Hyung-Seok Lim‡
a,
Daun Kim‡a,
Jun-Ki Hwanga,
Yu-Jeong Kima,
Yang-Kook Sunb and
Kyung-Do Suh*a
aDepartment of Chemical Engineering, College of Engineering, Hanyang University, Seoul, 133-791, Republic of Korea. E-mail: kdsuh@hanyang.ac.kr
bWCU Department of Energy Engineering, College of Engineering, Hanyang University, Seoul, 133-791, Republic of Korea
First published on 6th May 2015
In this study, we propose a fabrication method for highly monodisperse magnetite/carbon (Fe3O4/C) composite microspheres with a mesoporous structure. Highly monodisperse porous polystyrene (PS) microspheres are synthesized by traditional seeded polymerization. Textural properties of porous PS microspheres can be controlled by using different amounts of diluent. In order to carbonize and introduce ferrous (Fe2+) and ferric (Fe3+) ions into the pores of PS microspheres, the sulfonation reaction is carried out using sulfuric acid. Fe3O4 nanocrystals are formed in the pores as well as on the surface of the sulfonated porous PS microspheres by a simple wet chemical method. The obtained mesoporous structure of the Fe3O4/C composite microspheres is still retained after a heat treatment in a nitrogen atmosphere. The homogeneous distribution of Fe3O4 nanocrystals in the porous carbon matrix was analyzed through elemental mapping by preparing cross-sections using focused ion beam scanning electron microscopy milling. When the composite electrodes are tested as an anode material in a Li-ion half-cell, the mesoporous Fe3O4/C composite microspheres exhibit not only a high reversible capacity of 562 mA h g−1 after 100 cycles at 1 C but also good capacity retention at various current rates (0.1–10 C) with a high coulombic efficiency of above 99%.
Herein, we report an efficient strategy to homogeneously disperse nanosized Fe3O4 anodes in carbon phase and enhance the rate-capability. The highly monodisperse Fe3O4/porous carbon (Fe3O4/PC) composite microspheres are designed for the fast mass- and charge-transfer. The fabrication process of the designed composite microspheres is shown in Fig. 1. Sulfonated polystyrene microspheres (SPS) having a porous structure are synthesized as a carbon matrix for nanosized-Fe3O4 storage. Nanosized-Fe3O4 particles are formed in pores of the SPS microspheres with a homogeneous distribution by a wet chemical method using two types of Fe metal precursors. The total Fe3O4 content and specific surface area of composite microspheres depend on the total pore volume of porous polymer microspheres. Electrochemical performance measurements demonstrate that the resulting carbonized Fe3O4/C composite microspheres exhibit much higher reversible capacity than that of the porous carbon microspheres in addition to excellent cyclability and rate-capability. In particular, SPS having a larger pore volume can contain more nanosized-Fe3O4 particles increasing the specific surface area and show higher specific capacity and better capacity retention even at high current rates.
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Fig. 1 Schematic illustration of the fabrication process of the mesoporous Fe3O4/C composite microspheres. |
Sample | Conditions |
---|---|
PS-H4 | Porous PS microspheres fabricated with 4 g of heptane |
PS-H7 | Porous PS microspheres fabricated with 7 g of heptane |
SPS-H4 | Sulfonated PS-H4 |
SPS-H7 | Sulfonated PS-H7 |
PC-H4 | Carbonized SPS-H4 without Fe3O4 nanocrystals |
PC-H7 | Carbonized SPS-H7 without Fe3O4 nanocrystals |
FC-H4 | Heat treated Fe3O4/SPS-H4 composite microspheres |
FC-H7 | Heat treated Fe3O4/SPS-H7 composite microspheres |
Fig. S1† shows OM and SEM images of polymer particles of each step during the seeded polymerization process. Fig. 2 shows optical microscopy (OM) images of PS-H4 (a), PS-H7 (c), SPS-H4 (b) and SPS-H7 (d), which had porous structures and spherical shapes. The average diameters of the porous PS microspheres increased from 7.9 to 9 μm with higher heptane content, as shown in Fig. 2a and c. After sulfonation of PS-H4 and PS-H7, a yellow colored powder was obtained, and their intrinsic shapes were still retained, as shown in Fig. 2b and d. Fig. S2† shows SEM images of highly monodisperse porous SPS microspheres. The incorporation of SO3− functional groups to the porous PS microspheres was confirmed by IR spectroscopy measurements.
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Fig. 2 OM images of porous PS microspheres: (a) PS-H4 and (c) PS-H7, and porous PS microspheres after sulfonation: (b) SPS-H4 and (d) SPS-H7. |
Fig. 3 shows IR spectra of the porous PS microspheres before (a and b) and after (c and d) sulfonation for 24 h. The porous SPS microspheres have a broad absorption band in the region of 1320–1052 cm−1 and a sharp absorption band at 1000 cm−1 due to the stretching vibrations from the incorporation of SO groups, as shown in Fig. 3c and d. The porous PS microspheres were successfully sulfonated by acid treatment using sulfuric acid.
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Fig. 3 FT-IR spectra of porous PS microspheres: (a) PS-H4 and (b) PS-H7, and sulfonated porous PS microspheres: (c) SPS-H4 and (d) SPS-H7. |
After Fe3O4 nanoparticles are formed in SPS microspheres, Fe3O4/SPS composite microspheres were obtained. Fig. 4 shows SEM images of the (a) Fe3O4/SPS-H4, (d) Fe3O4/SPS-H7, (b) Fe3O4/C-H4 (FC-H4) and (e) Fe3O4/C-H7 (FC-H7) at low (larger images) and high magnification (insets). After incorporation of Fe ions into the porous SPS microspheres, Fe3O4 nanocrystals were formed by a wet chemical reaction in the presence of ammonium hydroxide. The residual clusters consisting of Fe3O4 nanocrystals are not observed in Fig. 4a and d because the supernatant containing residual Fe ions was removed after introduction of the iron ions into the porous SPS microspheres. Fig. 4b and e show the carbonized-Fe3O4/SPS-H4 and Fe3O4/SPS-H7, which were heat treated at 600 °C for 7 h under a nitrogen atmosphere. Although the average diameters of both samples decreased after heat treating for a long time at a high temperature, as shown in Fig. 4b and e, their porous structures were still retained without collapse, as shown in cross-sectional images of Fig. 4c and f.
The internal small images of Fig. 4c and f are cross-sectional EDX mapping images of FC-H4 and FC-H7, which indicate that Fe3O4 nanocrystals are well dispersed in a carbon matrix (yellow colored dots display Fe atoms).
Fig. 5 shows the XRD patterns of (a) FC-H4 and (b) FC-H7. Both samples show main peaks at 2θ = 30.09°, 35.43°, 43.00°, 54.07°, 57° and 62.5°, which are about the typical XRD peaks of crystalline Fe3O4. Broad peaks corresponding to disordered carbon patterns were observed in the overall region. These results demonstrate that Fe3O4 nanocrystals were contained in the disordered carbon matrix, as shown above in cross-sectional mapping images in Fig. 4c and f. In addition, it seems that peak broadening of FC-H7 is sufficiently larger than FC-H4. According to this result, it can be estimated by using the (311) peak that crystallite size of Fe3O4 contained in FC-H7 is smaller than that of FC-H4.
Fig. 6 exhibits nitrogen adsorption–desorption isotherms and BJH pore-size distributions of SPS-H4, SPS-H7, FC-H4 and FC-H7. The distribution in pore size of porous SPS microspheres was relatively broad (10–160 nm), as shown insets in Fig. 6a and b. However, Fe3O4/C composite microspheres showed a narrow pore-size distribution below 10 nm because nano-sized Fe3O4 crystals were formed in pores and on the surface of SPS microspheres before carbonization. Nitrogen adsorption–desorption isotherms of the FC-H4 and FC-H7 exhibit isotherms of type IV of the IUPAC classification featuring a pronounced step due to the capillary condensation and desorption of nitrogen gas, which demonstrates Fe3O4/C composite microspheres have large mesopores. Differences in specific surface area, total pore volumes and average pore sizes of SPS-H4, SPS-H7, FC-H4 and FC-H7 analyzed by BET and BJH methods were summarized in Table 2. The total pore volumes of SPS-H4 and SPS-H7 were 0.273 cm3 g−1 and 0.423 cm3 g−1, respectively. As mentioned above, using more heptane increased the average diameter of the polymerized porous microspheres. The total pore volume of SPS-H7, having similar average pore size to SPS-H4, was larger than that of SPS-H4.
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Fig. 6 Nitrogen adsorption–desorption isotherms and (insets) BJH pore-size distributions of (a) SPS-H4, (b) SPS-H7, (c) FC-H4 and (d) FC-H7. |
Sample | Specific surface area (m2 g−1) | Total pore volume (cm3 g−1) | Average pore radius (nm) |
---|---|---|---|
SPS-H4 | 18.5 | 0.273 | 15.5 |
SPS-H7 | 19.9 | 0.423 | 15.4 |
FC-H4 | 110.8 | 0.296 | 1.9 |
FC-H7 | 232.5 | 0.504 | 1.9 |
Fe3O4/C composite microspheres showed a dramatic increase of specific surface area due to the nano-sized Fe3O4 crystals. Especially, the specific surface areas of FC-H7 increased more than 10 times because of the higher content and smaller crystallite size of Fe3O4 formed in pores than those of FC-H4 as mentioned above in Fig. 5. Thermogravimetric analysis (TGA) thermograms of the FC-H4 and FC-H7 are shown in Fig. 7. The TGA measurement was used to reveal the chemical composition of the final composite microspheres. The first weight loss took place at below 200 °C, which corresponds to the evaporation of the weakly adsorbed moisture and decomposition of other small molecules like labile oxygen functional groups. Then, the mass of samples slightly increased because of the oxidation of Fe3O4 nanocrystals adsorbed onto the surface of the composite microspheres. The rapid weight loss arose between 380 °C and 450 °C, which can be attributed to oxidation of carbon with oxygen injected during measurement.
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Fig. 7 TGA plots of (black line) FC-H4 and (red line) FC-H7 under an air conditions at a heating rate of 5 °C min−1. |
Although both TGA curves exhibited similar weight loss trends, the FC-H7 had a higher residual weight of 34.8 wt% than that of 30 wt% for the FC-H4. This indicates that the porous SPS microspheres, having larger pore volumes could contain a higher content of Fe3O4 nanocrystals via a wet chemical method.
In order to compare the electrochemical performance of the Fe3O4/C microspheres, porous carbon microspheres without Fe3O4 nanocrystals were prepared and their electrochemical properties were confirmed. The morphologies of the black-colored powder and characteristics were confirmed by SEM and Raman spectroscopy, as shown in Fig. S3 and S4.† SEM images show two spherical porous carbon spheres with different particle size named PC-H4 and PC-H7. In the Raman spectrum of the PC-H4, the G band was broadened and shifted to 1592 cm−1, and a broad D band at 1336 cm−1 also appears. The Raman spectrum of PC-H7 also contained both D and G bands (at 1592 cm−1 and 1335 cm−1, respectively). The D/G intensity ratio of the PC-H4 and PC-H7 had values of 0.724 and 0.736. Therefore, the PC-H4 and PC-H7 were composed of hard carbon having graphite and a disordered structure.
All voltage profiles were measured at a 1 C-rate except the first two cycles at a 1/20 C rate. The voltage profiles of the (a) PC-H4 and (b) PC-H7 for the first three cycles and 100th cycle are shown in Fig. S5.† Both the PC-H4 and PC-H7 composite electrodes show a similar staging process evolving at the typical low voltage values where Li-ion insertion occurs in a carbonaceous matrix at the first discharge curve. In the charge process, a similar trend of Li ion extraction is also seen in the first charge curves of the PC-H4 and PC-H7 electrodes. The initial large irreversible capacities (756 and 750 mA h g−1) of both samples are expected phenomena that result from the decomposition of electrolyte and the formation of a solid electrolyte interface (SEI) layer on the surface of active materials. The voltage profiles of the FC-H4 and FC-H7 are shown in Fig. 8a and b. Both Fe3O4/carbon composite electrodes exhibit similar first discharge curves with a small voltage plateau at around 1.5 V, which can be attributed to the formation of LixFe3O4 intermediates. The voltage plateau at around 0.8 V was also seen in both electrodes, and should be attributed to the reaction Fe3O4 + 8Li+ + 8e− ↔ 3Fe0 + 4Li2O. In the first charge process, two small plateaus were observed at about 1.6 V and 1.9 V, corresponding to the oxidation of Fe0 to Fe2+ and Fe3+, respectively.10 The FC-H4 and FC-H7 composite electrodes show smaller irreversible capacities in the first discharge process and higher reversible capacities at all cycles compared to those of PC-H4 and PC-H7. Fig. 8c shows cycling performance of the (inverted triangle) PC-H4, (triangle) PC-H7, (square) FC-H4 and (circle) FC-H7 composite electrodes, tested between 0.02 and 3.0 V at the rate of 1/20 C (first two cycles) and 1 C up to 100 cycles. All electrodes show good cyclability with high efficiency (>99%) at all cycles, as shown in Fig. 8c. Among all electrodes, the capacity of FC-H7 electrodes was highest, which showed good capacity retention without capacity decay even after 100 cycles at 1 C rate.
The higher reversible capacity of FC-H7 than that of the FC-H4 electrode was expected from the larger total pore volume, about two times that of FC-H4, and a higher amount of Fe3O4 nanocrystals in the carbon matrix. Although the FC-H4 and FC-H7 electrodes have a large amount of Fe3O4 nanocrystals, 30 to 35 wt%, they exhibit excellent cycle performance because the mesopores in the carbon matrix accommodate the volume variation of nanosized-Fe3O4 during electrochemical processes. The rate performance is evaluated by discharging at 0.2 C and charging at various current rates in the voltage range of 0.02–3.0 V and displayed in Fig. 8d. FC-H4 and FC-H7 electrodes exhibit high capacity at all current rates due to the narrow size distribution and porosity of the Fe3O4/C composite microspheres. In particular, the FC-H7 electrode exhibits a higher discharge–charge capacity than that of the FC-H4 electrode because of a higher amount of Fe3O4 nanocrystals, as shown in Fig. 7. The discharge capacities at different current rates are 642, 570, 565, 563, 529 and 512 mA h g−1 at 0.1, 0.2, 0.5, 1, 5 and 10 C, respectively. The capacity ultimately returns to above 640 mA h g−1 at 0.1 C. In addition, the capacity retention is better than that of the FC-H4 electrode with high columbic efficiency. The higher capacity and better rate capability of the FC-H7 electrode are mainly attributed to more Fe3O4 nanocrystals in an amorphous carbon matrix, lots of mesopores and higher specific surface area, as mentioned above. Existing mesopores not only provide the volume for expansion of Fe3O4 nanocrystals, but it also allows for more efficient transport of electrons and Li-ions during the lithiation–delithiation processes. To demonstrate the improvement of our Fe3O4/C composite materials, we also tested the electrochemical performance of coin-cell made with bare Fe3O4 nanoparticles. This bare Fe3O4 composite electrode was prepared under the same condition with other electrodes that we made (active material:
super-P
:
binder = 7
:
1
:
2, w/w/w). Fig. S6† exhibits the (a) cycling performance (1 C) and (b) the specific capacity as a function of the various cycling rates (0.1–5 C) of bare Fe3O4 composite electrode. The discharge capacities were about 30 mA h g−1 from third cycle to 100th cycle while the first discharge capacity at 0.05 C was about 1500 mA h g−1, as shown in Fig. S6a.† The rapid capacity fading was also observed in the C-rate test (Fig. S6b†). In light of these results, the porous carbon matrix acts an important role for the prevention of capacity fading.
To understand the textural effect of porous Fe3O4/C composite microspheres on the kinetics of the charge- and mass-transfer reaction, the electrochemical impedance spectroscopy (EIS) analysis was performed. Fig. 9a shows Nyquist plots of FC-H4 and FC-H7 composite electrodes (red circle and black square) at 100th cycle. The electrochemical system can be modeled by an equivalent circuit as shown in Fig. 9b. Fig. 9 exhibited two overlapping semi-circles at high frequency. The high frequency one is attributed to the SEI film resistance (RSEI). The medium frequency one is associated with the double-layer capacitance (Cdl) and charge-transfer resistance (Rct) of Fe3O4/C composite electrodes. In low frequency, the Warburg-type straight lines show an angle approaching 68.8° and 45.3° to the Z′-axis indicating that the resistance associated the mass transfer depends on the porosity and the surface area of Fe3O4/C composite electrodes. According to the fitted values for two types of cells, the radius of semi-circles at medium frequency of FC-H7 composite electrode is smaller than that of FC-H4 composite electrode while the semi-circles at high frequency are similar, which indicated that the charge transfer resistance of FC-H7 (195 Ω) composite cell is smaller than that of the cell made with FC-H4 (268 Ω). Due to the much higher specific surface and larger pore volume which improve electrochemical kinetic characteristics of Li-ions, FC-H7 composite electrode exhibited better capacity retention even at high current rates.
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Fig. 9 (a) Nyquist plots of (red circle) FC-H4 and (black square) FC-H7 composite electrodes at 100th cycle. (b) The equivalent circuit used to model the impedance spectra. |
Footnotes |
† Electronic supplementary information (ESI) available: OM images of synthetic process; SEM images of porous PS microspheres after sulfonation process; SEM images and Raman spectra of the heat-treated SPS microspheres; voltage profiles of PC-H4 and PC-H7; cycling and C-rate performance of the bare Fe3O4 electrode. See DOI: 10.1039/c5ra05732a |
‡ These authors contributed equally to this work. |
This journal is © The Royal Society of Chemistry 2015 |