Xudong Liua,
Mingming Wenc,
Yanming Zhao*bc,
Youzhong Dongc,
Qinghua Fanc,
Quan Kuangc and
Qidong Lia
aSchool of Material Science and Engineering, South China University of Technology, China
bState Key Laboratory of Luminescent Materials and Devices, South China University of Technology, Guangzhou, 510640, P. R. China. E-mail: zhaoym@scut.edu.cn; Fax: +86-20-85511266; Tel: +86-20-87111963
cSchool of Physics, South China University of Technology, Guangzhou, 510640, China
First published on 12th August 2016
Cheese-like bulk carbon with nanoholes has been successfully fabricated from egg white via a simple annealing method by using distilled water as a green clean “corrosive agent”. X-ray diffractions and SEM images show the decomposition product of boiled egg white after annealing is bulk carbon, containing NaCl and KCl with a trace amount of nitrogen doping. After ultrasonic washing and centrifugation, the distilled water removed the NaCl and KCl nanocrystals from the bulk carbon completely and retained empty spaces, which eventually leads to the formation of a cheese-like structured bulk carbon with nanoholes. Our electrochemical tests show this cheese-like bulk carbon with nanoholes has a high specific capacity and good cycling performance and rate stability when evaluated as an anode material for lithium-ion batteries. Meanwhile, the electrochemical performances as an anode material for a sodium-ion battery are also displayed for comparison.
Utilizing sustainable biomass for the energy applications has received much attention in the scarcity of fossil energy. Lignin (rich in paper pulp sludge) and alginate extracted from brown algae have found interesting application in LIBs.19,20 However, proteins, another main component of biomass, are not being widely concerned on the application of energy storage at present, in our daily life, there are large quantities of protein-rich biomasses available, such as beer beverage and food industry byproducts and seaweed. Millions of chicken eggs are employed to cultivate various antibodies from the egg yolk or to extract “all natural” chemicals for anti-microbial and cosmetic industries.21 This process generates large quantities of nonedible chicken egg-based wastes, therefore, the works about these egg-based wastes on the applications of environment friendly and value-added green energy is very valuable.
In this paper, we employ egg white as a model protein-based precursor, use distilled water as a green clean “corrosive agent” and a simple annealing method for industrial production to obtain cheese-like bulk carbon with nanoholes. To demonstrate our approach, the egg white was annealing at a high temperature in reducing atmosphere, then ultrasonic washing the decomposition product in distilled water, and after centrifugation and drying we achieved cheese-like bulk carbon with nanoholes. Our electrochemical tests show this cheese-like bulk carbon with nanoholes have a high specific capacity and good performance in cycling and rate stability when evaluated as anode material for Li-ion battery compared to the Na-ion anode. Most importantly, because of its good electronic conductivity and structural stability, it also has the hope to be able to combine with other nanosize materials which as a bearer frame to improve electrochemical performance jointly in future work.
000 rpm to get black precipitations, another same twice washing and centrifugation treatments were again for this black precipitation to obtain the final cheese-like bulk carbon with nanohole products.
:
1
:
1 in N-methyl-2-pyrrolidone (NMP). The obtained slurries were coated on Cu foil uniformly and the active materials loading on electrodes were 3 mg. Two-electrode electrochemical cells were assembled in a Mikrouna glove box filled with ultra-high argon. When as Li-ion battery anode, the lithium metal foils were used as counter electrodes, Celgard 2320 as separator, and 1 M LiPF6 in EC (ethylene carbonate)
:
DMC (dimethyl carbonate) (1
:
1 vol%) was used as electrolyte. When as Na-ion battery anode, the sodium metal foils were used as counter electrodes, a glass fiber as separator, and 1 M NaPF6 in EC
:
DMC (1
:
1 vol%) was used as electrolyte. Electrochemical impedance spectroscopy (EIS) was collected on an AUTOLAB PGSTAT302N (Metrohm, Netherlands). The impedance spectra were recorded by applying an ac voltage of 5 mV in the frequency range from 1 MHz to 0.01 Hz.
The porous feature of the carbon was further investigated by Brunauer–Emmett–Teller (BET) analysis via nitrogen adsorption and desorption measurement, and the corresponding Barrett–Joyner–Halenda (BJH) pore size distribution plot are as an inset shown in Fig. 1c. The nitrogen sorption isotherm reveals a typical type IV isotherm with H3-type loop hysteresis. The adsorption jump in the isotherm appears between the partial pressures (p/p0) of 0.5–1.0 due to the capillary condensation in the porous channels and/or cages. The pore size distribution curve shows that the as-prepared cheese-like structure bulk carbon has a main pore distribution from 40 to 150 nm with a mean pore size of 85.3 nm, which corroborates the SEM observations. The specific surface area of cheese-like structure bulk carbon is calculated to be 360.6 m2 g−1. This porous structure increases the specific surface enormously, not only buffering the local volume change, but also improve the ionic conductivity by increasing the contact area between the electrode and electrolyte which will greatly contribute to the improvement of electrochemical performance discussed in following.
Since the egg white is a protein-rich biomass, to confirm whether there are main characteristic elements of protein doping in the decomposition product after heat treatment is needed. Fig. 2 shows the XPS results of C, N, S, Na, K and Cl elements before (black frame) and after (green frame) ultrasonic washing after annealing process. It reveals that there is still trace amount of nitrogen existed in the bulk carbon after annealing process. The XPS of C 1s exhibits three peaks by curve fitting, the main peak at 284.8 eV is related to the graphite-like sp2 C (C1), which indicates that most of the C atoms in the bulk carbon are arranged in a conjugated honeycomb lattice. The two weak peaks located at 285.8 eV and 288.1 eV reflect the different bonding structures of the C–N bonds, corresponding to the N–sp2 C (C2) and N–sp3 C bonds (C3) respectively.22,23 The N 1s peak can also be split into three peaks which means nitrogen atoms in the prepared bulk carbon also exist in three states, namely, pyridine-like (N1), pyrrolic (N2) and graphitic (N3) nitrogen atoms, corresponding to binding energy peaks at 398.6 eV, 400.6 eV and 403.8 eV respectively.22,23 Combined with the above results of C 1s and N 1s, we can infer that the trace amount of N is doping in the carbon structure instead of a mixture of impurity.
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| Fig. 2 XPS of C, N, S, Na, K and Cl elements before (black frame) and after (green frame) ultrasonic washing. | ||
Meanwhile, it is worth noting that there is no sulfur existed in the decomposition product from the results of XPS examination, it could attribute to pyrolysis release in the form of SOx during the annealing process. According to the XPS results of Na 1s (1071.6 eV), K 2p (292.3 eV) and Cl 2p (199.1 eV), the NaCl and KCl are removed from the bulk carbon completely after ultrasonic washing which is consistent with the EDX examination shown in Fig. 1b.
In order to describe the formation mechanism simply and vividly, we put forward a schematic diagram for this process shown in Fig. 3. When we placed the boiled egg white in a high temperature annealing for some time, the bulk carbon containing nanocrystal NaCl and KCl particles were obtained, which is similar to the jujube uniformly distributed in the jujube cake. After ultrasonic washing, the nanocrystal NaCl and KCl were removed by distilled water completely, and the places where they existed left empty spaces with nanosize which leads to the formation of cheese-like bulk carbon with nanoholes eventually.
Fig. 4a shows the typical discharge–charge curves for the first three cycles of cheese-like bulk carbon with nanoholes electrodes when as Li-ion and Na-ion anode materials. The first discharge and recharge capacities of 1183 mA h g−1 and 687.9 mA h g−1 (Li-ion anode), 386.1 mA h g−1 and 110.1 mA h g−1 (Na-ion anode) can be obtained during the first cycle, while the corresponding initial coulombic efficiencies (CEs) are 58.2% and 28.5%. The discharge capacities are larger than the recharge capacities for the first cycle, leading to the relatively poor initial CEs. This is a common drawback for these high-capacity anode materials caused by the great fading capacity between insertion and de-insertion process.9 It can be attributed to the side reactions such as formation of solid electrolyte interface (SEI) layer and irreversible reaction related to the Li and Na storage mechanism during the first insertion process discussed in Fig. 4e. After the first cycle, both of their CEs quickly increase and remain as nearly 100% thereafter, and the electrode reactions show a high reversibility as the third cycle can repeat well with the specific capacity of the second cycle for the two electrodes. From the second cycle, both of their discharge–charge capacities slowly decrease along the cycle number, after 100 cycles, charge capacities of ∼470 mA h g−1 (Li-ion anode) and ∼35 mA h g−1 (Na-ion anode) were obtained, with the capacity retentions of ∼72% and ∼31% compared to the second cycle shown in Fig. 4b. It is obviously that the electrochemical performance of Li-ion anode is much better than the Na-ion anode, this could be attributed to the smaller Li-ion radius with higher Li-ion conductivity compared to the Na-ion anode.
The first three consecutive electrochemical voltages spectroscopy (EVS) differential capacity curves are shown in Fig. 4c. Differences of discharge EVS curves with that first cycling procedure are evidences for the existence of side reactions such as the formation of SEI layer and irreversible reactions which leading to the great fading capacity shown in Fig. 4a. The number of reduction peaks for the first insertion process is more than the following cycles during the mainly phase transformation between 0.005 V and 1.0 V. It is believed that more complex side reactions and irreversible reactions happened due to a higher surface activity caused by the high specific surface area of the carbon electrode.24,25 The oxidation peaks observed in EVS curves of the 1st–3rd cycle remain fairly consistent, indicating a similar de-insertion process, and the overlapping of EVS curves in subsequent cycles reveals good reversibility of electrochemical reactions for the two electrodes.
Fig. 4d shows the rate capability of them at various discharge/charge current densities. In the 1st–10th cycle, they have reversible discharge–charge capacities of ∼580 mA h g−1 (Li-ion anode) and ∼95 mA h g−1 (Na-ion anode) at 5 mA g−1 which are consistent with the cycling stability in Fig. 4b. As the current density changed from 100 mA g−1 to 5 mA g−1 after 50 cycles, considerable higher capacity ∼510 mA h g−1 can still be recovered for the Li-ion anode electrode compared to the Na-ion anode electrode (∼50 mA h g−1), indicating a stable rate as well as a good cycling capability.
Fig. 4e shows the amount of Li+/mol and Na+/mol insertion for the two electrodes during the first cycle. As we can see, a total of 0.530 mol Li+ and 0.173 mol Na+ per formula are inserted in the electrodes during the first insertion, while 0.222 mol Li+ and 0.124 mol Na+ are residual after de-insertion in the electrodes, which means a total of 0.308 mol Li+ and 0.049 mol Na+ per formula participate in the reversible reaction for the first cycle. According to the amount of Li+/mol and Na+/mol insertion for the two electrodes during the first cycle, the following equations are proposed for this cheese-like bulk carbon system:
| C + 0.530Li+ + 0.530e− → Li0.53C | (1) |
| C + 0.173Na+ + 0.173e− → Na0.173C | (2) |
| Li0.53C → Li0.222C + 0.308Li+ + 0.308e− | (3) |
| Na0.173C → Na0.124C + 0.049Na+ + 0.049e− | (4) |
| Li0.222C + xLi+ + xe− ⇄ Li0.222+xC | (5) |
| Na0.124C + xNa+ + xe− ⇄ Na0.124+xC | (6) |
A total of 0.530 mol Li+ and 0.173 mol Na+ per formula are inserted in the initial discharge process (eqn (1) and (2)) to form an structure of Li0.53C and Na0.173C corresponding to the actual capacity of 1183 mA h g−1 and 386.1 mA h g−1. When the electrodes material were recharged to 2.5 V, only 0.308 mol Li+ and 0.049 mol Na+ per formula extracted from the electrodes with a reversible capacity of 687.9 mA h g−1 and 110.1 mA h g−1 (eqn (3) and (4)). Meanwhile, two new phases of Li0.222C and Na0.124C were completely formed, and these two phases are responsible for the subsequent reversible discharge/charge cycles (eqn (5) and (6)). That is to say, the full discharged products Li0.53C and Na0.173C cannot be returned to the original carbon material completely by the first de-insertion process and the Li0.222C and Na0.124C are the final recharged products in our voltage window. These residual 0.222 mol Li+ and 0.124 mol Na+ in the electrodes after the first de-insertion contribute to the formation of SEI layer and irreversible reaction which are responsible for the large irreversible capacity loss and poor CEs in the first cycle shown in Fig. 4a and b.
To understand the electrochemical dynamic behavior of electrodes, electrochemical impedance spectroscopy (EIS) were measured after running three cycles with an applied voltage at 2.5 V (rest for 3 hours) shown in Fig. 5. The EIS curves for the electrodes when as anode for Li-ion and Na-ion batteries are similar and the inset is an equivalent electrical circuit model for analyzing impedance spectra in Fig. 5a. Each resistance Ri, Ri||CPEi and W components are sectioned as circuit elements (i) and (ii) with W (iii) which are attributed to regions shown in the Nyquist plots.26 The depressed semicircles are indicative of inhomogeneous nature of the electrode and this is accounted for by considering constant phase elements (CPEs) instead of pure capacitors in the equivalent circuit.27–29 Amplified region of high and intermediate frequency for the two electrodes is shown in Fig. 5b. The region (i) higher than 20 kHz represented by Re is attributed to the resistance of the electrolyte and cell components. The depressed semicircle observed in the intermediate frequency range (20 kHz to 31.6 Hz and 19.9 kHz to 12.6 Hz) is attributed to section (ii), which represents the charge transfer resistance Rct, and double layer capacitance CPEct. The straight line in the low-frequency region (<31.6 Hz and <12.6 Hz) is attributed to the diffusion of the lithium or sodium ions into the bulk of electrode material. It was clear to observe that the radius of the semicircle, at the intermediate frequency region for Li-ion electrode, is smaller than the Na-ion electrode which may indicate lower charge transfer impedance leading to a better electrochemical performance compared to the Na-ion anode electrode.
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