Li4Ti5O12/graphene nanoribbons composite as anodes for lithium ion batteries
© Medina IV. et al. 2015
Received: 28 May 2015
Accepted: 14 October 2015
Published: 26 October 2015
In this paper, we report the synthesis of a Li4Ti5O12/Graphene Nanoribbons (LTO/GNRs) composite using a solid-coating method. Electron microscope images of the LTO/GNRs composite have shown that LTO particles were wrapped around graphene nanoribbons. The introduction of GNRs was observed to have significantly improved the rate performance of LTO/GNTs. The specific capacities determined of the obtained composite at rates of 0.2, 0.5, 1, 2, and 5 C are 206.5, 200.9, 188, 178.1 and 142.3 mAh·g−1, respectively. This is significantly higher than those of pure LTO (169.1, 160, 150, 106 and 71.1 mAh·g−1, respectively) especially at high rate (2 and 5 C). The LTO/GNRs also shows better cycling stability at high rates. Enhanced conductivity of LTO/GNRs contributed from the GNR frameworks accelerated the kinetics of lithium intercalation/deintercalation in LIBs that also leads to excellent rate capacity of LTO/GNRs. This is attributed to its lower charge-transfer resistance (Rct = 23.38 Ω) compared with LTO (108.05 Ω), and higher exchange current density (j = 1.1 × 10−3 mA cm−2)—about 20 times than those of the LTO (j = 2.38 × 10−4 mA cm−2).
KeywordsLIBs, Li4Ti5O12 Graphene nanoribbons Anode Capacity
As a most effective and practical technology, lithium ion batteries (LIBs) continue to provide a promising solution to increasing energy demands of portable devices such as mobile phones and laptops. LIBs are also explored as promising for electric vehicles (EVs), hybrid electric vehicles (HEVs) and energy storage systems in terms of their high power density, long cycle life and high safety(Armand and Tarascon 2008; Scrosati and Garche 2010).
Lithium titanate (Li4Ti5O12, LTO) is regarded as a favorable anode material, since the traditional carbon/graphite materials have shown some critical issues including poor cyclic life; and high reactivity with the electrolyte solution that easily contributes to the thermal runaway of batteries under certain reported conditions (Yao et al. 2005). Li4Ti5O12 anode material is a zero-strain insertion material whose lattice dimension does not change during charge/discharge processes, and is thus ideal for long-life rechargeable batteries (Ohzuku et al. 1995). LTO with a theoretical capacity of 175 mAh·g−1 has excellent Li+ insertion and extraction reversibility in the voltage range of 1.0–2.5 V. Additionally, LTO has a very flat voltage plateau close to 1.55 V (vs. Li/Li+), which sufficiently avoids the formation of metallic lithium, thus resulting in improvement of the safety of lithium-ion batteries (Zhang and Li 2013). However, one practical problem associated with unmodified Li4Ti5O12 is its poor rate performance, resulting from its inherent low electronic conductivity and moderate Li+ diffusion coefficient (Kavan et al. 2003; Wagemaker et al. 2008; Ouyang et al. 2007). Numerous strategies amongst others have been attempted to improve Li4Ti5O12 such as tailoring the particle size of the materials to the nanometer-scale, doping with other elements, and coating with different carbon materials (Zhang and Li 2013; Jung et al. 2011; Hao et al. 2005; Kim et al. 2010; Sorensen et al. 2006; Yi et al. 2010).
Graphene nanoribbons (GNRs) are strips of graphene with outstanding electronic properties. GNRs have been used in a wide range of device materials (Han et al. 2007; Jian et al. 2012; Kosynkin et al. 2009; Jiao et al. 2009). Recent theoretical and experimental studies have shown that GNRs can enhance lithium storage capacity through edge effect (Uthaisar et al. 2009; Bhardwaj et al. 2010). On the basis of the unzipping mechanism (Uthaisar et al. 2009; Bhardwaj et al. 2010), a large number of edge sites are created during the formation of GNRs, which might produce more electrochemically active sites for charge transfer during charge/discharge when compared to graphene and carbon nanotubes. Moreover, GNRs, having large aspect ratios and high surface area, might provide an excellent conductive matrix with good mechanical flexibility for anode or cathode materials to accommodate the volume changes during change/discharge cycles. GNRs composited with SnO2 (Dong et al. 2015), Fe3O4 (Lin et al. 2014) and MnO2 (Li et al. 2013) have been reported as anodes, with V2O5 (Yang et al. 2014) as cathodes in LIBs. Those results have demonstrated that the formation of more edge sites in GNRs does not lead to a loss in the conductivity of the composites. However, to date, the use of GNRs to stimulate enhanced LTO electrochemical performance for LIBs has not been reported. In this work, the LTO anode performance for LIBs using GNRs as additive is investigated and reported as a first.
Synthesis of materials
A modified Hummer’s method was used to synthesize graphene oxide nanoribbons (GONRs) (Hummers and Offeman 1958). Firstly, 600 mg of MWCNTs (50–80 nm, Cheap Tubes Inc, Cambridgeport, VT, USA) were suspended in 144 mL of sulfuric acid (H2SO4) (98 %, Aldrich) and stirred for 1 h. Then, 16 mL of concentrated H3PO4 was added with further stirring for 15 min. Following the stirring, 300 mg of KMnO4 (99.9 %, Aldrich) was slowly added to the mixture with the reaction taking place for 2 h at 65 °C. The resultant product waspoured over 400 mL of ice, with 20 mL of H2O2 (30 %, ACE, South Africa). The product was cooled to room temperature then filtered using a 200 nm pore size PTFE membrane. The product was washed sequentially with 30 % HCl (24 mL each), ethanol (ACE, South Africa) and ether (ACE, South Africa). Lastly, the black solid product was dried at 90 °C overnight under vacuum.
The GONRs formed from the above process was then reduced thermally. Using a tube furnace, a temperature of 250 °C was reached before a 1:1 Ar:H2 gaseous mixture was introduced and maintained for 1 hour.
Anatase TiO2 (220 nm in average particle diameter and 99.5 % in purity, Hangzhou Wanjing New Material Co., Ltd) and Li2CO3 (99.9 % in purity, Shanghai China Lithium Industrial Co., Ltd.) were used as raw materials. Li4Ti5O12 was prepared by a solid-state reaction method. The stoichiometric amounts of Li2CO3 and anatase TiO2 with molar ratio of Li:Ti = 0.82:1 were mixed with ethanol as dispersant by planetary ball-milling. The ball-milled mixture was heated in a furnace at 800 °C in air for 18 h, followed by mechanical crushing to obtain the final Li4Ti5O12.
LTO/GNRs (5 % wt GNRs) composites was formed by mechanical mixing method.
The morphological and structural properties of the GNRs were determined using X-ray diffraction (XRD, SCINTAG-XDS 2000), transmission electron microscopy (TEM, Hitachi H-7000 200 kV), and scanning electron microscopy coupled with energy dispersive spectroscopy (SEM/EDS) (JSM-7500F SEM/EDS). Battery performance was conducted on a Maccor testing system. Electrochemical performance was tested with a Biologic potentiostat.
Coin cells assembly and electrochemical measurements
LTO or LTO/GNRs was dispersed homogeneously in a slurry with 10 % poly (vinylidene fluoride) binder with 10 % PRINTEX XE 2-B in N-methylpyrrolidione (NMP) solvent. The slurry was subsequently cast onto a Cu foil current collector and then dried overnight under vacuum at 110 °C. In the coin cell, metallic lithium foil was used as the counter and reference electrodes; the electrolyte used was a 1 mol/L LiPF6 in a 1:1 solvent mixture of ethylene carbonate and diethyl carbonate (EC/DEC). Electrochemical measurements were carried out between 1.0 and 2.5 V vs Li+/Li0 with CR2032 coin cells. The capacity of the cell was calculated on the basis of the total mass of the active material (LTO).
Results and discussion
Structure and morphology
Figure 2 shows both TEM and SEM structures of GONRs, LTO and LTO/GNRs. As observed from the TEM image in Fig. 2a, MWNTs were completely unzipped, resulting in wavy-structure. GNRs strips shown in Fig. 2a had an average width of 75–150 nm. The typical unzipped nanoribbons with multi-layered structures are as shown by SEM images (Fig. 2b). In contrast, the LTO particlesof a size range from 100–800 nm are presented (Fig. 2c). It is worth noting from LTO particles in Fig. 2d that these were wrapped around graphene nanoribbons.
The cycling performance of LTO and LTO/GNRs were tested at a 2 C rate for 100 cycles. It is seen from Fig. 3d that the initial discharge capacities of the LTO and LTO/GNRs were 121.4 and 178.2 mAh·g−1, respectively, and the retained discharge capacities were 73.4 and 94.7 mAh·g−1 after 100 cycles. The excellent cyclic stability and high-rate capacity of LTO/GNRs could be related to increased conductivity of LTO/GNRs.
The anode peak of LTO/GNRs is negatively shifted by 70 mV (from Fig. 4c) with almost double the current density compared with LTO. This further suggests that LTO/GNRs has a better electrochemical performance than that of LTO. It was observed that with increasing the scan rate, the intercalation and de-intercalation peaks shift to lower and higher potentials, respectively. However, smaller potentials shifts were noticed for LTO/GNRs than that of LTO between intercalation and de-intercalation peaks, thus showing improved kinetics by incorporating cathodically-induced graphene nanoribbons. As displayed in Fig. 4d, the peak current (j) exhibits a linear relation with the square root of the scan rate (ʋ1/2), which indicates a diffusion-controlled process rather a surface-controlled one (Li et al. 2013).
Electrochemical properties of the LTO/GNRs and the LTO electrode
2.38 × 10−4
1.1 × 10−3
In summary, LTO/GNRs composites were shown to provide improved discharge capacities of 206.5 and 142.3 mAh·g−1 at 0.2 and 5 C, respectively, which is higher than those of pristine LTO (169.1 and 71.1 mAh·g−1). Therefore, GNRs additives were proved to have improved the LTO rate performance, especially at high rates. The enhanced conductivity LTO/GNRs, which are contributed from the GNR Framework and high conductivity, results in accelerated kinetics for lithium intercalation/de-intercalation within LIBs that also leads to excellent rate capacity of LTO/GNRs.
PM was involved in synthesis of GNRs and assisted battery performance testing. HZ was involved synthesis and characterizations of LTO and LTO/GNRs and battery performance testing as well as writing. PA assisted experiments. AS and LL assisted equipment. BF and MM assisted writing. All authors read and approved the final manuscript.
The authors are thankful for the financial support from National Science Foundation Graduate Research Fellowship award (Grant No. DGE-1441403, USA), NSF Graduate Research Opportunities Worldwide (GROW) travel award from USA. The United States Agency for International Development (USAID) Research and Innovations Fellowship and Grant from CSIR of South Africa (No. HTR046P).
The authors declare that they have no competing interests.
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- Armand M, Tarascon J (2008) Building better batteries. Nature 451(7179):652–657View ArticleGoogle Scholar
- Bhardwaj T, Antic A, Pavan B et al (2010) Enhanced electrochemical lithium storage by graphene nanoribbons. J Am Chem Soc 132(36):12556–12558View ArticleGoogle Scholar
- Dong Y, Zhao Z, Wang Z et al (2015) Dually fixed SnO2 nanoparticles on graphene nanosheets by polyaniline coating for superior lithium storage. ACS Appl Mater Interfaces 7(4):2444–2451View ArticleGoogle Scholar
- Goriparti S, Miele E, De Angelis F et al (2014) Review on recent progress of nanostructured anode materials for Li-ion batteries. J Power Sources 257:421–443View ArticleGoogle Scholar
- Han MY, Özyilmaz B, Zhang Y et al (2007) Energy band-gap engineering of graphene nanoribbons. Phys Rev Lett 98(20):206805View ArticleGoogle Scholar
- Hao Y, Lai QY, Liu D et al (2005) Synthesis by citric acid sol-gel method and electrochemical properties of Li4Ti5O12 anode material for lithium ion battery. Mater Chem Phys 94(2–3):382–387View ArticleGoogle Scholar
- Hummers WS Jr, Offeman RE (1958) Preparation of graphitic oxide. J Am Chem Soc 80(6):1339View ArticleGoogle Scholar
- Jian Z, Zhao L, Wang R et al (2012) The low-temperature (400 °C) coating of few-layer graphene on porous Li4Ti5O12 via C28H16Br2 pyrolysis for lithium-ion batteries. RSC Adv 2(5):1751–1754View ArticleGoogle Scholar
- Jiao L, Zhang L, Wang X et al (2009) Narrow graphene nanoribbons from carbon nanotubes. Nature 458(7240):877–880View ArticleGoogle Scholar
- Jung HG, Myung ST, Yoon CS et al (2011) Microscale spherical carbon-coated Li4Ti5O12 as ultra high power anode material for lithium batteries. Energy Environ Sci 4(4):1345–1351View ArticleGoogle Scholar
- Kavan L, Procházka J, Spitler TM et al (2003) Li Insertion into Li4Ti5O12 (Spinel) charge capability vs. particle size in thin-film electrodes. J Electrochem Soc 150(7):A1000–A1007View ArticleGoogle Scholar
- Kim H, Bak S, Kim K (2010) Li4Ti5O12/reduced graphite oxide nano-hybrid material for high rate lithium-ion batteries. Electrochem Commun 12(12):1768–1771. doi:https://doi.org/10.1016/j.elecom.2010.10.018 View ArticleGoogle Scholar
- Kosynkin DV, Higginbotham AL, Sinitskii A et al (2009) Longitudinal unzipping of carbon nanotubes to form graphene nanoribbons. Nature 458(7240):872–876View ArticleGoogle Scholar
- Li L, Raji AO, Tour JM (2013) Graphene-wrapped MnO2–graphene nanoribbons as anode materials for high-performance lithium ion batteries. Adv Mater 25(43):6298–6302View ArticleGoogle Scholar
- Lin J, Raji AO, Nan K et al (2014) Iron oxide nanoparticle and graphene nanoribbon composite as an anode material for high-performance Li-ion batteries. Adv Funct Mater 24(14):2044–2048View ArticleGoogle Scholar
- Ohzuku T, Ueda A, Yamamoto N (1995) Zero-strain insertion material of Li [Li1/3Ti5/3] O4 for rechargeable lithium cells. J Electrochem Soc 142(5):1431–1435View ArticleGoogle Scholar
- Ouyang CY, Zhong ZY, Lei MS (2007) Ab initio studies of structural and electronic properties of Li4Ti5O12 spinel. Electrochem Commun 9(5):1107–1112. doi:https://doi.org/10.1016/j.elecom.2007.01.013 View ArticleGoogle Scholar
- Ri SG, Zhan L, Wang Y et al (2013) Li4Ti5O12/graphene nanostructure for lithium storage with high-rate performance. Electrochim Acta 109:389–394View ArticleGoogle Scholar
- Scrosati B, Garche J (2010) Lithium batteries: status, prospects and future. J Power Sources 195(9):2419–2430View ArticleGoogle Scholar
- Sorensen EM, Barry SJ, Jung H et al (2006) Three-dimensionally ordered macroporous Li4Ti5O12: effect of wall structure on electrochemical properties. Chem Mater 18(2):482–489View ArticleGoogle Scholar
- Sun X, Hegde M, Zhang Y et al (2014) Structure and electrochemical properties of spinel Li4Ti5O12 nanocomposites as anode for Lithium-ion battery. Int J Electrochem Sci 9:1583Google Scholar
- Uthaisar C, Barone V, Peralta JE (2009) Lithium adsorption on zigzag graphene nanoribbons. J Appl Phys 106(11):113715View ArticleGoogle Scholar
- Wagemaker M, van Eck ER, Kentgens AP et al (2008) Li-ion diffusion in the equilibrium nanomorphology of spinel Li4 × Ti5O12. J Phys Chem B 113(1):224–230View ArticleGoogle Scholar
- Yang Y, Li L, Fei H et al (2014) Graphene nanoribbon/V2O5 cathodes in lithium-ion batteries. ACS Appl Mater Interfaces 6(12):9590–9594. doi:https://doi.org/10.1021/am501969m View ArticleGoogle Scholar
- Yao X, Xie S, Chen C et al (2005) Comparisons of graphite and spinel Li4Ti5O12 as anode materials for rechargeable lithium-ion batteries. Electrochim Acta 50(20):4076–4081View ArticleGoogle Scholar
- Yi T, Jiang L, Shu J et al (2010) Recent development and application of Li4Ti5O12 as anode material of lithium ion battery. J Phys Chem Solids 71(9):1236–1242View ArticleGoogle Scholar
- Zhang Q, Li X (2013) Recent developments in the doped-Li4Ti5O12 anode materials of lithium-ion batteries for improving the rate capability. Int J Electrochem Sci 8:6449–6456Google Scholar