 min plasma-treated GFSC under different bending angles. (c) Digital photos of four pieces of 1 min plasma-treated GFSCs connected in-series after connected to LED. (d) Cycle stability of the 1 min plasma-treated GFSC.

18

ACS Paragon Plus Environment

Page 19 of 36 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

ACS Applied Materials & Interfaces

To verify the feasibility of our GFSCs in practice, we tested a GFSC system by assembling four pieces of 1 min plasma-treated GFSCs in-series. It was found that the CV (Figure 6a) and GCD (Figure 6b) curves of the as-assemble 1 min-GFSC under different bending angles are well maintained with very similar shape, suggesting its excellent flexibility. As shown in Figure 6c, the integrated GFSC can successfully power up a single piece of LED (Figure 6c), which has never been done by as-prepared GFSC. In Figure 6d, the assembled GFSC also exhibits excellent cycling performance with 96.1% capacitance retention after 20,000 GCD cycles, suggesting its outstanding stability with a long cycle life. Conclusions In summary, we report a very simple, green, fast but robust plasma treatment method to manufacture graphene fiber-based supercapacitors with high energy density (0.80 µWh/cm2 in PVA/H2SO4 gel electrolyte, 18.12 µWh/cm2 in PVDF/EMIMBF4 based gel electrolyte) in large scale. The ultrafast plasma treatment is found to enhance the electrochemical performance of GFSCs by simultaneously tuning the pore size distribution with high micro-porosity and enhancing hydrophilicity of graphene fiber electrodes. Compared to as-prepared GFSCs, the 1 min plasma-treated GFSC shows 33.1% higher specific capacitance (36.25 mF/cm2) at a current density of 0.1 mA/cm2 in PVA/H2SO4 electrolyte and very stable tensile property. The plasma-treated GFSCs also exhibit excellent cycling stability and flexibility. Acknowledgements We are grateful to the funding supports from the “DHU Distinguished Young 19

ACS Paragon Plus Environment

ACS Applied Materials & Interfaces 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

Page 20 of 36

Professor Program”, Key Laboratory of Textile Science & Technology (Donghua University), Ministry of Education (KLTST201606), the National Natural Science Foundation

of

China

(No.51603036),

and

Young Elite Scientists Sponsorship Program by CAST (2017QNRC001). We also acknowledge Prof. Ying Ma at the Donghua University for her technical support and helpful discussion on plasma treatment. Supporting Information Supporting Information Available: Typical stress–strain curve and FTIR spectra of as-prepared graphene fiber and plasma-treated graphene fiber. Digital photos of four pieces of 1 min plasma-treated GFSCs connected in-series. CV curves of GFSC devices in PVDF/EMIMBF4 electrolyte. Raman spectra of graphene fiber as control and 1 min plasma treated graphene fiber. XPS spectra of GOF (graphene oxide fiber) and 300-GOF (the graphene oxide fiber after 300 oC thermal reduction). References (1) Hu, Y.; Cheng, H.; Zhao, F.; Chen, N.; Jiang, L.; Feng, Z.; Qu, L. All-In-One Graphene

Fiber

Supercapacitor.

Nanoscale

2014,

6,

6448-6451,

DOI:

10.1039/c4nr01220h. (2) Gao, Y.-P.; Zhai, Z.-B.; Huang, K.-J.; Zhang, Y.-Y. Energy Storage Applications of Biomass-Derived Carbon Materials: Batteries and Supercapacitors. New Journal of

Chemistry 2017, 41, 11456-11470, DOI: 10.1039/c7nj02580g. (3) Kaltenbrunner, M.; White, M. S.; Glowacki, E. D.; Sekitani, T.; Someya, T.; Sariciftci, N. S.; Bauer, S. Ultrathin and Lightweight Organic Solar Cells with High 20

ACS Paragon Plus Environment

Page 21 of 36 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

ACS Applied Materials & Interfaces

Flexibility. Nature Communications 2012, 3, DOI: 10.1038/ncomms1772. (4) Zhang, K.; Wang, S.; Zhang, X.; Zhang, Y.; Cui, Y.; Qiu, J. Thermoelectric Performance of P-Type Nanohybrids Filled Polymer Composites. Nano Energy 2015,

13, 327-335, DOI: 10.1016/j.nanoen.2015.03.004. (5) Zhang, K.; Qiu, J.; Wang, S. Thermoelectric Properties of PEDOT Nanowire/PEDOT

Hybrids.

Nanoscale

8,

2016,

8033-8041,

DOI:

10.1039/c5nr08421k. (6) Zhang, K.; Wang, S. Thermal and Electronic Transport of Semiconducting Nanoparticle-Functionalized Carbon Nanotubes. Carbon 2014, 69, 46-54, DOI: 10.1016/j.carbon.2013.11.055. (7) Pushparaj, V. L.; Shaijumon, M. M.; Kumar, A.; Murugesan, S.; Ci, L.; Vajtai, R.; Linhardt, R. J.; Nalamasu, O.; Ajayan, P. M. Flexible Energy Storage Devices Based on Nanocomposite Paper. Proceedings of the National Academy of Sciences of the

United States of America 2007, 104, 13574-13577, DOI: 10.1073/pnas.0706508104. (8) Fu, Y.; Cai, X.; Wu, H.; Lv, Z.; Hou, S.; Peng, M.; Yu, X.; Zou, D. Fiber Supercapacitors Utilizing Pen Ink for Flexible/Wearable Energy Storage. Advanced

Materials 2012, 24, 5713-5718, DOI: 10.1002/adma.201202930. (9) He, N.; Pan, Q.; Liu, Y.; Gao, W. Graphene-Fiber-Based Supercapacitors Favor N-Methyl-2-Pyrrolidone/Ethyl

Acetate

as

The

Spinning

Solvent/Coagulant

Combination. Acs Applied Materials & Interfaces 2017, 9, 24568-24576, DOI: 10.1021/acsami.7b05982. (10) Wang, K.; Meng, Q.; Zhang, Y.; Wei, Z.; Miao, M. High-Performance Two-Ply 21

ACS Paragon Plus Environment

ACS Applied Materials & Interfaces 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

Page 22 of 36

Yarn Supercapacitors Based on Carbon Nanotubes and Polyaniline Nanowire Arrays.

Advanced Materials 2013, 25, 1494-1498, DOI: 10.1002/adma.201204598. (11) Meng, Q.; Wu, H.; Meng, Y.; Xie, K.; Wei, Z.; Guo, Z. High-Performance All-Carbon Yarn Micro-Supercapacitor for An Integrated Energy System. Advanced

Materials 2014, 26, 4100-4106, DOI: 10.1002/adma.201400399. (12) Salanne, M.; Rotenberg, B.; Naoi, K.; Kaneko, K.; Taberna, P. L.; Grey, C. P.; Dunn, B.; Simon, P. Efficient Storage Mechanisms for Building Better Supercapacitors. Nature Energy 2016, 1, DOI: 10.1038/nenergy.2016.70. (13) Jaeckel, N.; Simon, P.; Gogotsi, Y.; Presser, V. Increase in Capacitance by Subnanometer Pores in Carbon. Acs Energy Letters 2016, 1, 1262-1265, DOI: 10.1021/acsenergylett.6b00516. (14) Lin, T.; Chen, I. W.; Liu, F.; Yang, C.; Bi, H.; Xu, F.; Huang, F. Nitrogen-Doped Mesoporous Carbon of Extraordinary Capacitance for Electrochemical Energy Storage. Science 2015, 350, 1508-1513, DOI: 10.1126/science.aab3798. (15) Yu, J. L.; Wang, M.; Xu, P.; Cho, S. H.; Suhr, J.; Gong, K.; Meng, L. H.; Huang, Y. D.; Byun, J. H.; Oh, Y.; Yan, Y. S.; Chou, T. W. Ultrahigh-Rate Wire-Shaped Supercapacitor Based on Graphene Fiber. Carbon 2017, 119, 332-338, DOI: 10.1016/j.carbon.2017.04.052. (16) Sun, H.; Mei, L.; Liang, J.; Zhao, Z.; Lee, C.; Fei, H.; Ding, M.; Lau, J.; Li, M.; Wang, C.; Xu, X.; Hao, G.; Papandrea, B.; Shakir, I.; Dunn, B.; Huang, Y.; Duan, X. Three-Dimensional Ultrahigh-Rate

Holey-Graphene/Niobia

Energy

Storage.

Science

Composite 2017,

22

ACS Paragon Plus Environment

356

Architectures ,

599-604,

for DOI:

Page 23 of 36 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

ACS Applied Materials & Interfaces

10.1126/science.aam5852. (17) Chen, S.; Ma, W.; Xiang, H.; Cheng, Y.; Yang, S.; Weng, W.; Zhu, M. Conductive, Tough, Hydrophilic Poly(Vinyl Alcohol)/Graphene Hybrid Fibers for Wearable Supercapacitors.

Journal

of

Power

Sources

2016,

319,

271-280,

DOI:

10.1016/j.jpowsour.2016.04.030. (18) Meng, Y. N.; Zhao, Y.; Hu, C. G.; Cheng, H. H.; Hu, Y.; Zhang, Z. P.; Shi, G. Q.; Qu, L. T. All-Graphene Core-Sheath Microfibers for All-Solid-State, Stretchable Fibriform Supercapacitors and Wearable Electronic Textiles. Advanced Materials 2013, 25, 2326-2331, DOI: 10.1002/adma.201300132. (19) Veerasubramani, G. K.; Krishnamoorthy, K.; Pazhamalai, P.; Kim, S. J. Enhanced Electrochemical Performances of Graphene Based Solid-State Flexible Cable Type Supercapacitor Using Redox Mediated Polymer Gel Electrolyte. Carbon 2016, 105, 638-648, DOI: 10.1016/j.carbon.2016.05.008. (20) Ma, W. J.; Chen, S. H.; Yang, S. Y.; Chen, W. P.; Weng, W.; Zhu, M. F. Bottom-Up Fabrication of Activated Carbon Fiber for All-Solid-State Supercapacitor with Excellent Electrochemical Performance. Acs Applied Materials & Interfaces 2016, 8, 14622-14627, DOI: 10.1021/acsami.6b04026. (21) Pu, X.; Li, L.; Liu, M.; Jiang, C.; Du, C.; Zhao, Z.; Hu, W.; Wang, Z. L. Wearable Self-Charging Power Textile Based on Flexible Yarn Supercapacitors and Fabric Nanogenerators.

Advanced

Materials

2016,

28,

98-105,

DOI:

10.1002/adma.201504403. (22) Ma, W.; Chen, S.; Yang, S.; Chen, W.; Cheng, Y.; Guo, Y.; Peng, S.; Ramakrishna, 23

ACS Paragon Plus Environment

ACS Applied Materials & Interfaces 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

Page 24 of 36

S.; Zhu, M. Hierarchical MnO2 Nanowire/Graphene Hybrid Fibers with Excellent Electrochemical Performance for Flexible Solid-State Supercapacitors. Journal of

Power Sources 2016, 306, 481-488, DOI: 10.1016/j.jpowsour.2015.12.063. (23) Reis, R.; Dumee, L. F.; Tardy, B. L.; Dagastine, R.; Orbell, J. D.; Schutz, J. A.; Duke, M. C. Towards Enhanced Performance Thin-Film Composite Membranes via Surface Plasma Modification. Scientific Reports 2016, 6, DOI: 10.1038/srep29206. (24) Buonomenna, M. G.; Lopez, L. C.; Davoli, M.; Favia, P.; d'Agostino, R.; Drioli, E. Polymeric Membranes Modified via Plasma for Nanofiltration of Aqueous Solution Containing Organic Compounds. Microporous and Mesoporous Materials 2009, 120, 147-153, DOI: 10.1016/j.micromeso.2008.06.032. (25) Chen, J.-Z.; Wang, C.; Hsu, C.-C.; Cheng, I. C. Ultrafast Synthesis of Carbon-Nanotube Counter Electrodes for Dye-Sensitized Solar Cells Using An Atmospheric-Pressure

Plasma

Jet.

Carbon

2016,

98,

34-40,

DOI:

10.1016/j.carbon.2015.10.078. (26) Liu, L.; Ye, D.; Yu, Y.; Liu, L.; Wu, Y. Carbon-Based Flexible Micro-Supercapacitor Fabrication via Mask-Free Ambient Micro-Plasma-Jet Etching.

Carbon 2017, 111, 121-127, DOI: 10.1016/j.carbon.2016.09.037. (27) Chen, J.-Z.; Liao, W.-Y.; Hsieh, W.-Y.; Hsu, C.-C.; Chen, Y.-S. All-Vanadium Redox Flow Batteries with Graphite Felt Electrodes Treated by Atmospheric Pressure Plasma

Jets.

Journal

of

Power

Sources

2015,

274,

894-898,

DOI:

10.1016/j.jpowsour.2014.10.097. (28) Kim, H. J.; Jeong, H. K. Direct Reform of Graphite Oxide Electrodes by Using 24

ACS Paragon Plus Environment

Page 25 of 36 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

ACS Applied Materials & Interfaces

Ambient Plasma for Supercapacitor Applications. Chemical Physics Letters 2017, 686, 49-54, DOI: 10.1016/j.cplett.2017.08.039. (29) Kuok, F.-H.; Liao, C.-Y.; Wan, T.-H.; Yeh, P.-W.; Cheng, I. C.; Chen, J.-Z. Atmospheric Pressure Plasma Jet Processed Reduced Graphene Oxides for Supercapacitor Application. Journal of Alloys and Compounds 2017, 692, 558-562, DOI: 10.1016/j.jallcom.2016.09.056. (30) Liu, H.-W.; Liang, S.-p.; Wu, T.-J.; Chang, H.; Kao, P.-K.; Hsu, C.-C.; Chen, J.-Z.; Chou, P.-T.; Cheng, I. C. Rapid Atmospheric Pressure Plasma Jet Processed Reduced Graphene Oxide Counter Electrodes for Dye-Sensitized Solar Cells. Acs

Applied Materials & Interfaces 2014, 6, 15105-15112, DOI: 10.1021/am503217f. (31) Wan, T.-H.; Chiu, Y.-F.; Chen, C.-W.; Hsu, C.-C.; Cheng, I. C.; Chen, J.-Z. Atmospheric-Pressure Plasma Jet Processed Pt-Decorated Reduced Graphene Oxides for Counter-Electrodes of Dye-Sensitized Solar Cells. Coatings 2016, 6, DOI: 10.3390/coatings6040044. (32) Yang, C.-H.; Kuok, F.-H.; Liao, C.-Y.; Wan, T.-H.; Chen, C.-W.; Hsu, C.-C.; Cheng, I. C.; Chen, J.-Z. Flexible Reduced Graphene Oxide Supercapacitor Fabricated Using a Nitrogen Dc-Pulse Atmospheric-Pressure Plasma Jet. Materials

Research Express 2017, 4, DOI: 10.1088/2053-1591/aa5ed5. (33) Karahan, H. A.; Ozdogan, E. Improvements of Surface Functionality of Cotton Fibers by Atmospheric Plasma Treatment. Fibers and Polymers 2008, 9, 21-26, DOI: 10.1007/s12221-008-0004-6. (34) Zhang, Y.; Lu, Y.; Feng, S.; Liu, D.; Ma, Z.; Wang, S. On-Site Evolution of 25

ACS Paragon Plus Environment

ACS Applied Materials & Interfaces 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

Ultrafine ZnO Nanoparticles from Hollow Metal Organic Frameworks for Advanced Lithium Ion Battery Anodes. Journal of Materials Chemistry A 2017, 5, 22512-22518, DOI: 10.1039/c7ta08284c. (35) Tao, L.; Lin, C.-Y.; Dou, S.; Feng, S.; Chen, D.; Liu, D.; Huo, J.; Xia, Z.; Wang, S. Creating Coordinatively Unsaturated Metal Sites in Metal-Organic-Frameworks as Efficient Electrocatalysts for The Oxygen Evolution Reaction: Insights into The Active Centers. Nano Energy 2017, 41, 417-425, DOI: 10.1016/j.nanoen.2017.09.055. (36) Wang, Y.; Xie, C.; Zhang, Z.; Liu, D.; Chen, R.; Wang, S. In Situ Exfoliated, N-Doped, and Edge-Rich Ultrathin Layered Double Hydroxides Nanosheets for Oxygen Evolution Reaction. Advanced Functional Materials 2018, 28, DOI: 10.1002/adfm.201703363. (37) Wang, Y.; Zhang, Y.; Liu, Z.; Xie, C.; Feng, S.; Liu, D.; Shao, M.; Wang, S. Layered Double Hydroxide Nanosheets with Multiple Vacancies Obtained by Dry Exfoliation as Highly Efficient Oxygen Evolution Electrocatalysts. Angewandte

Chemie-International Edition 2017, 56, 5867-5871, DOI: 10.1002/anie.201701477. (38) Sun, H.; Zhang, Y.; Zhang, J.; Sun, X.; Peng, H. Energy Harvesting and Storage in 1D Devices. Nature Reviews Materials 2017, 2, DOI: 10.1038/natrevmats.2017.23. (39) Xiao, Z.; Wang, Y.; Huang, Y.-C.; Wei, Z.; Dong, C.-L.; Ma, J.; Shen, S.; Li, Y.; Wang, S. Filling the Oxygen Vacancies in Co3O4 with Phosphorus: An Ultra-Efficient Electrocatalyst for Overall Water Splitting. Energy & Environmental Science 2017, 10, 2563-2569, DOI: 10.1039/c7ee01917c. (40) Zheng, X.; Yao, L.; Mei, X.; Yu, S.; Zhang, W.; Qiu, Y. Comparing Effects of 26

ACS Paragon Plus Environment

Page 26 of 36

Page 27 of 36 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

ACS Applied Materials & Interfaces

Thermal Annealing and Chemical Reduction Treatments on Properties of Wet-Spun Graphene Fibers. Journal of Materials Science 2016, 51, 9889-9901, DOI: 10.1007/s10853-016-0222-z. (41) Marcano, D. C.; Kosynkin, D. V.; Berlin, J. M.; Sinitskii, A.; Sun, Z.; Slesarev, A.; Alemany, L. B.; Lu, W.; Tour, J. M. Improved Synthesis of Graphene Oxide. Acs

Nano 2010, 4, 4806-4814, DOI: 10.1021/nn1006368. (42) Zheng, X.; Zhang, K.; Yao, L.; Qiu, Y.; Wang, S. Hierarchically Porous Sheath-Core Graphene-Based Fiber-Shaped Supercapacitors with High Energy Density.

Journal

of

Materials

Chemistry

A

2018,

6,

896-907,

DOI:

10.1039/c7ta08362a. (43) Kou, L.; Huang, T.; Zheng, B.; Han, Y.; Zhao, X.; Gopalsamy, K.; Sun, H.; Gao, C. Coaxial Wet-Spun Yarn Supercapacitors for High-Energy Density and Safe Wearable Electronics. Nature Communications 2014, 5, DOI: 10.1038/ncomms4754. (44) Zhang, M. Synthesis, Characterization of Graphene and The Application of Graphene Carbon

Nanotube Composite in Fabricating Electrodes. 2015, 1-91.

(45) Zheng, B.; Huang, T.; Kou, L.; Zhao, X.; Gopalsamy, K.; Gao, C. Graphene Fiber-Based Asymmetric Micro-Supercapacitors. Journal of Materials Chemistry A 2014, 2, 9736-9743, DOI: 10.1039/c4ta01868k. (46) Chen, Q.; Meng, Y.; Hu, C.; Zhao, Y.; Shao, H.; Chen, N.; Qu, L. MnO2-Modified Hierarchical Graphene Fiber Electrochemical Supercapacitor.

Journal of Power Sources 2014, 247, 32-39, DOI: 10.1016/j.jpowsour.2013.08.045. (47) Bae, J.; Park, Y. J.; Lee, M.; Cha, S. N.; Choi, Y. J.; Lee, C. S.; Kim, J. M.; Wang, 27

ACS Paragon Plus Environment

ACS Applied Materials & Interfaces 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

Z. L. Single-Fiber-Based Hybridization of Energy Converters and Storage Units Using Graphene as Electrodes. Advanced Materials 2011, 23, 3446-3449, DOI: 10.1002/adma.201101345. (48) Wang, D. W.; Li, F.; Liu, M.; Lu, G. Q.; Cheng, H. M. 3D Aperiodic Hierarchical Porous Graphitic Carbon Material for High-Rate Electrochemical Capacitive Energy Storage. Angewandte Chemie-International Edition 2009, 48, 1525-1525, DOI: 10.1002/anie.200702721. (49) Hao, P.; Zhao, Z.; Leng, Y.; Tian, J.; Sang, Y.; Boughton, R. I.; Wong, C. P.; Liu, H.; Yang, B. Graphene-Based Nitrogen Self-Doped Hierarchical Porous Carbon Aerogels Derived from Chitosan for High Performance Supercapacitors. Nano Energy 2015, 15, 9-23, DOI: 10.1016/j.nanoen.2015.02.035. (50) Wu, H.; Yu, Y.; Gao, W.; Gao, A.; Qasim, A. M.; Zhang, F.; Wang, J.; Ding, K.; Wu, G.; Chu, P. K. Nickel Plasma Modification of Graphene for High-Performance Non-Enzymatic Glucose Sensing. Sensors and Actuators B-Chemical 2017, 251, 842-850, DOI: 10.1016/j.snb.2017.05.128. (51) Pimenta, M. A.; Dresselhaus, G.; Dresselhaus, M. S.; Cancado, L. G.; Jorio, A.; Saito, R. Studying Disorder in Graphite-Based Systems by Raman Spectroscopy.

Physical Chemistry Chemical Physics 2007, 9, 1276-1291, DOI: 10.1039/b613962k. (52) Ammar, M. R.; Galy, N.; Rouzaud, J. N.; Toulhoat, N.; Vaudey, C. E.; Simon, P.; Moncoffre, N. Characterizing Various Types of Defects in Nuclear Graphite Using Raman Scattering: Heat Treatment, Ion Irradiation and Polishing. Carbon 2015, 95, 364-373, DOI: 10.1016/j.carbon.2015.07.095. 28

ACS Paragon Plus Environment

Page 28 of 36

Page 29 of 36 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60

ACS Applied Materials & Interfaces

(53) Meng, Q.; Wang, K.; Guo, W.; Fang, J.; Wei, Z.; She, X. Thread-Like Supercapacitors Based on One-Step Spun Nanocomposite Yarns. Small 2014, 10, 3187-3193, DOI: 10.1002/smll.201303419. (54) Huang, Y.; Hu, H.; Huang, Y.; Zhu, M.; Meng, W.; Liu, C.; Pei, Z.; Hao, C.; Wang, Z.; Zhi, C. From Industrially Weavable and Knittable Highly Conductive Yarns to Large Wearable Energy Storage Textiles. Acs Nano 2015, 9, 4766-4775, DOI: 10.1021/acsnano.5b00860. (55) Wang, S.; Liu, N.; Su, J.; Li, L.; Long, F.; Zou, Z.; Jiang, X.; Gao, Y. Highly Stretchable and Self-Healable Supercapacitor with Reduced Graphene Oxide Based Fiber Springs. Acs Nano 2017, 11, 2066-2074, DOI: 10.1021/acsnano.6b08262. (56) Chen, G.; Chen, T.; Hou, K.; Ma, W.; Tebyetekerwa, M.; Cheng, Y.; Weng, W.; Zhu, M. Robust, Hydrophilic Graphene/Cellulose Nanocrystal Fiber-Based Electrode with High Capacitive Performance and Conductivity. Carbon 2018, 127, 218-227, DOI: 10.1016/j.carbon.2017.11.012.

29

ACS Paragon Plus Environment

ACS Applied Materials & Interfaces 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46

Page 30 of 36

Wet spinning

LGO PGF

Electrolyte Assembly

Plasma treatment

Silver PET substrate

PGF

Thermal annealing

GF

ACS Paragon Plus Environment

GOF

Page 31 of 36 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46

ACS Applied Materials & Interfaces

b

a

20 μm

c

30 μm

d

30 μm

20 μm

ACS Paragon Plus Environment

ACS Applied Materials & Interfaces 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46

ACS Paragon Plus Environment

Page 32 of 36

Page 33 of 36 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46

ACS Applied Materials & Interfaces

ACS Paragon Plus Environment

ACS Applied Materials & Interfaces 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47

ACS Paragon Plus Environment

Page 34 of 36

Page 35 of 36 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46

ACS Applied Materials & Interfaces

ACS Paragon Plus Environment

Plasma 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25

ACS Applied Materials & Interfaces

Porous graphene fiber

ACS Paragon Plus Environment

Page 36 of 36