Tiantian Gu‡
,
Min Zhou‡,
Mengyun Liu,
Kangli Wang*,
Shijie Cheng and
Kai Jiang*
State Key Laboratory of Advanced Electromagnetic Engineering and Technology, School of Electrical and Electronic Engineering, State Key Laboratory of Materials Processing and Die & Mould Technology, College of Materials Science and Engineering, Huazhong University of Science and Technology, Wuhan, Hubei, China 430074. E-mail: kjiang@hust.edu.cn; klwang@hust.edu.cn
First published on 19th May 2016
A polyimide–MWCNT composite (PNP@CNT) synthesized from 1,4,5,8-naphthalenetetracarboxylic-dianhydride (NTCDA) and phenylene diamine (PDA) was investigated as a novel anode for aqueous Na-ion batteries. This composite demonstrates a high reversible capacity of 149 mA h g−1 at quite a low potential of −0.65 V (vs. SCE), superior rate capability and long-term cycling stability. The feasibility of PNP@CNTs in aqueous Na-ion full batteries is also confirmed in conjunction with the Na0.44MnO2 cathode, possibly serving as a high performance aqueous Na host anode for large-scale electric energy storage applications.
Intensive efforts have been aimed at developing novel aqueous Na-host anode shifting from inorganic to organic compounds.16,17 Polyimide, a redox-active organic polymer with high mechanical strength, is considered to be a promising candidate for aqueous Na-ion batteries because of its resource abundance, structural diversity and stability in aqueous electrolyte.18,19 Furthermore, the flexible polymer backbone could provide higher mobility of the large-sized Na+ which can effectively improve the poor kinetics of the Na+ insertion/desertion reactions.20–23 During the past years, various kinds of polyimide have been investigated as Na-host electrode,24–26 but only few of them can work well in aqueous electrolytes due to the sloping high potential (above −0.5 V vs. SCE),19,27 thus resulting in low energy density in the practical full cells. As the electrochemical window of the aqueous electrolyte is quite narrow, it is of great importance to develop high performance polyimide anode with sufficiently low and flat redox potential. The electrochemical performance of redox-active polymer is strongly dependent on the polymer structure, thus designing highly conjugated polyimide skeleton by adjusting the dianhydride and diamine component can effectively optimize the redox potential of the polyimide.18,26 Based on this consideration, we focus on poly-(naphthalene four formyl phenylene diamine) (PNP), synthesized from 1,4,5,8-naphthalenetetracarboxylic dianhydride (NTCDA) and phenylene diamine (PDA). The unique structure of benzene ring (PDA) and naphthalene ring (NTCDA) will enlarge the π-conjugation system of the polymer backbone, thus resulting in a highly conjugated structure, which lead to a planar voltage plateau and high conductivity of the polymer backbone. Moreover, the electrochemical performance of PNP can be further improved by the addition of MWCNTs. The high conductivity and strong mechanical properties of the CNTs can not only provide a cross-linked conducting-network for the polymer backbone, but also enable a robust structure to realize stable cycling performances.
In this paper, a polyimide–MWCNTs composite (PNP@CNTs) was prepared via a facile dehydration condensation reaction with the addition of MWCNTs, and investigated as a novel Na-storage anode in aqueous electrolyte for the first time. The as prepared PNP@CNTs demonstrated a high reversible capacity of 149 mA h g−1 at a quite low potential of −0.65 V (vs. SCE) with flat discharge plateaus, superior rate capability at 20C (1C = 100 mA g−1) and excellent cycling stability over 500 cycles, possibly serving as a low cost and cycling-stable organic anode for aqueous Na-ion batteries.
Na0.44MnO2 was prepared according to the method previously reported.9 A typical experimental procedure was to dissolve 0.53 g Na2CO3, 4.9 g Mn(Ac)2 and 1.05 g citric acid in distilled water and stir to obtain a clear and viscous gel. The resultant gel was dried at 120 °C for 12 h, heat-treated at 350 °C for 4 h and 850 °C for 6 h in air to obtain the final product.
For IR characterizations, the electrode samples at different charge and discharge states taken out from the disassembled cells were firstly rinsed with deionized water for several times and dried at 80 °C in vacuum for 60 min.
For ICP analysis of Na content, the dried electrode samples were burnt in a tubular furnace at 600 °C for 10 h. The as-obtained sodium oxide residue was then dissolved in HNO3 for the atomic emission analysis using IRIS Intrepid III XSP spectrometer.
The morphology of the as-prepared PNP and PNP@CNTs were further characterized by scanning electron microscopy (SEM). As shown in Fig. 1, the PNP polymer appear as uneven agglomerates with large size of ∼1 μm (Fig. 1b), while the PNP@CNTs composite emerges as well-defined particles of 100 nm particles cross-linked with CNTs (Fig. 1c). It is well-established that the highly conductive MWCNTs network can provide abundant electrochemically active areas for Na+ insertion/extraction reactions. The chemical structure of PNP was confirmed by FT-IR spectrometry. The FT-IR spectrum in Fig. 1d reflects all the characteristic absorptions of a typical naphthalene-derived polyimide: such as the stretching vibration of the C–N (1344 cm−1) and naphthalene ring (1582 cm−1). The bands at 1714 cm−1, 1672 cm−1 and 768 cm−1 are assigned to asymmetric and symmetric stretching vibrations of the CO bond.
The characteristic stretching modes of the benzene ring (PDA) can be detected at 1514 cm−1. The Brunauer–Emmett–Teller (BET) measurement suggests a mesoporous structure of the PNP particles, as evidenced by the nitrogen adsorption/desorption isotherms of IV type (Fig. S1†). Based on the BET analysis, the specific surface areas of the bulk PNP and PNP@CNTs were measured to be 8.7546, 24.8775 m2 g−1, respectively. Fig. 1e presents the thermogravimetry analyses (TGA) curves of PNP and PNP@CNTs, the carbon contents in the PNP@CNTs is calculated to be ∼10%.
The electrochemical reactivity of the PNP@CNTs was investigated by cyclic voltammetry (CV) at a scan rate of 2 mV s−1. As shown in Fig. 2b, the main CV features of the PNP@CNTs polymer appear as two pairs of well-defined redox peaks located at −0.78/−0.6 V and −0.58/−0.4 V (vs. SCE), resembling very much the CV patterns of polyimide electrodes in organic electrolytes,18 implying a reversible two-electron enolization reaction of the carbonyl group in the polyimide structure (Fig. 2a). In addition, the two pairs of redox peaks appeared quite equally in the peak area, keeping almost unchanged during the subsequent cycles, suggesting excellent electrochemical reversibility and cycling stability. Noteworthy, in the first anodic scan, there is only one broad peak occurring at −0.78 V which can be attributed to an initial activation process of the polymer chains. As the activity of the polymer is associated with the polymer skeleton and the surface structure of the polymer particles, the as-prepared inert chains can be activated during the first few charge–discharge cycles.
The electrochemical performance of the PNP@CNTs was further evaluated by galvanostatic charge–discharge cycling in 1 M Na2SO4 solution (PH = 7) using three-electrode cells. Fig. 2c shows the typical discharge–charge profiles of the PNP@CNTs electrode at the current density of 1C (100 mA g−1). In accordance with its CV features, the charge/discharge files of the polymer electrode shows planar voltage plateau at quite a low potential of −0.65 V (vs. SCE).
The charge and discharge capacities of PNP@CNTs in the first cycle are 149 and 132.3 mA h g−1, corresponding to an initial columbic efficiency of 88.8% which is much higher than other aqueous organic anode reported previously.19,27 The coulombic efficiency rapidly rose up to ∼100% in the subsequent cycles and the reversible capacity of the PNP@CNTs anode decreases slowly in the first 5 cycles and remains stable at ∼125 mA h g−1. The capacity decrease in the first few cycles can be ascribed to the slight solubility of the reduction products of the oligomers in aqueous electrolytes. It is worth noted that the high initial coulombic efficiency, low redox potential and high reversible capacity of the PNP@CNTs guarantee the feasibility of its practical application as aqueous Na-storage anode.
In addition to the dramatically high capacity, the PNP@CNTs electrode also exhibits superior high rate capability and long cycling stability. Fig. 2d compares the rate capability of the PNP and PNP@CNTs electrodes. The PNP@CNTs electrode delivers a reversible capacity of 132, 120, 115, 110, 102 mA h g−1 at different current densities of 1, 2, 5, 10, 15C (1C = 100 mA g−1), respectively. Even at a very high current density of 20C, a capacity of ∼92 mA h g−1 is still delivered, corresponding to 70% of the capacity obtained at 1C. In contrast, the PNP electrode shows much poor rate performances and the reversible capacity is rapidly declined to less than 70 mA h g−1 when the current density increases to 20C (50% of that obtained at 1C), indicating a significant enhancement in rate capability of the PNP after hybridized with MWCNTs. The excellent rate capability of the PNP@CNTs can be attributed to the unique structure of the highly conjugated polymer skeleton interconnected with conductive CNTs network, which can not only facilitate the Na+ diffusion with a low ion-transport resistance restrictions, but also ensure an efficient and continuous path for electron transport. The long-term cycling performances of the PNP@CNTs was further evaluated at a high current density of 10C. As shown in Fig. 2e, the reversible capacity of the PNP@CNTs anode decreases slowly during the first 10 cycles and then remains stable over the subsequent 500 cycles. In addition, the coulombic efficiency stabilized to >99% after a few cycles, indicating a stable electrochemical reversibility. The outstanding cyclability of the PNP@CNTs electrode should be benefited from the robust structure of the PNP@CNTs electrode originated from the large π-conjugated polymer backbone and high mechanical strength of the carbon additives (CNTs).
In order to further confirm the carbonyl enolization reaction mechanism described above, ex situ FT-IR analysis was carried out to characterize the changes in the bonding states of the PNP backbones at different depths of charge and discharge. As shown in Fig. 3, the pristine electrode presents a typical adsorption pattern of the as-prepared PNP. When first discharged to −1.0 V, the bands at 1714 (CO), 1672 (C
O) cm−1 were almost indiscernible, while the peaks at 1642 cm−1 appeared, reflecting a total conformational change of the carbonyl groups to the enol structure. When charged to −0.6 V, the band of the C
O bond reemerged but shifted to 1710 and 1667 cm−1, suggesting a partial oxidation of the enol structure to the C
O structure. At the fully charged state of 0 V, all the bands recovered to the original positions, implying a high reversibility of the enolization reaction of the carbonyl groups in the PNP structure. Furthermore, the quantitative ICP characterization of the PNP@CNTs electrode confirmed the enolazation reaction of 2 Na storage reaction mechanism in the polymer anode.
To evaluate the practical feasibility of the polymer as an anode for aqueous Na-ion batteries, an aqueous Na-ion full cell was fabricated using Na0.44MnO2 (NMO) as the cathode and PNP@CNTs as the anode. NMO was synthesized by solid-state reaction as described in the experiment section. The NMO cathode demonstrates a reversible capacity of ∼40 mA h g−1 at average potential of ∼0.25 V (vs. SCE) (see ESI Fig. S3†). Fig. 4 demonstrates the charge/discharge profiles of the coin type PNP@CNTs/NMO battery. This aqueous Na-ion full battery shows a discharge voltage of 0.8 V and delivers a reversible capacity of 92 mA h g−1 in terms of anode capacity. This cell can be well cycled at a high rate of 5C (1C = 100 mA g−1) over 200 cycles, delivering the energy density of 25 W h kg−1, suggesting a possible application of the PNP@CNTs composite as an organic anode for practical aqueous Na-ion full battery applications. Particularly, the coulombic efficiency of the full cell increase rapidly closed to 100% in the first 5 cycles, implying a very high electric energy conversion efficiency which is of great concern for the practical electric storage applications.
Footnotes |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c6ra09075c |
‡ These authors contributed equally to this work. |
This journal is © The Royal Society of Chemistry 2016 |