Open Access Article
This Open Access Article is licensed under a Creative Commons Attribution-Non Commercial 3.0 Unported Licence

Flexible quasi-solid-state zinc ion batteries enabled by highly conductive carrageenan bio-polymer electrolyte

Yuan Huang a, Jiuwei Liua, Jiyan Zhanga, Shunyu Jinb, Yixiang Jiangc, Shengdong Zhanga, Zigang Lic, Chunyi Zhid, Guoqing Due and Hang Zhou*a
aSchool of Electronic and Computer Engineering, Peking University Shenzhen Graduate School, Shenzhen 518055, PR China. E-mail: zhouh81@pkusz.edu.cn
bCenter for Micro- and Nanoscale Research and Fabrication, University of Science and Technology of China, Hefei, PR China
cState Key Laboratory of Chemical Oncogenomics, School of Chemical Biology & Biotechnology, Peking University Shenzhen Graduate School, Shenzhen 518055, Guangdong, China
dDepartment of Materials Science and Engineering, City University of Hong Kong, 83 Tat Chee Avenue, Kowloon, Hong Kong 999077, China
eZinergy Shenzhen Limited, Taohuayuan Science Park, Shenzhen 518101, China

Received 13th February 2019 , Accepted 17th May 2019

First published on 24th May 2019


Abstract

Flexible Zn–MnO2 batteries as wearable electronic power source have attracted much attention in recent years due to their low cost and high safety. To promote the practical application of flexible Zn–MnO2 batteries, it is imperative to develop flexible, mechanically robust and high performance solid state electrolyte. Herein, we construct a rechargeable quasi-solid-state zinc ion battery using kappa-carrageenan bio-polymer electrolyte. The kappa-carrageenan electrolyte is eco-friendly, low cost, and highly conductive (3.32 × 10−2 S cm−1 at room temperature). The mechanical robustness of kappa-carrageenan electrolyte is further reinforced by using a rice paper as scaffold. Benefiting from high ionic conductivity of the bio-polymer electrolyte, our zinc ion battery delivers a significant high energy density and power density (400 W h kg−1 and 7.9 kW kg−1, respectively), high specific capacity (291.5 mA h g−1 at 0.15 A g−1), fast charging and discharging capability (120.0 mA h g−1 at 6.0 A g−1). The zinc ion battery with bio-polymer electrolyte also shows excellent cycling stability and high bending durability. This work brings new research opportunities in developing low-cost flexible solid-state zinc ion batteries using green natural polymer.


1. Introduction

In recent years, the rapid development of flexible electronics has triggered a huge research demand on flexible power sources. A lot of important work on flexible-based energy storage devices has been reported.1–4 As the flexible or wearable electronics are usually closely attached to human body, one would expect the flexible batteries to have higher safety and environmental standards than other batteries. In this regard, aqueous electrolyte based zinc ion batteries (ZIBs) have drawn a lot of interest not only because they are highly reliable and environmentally friendly, but also because of the abundance of the raw materials, such as Zn sources.5–12 Conventionally, neutral or mildly acidic sulfate salt aqueous solutions such as ZnSO4 solution are employed in ZIBs as their electrolytes. Compared to other salts, the sulfate salt solution provides higher ionic conductivity and larger electrochemically stable window.13 More importantly, the recharge ability of aqueous Zn–MnO2 batteries can be significantly improved by optimizing the amount of MnSO4 salt in the ZnSO4 aqueous electrolyte.14 Nonetheless, aqueous based electrolyte in the battery of this kind is likely to leak under mechanical stress such as bending or stretching, leading to degradation or failure of the batteries. To further promote the ZIBs for wearable or flexible electronics application, it is very critical to develop exclusive ZIBs solid-state electrolytes which can avoid electrolyte leakage while maintaining high flexibility.

So far, several types of zinc ion conducting polymer electrolytes have been invented, such as electrolytes based on ZnCl2/polyvinyl-alcohol (PVA) gel-like electrolyte, and ZnTf2 in combination with poly(vinilydenefluoride-co-hexafluoropropylene).15,16 Nonetheless, the ZIBs based on the former ZnCl2/PVA electrolyte showed very narrow voltage plateaus,13 while the later one, ZnTf2 based electrolyte, suffers from low ionic conductivity (3.82 × 10−3 S cm−1).16 It is only until recently that high conductive zinc ion solid-state electrolyte for wearable ZIBs has been reported. Examples include a gelatin and PAM based hierarchical polymer electrolyte17 and ZnSO4/MnSO4/xanthan gum electrolyte,13 which exhibit high ionic conductivities of 1.76 × 10−2 and 1.46 × 10−2 S cm−1, respectively. Inspired by the above previous works, in an attempt to further minimize the manufacturing cost and environmental impact, we initialize an investigation on bio-degradable solid-state electrolytes with high zinc ion conductivity, and with easy fabrication process.

Herein, we utilize kappa-carrageenan, a natural polymer which has been widely used in biomedical and food application,18 to form solid-state ZnSO4/MnSO4 electrolyte and achieve highly flexible ZIBs with MnO2-based hybrid cathodes. The structure of kappa-carrageenan (Fig. 1a), with formula of C24H36O25S2−2, is consist of alternating 3-linked β-D-galactose-4-sulfate and 4-linked 6-anhydro-α-galactopyranose having one negative charge per disaccharide repeating unit.19 The structure of kappa-carrageenan consists of hydroxyl groups, which enables the formation of coordinate bonds with cations. It is abundant in nature, non-toxic, renewable, biocompatible, and cost effective compared to synthetic polymers.20 A few works have been reported in literature to make polymer electrolytes using kappa-carrageenan, such as biopolymer electrolytes based on carboxymethyl kappa-carrageenan and ionic liquid 1-butyl-3-methylimidazolium chloride,21 biopolymer blend based on kappa-carrageenan and cellulose derivatives,22 which exhibit ionic conductivities of 5.76 ± 0.20 × 10−3 and 3.25 × 10−4 S cm−1, respectively. Moreover, kappa-carrageenan also has been used as electrolyte for energy storage devices (e.g. supercapacitors,23,24 and Al/air batteries25), where they achieve solid-state electrolyte with mechanical stability or high values of ionic conductivities. In the present work, the preparation of the bio-polymer electrolyte was completed by dissolving kappa-carrageenan in aqueous ZnSO4/MnSO4 solution, and filled the solution in the network of rice paper. The biopolymer electrolyte with rice paper is denoted as KCR electrolyte. The rice paper is adopted to effectively reduce the chances of short circuit as well as improve the mechanical robustness of solid-state electrolyte. The KCR electrolyte fabrication process is simple and efficient. It does not need water and oxygen-free environment or other protection measures, which is ideal for scaling up production. The KCR electrolyte maintains remarkable flexibility and exhibits an ultra-high ionic conductivity of 3.32 × 10−2 S cm−1 at room temperature, one of the best record reported so far for ZIBs solid-state electrolyte. The ZIBs with KCR demonstrates a high specific capacity of 291.5 mA h g−1 at 0.15 A g−1, fast charging and discharging capability (120.0 mA h g−1 at 6.0 A g−1), good cycling stability, and high reliability bearing cycles of bending.


image file: c9ra01120j-f1.tif
Fig. 1 (a) The molecular formula of kappa-carrageenan. (b) Photograph of kappa-carrageenan electrolyte after adding 2 M ZnSO4 and 0.1 M MnSO4 aqueous solutions. (c) FTIR spectra of pure kappa-carrageenan polymer and ZnSO4/MnSO4 added kappa-carrageenan electrolyte. (d) SEM image of KCR electrolyte. (e) The cross-sectional SEM image of KCR electrolyte. (f) AC impedance spectra of the kappa-carrageenan electrolyte without rice paper and the KCR electrolyte. Inset in (f): photograph of a folded KCR electrolyte sample.

2. Experimental

2.1. Preparation of KCR electrolyte, cathode and anode

1 g pristine kappa-carrageenan (Aladdin) was added into 5 mL the mixture solution of 2 mol L−1 ZnSO4 (AR grade, Mcaklin) and 0.1 mol L−1 MnSO4 (AR grade, Mcaklin), followed by intensive stirring at room temperature until the kappa-carrageenan was dissolved. After that, rice paper was immersed into the mixture. Kappa-carrageenan based hydrogel was formed in the rice paper pores after solidification, and a KCR film with good flexibility was obtained.

The MnO2 nanosheets were synthesized by a hydrothermal method and the MnO2/reduced graphene oxide (MnO2/rGO) electrodes were prepared using a vacuum filtration method.26 Zn was deposited on carbon cloth by an electrodeposition method.15 The mass loading of MnO2 is 3 mg cm−2. The mass loading of the cathode (including MnO2, rGO, and carbon cloth) is 17.75 mg cm−2. The mass loading of the anode (including electroplated Zn and carbon cloth) is 23.51 mg cm−2.

2.2. Structure and morphology characterization

The morphologies were characterized by a field-emission scanning electron microscope (FESEM, Zeiss SUPRA-55). Transmission electron microscopy (TEM) measurements were also carried out with a Tecnai F20 (FEI) microscope operating at 200 kV. The crystallinity and phases of the samples were examined by X-ray diffraction (XRD, D8 Advance). FTIR spectra of samples were performed with a Bruker Vertex 70 Fourier transform infrared spectrometer.

2.3. Electrochemical characterization

The electrochemical properties of KCR electrolyte were characterized by using MnO2/rGO electrode as cathode and electroplated Zn on carbon cloth as anode. Cyclic voltammetry was conducted at a scanning rate of 0.2 mV s−1 between 1.0 and 1.9 V vs. Zn2+/Zn (CHI660, Shanghai CH Instrument Co., Ltd.). Galvanostatic charging/discharging cycles were tested at different current density on a multichannel battery test system (CT2001A, Wuhan Kingnuo Electronic Co., Ltd.). The ionic conductivity of KCR electrolyte was characterized by placing a piece of KCR electrolyte between two stainless sheets. Impedance measurements were carried out between 10 kHz to 0.01 Hz with an AC amplitude of 5 mV (CHI 660C, Shanghai CH Instrument Co., Ltd.). The equation of ionic conductivity can be expressed as σ = l/RA, where σ is conductivity, and l, R, and A represent the thickness of the KCR electrolyte, the bulk resistance (the real impedances at the highest frequency), and the area of the KCR electrolyte. Energy (W h kg−1) density and power density (W kg−1) were calculated by using the following equations
image file: c9ra01120j-t1.tif

P = E/t
where I is the discharging current, U is the cell voltage, dt is the time differential, m is the mass of the MnO2, and t is the discharging time.

3. Results and discussion

Fig. 1b shows the photographs of the kappa-carrageenan after adding ZnSO4/MnSO4 aqueous solution. The kappa-carrageenan electrolyte appears to be a very stable and uniform gel electrolyte. The Fourier-transform infrared spectroscopy (FTIR) spectra of the pure kappa-carrageenan polymer and the kappa-carrageenan electrolyte are shown in Fig. 1c. The red line in Fig. 1c represents the basic characteristics of kappa-carrageenan. As reported previously, the band around 3444 cm−1, 2912 cm−1, and 1640 cm−1 were related to O–H stretch, C–H stretch, and asymmetric vibration of –COO.27 The typical band around 1248 cm−1, and 1068 cm−1, and 848 cm−1 corresponds to O[double bond, length as m-dash]S[double bond, length as m-dash]O symmetric vibration, C–O stretching, and C4–O–S stretching vibration.27 The band near 928 cm−1 proved the existence of C–O–C of 3,6-anhydro-D-galactose.27 Compared with FTIR spectrum of the kappa-carrageenan, the intensity of the peak around 1116 cm−1 in the FTIR spectrum of the kappa-carrageenan electrolyte becomes dominant, which is directly related to the existence of SO42−.13

Pure kappa-carrageenan electrolyte film can be deposited by a simple casting method. However, the as-deposited film is fragile. In order to improve the mechanical strength and flexibility, a Chinese painting rice paper was introduced as a flexible scaffold during fabrication to complete the flexible KCR electrolyte. The rice paper is well known for its excellent wettability, tensile strength and high flexibility. Fig. S1a shows the scanning electron microscope (SEM) image of the rice paper used in this work. The rice paper is comprised of randomly crosslinked fibers with an average diameter of ∼10 μm, and a thickness of ∼50 μm measured from the cross-sectional SEM image (Fig. S1b). By immersing the rice paper into the kappa-carrageenan electrolyte, a final solid-state KCR electrolyte film with thickness of ∼100 μm thick was obtained, as shown in Fig. 1d and e.

Sufficient flexibility is essential for the application of solid-state electrolytes in flexible ZIBs. The KCR demonstrates excellent flexibility and can be repeatedly bent (inset in Fig. 1f). The ionic conductivity of KCR films was obtained from the AC impedance spectra (Fig. 1f). It exhibits a high ionic conductivity of 3.32 × 10−2 S cm−1 at room temperature. Compared with other zinc ion conducting polymer electrolytes in literature, the KCR electrolyte shows the highest conductivity to the best of our knowledge (Table S1). It is worth noting the rice paper in KCR has no contribution to the ionic conductivity of KCR film. The remarkable flexibility together with high ionic conductivity empowers the KCR to be an ideal electrolyte for flexible solid-state ZIBs.

Solid-state ZIBs are then assembled in an open-air environment using MnO2/rGO composite cathode, electroplated zinc anode, and the KCR electrolyte (Fig. S2a). In this work, α-MnO2 nanosheets were synthesized by a hydrothermal method.26 The SEM image (Fig. S2b) and the TEM image (Fig. S2c) discloses the nanosheet structure and crumpled surface of α-MnO2, respectively. In Fig. S3, all Bragg peaks in X-ray powder diffraction (XRD) pattern of the MnO2 can be indexed to the crystalline phase of α-MnO2 (JCPDS: 44-0141). A flexible MnO2/rGO composite electrode and electroplated Zn on carbon cloth were used as cathode and anode, respectively.26 The XRD patterns of the crystalline phases of electroplated zinc are presented in Fig. S4, where all the diffraction peaks of electroplated zinc are well-indexed to the characteristic peaks of zinc (JCPDS: 4-831). The freestanding Zn nanosheets homogeneously grown on the carbon fiber are disclosed in the SEM image of Fig. S2d.

Fig. 2a plots the cyclic voltammogram of solid-state ZIBs with KCR electrolyte. The reversible redox peaks (reduction peaks: 1.238 and 1.364 V, oxidation peak: 1.584 V) can be clearly observed. The charging and discharging profiles of the samples at the first two cycles are shown in Fig. 2b, which presents two discharge plateaus mainly due to the subsequent H+ and Zn2+ insertion/extraction process during the discharging/charging.28 The fabricated ZIBs deliver capacities of 278.5 and 287.1 mA h g−1 at 0.15 A g−1 in the initial two cycles. Fig. 2c shows the rate performance of solid state ZIBs. The battery can deliver discharging capacity of ∼291.5 mA h g−1 at 0.15 A g−1. Impressively, ZIBs with KCR electrolyte achieve a high discharge capability of 120.0 mA h g−1 at a high current density of 6.0 A g−1. The discharge time is limited to only 72 s. These results indicate a good rate capability and ultrafast charge–discharge ability of ZIBs with KCR electrolyte. Such rate performance of our ZIBs with KCR electrolyte outperforms most of the reported ZIBs (Zn–MnO2) with other solid-state electrolytes (Table S2), such as Zn–MnO2 battery with PVA electrolyte (76 mA h g−1 at 5.58 A g−1),15 Zn–MnO2 battery with xanthan gum (120–150 mA h g−1 at 3.08 A g−1)13 and Zn–MnO2 battery with gelatin and polyacrylamide based hierarchical polymer electrolyte (150 mA h g−1 at 1.848 A g−1).17 When cycling back to 0.15 A g−1, a discharge capacity of 273.0 mA h g−1 is recovered. This superior rate performance can be attributed to the following factors: (1) the KCR electrolyte exhibits an ultra-high ionic conductivity, which improves the rate performance of ZIBs; (2) the presence of rGO in the cathode effectively enhances the charge transport (Fig. S5).


image file: c9ra01120j-f2.tif
Fig. 2 (a) Cyclic voltammogram of the solid-state ZIBs with KCR electrolyte. (b) The charging/discharging profiles of the first and second cycles at the current density of 0.15 A g−1. (c) Specific capacities of the solid-state ZIBs at various current densities. (d) Ragone plots of the solid-state ZIBs with KCR electrolyte. The values reported from other solid-state ZIBs are included for comparison.13,15,29

The energy and power densities of our battery (based on the mass of MnO2) with KCR electrolyte are shown in Fig. 2d and Table S3. The maximum energy density is 400 W h kg−1 and peak power density is 7.9 kW kg−1, both of which are higher than previous reported values from flexible ZIBs with xanthan gum and PVA electrolyte (LiCl–ZnCl2–PVA) based Zn–MnO2 battery.13,29 At high current rates, the energy density of ZIBs with KCR electrolyte are higher than that of the PVA electrolyte (LiCl–ZnCl2/MnSO4–PVA) based Zn–MnO2 battery,15 while the power densities are comparable (171 W h kg−1/7.9 kW kg−1 (for ZIBs with KCR electrolyte) vs. 110 W h kg−1/8.6 kW kg−1 (for ZIBs with PVA electrolyte)). Taking the total mass of the cell (including MnO2, rGO, electroplated Zn and current collectors (carbon cloth)) into consideration, the gravimetric energy density of battery is 29.1 W h kg−1.

The cycling performance of the solid-state ZIBs with KCR electrolyte is then tested at high rates (6.0 A g−1). As shown in Fig. 3a, 80% of its initial capacity still remained even the cyclic number extended to 450 cycles at 6.0 A g−1, indicating the excellent cycling stability of the solid-state ZIBs with KCR electrolyte. The morphological characterization of the cathode and anode was carried out after 450 cycles. As shown in Fig. 3b, the SEM image of the MnO2 after cycling test demonstrates a nanosheet structure similar to that before the test. In addition, the freestanding Zn nanosheets can be observed in the SEM image of Zn anode after 450 cycles (Fig. 3c). These results indicate that the morphology of cathode and anode materials remain almost unchanged as compared to the morphology of the pristine MnO2 and Zn. The experimental results suggest utilization of KCR electrolyte maintains structural stability of MnO2 cathode and Zn anode, which improves the stability of the solid-state ZIBs. Fig. S6a further shows the SEM image of a fresh zinc foil, which has a very smooth surface. When utilized as an anode and cycled at 6.0 A g−1 for 100 cycles in the aqueous electrolyte, the surface of zinc foil becomes textured and zinc dendrite formation is observed (Fig. S6b). In contrast, the zinc foil after 100 cycles at 6.0 A g−1 in KCR electrolyte showed evener surface and no noticeable zinc dendrites are observed (Fig. S6c). Based on the above results, it is found that the utilization of KCR electrolyte significantly inhibits the growth of Zn dendrites, which effectively reduce the chances of short circuit. The exceptional electrochemical performance indicates that the ZIBs with KCR electrolyte are promising as high-performance, long-life, low-cost and environmentally-friendly flexible energy storage devices.


image file: c9ra01120j-f3.tif
Fig. 3 (a) Cycling stability of the solid-state ZIBs with KCR electrolyte cycled at 6.0 A g−1 and corresponding coulombic efficiency. SEM images of (b) the MnO2 cathode and (c) the electroplated Zn anode after 450 charge/discharge cycles.

Flexibility is essential for the application of solid-state ZIBs in wearable electronics. To test the flexibility of the solid-state ZIBs with KCR electrolyte, the fabricated devices were bended around a radius of 1.37 cm. Experimental results show that the batteries still maintained the discharge profile and AC impedance spectra after test (Fig. 4a and S7). The flexibility of the solid-state ZIBs with KCR electrolyte was further verified by continuously bending the battery by 180°. After 300 bending cycles, 95% capacity was retained (Fig. 4b). These observations demonstrate a good mechanical stability of the KCR electrolyte. Moreover, the solid-state ZIBs with KCR electrolyte successfully powered a timer under bending condition, demonstrating its promising potential in personalized wearable electronics (Fig. 4c). This good flexibility is due to the excellent flexibility of the materials in the battery, including the KCR electrolyte and the carbon cloth current collector. The solid-state ZIBs also powered a timer when the entire device was immersed in water, demonstrating its good waterproofness (Fig. 4d).


image file: c9ra01120j-f4.tif
Fig. 4 (a) Discharge curves under normal and bending conditions. (b) The bending test of solid-state ZIBs with KCR electrolyte for 300 cycles. (c) A solid-state ZIB with KCR electrolyte powers a timer under 180 degrees of bending conditions. (d) A solid-state ZIB with KCR electrolyte powers a timer when the battery is fully immersed in the water.

4. Conclusions

In summary, we successfully prepare a non-toxic, high-ionic conductivity, low-cost and environmentally-friendly, flexible quasi-solid-state electrolyte for ZIBs application. The ZIBs with such electrolyte show a high specific capacity, fast charging and discharging capability, good cycling stability, and high reliability bearing cycles of bending. The utilization of KCR electrolyte maintains structural stability of cathode and anode after long cycling, which improves the stability of the solid-state ZIBs. With the excellent electrochemical performance and the ease of fabrication, such ZIBs with KCR electrolytes are very promising for use as wearable energy storage devices.

Conflicts of interest

There are no conflicts to declare.

Acknowledgements

This work is supported by the China Postdoctoral Science Foundation funded project (2017M620517). Yuan Huang and Zigang Li would like to acknowledge financial support from the Shenzhen Science and Technology Innovation Committee (No. JCYJ20170818090257257, and No. KQJSCX 20170728101942700).

References

  1. M. Balogun, Y. Hao, L. Yang, W. Qiu, Y. Huang and Z. Liu, Energy Environ. Sci., 2018, 11, 1859–1869 RSC .
  2. X. Huang, G. Diao, S. Li, M. Balogun, N. Li and Y. Huang, RSC Adv., 2018, 8, 17056–17059 RSC .
  3. B. Long, L. Luo, H. Yang, M. Balogun, S. Song and Y. Tong, ChemistrySelect, 2018, 3, 6965–6971 CrossRef CAS .
  4. G. Diao, M.-S. Balogun, S.-Y. Tong, X. Guo, X. Huang, Y. Mao and Y. Tong, J. Mater. Chem. A, 2018, 6, 15274–15283 RSC .
  5. Y. Fu, Q. Wei, G. Zhang, X. Wang, J. Zhang, Y. Hu, D. Wang, L. Zuin, T. Zhou, Y. Wu and S. Sun, Adv. Energy Mater., 2018, 8, 1801445 CrossRef .
  6. J. Huang, Z. Wang, M. Hou, X. Dong, Y. Liu, Y. Wang and Y. Xia, Nat. Commun., 2018, 9, 2906 CrossRef PubMed .
  7. D. Chao, C. Zhu, M. Song, P. Liang, X. Zhang, N. H. Tiep, H. Zhao, J. Wang, R. Wang, H. Zhang and H. J. Fan, Adv. Mater., 2018, 30, 1803181 CrossRef PubMed .
  8. F. Mo, H. Li, Z. Pei, G. Liang, L. Ma, Q. Yang, D. Wang, Y. Huang and C. Zhi, Sci. Bull., 2018, 63, 1077–1086 CrossRef CAS .
  9. P. Hu, T. Zhu, X. Wang, X. Wei, M. Yan, J. Li, W. Luo, W. Yang, W. Zhang, L. Zhou, Z. Zhou and L. Mai, Nano Lett., 2018, 18, 1758–1763 CrossRef CAS PubMed .
  10. L. Kang, M. Cui, F. Jiang, Y. Gao, H. Luo, J. Liu, W. Liang and C. Zhi, Adv. Energy Mater., 2018, 8, 1801090 CrossRef .
  11. K. Lu, B. Song, Y. Zhang, H. Ma and J. Zhang, J. Mater. Chem. A, 2017, 5, 23628–23633 RSC .
  12. L. Ma, S. Chen, H. Li, Z. Ruan, Z. Tang, Z. Liu, Z. Wang, Y. Huang, Z. Pei, J. A. Zapiena and C. Zhi, Energy Environ. Sci., 2018, 11, 2521–2530 RSC .
  13. S. Zhang, N. Yu, S. Zeng, S. Zhou, M. Chen, J. Di and Q. Li, J. Mater. Chem. A, 2018, 6, 12237–12243 RSC .
  14. H. Pan, Y. Shao, P. Yan, Y. Cheng, K. S. Han, Z. Nie, C. Wang, J. Yang, X. Li, P. Bhattacharya, K. T. Mueller and J. Liu, Nat. Energy, 2016, 1, 16039 CrossRef CAS .
  15. Y. Zeng, X. Zhang, Y. Meng, M. Yu, J. Yi, Y. Wu, X. Lu and Y. Tong, Adv. Mater., 2017, 29, 1700274 CrossRef PubMed .
  16. J. P. T. Guisao and A. J. F. Romero, Electrochim. Acta, 2015, 176, 1447–1453 CrossRef CAS .
  17. H. Li, C. Han, Y. Huang, Y. Huang, M. Zhu, Z. Pei, Q. Xue, Z. Wang, Z. Liu, Z. Tang, Y. Wang, F. Kang, B. Li and C. Zhi, Energy Environ. Sci., 2018, 11, 941–951 RSC .
  18. N. K. Zainuddin and A. S. Samsudin, Mater. Today Commun., 2018, 14, 199–209 CrossRef CAS .
  19. P. C. Selvin, P. Perumal, S. Selvasekarapandian, S. Monisha, G. Boopathi and M. V. L. Chandra, Ionics, 2018, 24, 3535–3542 CrossRef .
  20. S. Rudhziah, A. Ahmad, I. Ahmad and N. S. Mohamed, Electrochim. Acta, 2015, 175, 162–168 CrossRef CAS .
  21. I. J. Shamsudin, A. Ahmad, N. H. Hassan and H. Kaddami, Ionics, 2016, 22, 841–851 CrossRef CAS .
  22. S. Rudhziah, M. S. A. Rani, A. Ahmad, N. S. Mohamed and H. Kaddami, Ind. Crops Prod., 2015, 72, 133–141 CrossRef CAS .
  23. M. M. Pérez-Madrigal, F. Estrany, E. Armelin, D. D. Díaz and C. Alemán, J. Mater. Chem. A, 2016, 4, 1792–1805 RSC .
  24. X. Hu, L. Fan, G. Qin, Z. Shen, J. Chen, M. Wang, J. Yang and Q. Chen, J. Power Sources, 2019, 414, 201–209 CrossRef CAS .
  25. T. M. D. Palma, F. Migliardini, D. Caputo and P. Corbo, Carbohydr. Polym., 2017, 157, 122–127 CrossRef PubMed .
  26. Y. Huang, J. Liu, Q. Huang, Z. Zheng, P. Hiralal, F. Zheng, D. Ozgit, S. Su, S. Chen, P.-H. Tan, S. Zhang and H. Zhou, npj Flexible Electronics, 2018, 2, 21 CrossRef .
  27. L. Fan, L. Wang, S. Gao, P. Wu, M. Li, W. Xie, S. Liu and W. Wang, Carbohydr. Polym., 2011, 86, 1167–1174 CrossRef CAS .
  28. W. Sun, F. Wang, S. Hou, C. Yang, X. Fan, Z. Ma, T. Gao, F. Han, R. Hu, M. Zhu and C. Wang, J. Am. Chem. Soc., 2017, 139, 9775–9778 CrossRef CAS PubMed .
  29. K. Wang, X. Zhang, J. Han, X. Zhang, X. Sun, C. Li, W. Liu, Q. Li and Y. Ma, ACS Appl. Mater. Interfaces, 2018, 10, 24573–24582 CrossRef CAS PubMed .

Footnotes

Electronic supplementary information (ESI) available. See DOI: 10.1039/c9ra01120j
Yuan Huang and Jiuwei Liu contributed equally to this work.

This journal is © The Royal Society of Chemistry 2019