Open Access Article
Hao Guo*a,
Mingyue Wanga,
Rui Xueb,
Jing Yaoa,
Xuejiao Wanga,
Longwen Zhanga,
Jianfeng Liua and
Wu Yang
*a
aKey Lab of Eco-Environments Related Polymer Materials of MOE, Key Lab of Bioelectrochemistry and Environmental Analysis of Gansu Province, College of Chemistry and Chemical Engineering, Northwest Normal University, Lanzhou 730070, P. R. China
bProvincical Key Laboratory of Gansu Higher Education for City Environmental Pollution Control, College of Chemistry and Chemical Engineering, Lanzhou City University, Lanzhou 730070, P. R. China
First published on 1st May 2019
A new COF (NWNU-COF-4) linked by an aryl ether bond (Ar–O–Ar) was synthesized by the condensation reaction of 2,4,6-trihydroxypyrimidine and trinitrophenol under simple and easy reaction conditions. Fourier transform infrared spectroscopy (FT-IR), X-ray photoelectron spectroscopy (XPS), N2 adsorption–desorption, thermogravimetric analysis (TGA), powder X-ray diffraction (XRD) and scanning electron microscopy (SEM) were utilized to characterize the product. The BET specific surface area of NWNU-COF-4 was 21.33 m2 g−1, and its pore size was about 1.351 nm. Additionally, this method of preparation was simple and cheap. The electrochemical measurements showed that the synthesized NWNU-COF-4 had excellent pseudocapacitive performance with maximum specific capacitance of 133.44 F g−1 at 0.3 A g−1 in 6 mol L−1 KOH electrolyte. When the current density increased by 10 times (3.0 A g−1), the specific capacitance was 114.12 F g−1, and the retention rate was 82%. After 10
000 GCD cycles, the capacitance still kept 94% of its initial capacitance.
With the increasing demand of new green sustainable energy to face the deepening energy crisis and environmental pollution, supercapacitors attracted much attention as a new energy storage device due to their performance of high power density, high capacitance, long cycling life, low maintenance cost and environmental friendliness. Generally, the electrode materials of supercapacitor can be summarized in three types: carbon material, conducting polymers and metal oxides.27 Recently, metal–organic frameworks (MOFs) was used as electrode material of supercapacitor owing to the redox behavior of metal cations inside MOFs.28 Nowadays, as a new type of porous organic framework material, the redox behavior of organic monomers inside COFs,29 such as anthraquinone, enables them as pseudocapacitive material for supercapacitors.
Herein we report a new COF linked by ether bond prepared under ordinary conditions and explore its application in supercapacitors as electrode material. A new 2D COFs (termed NWNU-COF-4) was designed and synthesized by the reaction of nitro-group (–NO2) and hydroxyl (–OH) for the first time. NWNU-COF-4 was constructed by the condensation of trinitrophenol and 2,4,6-trihydroxypyrimidine acid (Scheme 1) in the solvent of N-methyl pyrrolidone (NMP). The NWNU-COF-4 was coated on Ni foam as an electrode material, which exhibited good supercapacitor performance.
| C = IΔt/ΔV | (1) |
The energy density (E) and power density (P) of the asymmetric two-electrode cell are calculated by eqn (2) and (3)
![]() | (2) |
![]() | (3) |
N bonds. The peaks at 1413 cm−1, 1489 cm−1 and 1622 cm−1 belong to the aromatic rings. The peak at 1085 cm−1 is assigned to the ether bond, which proves that the NWNU-COF-4 linked by ether bond (–O–) was synthesized successfully. In addition, the characteristic peaks of –NO2 and –OH can be observed at 1369 cm−1 and 1301 cm−1 respectively, due to the rest of the reactants and dangling bonds.
Fig. 1 shows the typical XPS survey spectrum and high-resolution elemental scan of N1s, which were recorded from the NWNU-COF-4. As shown in Fig. 1(a), XPS survey spectrum, C, N, O were detected at the binding energy of 286.8 eV, 403.2 eV, and 534.4 eV respectively. O1s high resolution XPS spectra included three chemical species with binding energy at about 533.07, 532.0 and 531.14 eV (Fig. 1(b)), which attributable to C–O–C, C–O–H, and N–O respectively. These results demonstrated that NWNU-COF-4 was synthesized successfully.
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| Fig. 1 The XPS spectra of NWNU-COF-4. (a) The typical XPS survey spectrum of NWNU-COF-4; (b) the high resolution XPS spectra of O1s for NWNU-COF-4. | ||
The crystalline structure of NWNU-COF-4 was determined by powder X-ray diffraction (PXRD), and possible extended structures based on hexagonal unit cells were modeled as shown in Fig. 2(a and b). A hexagonal unit cell with the parameters a = b = 8.985616 Å, c = 4.645 Å and α = β = 90°, γ = 120° was deduced by Accelrys' Materials Studio 7.0 software. The corresponding curve (Fig. 2d) is closer to the experimental data (Fig. 2c). Peaks at 2θ = 25.71° and 28.87° correspond to the (1, 1, 1) plane of KOH and (2, 0, 0) plane of KCl respectively by comparing with the PDF cards, due to the small amount of potassium chloride and potassium hydroxide in the product were not completely removed. On the other hand, the peak at about 27.61° correspond to the π–π stacking between COF layers, and could be assigned to (0, 0, 1) planes.30
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| Fig. 2 (a) The lateral view and (b) top view of NWNU-COF-4; (c) experimental and (d) simulated patterns of NWNU-COF-4. C: gray, N: blue, O: red, and H atoms are omitted for clarity. | ||
SEM images of NWNU-COF-4 are displayed in Fig. 3, from which we can observe that NWNU-COF-4 is three dimensional network structure with rough surface, and its internal structure is very loose. There are some amorphous particles on the surface of the material.
The permanent porosity of NWNU-COF-4 was demonstrated by N2 adsorption–desorption analysis at 77.350 K (Fig. 4). The isotherm shows a sharp increase in the gas uptake below P/P0 = 1.0. The Brunauer–Emmett–Teller (BET) surface area was calculated to be 21.33 m2 g−1, the total pore volume was calculated to be 0.198 cm3 g−1. The pore size distribution was calculated by Barrett–Joyner–Halenda (BJH) models, resulting a value of 13.51 Å. Thermogravimetric analysis (TGA) was used to evaluate the thermostability of NWNU-COF-4. The curve of TGA is showed in Fig. S2.† The stage below 100 °C with weight loss ∼2% is due to desorption of small amounts of water. The stage from 150 °C to 300 °C, the weight loss ∼7% can be attributed to desorption of solvent NMP and the decomposition of the reactants. An obvious weight loss process from 300 °C to 500 °C indicates that the framework structure of NWNU-COF-4 is collapsed, and the product is decomposed and gasified gradually. As the temperature continues to rise up to 800 °C, the molecular structure is further destroyed and decomposed.
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| Fig. 4 N2 adsorption and desorption isotherm of NWNU-COF-4. Inset: pore size distribution for NWNU-COF-4 measured at 77.3 K. | ||
The redox peak currents of NWNU-COF-4 are linearly proportional to the square root of scan rate (ν) from 5 mV s−1 to 500 mV s−1 with regression equations (Fig. S3†): IOx (A) = 0.01338 − 0.28694ν1/2 (R2 = 0.99801), IRe (A) = −0.00833 + 0.23714ν1/2 (R2 = 0.99880) respectively, indicating that the electrochemical process of NWNU-COF-4 is diffusion-controlled. Galvanostatic charge–discharge measurements were carried out at different current densities (0.3, 0.4, 0.5, 1.0, 1.5, 2.0, 3.0, 5.0, 8.0, 10.0, 15.0 A g−1) to evaluate the specific capacitance of NWNU-COF-4. Fig. 5(b) shows the GCD curves for different charging current densities. The plateaus at ∼0.25 V to approximately ∼0.45 V further verifies the pseudocapacitance behavior of NWNU-COF-4. The highest specific capacitance of NWNU-COF-4 is 133.44 F g−1 at the current density of 0.3 A g−1. When the current density increases by 10 times, 3.0 A g−1, the specific capacitance is 114.12 F g−1 with the retention rate of 82%. Even though the current density increased by 50 times (15 A g−1), the specific capacitance is 75 F g−1, and the retention rate is 56% (Fig. 5c), indicating a good rate performance of NWNU-COF-4.
The results of the cycling stability experiments illustrate an excellent stability of NWNU-COF-4 (Fig. 5d). The cycling stability performance was evaluated by GCD test at current density of 1 A g−1 within potential window of 0–0.5 V. As shown in Fig. 5d, after 10
000 GCD cycles the capacitance still keep 94% of its initial capacitance, indicating its excellent cycling stability as a durable pseudocapacitive electrode material. Table 1 lists a comparison of the capacitance performances of synthesized NWNU-COF-4 with the reference results reported previously based on COF electrode materials. It can be found that except TpPA-(OH)2 (ref. 30) and TDFP-1,33 the prepared COF material possessed the highest specific capacitance. It is notable that the synthesized NWNU-COF-4 had the best cycle performance and high-rate performance at higher current density.
| Electrode materials | Electrolytes | Specific capacitance (F g−1) | Current density (A g−1) | Retention (%) (cycle@current density (A g−1)) | Potential window (V) | Specific capacitance retention (%) current density (A g−1) | Ref. |
|---|---|---|---|---|---|---|---|
| a Potential scan rate in unit of mV s−1.b Current density in unit of mA cm−2.c Specific capacitance in unit of mF cm−2. | |||||||
| DAAQ-TFP COF | 1 M H2SO4 | 48 | 0.1 | 84.5(5000@0.1) | −0.3 to 0.3 | 28.6(0.1 to 2.0) | 22 |
| TpBD-(OH)2 | 1M PBS | 90 | 0.5 | — | 0–0.7 | 49(0.5 to 5) | 30 |
| TpPA-(OH)2 | 1M PBS | 416 | 0.5 | 66(1000@5) | −0.2 to 0.5 | 58(2 to 20a) | 30 |
| COFDAAQ-BTA-3DG | 1M KOH | 32.6c | 0.025b | 30(500@0.5b) | −1.05 to −0.4 | 16.3(0.025 to 2.53b) | 31 |
| DAB-TFP-COF | 1 M H2SO4 | 79.1 | 20a | 92(6000@2) | −0.3 to 0.35 | — | 32 |
| TDFP-1 | 0.1 M H2SO4 | 418 | 0.5 | 95(1000@10) | −0.45 to 0.5 | — | 33 |
| NH2-f-MWCNT@COFTTA-DHTA | 1 M Na2SO4 | 127.5 | 0.4 | 96(1000@0.4) | 0–0.7 | 77(0.4 to 2) | 34 |
| NWNU-COF-4 | 6 M KOH | 133.44 | 0.3 | 94(10 000@5) |
0–0.5 | 82(0.3 to 3) | This work |
| 56(0.3 to 15) | |||||||
EIS was also employed at the potential of 0.3291 V in 6 M KOH over the frequency range of 0.01 Hz to 10
000 kHz. Fig. 6 shows Nyquist plots of NWNU-COF-4. The Nyquist plot displays an unconspicuous semicircle at the high frequency range and a straight line at the low frequency region. The small semicircle at the high frequency range corresponds to low charge transfer resistance, and the straight line corresponds to diffusive resistance of the electrolyte. The phase angle of the straight line in low frequency region is larger than 45°, indicating a good ion mobility of electrode. The intercept at Z′ axis represents the equivalent series resistance, was consist of intrinsic resistance of electrode material, ionic resistance of electrolyte and contact resistance at the interface of electrode material/Ni foam.28 The value of equivalent series resistance is 0.56 Ω.
To further estimate the practical applications of NWNU-COF-4, we fabricated the asymmetric two-electrode cell and measured its capacitance properties in 3 M KOH electrolyte. The asymmetric two electrode cell was constructed by using the NWNU-COF-4 electrode as positive electrode and commercially activated carbon (AC) as negative electrode, respectively. Fig. S4† shows the CV curves of NWNU-COF-4 and AC electrodes at 30 mV s−1, respectively. The potential window of AC is −1 to 0 V, and the potential window of NWNU-COF-4 is 0–0.6 V, thus the maximum operation potential windows of two-electrode cell can be extended to be 1.6 V.
The CV curves of two-electrode cell at scan rates of 5–200 mV s−1 are showed in Fig. 7a. The shape of the CV curves illustrates the behaviors of electric double-layer capacitance and caradaic capacitance at all scan rates. Typical GCD curves of the two-electrode cell at different current densities from 0.5 to 10 A g−1 are showed in Fig. 7b. The constructed ASC exhibits the highest specific capacity of 42.84 F g−1 at the current density of 0.5 A g−1, and retains 46.87% of its initial capacity at 10 A g−1 (Fig. S5†). In addition, the two-electrode cell delivers an energy density of 14.85 W h kg−1 at a power density of 394.83 W kg−1, which is superior to the other reported COF based electrode materials.35
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| Fig. 7 (a) CV curves of the two-electrode cell at the different scan rates. (b) GCD curves of the two-electrode cell at different current densities. | ||
000 GCD cycles. In addition, the asymmetric two electrode cell assembled by using NWNU-COF-4 and activated carbon (AC) delivered an energy density of 14.85 W h kg−1 at a power density of 394.83 W kg−1. These results demonstrated the promising applications of NWNU-COF-4 as supercapacitor electrode materials.
Footnote |
| † Electronic supplementary information (ESI) available. See DOI: 10.1039/c9ra01357a |
| This journal is © The Royal Society of Chemistry 2019 |