Feixiang Wu,
Zhixing Wang*,
Xinhai Li and
Huajun Guo
School of Metallurgy and Environment, Central South University, Changsha 410083, P.R. China. E-mail: zhixing.csu@gmail.com; Fax: +86-731-88836633; Tel: +86-731-88836633
First published on 7th August 2014
The low cost production of Ti-containing nanomaterials from natural resources is an attractive method for producing materials suitable for the growing energy storage industry. In this work, natural ilmenite is transformed into either Li4Ti5O12 microspheres or TiO2 nanowires through a series of chemical and thermal processes by crossing metallurgy and material science. The produced well-crystallized Li4Ti5O12 microspheres are composed of nanosized particles that show high cycle stability, coulombic efficiencies, and rate capability for C-rates as high as 20 C. The initial discharge capacities are 173.1, 168.5, 167.2, 163.4, 160.0, 155.4 and 142.7 mA h g−1 at the 0.1, 0.5, 1, 2, 5, 10 and 20 C-rates, respectively. After 100 cycles, the as-prepared Li4Ti5O12 retains 99.1%, 98.9%, 96.8% and 91.8% of its initial discharge capacities at the 2, 5, 10 and 20 C-rates, respectively. The synthesized echinus-like anatase TiO2 nanowire aggregations also demonstrate excellent cycling performance, even at high current densities.
Graphite is the current industry anode material for Li-ion batteries; however, it has limitations. First, the theoretical capacity is lower than many other materials, which can intercalate or alloy with Li. Second, the low potential for lithium intercalation can lead to the lithium plating during charging. Li commonly plates as dendrites, which have significant safety concerns. Another issue originates from the charge consumption required to form the solid electrolyte interphase (SEI) layer that is essential to electrode stability in terms of the capacity, power retention, and cycle life.6–10
Spinel lithium titanate (Li4Ti5O12) and anatase titanium dioxide (TiO2) have been viewed as two promising alternative anode materials to graphite in Li-ion batteries.11–15 Spinel Li4Ti5O12 has a theoretical capacity of 175 mA h g−1 with high deintercalation reversibility.16–18 Due to the flat Li+ insertion potential of ∼1.55 V for Li4Ti5O12, above the reduction potential of electrolyte solvents, a SEI film will not form on Li4Ti5O12, which may allow for a reduced irreversible capacity. Further, as a “zero-strain” insertion material, it has an excellent cycling performance. In comparison, anatase TiO2 is a fast Li insertion/extraction host with an insertion potential ∼2.0 V, low volume expansion (3–4%) during lithium insertion, and a high theoretical capacity of 336 mA h g−1.19,20 These features make them two promising anode materials for large-scale long-life energy storage batteries. However, both of them are still far away from being perfect because of their low electronic conductivity, which limits their rate stability.
Nanostructured TiO2 and Li4Ti5O12 are conventionally prepared from TiO2 or Ti-based organic compounds. Generally, these highly pure raw compounds are prepared from Ti-containing ores or other Ti slag via complex, expensive, energy consuming processes that remove impurities. In this paper, new methods to synthesize nanostructured TiO2 and Li4Ti5O12 from natural ilmenite (FeTiO3) through a series of easily replicated processes are proposed: TiO2 nanowire synthesis by a high temperature hydrothermal method and Li4Ti5O12 microspheres synthesis by spray drying. Natural ilmenite (FeTiO3) is one of the primary global sources of titanium dioxide. In China, commercially, pigment grade titanium dioxide is mainly produced by complex sulfate processes with the generation of a large amount of waste acidic iron(II) solutions and FeSO4·7H2O waste slag, which causes not only severe environmental problems but also a waste of iron resources. Finally, the obtained pigment grade titanium dioxide is often used to prepare high purity nanostructured TiO2 and organic Ti-contained compounds by using complex metallurgical extraction and materials preparation processes, which are extensively used in coatings, paper, porcelain, plastics, catalysts, cosmetics, gas sensors and energy.
In previous publications, we used hydrochloric acid as a leachant to dissolve mechanically activated ilmenite to obtain a lixivium (or filtrate), which was used to prepare LiFePO4.21,22 In this process, another product of the hydrolyzed titania residue was used to prepare Li4Ti5O12 directly after two-step alkaline leaching.23 The obtained Li4Ti5O12 particles were not uniform and the electrochemical performance was very poor.23 The obtained hydrolyzed titania residue was hard to use by the chlorination process. Owing to its high chemical activity and reaction with H2O2 and NH3·H2O, Ti could be easily and selectively extracted from the high Ti-containing residue by alkaline-hydrogen peroxide leaching.24 The lixivium from the hydrolyzed titania residue was used to synthesize TiO2 nanosheets from which Li4Ti5O12 was prepared; however, the performance was poor and this method consumed significant LiOH.25
In this work, we combine the metallurgical extraction and materials preparation together to develop a series of short processes to synthesize Li-ion battery anode materials TiO2 and Li4Ti5O12 from natural ilmenite. In this method, TiO2 does not need to be prepared from the lixivium of the ammonia titanium peroxide solution, as in previous work.25 Here, only LiOH was added into the lixivium to obtain a lithium (ammonia) titanium peroxide solution which was used to prepare Li4Ti5O12 microspheres. Moreover, the addition of NaOH to the lixivium of the ammonia titanium peroxide solution has a profound significance of not only decreasing the content of SiO2 in the TiO2, but also forming uniform TiO2 nanowires.
The major element of Ti in ilmenite is utilized to prepare high performance TiO2 and Li4Ti5O12, which can be used in Li-ion batteries. The produced Li4Ti5O12 microspheres show a very good performance, even better than our results using analytically pure and organic titanium compounds.26,27 The produced TiO2 nanowires also show a good performance and high purity; thus, through these methods, stable Li-ion materials can be synthesized using processes that reduce redundancy, reduce the cost of production, and reduce the negative environmental impact from the hazardous waste slag and acid to environment.
TiO2 | FeO | Fe2O3 | MgO | SiO2 | Al2O3 | CaO | MnO2 |
---|---|---|---|---|---|---|---|
47.60 | 32.81 | 7.25 | 5.64 | 3.35 | 1.66 | 0.70 | 0.663 |
FeTiO3 + 4HCl → Fe2+ + TiOCl42− + 2H2O | (1) |
![]() | (2) |
The lixivium of the ammonia titanium peroxide solution was prepared by alkaline-hydrogen peroxide leaching of the hydrolyzed titania residue via previously reported methods.24,25 The hydrolyzed titania residue powder (5 g) was placed in a 500 ml round-bottomed flask, which was attached to a reflux condenser. 10 wt% ammonia solution (60 g) was added in the flask and a white slurry was observed. The white slurry was maintained at 35 °C in a thermostatically controlled water bath, equipped with a digitally controlled thermometer (within ±2 °C). Hydrogen peroxide solutions containing 10 wt% H2O2 (180 g) was then added to the white slurry to react with Ti under vigorous stirring of 300 rpm. After 20 min, the solution was rapidly cooled and filtered, and then aqueous ammonia titanium peroxide solution was obtained according to eqn (3).
TiO2·nH2O + H2O2 + NH3·H2O → (NH4)x(TiOy)(O2)z(OH)j(dissoluble) + H2O | (3) |
![]() | (4) |
14 mm diameter electrodes with typical mass loadings of 1.95–2 mg cm−2 were tested in 2025-type coin cells versus metallic Li. The produced electrodes were composed of 80 wt% Li4Ti5O12 (or TiO2) powders, 10 wt% carbon black, and 10 wt% poly(vinylidene fluoride) as the binder. After mixing in N-methyl pyrrolidinone, the slurry was uniformly cast on a thin copper foil and dried in vacuum for 12 h at 120 °C. Note that an electrolyte of LiPF6 in carbonate (EC:
EMC
:
DMC = 1
:
1
:
1 by volume) was used, and a polypropylene separator was used. Cells were assembled in a dry argon-filled glove box and were charged and discharged at room temperature over voltage ranges of 1.0–2.5 V and 1.0–3.0 V for Li4Ti5O12 and TiO2 versus Li/Li+, respectively.
The voltage profiles of Li4Ti5O12 microspheres at room temperature in the charge–discharge test at various current densities are shown in Fig. 4. The cell was first cycled at C/10 for 3 cycles, C/2 for 5 cycles, 1 C for 50 cycles, 2 C for 100 cycles, 5 C for 100 cycles, 10 C for 100 cycles, 20 C for 100 cycles, and then returned to 0.1 C for 10 cycles. At all C-rates, the charge–discharge curves exhibit a long and flat voltage plateau. In the first discharge process, the as-prepared Li4Ti5O12 electrode exhibits a remarkably high initial discharge capacity at 0.1 C-rate, up to 173.1 mA h g−1, which is almost equal to its theoretical capacity (175 mA h g−1). The subsequent Li+ extraction, proceeding up to 2.5 V, shows a capacity of 170.2 mA h g−1, with a high coulombic efficiency (ratio of extraction to insertion capacity) of 98.32%. By increasing the C-rate, the cell shows 168.5, 167.2, 163.4, 160.0, 155.4 and 142.7 mA h g−1 at 0.5, 1, 2, 5, 10 and 20 C-rates, respectively. The capacities at all charge–discharge rates are much larger than other Li4Ti5O12 and Li4Ti5O12/C electrodes made by chemically pure or analytically pure Titanium compounds.26–44 Moreover, the cycling performance of the as-prepared Li4Ti5O12 is shown in Fig. 4(b). As can be seen, the cycling curves of discharge and charge coincided with each other, indicating a high coulombic efficiency in the charge/discharge of this cell. At all the current densities, after 50 or 100 cycles, the as-prepared Li4Ti5O12 electrode retains 97.9%, 99.1%, 98.9%, 96.8% and 91.8% of its initial discharge capacities at the 1, 2, 5, 10 and 20 C-rates, respectively. In the last 10 cycles at C/10 rate, the charge capacity of 459th retains 103.9% of 468th charge capacity. The excellent electrochemical performance might be attributed to the as-prepared Li4Ti5O12 microspheres obtained by this novel method and natural ilmenite. The as-produced Li4Ti5O12 microspheres composed of nanoparticles of around 100 nm contained a rough surface and inside pores. These nanosized Li4Ti5O12 particles connected with each other forming an interconnected Li4Ti5O12 nano-network, which provides a massive interface among the nanoparticles and can be the bridge for electron and Li+ transport through a shorter path within and between the nano-particles. Moreover, the inside pores make a larger electrode–electrolyte contact area for Li+ insertion/extraction in the rough and porous spherical particles. Therefore, the as-prepared Li4Ti5O12 shows an excellent high-rated cycling performance, which is better than our previous Li4Ti5O12 microspheres obtained by chemically pure or analytically pure titanium compounds (Table 2).
Samples | Discharge capacities (mA h g−1) at different C-rates | Cycling performances (%) at different C-rates | |||||||||
---|---|---|---|---|---|---|---|---|---|---|---|
0.1 C | 0.5 C | 1 C | 2 C | 5 C | 10 C | 20 C | 2 C | 5 C | 10 C | 20 C | |
Ti(OC4H9)4-organic26 | 174.8 | 170.5 | 167.5 | 165.3 | 158.2 | 152.1 | 111.9 | 96.9 | 98.8 | 89.3 | 89.0 |
Ilmenite-this work | 173.1 | 168.5 | 167.2 | 163.4 | 160.0 | 155.4 | 142.7 | 99.1 | 98.9 | 96.8 | 91.8 |
Fig. 4(c) shows the first and 468th charge–discharge curves of Li4Ti5O12 at C/10 rate. After a total of 450 cycles at miscellaneous current densities, the cell returns to C/10 and still retains a remarkably high discharge capacity of 168.8 mA h g−1 which is 97.6% of the initial discharge capacity at 0.1 C-rate. As can be seen in Fig. 4(d), all of the five cycles have a sharp pair of cathodic/anodic peaks centered at 1.50 V and 1.63 V, corresponding to the lithium insertion/extraction in the spinel Li4Ti5O12 lattice, which are in accordance with the plateaus of the discharging–charging curves. The measured value of the ratio for peak currents ipa/ipc is nearly 1, and the integral voltammetric area of the discharging–charging branches is almost equal. Moreover, after 471 cycles, 5 cyclic voltammograms coincided with each other, indicating very perfect coulombic efficiency. After comparing the SEM images of the electrodes before and after cycling in Fig. 4(e) and (f), the nano-micron structure is still maintained and stable after ∼500 cycles, which is due to the “zero-strain” during charge and discharge. As can be seen from the results in Fig. 4, this Li4Ti5O12 shows a very steady-going structure, high capacities and high cycling performance even after hundreds of cycles at high C-rates.
When boiling the sodium titanium peroxide solution, the H2O2 is gradually decomposed. Due to the interfacial tension, van der Waals attractive forces, and other factors, the titanate nucleus would aggregate together to form “multi-nuclei.” Subsequently, the titanate “multi-nuclei” gradually grow up and assemble into a micro spherical shape along with H2O2 decomposition. The precursor is calcined at 300 °C for 3 h to synthesize anatase TiO2. As shown in Fig. 2(g)–(i), the morphology images of the precursor and as-prepared TiO2 are the similar echinus-like structure with a diameter about 0.5–1.5 μm, which shows a high BET SSA of 20.2 m2 g−1. The as-prepared TiO2 maintains the morphology of the precursor, which is attributed to the low calcined temperature. The enlarged image of the particles of the as-prepared TiO2 in Fig. 5(a) shows that the spherical particles or microspheres are composed of aggregated nanowires, which is consistent with the TEM images (Fig. 5(b) and (c)). As shown in Fig. 5(b) and (c), the morphology images of the as-prepared TiO2 are the echinus-like structure with aggregated nanowires. These nanowires are acicula-shaped with a diameter in the range of 14.4 nm and a length of about 200–500 nm. From Fig. 2(g), there is no obvious circle in the inset SAED pattern, indicating that there is no appearance of crystalline phases, which is in accordance with the XRD results of the precursor. However, the SAED pattern in Fig. 5(e), with several marked rings corresponding to TiO2 (1 0 1), (0 0 4), (2 0 0) and (2 1 1) planes, can be indexed to anatase TiO2 (JCPDS card no. 65-5714). Fig. 5(f) shows the HRTEM images of the as-prepared TiO2 nanoparticles. As can be seen, there is a lattice fringe with a lattice spacing of about 3.51 Å, corresponding to (1 0 1) inter planar spacing of TiO2, which indicates the well-crystallized anatase phase in the nanostructured materials. The inset SAED patterns are obtained by Fourier transformation in a selected area of the HRTEM images. The inset FFT image in Fig. 5(f) also gives a sharp spot, corresponding to the (1 0 1) plane of anatase TiO2.
Fig. 6(a) shows the initial three potential-capacity profiles of anatase TiO2 at the current density of 20 mA g−1. In these three cycles, the charge–discharge curves exhibit a long and flat voltage plateau at about 1.77 and 1.88 V for discharging and charging, respectively. In the first discharge process, anatase TiO2 shows 291.9 mA h g−1 at a current density of 20 mA g−1. The subsequent Li+ extraction of anatase TiO2 shows a capacity of 248.2 mA h g−1. It displays a relative low coulombic efficiency (ratio of extraction to insertion capacity) and a large irreversible capacity. However, in the subsequent two cycles, the discharge–charge curves gradually coincided with each other, indicating a lower irreversible capacity and a higher coulombic efficiency. The fade of the curve between the first and subsequent cycles shows the large irreversible process after the insertion of Li into the TiO2 anatase structure. This phenomenon is tentatively ascribed to the side reaction of trace surface adsorbed water because of the large specific surface area. The trace water in the anatase TiO2 could react irreversibly with lithium forming Li2O inside the inter layers or on the surface, which is the major reason for the larger capacity loss. The discharging–charging tends to be stabilized in the following cycles, because the binding water is consumed gradually during the first several cycles.45,46 Fig. 6(b) shows the CV pattern of the anatase TiO2 electrodes. Three cathodic peaks of lithium insertion can be found in the voltammogram near 1.50, 1.55 and 1.71 V vs. Li+/Li; moreover, three anodic peaks of lithium extraction at 1.55, 1.67 and 2.03 V vs. Li+/Li are observed. The sharp pair of peaks (1.71 and 2.03 V) appears to be the lithium insertion/extraction in the anatase TiO2 lattice, which is in accordance with the plateaus of the discharging–charging curves in Fig. 6(a); however, the other two pairs at the lower potential region are characteristic of the capacitive charging process, which may represent a different mechanism of lithium intercalation into the TiO2 host.45
Fig. 7(a) shows the discharge and charge capacities of TiO2 at different current densities. The cell was first cycled at 20 mA g−1 for 3 cycles, 100 mA g−1 for 5 cycles, 200 mA g−1 for 20 cycles, 400 mA g−1 for 50 cycles, 1000 mA g−1 for 100 cycles, 2000 mA g−1 for 100 cycles, and then returned to 20 mA g−1 for 10 cycles. At all current densities, the charge–discharge curves exhibited obvious and flat voltage plateaus. The initial discharge capacities of TiO2 are 291.9, 230.9, 222.6, 202.7, 177.3 and 142.6 mA h g−1 at the current densities of 20, 100, 200, 400, 1000 and 2000 mA g−1, respectively. Moreover, the cycling performance of TiO2 is shown in Fig. 7(b). As can be seen, TiO2 shows a very good cycling performance. After 20 cycles, the TiO2 retains 96.8% of the initial charge capacity at the current density of 200 mA g−1. At the current density of 400 mA g−1, TiO2 retains 95.6% of the initial charge capacity after 50 cycles. After 100 cycles, TiO2 retains 91.9% and 86.9% of the initial charge capacities at the current densities of 1000 and 2000 mA g−1, respectively. Compared to the previous TiO2 nanowires prepared by same method using organic titanium compounds, the produced TiO2 nanowires in this work show a better rate performance as can be seen in Table 3. (We cannot compare the cycling performance due to the different cycling programs.) Fig. 7(c) shows the second and 288th charge–discharge curves of the anatase TiO2 at a current density of 20 mA g−1. After a total of 270 cycles at 200, 400, 1000 and 2000 mA g−1, the cell returns to 20 mA g−1 and still exhibits a remarkably high discharge capacity of 227.3 mA h g−1, which is 89.3% of the second discharge capacity at 20 mA g−1. As can be seen from the results in Fig. 7, the anatase TiO2 prepared by natural ilmenite shows a very steady-going structure, a high capacity and a high cycling performance even after hundreds of cycles at high current densities.
Samples | Discharge capacities (mA h g−1) at different current densities | Cycling performances (%) at different current densities | ||||||
---|---|---|---|---|---|---|---|---|
200 mA g−1 | 400 mA g−1 | 1000 mA g−1 | 2000 mA g−1 | 200 mA g−1 | 400 mA g−1 | 1000 mA g−1 | 2000 mA g−1 | |
Ti(OC4H9)4-organic47 | 221 | 195 | 117 | 90 | 82 (50 cycles) | 96 (50 cycles) | 96 (50 cycles) | 94 (50 cycles) |
Ilmenite-this work | 222.6 | 202.7 | 177.3 | 142.6 | 96.8 (20 cycles) | 95.6 (50 cycles) | 91.9 (100 cycles) | 86.9 (100 cycles) |
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