Study of a novel gel electrolyte based on poly-(methoxy/hexadecyl-poly(ethylene glycol) methacrylate) co-polymer plasticized with 1-butyl-3-methylimidazolium tetrafluoroborate

Long Wang, Hua-jun Zhu, Wei Zhai, Feng Cai, Xiao-min Liu* and Hui Yang*
College of Materials Science and Engineering, Nanjing Tech University, 5 Xinmofan Road, Nanjing, Jiangsu 210009, P. R. China. E-mail: liuxm@njtech.edu.cn; yanghui@njtech.edu.cn; Fax: +86-25-83587762; Fax: +86-25-83587260; Tel: +86-25-83587762 Tel: +86-25-83587260

Received 28th April 2014 , Accepted 12th August 2014

First published on 12th August 2014


Abstract

Compared with traditional liquid electrolytes, solid polymer electrolytes possess higher reliability and safety but much lower ionic conductivity, which can be improved by incorporating plasticizers to form gel polymer electrolytes (GPEs). However, the commonly employed plasticizers are flammable organic solvents which may cause safety issues. Herein, ionic liquid 1-bultyl-3-methylimidazolium tetrafluoroborate ([Bmim]BF4) is selected as the plasticizer to fabricate inflammable GPE due to its non-volatility and inflammability. The solid matrix is co-polymerized from methoxy-poly(ethylene glycol) methacrylate (MPEGM) and hexadecyl-poly(ethylene glycol) methacrylate (HPEGM). The effect of the electrolyte composition on its properties is systematically studied. The synthesized GPEs possess excellent thermal stability and exhibit relatively high ionic conductivity, among which the one named as PMH12-60, composed of 32 wt% MPEGM, 8 wt% HPEGM and 60 wt% [Bmim]BF4, presents an ionic conductivity comparable to liquid electrolytes, up to 1.13 × 10−3 S cm−1 at 30 °C. In addition, the GPE shows good compatibility with metallic lithium. Furthermore, the coin cell based on PMH12-60, with a LiFePO4 cathode and a lithium anode shows a discharge capacity as high as 145 mA h g−1 and 158 mA h g−1 when cycled at 30 °C and 50 °C, respectively, under the cycling rate of 0.1 C. Moreover, no obvious capacity loss is observed after 30 cycles at both temperatures.


1 Introduction

Polymer electrolytes in lithium ion batteries have attracted much attention recently due to their fabrication flexibility in shape and size for roll-up displays and wearable electronic devices,1,2 as well as the improvement of reliability and safety compared to the traditional carbonate based liquid electrolytes. The area of solid polymer electrolytes has gone through several developmental stages. The research work was initially carried out on polyethylene oxide (PEO) and/or its derivatives, which can dissolve lithium salts and exhibit high segmental flexibility for ion transport in the amorphous phase.3–5 However, the linear PEO-based solid polymer electrolytes (SPE) present fairly low ionic conductivity (10−7 to 10−8 S cm−1) due to their crystallization propensity at temperature below 65 °C. Several methods have been proposed to improve the ionic conductivity, including (1) the introduction of polar units6–10 or non-polar units11 into the main or side chains to form graft polymer electrolytes (10−5 S cm−1) and (2) the plasticization of non-aqueous plasticizer into SPE matrix to build gel polymer electrolytes (GPE) with improved ionic conductivity up to 10−3 S cm−1.12 Owing to the high ionic conductivity, organic solvents are widely employed as plasticizers to fabricate GPEs, but their volatility and flammability may cause serious safety issues which might be overcome by introducing non-volatile and nonflammable solvents as plasticizers.13–19 Recently non-volatile and inflammable room temperature ionic liquids (RTILs) have attracted much attention in electrochemical fields, since many of them exhibit high ionic conductivity and wide electrochemical window.20 Therefore, RTILs can be considered as novel plasticizers to fabricate GPEs with high safety and superior electrochemical properties. However, Ionic liquids don't behave only as plasticizers. They are able to reduce the polymer host–lithium cation interaction, thus increasing the mobility of the Li+ ion.

In our previous study,11 a novel polymer matrix named as PMH (Fig. 1) was synthesized by adopting two macro-monomers, methoxyl-poly(ethylene glycol) methacrylate (MPEGM, n = 7 or 12) and hexadecal-poly(ethylene glycol) methacrylate (HPEGM, n = 7). It has been found that the solid electrolyte copolymerized from 80 wt% MPEGM and 20 wt% HPEGM exhibits relatively high conductivity up to 1.26 × 10−4 S cm−1 at 30 °C, indicating that the co-polymer matrix might be a good candidate to fabricate gel polymer electrolytes. The gel polymer electrolyte with non-volatile tris(methoxypolyethyleneglycol) aluminate ester as plasticizer and PMH as matrix achieves ionic conductivity up to 0.59 × 10−3 S cm−1 at 30 °C.21 The gel polymer electrolyte prepared with PMH and dual plasticizers (polyethylene glycol dimethyl ether (PEGDME) and polyethylene glycol dilaurate (PEGDL)) exhibits excellent mechanical property and relatively high ionic conductivity up to 0.82 × 10−3 S cm−1 at 30 °C.12 Both studies suggest that PMH can be used to build GPE with high ionic conductivity and superior mechanical property.


image file: c4ra03661a-f1.tif
Fig. 1 Chemical structures of macro-monomers, (a) MPEGM, (b) HPEGM.

In this work, PMH and 1-butyl-3-methylimidazolium tetrafluoroborate ([Bmim]BF4) are used as matrix and plasticizer, respectively, to synthesize novel ionic liquid incorporated gel polymer electrolytes. The effect of the electrolyte composition on its properties, such as thermal stability, glass transition temperature (Tg), and ionic conductivity (σ), is systematically studied. The Li+ transference number (t+), lithium/GPE interfacial property and the charge–discharge performance of the built cell based on the synthesized GPE are also measured and discussed in detail. The synthesized GPEs possess excellent thermal stability and exhibit relatively high ionic conductivity, among which the one named as PMH12-60, composed of 32 wt% MPEGM (n = 12), 8 wt% HPEGM and 60 wt% [Bmim]BF4, presents the highest conductivity up to 1.13 × 10−3 S cm−1 at 30 °C.

2 Experiment section

2.1 Synthesis of methoxy-poly(ethylene glycol) methacrylate (MPEGM)

Methoxy-poly(ethylene glycol) methacrylate (n = 7, 12) were prepared by using methacryloyl chloride to esterify the terminal hydroxyl groups of methoxy poly(ethylene glycol) (MPEG350, 550). The mixture of 0.10 mol MPEG, 0.12 mol TEA and 250 ml dry dichloromethane (DCM) was well stirred at 0 °C in an ice-water bath. Methacryloyl chloride (0.12 mol) was added dropwise to the above mixture followed by 12 hour stir. After filtration, vacuum evaporation, and purification through silica gel column with petroleum aether and ethyl acetate at the volume ratio of 5[thin space (1/6-em)]:[thin space (1/6-em)]1 as eluent, a pale yellow product MPEGM was obtained after vacuum desolventizing. The chemical structure of MPEGM is shown in Fig. 1(a) and verified with IR.

2.2 Synthesis of hexadecyl-poly(ethylene glycol) methacrylate (HPEGM)

Hexadecyl-poly(ethylene glycol) methacrylate (n = 7) was prepared in a similar method to MPEGM with the following reagents: hexadecyl-poly(ethylene glycol) (HPEG578, 0.1 mol), triethylamine (0.12 mol), and methacryloyl chloride (0.12 mol). The final product purified through silica gel column is a yellow oily liquid. The chemical structure of HPEGM is shown in Fig. 1(b) and verified with IR.

2.3 Synthesis of ionic liquid [Bmim]BF4 (IL)

The [Bmim]BF4 ionic liquid was synthesized by anion exchange in an one-step reaction. The raw chemicals are N-methylimidazolium (99%, Aladdin), 1-bromobutane (≥98%, Aladdin) and sodium fluoroborate (99.99%, Aladdin). The mixture of the above three materials was heated to 80 °C in a stirred three-neck, round-bottom flask under nitrogen for 6 hours till white slurry was obtained. The slurry was kept in vacuum at 100 °C for 24 hours before centrifuge several times until the ionic liquid becomes colorless and viscous. The obtained ionic liquid was stored in glove box filled with argon prior to use. The water content in the synthesized IL was measured to be 105 ppm by Coulometer (831 KF, Netzsch, Germany).

2.4 Preparation of the polymer electrolyte (PMH7, PMH12)

The polymer electrolyte PMH7 was prepared in a similar method to PMHn-IL with the following reagents: MPEGM (n = 7), HPEGM, azobisisobutyronitrile (AIBN, Aldrich) and LiClO4 (99.9%, Aldrich), while the weight ratio of MPEGM (n = 7) to HPEGM is 4[thin space (1/6-em)]:[thin space (1/6-em)]1 and the molar ratio of Li to EO is set as 1[thin space (1/6-em)]:[thin space (1/6-em)]20. The polymer electrolyte PMH12 was prepared in a similar method to PMHn-IL with the following reagents: MPEGM (n = 12), HPEGM, azobisisobutyronitrile (AIBN, Aldrich) and LiClO4 (99.9%, Aldrich), while the ratio of MPEGM (n = 12) to HPEGM is 4[thin space (1/6-em)]:[thin space (1/6-em)]1 and the molar ratio of Li to EO is set as 1[thin space (1/6-em)]:[thin space (1/6-em)]20.

2.5 Preparation of the polymer electrolyte (PMH7-IL, PMH12-IL)

Certain amount of MPEGM (n = 7, 12), HPEGM, [Bmim]BF4, azobisisobutyronitrile (AIBN, Aldrich) and LiClO4 (99.9%, Aldrich) were dissolved in anhydrous tetrahydrofuran (THF). The mixture of LiClO4 and the PMHn copolymer at a desired ratio of [Li][thin space (1/6-em)]:[thin space (1/6-em)][EO] was stirred for 3 hours in an Ar-filled glove box and then evaporated under reduced pressure for 30 minutes at room temperature to obtain viscous solution. The solution was cast into the Teflon plate and dried at 60 °C under high vacuum for 12 hours to obtain the polymer electrolyte film. This film was cut into disks with 16 mm in diameter in an Ar-filled glove box for electrochemical test.

2.6 Physical property (IR, DSC and TGA)

IR spectra were recorded using a TENSOR 27 Fourier transform spectrometer over the range of 4000–400 cm−1 at 25 °C. 1H NMR spectra of the samples were obtained from a 500 MHz BRUKE NMR spectrometer in chloroform-d. The chemical shifts for 1H-NMR measurements were referred to tetramethylsilane (TMS) as internal standard. 13C NMR spectra were recorded with the same spectrometer in DMSO-d6.

Thermal analysis was conducted with a DSC200F3 (NETZSCH) differential scanning calorimeter over the temperature range from −100 to 100 °C under N2 atmosphere at the scan rate of 10 °C min−1. The sample, placed in an aluminum container, was first heated to 100 °C, then cooled down to −100 °C and scanned. Thermogravimetric analysis (TGA) was conducted under nitrogen environment at the heating rate of 10 °C min−1 from 25 °C to 500 °C by a TA instrument STA409PC (NETZSCH).

2.7 Electrochemical property

The ionic conductivity of the samples was measured by alternating current (A.C.) impedance spectroscopy using an impedance analyzer (PARSTAT2273) in the frequency range from 0.1 Hz to 106 Hz. The polymer electrolyte was sandwiched by two polished stainless steel electrodes, sealed in a testing cell within an argon-housed dry box. Then the testing cell was measured in the temperature range from 30 °C to 80 °C. The electrical conductivity (σ) can be calculated from the following relation,
 
σ = L/RbA (1)
where L is the thickness of the sample, A is the cross-sectional area of the sample, and Rb is the bulk resistance obtained from complex impedance plots.

The lithium ion transference number (t+) of the electrolyte was calculated according to the Evans and Abraham method22,23 by applying 50 mV polarization to the cell, with the following equation,

 
image file: c4ra03661a-t1.tif(2)
where ΔV is the potential applied across the cell, I0 and Is are the initial and steady-state dc current, Rb,0 and Rb,s are the initial and final resistance of the electrolyte, and Ri,0 and Ri,s are the initial and steady-state resistance of the passivating layer.

The electrochemical stability of the electrolyte was determined by linear sweep voltammetry (LSV) scan using Pt metal as the working electrode and lithium as the counter and reference electrode. The LSV scans were performed at the scan rate of 1 mV s−1 from 2.6 V to 5.4 V vs. Li+/Li at 30 °C. The interfacial resistance between electrolyte and lithium electrode was analyzed by A.C. Impedance spectroscopy using PARSTAT 2273 impedance analyzer for the Li/GPE/Li cell.

The coin-type (CR2032) lithium polymer cell was prepared using the GPE film, LiFePO4 and metallic lithium (Tianjing Zhongli, China) as electrolyte, cathode and anode, respectively. The cathode (LiFePO4, 99%) was purchased from Changsha Yunchou Power Technology, China (with d50 of 4 micron). The content of LiFePO4, conductive acetylene carbon black and PVDF of the fabricated electrode is 91%, 5% and 4%, respectively. In addition, the thickness and diameter of the electrode is 50 micron and 1.3 cm2, respectively. Furthermore, the active mass loading is measured as about 5 mg cm−2. The charge–discharge test of assembled cells was carried out using a BT-2000 battery testing system (Arbin, USA) in the voltage range of 2.5–4.0 V versus Li+/Li under 0.1 C (0.085 mA cm−2) rate at both 30 °C and 50 °C.

3 Results and discussion

3.1 IR spectra of [Bmim]BF4

Fig. 2 presents the IR spectra of the synthesized [Bmim]BF4. The structural formula of [Bmim]BF4 is shown in Fig. 3. The characteristic bands at 3161.4 cm−1 and 3121 cm−1 represent in-phase stretching vibration of C–H (C4, C5) and stretching vibration of C–H (C2), respectively. The characteristic bands at 2938.5 cm−1 and 2876.9 cm−1 correspond to antisymmetrical stretching vibration of –CH3, –CH2 and symmetrical stretching vibration of –CH2, respectively. The peak at 1574.1 cm−1 is the infrared absorption of the frame vibration of imidazole ring and stretching vibration of C[double bond, length as m-dash]C. The strong and broad peaks at 1058.0 cm−1 are due to the frame vibration of C–N and stretching vibration of B–F. The peak at 1171.4 cm−1 is attributed to the stretching vibration of N–Bu, N–Me in imidazole ring.24
image file: c4ra03661a-f2.tif
Fig. 2 IR spectra of [Bmim]BF4 (Bu: butyl Me: methyl).

image file: c4ra03661a-f3.tif
Fig. 3 The structural formula of [Bmim]BF4.

3.2 The glass transition temperature

Fig. 4(a) plots the differential scanning calorimetry curves of various polymer electrolytes and the corresponding polymer matrix PMHn (n = 7, 12). The symbol PMHn-x represents the gel polymer electrolyte composed of PMHn (n = 7, 12) and the ionic liquid, whileas x stands for the content of the ionic liquid. For example, the sample marked as PMH12-60 contains 60 wt% ionic liquid and PMH12 is the polymer matrix.
image file: c4ra03661a-f4.tif
Fig. 4 DSC traces for polymer electrolytes, (a) the different GPEs with the same concentration of lithium salt, (b) the PMH12-60 electrolyte with various concentration of lithium salt.

It is well known that the low glass transition temperature (Tg) is coupled with the high mobility of the EO chains.25 The Tg of PMH12 (−49.2 °C) is lower than that of PMH7 (−45.3 °C), since PMH12 with longer EO chains facilitating swing, is of better EO mobility than PMH7. The Tg of [Bmim]BF4 was reported as −85 °C.26 After [Bmim]BF4 is added as plasticizer, the resulting gel polymer electrolyte presents low Tg compared to the corresponding polymer itself. The addition of ionic liquid lowers crystallization tendency of the polymer and improves the mobility of the EO chains by expanding free volume of the EO chains. In addition, DSC in our measurement of gel polymer electrolyte doesn't exhibit any melting point of the neat IL, agreeing well with what reported in the literature.27 No crystallization of BMIMBF4 is observed in the DSC scan which might be explained by the difficulties of BMIM cations and BF4 anions to crystallize due to steric problem arising from the length of alkyl chain.27

The lithium salt concentration may also have impact on the physical properties of the polymer electrolyte. The PMH12-60 based GPEs containing different amount of lithium salt ([Li][thin space (1/6-em)]:[thin space (1/6-em)][EO] = 1[thin space (1/6-em)]:[thin space (1/6-em)]12, 1[thin space (1/6-em)]:[thin space (1/6-em)]16, 1[thin space (1/6-em)]:[thin space (1/6-em)]20, 1[thin space (1/6-em)]:[thin space (1/6-em)]24) are compared. The results are plotted in Fig. 4(b).It can be observed that with the increase of the lithium salt concentration, theTgof the GPE declines first, then goes up after [Li][thin space (1/6-em)]:[thin space (1/6-em)][EO] is above 1/20. Initially the presence of small amount lithium salt disrupts the crystallization of EO chains, lowering the glass transition temperature. After [Li][thin space (1/6-em)]:[thin space (1/6-em)][EO] is higher than 1/20, the enhanced inter- and intra-molecular coordination between Li+ and EO units limits the motion of EO chains, resulting in the rise of the glass transition temperature.

3.3 Thermal properties

The thermal stability of the ionic liquid, solid matrix PMHn (n = 7, 12) and the gel polymer electrolyte PMHn-x (n = 7, 12; x = 70, 60, 30) is analyzed by thermogravimetry under N2 atmosphere and the results are shown in Fig. 5(a) and (b). In the temperature range from 80 °C to 250 °C, no mass loss is observed for [Bmim]BF4, while small amount of weight loss is detected for PMHn and PMHn-ILs, presumably caused by the evaporation of low molecular weight components. In the temperature range from 250 °C to 500 °C, mass loss of 83 wt% is observed for pure IL corresponding to the decomposition of the IL. In the temperature above 250 °C, both the IL and PMHn decompose in one stage. In contrast, the PMHn-IL gel polymer electrolytes exhibit two-stage decomposition mechanism. Upon heated up, PMHn-IL experiences the decomplexation of PMHn-IL, degradation of PMH, followed by decomposition of the ionic liquid.28 It can be found that PMH7-IL decomposes at higher temperature than PMH12-IL, the reason could be that more EO chain presence in PMH12-IL reduces the crystallization propensity and makes it less stable. PMHn-IL starts to decompose at lower temperature than PMHn itself. The decomposition temperature of PMHn-IL decreases with the increase of the ionic liquid at low content, then goes up as shown in both Fig. 5(a) and (b). The small amount addition of the ionic liquid disrupts the crystallization in the polymer, and makes the PMHn-IL less stable and decomposes at lower temperature. When the content of the ionic liquid reaches certain level, the ionic liquid exists in PMHn-IL in the complex form and also in the free form but enclosed in PMHn.28 The existence of the ionic liquid in large quantity stabilizes the PMHn-IL electrolyte.
image file: c4ra03661a-f5.tif
Fig. 5 (a) The TG profiles for IL, PMH7, and several PMH7 based gel polymer electrolytes; (b) the TG profiles for IL, PMH12, and several PMH12 based gel polymer electrolytes.

3.4 Ionic conduction

Fig. 6(a) and (b) present the dependence of the conductivity (σ) on 1/T for the PMH7/PMH12 based polymer electrolytes containing plasticizer in the temperature range from 30 °C to 80 °C. The sample cell is equilibrated at the testing temperature for 60 min before-measurement. It can be seen clearly that at higher temperature, all electrolytes present higher conductivity because high temperature promotes the mobility of both EO chains and Li+ in the IL. The conductivity of PMH12 is higher than that of PMH7 at the same temperature. PMH12 shows low Tg and high chain mobility compared to PMH7. The conductivity is greatly enhanced after IL being plasticized into the PMH7/PMH12 matrix, since the introduction of plasticizer in polymer matrix suppresses the degree of crystallinity,28 encourages the motion of EO chains, lowers the required activation energy, decreases the glass transition temperature and improves the Li+ conductivity in the polymer electrolytes.12 More importantly, IL itself presents several orders higher conductivity than both polymer matrices. This is also the main reason that at the same temperature and based on the same matrix, the electrolyte with more IL exhibits higher conductivity. The second reason lies in the reality that the introduction of plasticizer enhances free volume expansion of the EO chains. With the same amount of IL plasticized, the PMH12 based electrolyte presents higher σ than the PMH7 based electrolyte. The gel polymer electrolyte containing more IL possesses better ionic conductivity, but may exhibit poor mechanical stability. Considering the mechanical strength and conductivity (1.13 × 10−3 S cm−1), PMH12-60 is selected for electrochemical performance evaluation.
image file: c4ra03661a-f6.tif
Fig. 6 Temperature dependence of ionic conductivity of polymer electrolytes (a) PMH7-IL and (b) PMH12-IL.

3.5 Transference number measurement

The bulk and interfacial resistance of the Li/PMH12-60/Li cell before and after polarization is measured by A. C. impedance. The results are plotted in Fig. 7. The inserted figure is the depolarization curve of the cell subjected to small DC polarization potential (50 mV) for sufficient time to reach steady-state. The data related to the t+ calculation is summarized in Table 1. Generally speaking, comparing two similar systems at the same temperature, the one with high resistance exhibits large transference number.29 The measured t+ values of these polymer electrolytes are between 0.26 and 0.35 (less than 0.5), suggesting that the contribution of Li+ to the total ionic conductivity is much less than the other ions, which is in good agreement with what reported in many gel polymer electrolyte studies.12,30 The gel electrolyte plasticized with IL exhibits a slightly higher t+ value than the corresponding solid polymer electrolyte. Moreover, the electrolyte plasticized with more IL is of higher t+ value.
image file: c4ra03661a-f7.tif
Fig. 7 Impedance spectra of the Li/PMH12-60/Li cell measured before and after polarization at 30 °C. Inserted figure: depolarization curve of the cell.
Table 1 The data related to Li+ transference number of electrolytes at [Li][thin space (1/6-em)]:[thin space (1/6-em)][EO] = 1[thin space (1/6-em)]:[thin space (1/6-em)]20
Electrolyte Rb,0 (Ω) Rb,s (Ω) Ri,0 (Ω) Ri,s (Ω) I0 (mA) Is (mA) t+
PMH7 226.4 241.9 673.8 890.4 0.046 0.022 0.26
PMH12 233.7 238.5 683.2 873.4 0.051 0.026 0.28
PMH7-30 168.5 205.2 604.8 779.4 0.025 0.006 0.23
PMH7-60 182.7 229.4 653.6 802.5 0.029 0.009 0.30
PMH7-70 178.3 223.2 628.9 822.4 0.031 0.011 0.32
PMH12-30 150.2 198.7 562.0 725.3 0.028 0.008 0.29
PMH12-60 170.4 212.2 609.3 798.3 0.024 0.008 0.33
PMH12-70 225.8 296.1 743.7 926.3 0.035 0.014 0.35


3.6 Interface stability resistance between lithium electrode and polymer electrolyte

The interfacial compatibility of the gel electrolyte with metallic lithium is a key factor since uncontrollable passivation on the lithium electrode may cause serious safety issues. The prepared ionic liquid and PMH matrix may contain trace amount of residual impurities and/or moisture which may increase the interfacial resistance between lithium electrode and electrolyte. In this study, the interfacial stability is analyzed by measuring the A. C. impedance of a Li/PMH12-60/Li coin-typed cell stored at room temperature under open circuit potential condition. Fig. 8(a) presents the Nyquist spectra and Fig. 8(b) shows the change in the area specific bulk (Rbulk) and interface resistances (Rintf) as a function of storage time. Generally, the interface between the polymer electrolyte and the Li electrode may exhibit high resistance up to the order of 103 Ω,19,31 due to imperfect contact and the formation of a passivation layer on the lithium electrode. In this study, Rbulk and Rintf in the fresh cell are 180 Ω cm2 and 556 Ω cm2, respectively. Rbulk increases slightly and stabilizes at 400 Ω cm2 after 12 days storage. This increase can be ascribed to the formation and growth of the passivation layer which affects the nature of the polymer electrolyte.32 In contrast, Rintf jumps in the first 72 hours, then decreases slightly along the time before 96 hours, afterwards it levels up to 1600 Ω cm2 in the next 72 hours before stabilizing. The initial sharp increase of the Rintf can be mainly attributed to the formation and growth of the passivation layer. Moreover, the trace amount of residual moisture and/or impurities (such as ethylene glycol) might react with Li to produce LiOH, Li2O and other Li organic compounds to increase the interfacial resistance.33 The decrease of the interfacial resistance during 72–96 hours might be claimed to the formation of an ion-conducting polymer layer produced by the reaction between Li and ester groups of PMH. This polymeric layer may prevent the corrosion of lithium electrode from the impurities. After 288 hours, Rintf reaches the steady value of 1680 Ω cm2, indicating that the PMH12-60 electrolyte is compatible with the lithium electrode well. The change of Rintf and Rbulk along the storage time suggests that the composition of the gel polymer electrolyte may be altered by the possible reactions between GPE/impurities and lithium electrode.
image file: c4ra03661a-f8.tif
Fig. 8 (a) Impedance profiles of Li/PMH12-60/Li, (b) the change in the area specific bulk and interface resistances (Rbulk and Rintf) as a function of storage time.

3.7 Electrochemical stability of the polymer electrolytes

The electrochemical stability of the electrolytes (PMH12-60), is studied by cyclic voltammogram scans with Pt as the working electrode and Li as the reference/counter electrodes (Fig. 9). With the extremely slow scan rate in this study (0.2 mV s−1), very small distance between the working and counter/reference electrode (50 μm), and a thick piece of metallic lithium as reference/counter electrode (which can keep the voltage of counter/reference side constant), it can be concluded that the IR drop in this experiment can be neglected. The obtained polymer electrolyte has a stable electrochemical window more than 4.5 V, suggesting that it can be applied to the practical lithium polymer battery.34 Nishida et al. also pointed out that 1-alkyl-3-methylimidazolium tetrafluoroborate has an electrochemical window of about 4 V measured via a three electrode cell.27 Even though the reduction of most dialkylimidatizoliums generally takes place at around 0.6 V to 1 V vs. Li+/Li,27,35 they can find application in the Li4Ti5O12 or lithium alloys based Li-ion cells.
image file: c4ra03661a-f9.tif
Fig. 9 Electrochemical stability of the polymer electrolytes.

3.8 Cell testing

A Li/PMH12-60/LiFePO4 based 2032 coin cell is cycled at 0.1 C (1 C = 170 mA g−1) for 30 cycles at both 30 °C and 50 °C. The discharge capacity versus cycle number at different temperature is presented in Fig. 10(a) and (b), respectively. The charge–discharge curves of the 1st, 15th and 30th cycle are exhibited in the inseted figures. As shown in Fig. 9(a), the discharge capacity is 125 mA h g−1 in the first cycle, gradually increases to 145 mA h g−1 during the initial 10 cycles, which can be explained as that the penetration of the ionic liquid from membrane to the porous electrode makes full utilization of the active materials.36 The coulombic efficiency is 95.2% in the 1st cycle and 98% in the following cycles. The irreversible capacity observed during these cycles is consumed in passivating the surface of the metallic lithium.37 As we discussed in the previous part, it takes some time to form a stable passivate film in the electrode/electrolyte interface. However, when the cell is cycled at 50 °C, the discharge capacity is 158 mA h g−1 (close to the theoretical value) in the first cycle, remains stable and presents no capacity fade after 30 cycles. The coulombic efficiency maintains at 92.3% in all 30 cycles. At elevated temperature, both transport and reaction kinetics are promoted, resulting in the improvement of discharge capacity. Moreover, side reactions from the residue impurities and lithium are also enhanced, which reduces coulombic efficiency. At both temperatures, slightly oblique curves are observed for all presented charge–discharge curves, which is different from the normal charge–discharge curves for LiFePO4. The possible reason is explained as follows. The transport of all ions in electrolyte contributes to the ionic conductivity, but only the transport of Li+ is relevant to the charge–discharge processes within a Li-ion cell. In polymer electrolyte plasticized with [Emim]BF4, it was reported that Emim+ has higher self-diffusion rate than Li+,38 which means that Li+ diffuses slower than Emim+. Hayamizu et al. proposed that the Li+ and anion form ion complexes and diffuse together while Emim+ becomes relatively free to move. But the transport of other ions may lead to cell polarization, which might cause the charge–discharge curves deviate from plateau.39 The excellent cycling performance at low current at both temperatures can be ascribed to the relatively high conductivity of the PMH12-60 gel electrolyte,40 as well as the good compatibility between PMH12-60 and metallic lithium.41
image file: c4ra03661a-f10.tif
Fig. 10 Cycle life test of Li/PMH12-60/LiFeO4 cell at 0.1 C. Inserted figure: charge–discharge curves of Li/PMH12-60/LiFePO4 cell. (a) At 30 °C, (b) 50 °C.

4 Conclusions

In this work, several gel polymer electrolytes based on the co-polymer matrix PMH and ionic liquid [Bmim]BF4 have been prepared by the solution casting method. The purpose using ionic liquid as the plasticizer is to improve the safety of gel polymer electrolyte since IL is non-volatile and inflammable. The dependence of the electrolyte properties on the composition is systematically studied. With the same amount of plasticizer, PMH12 exhibits low Tg and thus high ionic conductivity compared to PMH7, since PMH12 with longer EO chains has better mobility than PMH7. The existence of the ionic liquid in large quantity stabilizes the PMHn-IL electrolyte. The gel film PMH12(40%)/IL(60%) presents good mechanical properties and also exhibits relatively high conductivity (1.13 × 10−3 S cm−1 at 30 °C). In addition, this GPE shows good compatibility with metallic lithium. Furthermore, a coin cell based on this GPE, with LiFePO4 as cathode and metallic lithium as anode, shows discharge capacities as high as 145 mA h g−1 and 158 mA h g−1 when cycled at 30 °C and 50 °C, respectively, under the current rate of 0.1 C. Moreover, no obvious capacity fade is observed after 30 cycles at both temperatures.

Acknowledgements

This work was supported by Key Project of Natural Science Foundation of Jiangsu Province of China (Grant no. BK2011030), Key Project of Educational Commission of Jiangsu Province of China (Grant no. 11KJA430006) and the Priority Academic Program Development of Jiangsu Higher Education Institutions.

References

  1. M. Armand and J. M. Tarascon, Nature, 2008, 451, 652 CrossRef CAS PubMed.
  2. H. J. Ha, E. H. Kil, Y. H. Kwon, J. Y. Kim, C. K. Lee and S. Y. Lee, Energy Environ. Sci., 2012, 5, 6491 CAS.
  3. P. Judeinstein and F. Roussel, Adv. Mater., 2005, 17, 723 CrossRef CAS PubMed.
  4. E. Quartarone and P. Mustarelli, Chem. Soc. Rev., 2011, 40, 2525 RSC.
  5. D. Saikia, Y. H. Chen, Y. C. Pan, J. Fang, L. D. Tsai, G. T. K. Fey and H. M. Kao, J. Mater. Chem., 2011, 21, 10542 RSC.
  6. M. Higa, K. Yaguchi and R. Kitani, Electrochim. Acta, 2010, 55, 1380 CrossRef CAS PubMed.
  7. W. H. Hou and C. Y. Chen, Electrochim. Acta, 2004, 49, 2105 CrossRef CAS PubMed.
  8. W. H. Hou, C. Y. Chen and C. C. Wang, Polymer, 2003, 44, 2983 CrossRef CAS.
  9. S. M. Lee, W. L. Yeh, C. C. Wang and C. Y. Chen, Electrochim. Acta, 2004, 49, 2667 CrossRef CAS PubMed.
  10. P. Gavelin, R. Ljungback, P. Jannasch and B. Wesslen, Solid State Ionics, 2002, 147, 325 CrossRef CAS.
  11. X. Zuo, X. M. Liu, F. Cai, H. Yang, X. D. Shen and G. Liu, J. Mater. Chem., 2012, 22, 22265 RSC.
  12. X. Zuo, X. M. Liu, F. Cai, H. Yang, X. D. Shen and G. Liu, J. Power Sources, 2013, 239, 111 CrossRef CAS PubMed.
  13. K. M. Abraham and Z. Jiang, J. Electrochem. Soc., 1997, 144, L136 CrossRef CAS PubMed.
  14. F. Groce, F. Gerace, G. Dautzemberg, S. Passerini, G. B. Appetecche and B. Scrosai, Electrochim. Acta, 1994, 39, 2187 Search PubMed.
  15. I. Kelly, J. F. Owen and B. C. H. Steele, J. Mater. Chem., 1984, 168, 467 CAS.
  16. Y. Ito, K. Kanehori, K. Miyauchi and T. Kudo, J. Mater. Sci., 1987, 22, 1845 CrossRef CAS.
  17. K. M. Abraham, M. Alamgir and R. K. Reynolds, J. Electrochem. Soc., 1988, 135, 535 CrossRef CAS PubMed.
  18. L. Yang, J. Lin, Z. Wang, C. Wang, R. Zhou and Q. Liu, Solid State Ionics, 1990, 40, 616 CrossRef.
  19. K. M. Abraham, Z. Jiang and B. Carroll, Chem. Mater., 1997, 9, 1978 CrossRef CAS.
  20. Y. S. Ye, J. Rick and B. J. Hwang, J. Mater. Chem. A, 2013, 1, 2719 CAS.
  21. F. Cai, X. Zuo, X. M. Liu, L. Wang, W. Zhai and H. Yang, Electrochim. Acta, 2013, 106, 209 CrossRef CAS PubMed.
  22. J. Evans, C. A. Vincent and P. G. Bruce, Polymer, 1987, 28, 2324 CrossRef CAS.
  23. K. M. Abraham, Z. Jiang and B. Carroll, Chem. Mater., 1997, 9, 1978 CrossRef CAS.
  24. S. A. Katsyuba, E. E. Zvereva, A. Vidis and P. J. Dyson, J. Phys. Chem. B, 2007, 111, 352 CAS.
  25. Y. Masuda, M. Seki, M. Nakayama, M. Wakihara and H. Mita, Solid State Ionics, 2006, 177, 843 CrossRef CAS PubMed.
  26. T. Nishida, Y. Tashiro and M. Yamamoto, J. Phys. Chem. B, 2003, 120, 135 CAS.
  27. T. Nishida, Y. Tashiro and M. Yamamoto, J. Fluorine Chem., 2003, 120, 135 CrossRef CAS.
  28. Shalu, S. K. Chaurasia, R. K. Singh and S. Chandra, J. Phys. Chem. B, 2013, 117, 897 CrossRef CAS PubMed.
  29. H. H. Zheng, The electrolyte for Li-ion batteries, Chemical Industry Press, Beijing, 2007, p. 169 Search PubMed.
  30. Y. M. Lee, D. H. Ko, J. Y. Lee and J. K. Park, Electrochim. Acta, 2006, 52, 1582 CrossRef CAS PubMed.
  31. T. Niitani, M. Shimada, K. Kawamura and K. Kanamura, J. Power Sources, 2005, 146, 386 CrossRef CAS PubMed.
  32. W. Xu, K. S. Siow, Z. Q. Gao and S. Y. Lee, Solid State Ionics, 1998, 112, 1 CrossRef CAS.
  33. A. M. Stephan, Y. Saito, N. Muniyandi, N. G. Renganathan, S. Kalyanasundaram and R. N. Elizabeth, Solid State Ionics, 2002, 148, 467 CrossRef.
  34. Y. Kang, H. J. Kim, E. Kim, B. Oh and J. H. Cho, J. Power Sources, 2001, 92, 255 CrossRef CAS.
  35. G. H. Lane, Electrochim. Acta, 2012, 83, 513 CrossRef CAS PubMed.
  36. S. Y. Chew, J. Sun, J. Wang, H. K. Liu, M. Forsyth and D. R. MacFarlane, Electrochim. Acta, 2008, 53, 6460 CrossRef CAS PubMed.
  37. Q. Hu, S. Osswald, R. Daniel, Y. Zhu, S. Wesel, L. Ortiz and D. R. Sadoway, J. Power Sources, 2011, 196, 5604 CrossRef CAS PubMed.
  38. K. Hayamizu, Y. Aihara, H. Nakagawa, T. Nukuda and W. S. Price, J. Phys. Chem. B, 2004, 108, 19527 CrossRef CAS.
  39. H. Ye, J. Huang, J. J. Xu, A. Khalfan and S. G. Greenbaum, J. Electrochem. Soc., 2007, 154, A1048 CrossRef CAS PubMed.
  40. H. S. Jeong and S. Y. Lee, J. Power Sources, 2011, 196, 6716 CrossRef CAS PubMed.
  41. N. S. Choi and J. K. Park, Electrochim. Acta, 2001, 46, 1453 CrossRef CAS.

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