Dongdong Yu
Zhihong Tang1*
Haiyong He- 1School of Materials Science and Engineering, University of Shanghai for Science and Technology, Shanghai, China
- 2Ningbo Institute of Materials Technology and Engineering, Chinese Academy of Sciences, Ningbo, China
Due to the high specific energy density, lithium-sulfur batteries (LSBs) have great potential in energy storage devices for electric vehicle and electronic equipment. However, poor conductivity of sulfur, large volume expansion, and lithium polysulfide dissolution limit LSBs application and promotion. In this work, graphitic hollow carbon fibers (HCF) were fabricated as a matrix to encapsulate sulfur. And nickel particles were introduced into fibers (Ni@HCF) to improve the cycle stability of sulfur cathode. On one hand, hollow structures can encapsulate sulfur and limit lithium polysulfides dissolution, and the graphitic carbon walls can provide a fast electron transport channel. On the other hand, nickel particles can accelerate the conversion of lithium polysulfides. The study results show that the initial discharge specific capacity of Ni@HCF/S cathodes reaches 1,252 mAh g−1 at the current density of 0.1C. And the capacity can be maintained at 558 mAh g−1 after 200 cycles at the current density of 1C.
Introduction
Lithium-sulfur batteries (LSBs), possessing a high energy density of 2,600 Wh kg−1 and merits of low cost and abundance of active materials, have been deemed as the most potential secondary batteries to satisfy the demand for high-density energy storage devices (Chen et al., 2018; Tian et al., 2020). However, there are still some problems impeding the commercial application of LSBs. For instance, the insulating nature of sulfur/lithium sulfide (Li2S) hinders effective utilization of active materials, tremendous volumetric expansion/shrinkage during sulfur lithiation/delithiation process causes electrode structure deterioration, and active material loss induced by dissolution of lithium polysulfides results in capacity rapid decay (Li et al., 2018; Pang et al., 2018; Wang et al., 2018).
Carbonaceous materials have been proposed and demonstrated as an effective strategy to solve the above problems and enhance the cycling ability of sulfur cathodes. The high electrical conductivity of carbonaceous materials can remedy the insulating nature of sulfur, improving the utilization of active materials. The large volume change during sulfur charge and discharge can be alleviated by the flexible properties of carbonaceous materials. The most prominent advantage of carbonaceous materials may be derived from the employment of porous carbon. The porous structure can encapsulate sulfur and limit the dissolution of lithium polysulfides. Therefore, microporous/mesoporous carbon (Bai et al., 2016; Du et al., 2016; Chen et al., 2017; Jiang et al., 2018), macroporous carbon (Wang et al., 2015; Tang et al., 2017), and carbon nanotubes (CNTs) (Liu et al., 2017b; Luo et al., 2018b; Xin et al., 2012) have been proved with a greatly improved lithium storage performance. Among these porous carbon materials, CNTs exhibit prominent merit in encapsulating sulfur (Jin et al., 2016). The hollow structure can provide a large void space for sulfur loading and restrain lithium polysulfides migration. However, weak affinity toward LiPSs and sluggish redox kinetics still impede sulfur-carbon composite material from achieving high performance (Balach et al., 2018). To meet such a requirement, various polar materials including metals (Zeng et al., 2018; Zhang et al., 2018), metal oxides (Tao et al., 2016; Li et al., 2019), and metal sulfides (Liu et al., 2017a; Zhang et al., 2019) have been developed as lithium polysulfide absorbents and catalysts to enhance the LiPS redox kinetics. Wu et al. decorated multiwalled carbon nanotubes with nickel for sulfur cathode and achieved improved cycling stability and excellent rate capacity (Wu et al., 2017). Therefore, encapsulating sulfur into metal decorated carbon nanotubes is a feasible strategy to achieve high-performance lithium-sulfur batteries.
Here, we prepared graphitic hollow carbon fibers (HCF) with nickel modified by electrospinning and chemical vapor deposition methods. As shown in Figure 1, Ni@Al2O3 fibers fabricated by electrospinning were used as a template to deposit graphitic carbon. Then, Al2O3 components were removed by etching leaving a hollow structure for sulfur loading. The graphitic HCF can compensate for the poor conductivity of sulfur as well as prevent lithium polysulfides dissolution. The nickel particles distributing in fibers can promote lithium polysulfide decomposition and improve the redox kinetics. This particular structure gives rise to the Ni@HCF/S cathodes an excellent electrochemical performance, which is better than that of HCF/S and C/S cathodes. The strategy provides a practicable way to fabricate metal decorated HCF that possess great potential application in the electrode structure design.
FIGURE 1. Schematic illustration of the synthesis strategy used to prepare the Ni@HCF/S.
Results and Discussion
Figures 2A,B show the SEM images of HCFs and Ni@HCFs. Both HCFs and Ni@HCFs exhibited three-dimensional network structures consisting of fibers with a diameter of ca. 300 nm. Nickel particles uniformly scattered in the tube of Ni@HCFs. The TEM images were captured to demonstrate the structural details of Ni@HCFs, the hollow structure of fibers can be observed clearly, and the nickel particles were distributed uniformly in the tube (Figure 2C). The HRTEM image reveals that the tube walls with a thickness of 15 nm and lattice spacing of 0.36 nm (Figure 2D) manifested a highly graphitic carbon of Ni@HCFs. Further, Raman spectrum was adopted to characterize the carbon structure of Ni@HCFs (Figure 3A). Three obvious peaks located at 1,348 cm−1, 1585 cm−1, and 2,694 cm−1 can be observed, corresponding to the D band, the G band, and the 2D band of carbon materials, respectively. The value of ID/IG ratio of Ni@HCFs is 0.64, and I2D/ID is 1.21. The Raman spectrum results indicate the highly ordered carbon of Ni@HCFs (Lee et al., 2018; Luo et al., 2018a). The crystal structure of Ni@HCFs was investigated by X-ray diffraction (XRD) measurements (Figure 3B). The observed diffraction peaks at 44.4, 51.7, and 76.1° can be attributed to nickel (111), (200), and (220) crystal plane, and the peaks at 26.2° can be assigned to the graphitic carbon of Ni@HCF. The graphitic carbon walls can enhance the electrical conductivity and improve sulfur utilization. The nickel particles can promote the decomposition of LiPSs and accelerate the redox kinetics. The chemical states of Ni@HCF were investigated by X-ray photoelectron spectroscopy (XPS). The high-resolution XPS spectrum (Figure 3C) of Ni 2p containing two peaks centered at 854.1 and 862.2 eV is attributed to the Ni species (Madhu et al., 2015; Zhong et al., 2018). Thermogravimetric Analysis (TGA) was conducted to confirm the sulfur content. As shown in Figure 3D, the sulfur content of Ni@HCF/S was 70.12%, which was appropriate for the sulfur cathode.
FIGURE 2. SEM images of HCF (A) and Ni@HCF (B). (C and D) TEM images of Ni@HCF.
FIGURE 3. (A) Raman spectra of HCF. (B) XRD spectra of Ni@HCF. (C) Ni 2P XPS spectrum of Ni@HCF. (D) TGA curves of Ni@HCF/S in N2.
The melt-diffusion method was performed to load sulfur. Figures 3A,B show the SEM and TEM images of Ni@HCF/S composite, respectively. Sulfur was encapsulated in HCF, and no sulfur particle can be observed outside the fibers. The elemental mapping was performed to gain more insight into the component of Ni@HCF/S. As shown in Figures 4C–F, the fibers are composed of C, Ni, and S elements, exhibiting homogeneous distribution. Encapsulating sulfur in HCF can suppress the shuttle effect and improve the cycle stability.
FIGURE 4. (A) SEM images of Ni@HCF/S. (B) TEM image of Ni@HCF/S. The insert shows the SAED image of Ni@HCF/S. (C) STEM image of Ni@HCF/S and corresponding elemental mapping of C (d), Ni(e) and S(f).
Electrochemical performances of Ni@HCF/S are investigated as cathode materials for LIBs. Figure 5A shows the cyclic voltammetry (CV) curves of the Ni@HCF/S cathode in the voltage window of 1.6–2.8 V at a scan rate of 0.1 mV s−1. In the first cathodic sweep, two obvious peaks can be observed at 2.22 and 2.02 V, which can be associated with the discharge of S8 forming soluble lithium polysulfides (Li2Sn, 4 ≤ n ≤ 8) and further discharge lithium polysulfides generating insoluble Li2S2/Li2S (Manthiram et al., 2014; Seh et al., 2016). In the anodic sweep, a sharp peak located at 2.46V can be attributed to oxidization of Li2S2/Li2S (Manthiram et al., 2013; Manthiram et al., 2015). The galvanostatic charge/discharge curves of Ni@HCF/S and HCF/S cathodes (Figure 5B) manifest two plateaus of conventional LSBs (He et al., 2018; Wang et al., 2020), corresponding to the results of CV curves well. Ni@HCF/S cathode possesses a higher initial discharge plateau and lower charge overpotential, indicating faster kinetics than HCF/S cathode. In the first cycle, the Ni@HCF/S cathode delivers a reversible capacity of 1,252 mAh g−1 at 0.1C, which means a high sulfur utilization of 74.7%. Figure 5C shows the rate performance of Ni@HCF/S, HCF/S, and S/C cathodes at 0.1, 0.2, 0.5, 1, and 2C. All the cathodes possess discharge capacities of more than 1,100 mAh g−1 and then the discharge capacities of HCF/S and S/C cathodes dropped drastically in the initial five cycles. But Ni@HCF/S cathode capacity declines slowly and stabilizes at 970 mAh g−1 at the fifth cycle. Then Ni@HCF/S cathodes delivered capacities of 844, 723, 608, and 428 mAh g–1 at 0.2, 0.5, 1, and 2°C, much higher than HCF/S and S/C cathodes. The Nyquist plots of the Ni@HCF/S, HCF/S, and S/C cathodes were obtained using impedance spectroscopy as shown in Figure 5D. All the curves are composed of a semicircle at high frequencies associated with the charge transfer resistance (Rct) at the electrode/electrolyte interface and a sloping line at low frequencies related to the Warburg impedance (W0) (Su and Manthiram, 2012). The Rct value of the Ni@HCF/S cathode was 82.4 Ω cm−2, less than that of HCF/S (127.6 Ω cm−2) and S/C (202.5 Ω cm−2) cathodes, showing that Ni@HCF/S cathode has a faster interface response due to the accelerated redox kinetics by nickel particles. As shown in Figure 5E, the cycling performances of Ni@HCF/S, HCF/S, and S/C cathodes were measured over 200 charging/discharging cycles at 1C. The initial discharge capacity of 857 and 780 mAh g−1 for CNT/S and S/C cathodes rapidly dropped to 634 and 540 mAh g−1 at the 20th cycle, respectively. Then, the capacities for HCF/S and S/C cathodes steadily decayed down to 423 and 297 mAh g−1, corresponding to 49.3 and 38.1% of the initial value at the 200th cycle, respectively. For the Ni@HCF/S cathode, the cycling performance was improved, showing 64.1% capacity retention from 871 to 558 mAh g−1 over 200 cycles. The improved performance of Ni@HCF/S cathode can be attributed to the encapsulation of sulfur into tubes alleviating the shuttle effect of lithium polysulfides and acceleration of redox kinetics by nickel species.
FIGURE 5. (A) CV curves of the Ni@HCF/S cathode at a scan rate of 0.1 mv·s−1. (B) Galvanostatic charge-discharge profiles of Ni@HCF/S and HCF/S cathodes at a rate of 0.1C. (C) Rate performance and (D) Nyquist plots of the Ni@HCF/S, HCF/S, and C/S cathodes. (E) Long-term cycling stability of the Ni@HCF/S, HCF/S, and C/S cathodes at 1C for 200 cycles.
Conclusion
In summary, nickel decorated graphitic HCF are proved to be a potential structure for sulfur loading in LSBs. The graphitic walls of carbon tube increase the conductivity of composites; meanwhile, tube structure can encapsulate sulfur avoiding lithium polysulfides dissolution. Additionally, the nickel particles can promote the conversion of lithium polysulfides. The prepared Ni@HCF/S cathodes occupied a lower charge transfer resistance and maintained a capacity of 558 mAh·g−1 after 200 cycles at a rate of 1C, showing superior performance than HCF/S and C/S cathodes.
Experimental Section
Fabrication of Ni@HCF
Typically, 0.04 mol aluminum power (Sigma-Aldrich) was added to a 30 ml aqueous solution containing 6.7 ml formic acid (Sigma-Aldrich) and 7.0 ml acetic acid (Sigma-Aldrich). The mixture was heated to 70°C and reacted for 12 h; after cooling down naturally, impurities were removed by filtration. 0.2 g PEO and 0.4 g nickel nitrate (Sigma-Aldrich) were dissolved in the obtained solution to form a homogeneous solution for the electrospinning process. Al2O3 fiber templates were obtained by heating the electrospinning product at 500°C for 2 h. Subsequently, the chemical vapor deposition method was performed to grow carbon on the surface of Al2O3 fiber templates under the temperature of 1,100°C and the methane flow of five sccm for 20 min. Finally, the Ni@HCF was obtained by etching the Al2O3 component with NaOH. The HCF was fabricated by the same route without the addition of nickel nitrate.
Fabrication Composites Cathodes
The Ni@HCF/S composites were prepared through a melt-diffusion method. Typically, the prepared Ni@HCF and sublimed sulfur were ground together by a mass ratio of 7:3. And the mixture was transferred into an argon-filled autoclave and heated to 155°C for 12 h. Then, the slurry containing 80 wt% active materials, 10 wt% Super P, and 10 wt% poly(vinylidene fluoride) binder was cast on Al foil. At last, the slurry cast Al foil was punched into disks with a diameter of 12 mm. The sulfur loading of the disk was about 1.1 mg cm−2. HCF/S and C/S cathodes were fabricated by the same route with HCF and active carbon, respectively.
Cell Assembly and Test
CR2032 type coin cells were assembled with carbon-sulfur composite cathodes, single-layer PP separators, and lithium foil as the anode part. 40 μL of electrolyte composed of 1 M lithium bis(trifluoromethanesulfonyl)imide (LiTFSI) and 1 wt% lithium nitrate (LiNO3) into 1,3-dioxolane (DOL) and 1,2-dimethoxyethane (DME) (volume ratio, 1:1) was added, and the assembly process was performed in an argon-filled glove. Cyclic voltammogram (CV) curves, a voltage window of 1.6–2.8 V, were measured with a potentiostat/galvanostat 1470E from Solartron at a scan rate of 0.1 mV S−1. The galvanostatic charge-discharge cycling test was performed with a LAND battery test system. Electrochemical impedance spectroscopy (EIS) measurements were carried out using a frequency response analyzer 1455A from Solartron. The impedance spectra were recorded on cells in variable frequency form 106 Hz and 0.1 Hz with an amplitude of 10 mV.
Material Characterizations
Bruker D8 advanced diffractometer with Cu Kα (λ = 1.5406 Å) radiation (Bruker AXS, D8 Advance) was used to identify the crystalline phase of the prepared samples. SEM (FEI, QUANTA 250 FEG) and TEM (FEI, Tecnai F20) were employed to analyze the surface morphology and interior structure. Renishaw inVia reflex Raman spectrometer with an excitation wavelength of 532 nm was adopted to collect Raman spectra of the prepared samples.
Data Availability Statement
The original contributions presented in the study are included in the article/Supplementary Material; further inquiries can be directed to the corresponding author.
Author Contributions
DY carried out the experiment and wrote the manuscript with support from HH and ZT. All authors discussed the results and contributed to the final manuscript.
Funding
This work was financially sponsored by the Basic Research Program of Shanghai (19JC1410402), the Scientific Research and Innovation Program of Shanghai Education Commission (2019-01-07-00-07-E00015), the Hundred Talents Program, the National Natural Science Foundation of China (Grant No. 51872304), and the Ningbo S&T Innovation 2025 Major Special Program (2018B10024).
Conflict of Interest
The authors declare that the research was conducted in the absence of any commercial or financial relationships that could be construed as a potential conflict of interest.
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Keywords: lithium-sulfur batteries, hollow carbon fibers, graphitic carbon, nickel decoration, lithium polysulfide
Citation: Yu D, Tang Z and He H (2021) Encapsulating Sulfur Into Nickel Decorated Hollow Carbon Fibers for High-Performance Lithium-Sulfur Batteries. Front. Energy Res. 8:606529. doi: 10.3389/fenrg.2020.606529
Received: 15 September 2020; Accepted: 31 December 2020;
Published: 24 February 2021.
Edited by:
Ya You, Wuhan University of Technology, ChinaReviewed by:
Sen Xin, Institute of Chemistry (CAS), ChinaYuesheng Wang, Hydro-Québec’s Research Institute, IREQ, Canada
Maowen Xu, Southwest University, China
Copyright © 2021 Yu, Tang and He. This is an open-access article distributed under the terms of the Creative Commons Attribution License (CC BY). The use, distribution or reproduction in other forums is permitted, provided the original author(s) and the copyright owner(s) are credited and that the original publication in this journal is cited, in accordance with accepted academic practice. No use, distribution or reproduction is permitted which does not comply with these terms.
*Correspondence: He Haiyong, aGVoYWl5b25nQG5pbXRlLmFjLmNu; Zhihong Tang, emh0YW5nQHVzc3QuZWR1LmNu