Jung-Soo
Lee‡
a,
Ken
Sakaushi
*ab,
Markus
Antonietti
a and
Jiayin
Yuan
*a
aMax Planck Institute of Colloids and Interfaces, Colloid Chemistry Department, Am Mühlenberg 1 OT Golm, D-14476 Potsdam, Germany. E-mail: jiayin.yuan@mpikg.mpg.de
bNational Institute for Materials Science, International Center for Materials Nanoarchitectonics (MANA), 1-1 Namiki, Tsukuba, 305-0044 Ibaraki, Japan. E-mail: sakaushi.ken@nims.go.jp
First published on 30th September 2015
A series of poly(ionic liquid)s (PILs) were used as binders for lithium-ion battery (LIB) with a LiFePO4 cathode to explore their role and benefits in a model electrochemical energy storage system. The PILs are imidazolium-based and bear different main chain structures and alkyl substituents. The results nicely show that PILs both improve the cycling stability and specific capacity. When carefully designed, they especially exhibited a usually high electrochemical stability against oxidative conditions (=4.0 vs. Li/Li+). It is found that the PIL binders together with carbon additive form very effective Li+ and electron conducting pathways in the electrode. These finding illustrate that binder with carefully designed chemical structures can have a high potential to improve the electrochemical performance even of current rechargeable battery systems. A better Li+ and electron conduction is however of general importance for a wide spectrum of electrochemical devices.
Through very limited but inspiring primary studies,6–12 it is well known that even huger effects of polymer binders on the overall performance of many electrochemical devices can be expected, particularly with respect to the resulting mechanical properties and interactions with electrolytes and active material. PVDF has been extensively utilized as a standard choice for electrodes of, among many, LIBs due to its electrochemical inertness, especially for cathodes. The disadvantages of PVDF binders are its insulating character and a relatively large amount of electrolyte swelling. As a result, the adhesion of PVDF to electrode materials deteriorates under long operational run, and an increase in contact resistance between the active material and carbon material is found.12 As lifetime enters directly the costs per stored kWh of a practical large-scale energy storage system, any lifetime improvement is valuable, and a stable operation for more than a decade is desired.13 To overcome these drawbacks, newly designed binder materials are necessary. In our opinion, next-generation binders participating in the main electrochemical reactions, but being at same time electrochemically at least as stable as PVDF, can help address those problems.
Ionic liquids (ILs) are for a long time investigated for use in several electrochemical energy storage/conversion devices, due to their favorable physical properties such as negligible vapor pressure, high ion conductivity, chemical inertness and a broad electrochemical stability.14–21 Recently, the interest on poly(ionic liquid)s (PILs) were found to be a highly attractive class of functional polymers.22–27 To our knowledge, only in a recent paper a PIL copolymer in nanoparticulate form have been examined as binder for electrode of LIBs.28 In spite of the exciting and encouraging progress reported when applied to the cathode, these nanoparticle binders were nevertheless claimed to decompose under operation. It should however be possible to avoid this degradation when the binders are correctly designed by polymer chemistry. In our recent attempt, via modifying the building unit of PIL nanoparticles, we were able to extend the cycling stability of LIBs far beyond that based on PVDF binder. Nevertheless, the complicated synthetic chemistry to PIL nanoparticles not only makes the large-scale production unconventional but also restricts a deep insight in the electrochemical process of how these binders improve the electrode performance.29
Here, we demonstrate the good performance and high stability of more easy-to-synthesize linear chain PIL binders, while trying to describe mechanistically how they assist the electrochemical reactions in LIBs. The data can be described by formation of a favorable Li+ conducting polymer interface which acts as a heterojunction at the storage material grains. At the same time, while stabilizing and connecting the carbon additives, it forms a convenient electron conductive network.
Fig. 1 Chemical structures of three PIL binders used in this study. TFSI denotes the counter anion, bis(trifluoromethane sulfonyl)imide. |
The success in the monomer and PIL synthesis was confirmed by proton nuclear magnetic resonance (1H-NMR) spectra and Fourier transform infrared spectroscopy (FT-IR) in Fig. S1 and S2.† Gel permeation chromatography was performed to determine the number-average apparent molecular weight of the PILs, which are 130, 85 and 37 kDa, respectively (Fig. S3†). These PILs feature a high density of IL species, i.e. one per unit, as well as a multivalent binding power via the linear connection of the IL species into a polymer backbone. The polymers are expected to possess a broad electrochemical window and enhanced surface activity, two of the key requirements for binder materials. In the specific design of this work, 3 different PILs in terms of the backbone structure and substitution pattern on the imidazolium ring were chosen and are denoted as P1, P2, and P3, respectively. P1 has a polyvinylimidazolium-based backbone while P2 and P3 have a polystyrene-based one. Additionally, P2 and P3 differentiate in terms of blocking the alkalinity of the C2 position with a methyl unit.
The electrochemical properties of the PIL binders were investigated by several electrochemical techniques. First of all, we examined our binders using LiFePO4 as a model cathode material (a redox potential at 3.4 V vs. Li/Li+; a theoretical specific capacity of 170 mA h g−1) with a current density of 1C, which will assumes fully charge or discharge in one hour (=170 mA g−1).30–32 The charge–discharge curves show that PIL binders P1, P2 and P3 favorably delivered a higher specific capacity of 126, 132 and 137 mA h g−1, respectively, higher than the PVDF binder with 120 mA h g−1. This result indicates that PILs can make a higher specific capacity of the material accessible. In parallel, the electrodes with P1, P2 and P3 were proven stable until 100 cycles at the same current density (Fig. 2B).
Fig. 2 Electrochemical properties of LiFePO4 electrodes using different PIL binders. (A) Charge–discharge curves at a current density of 1C (=170 mA g−1). (B) Cycling performance up to 100 cycles at 1C. (C) Cycling performance up to 1000 cycles at 5C (=850 mA g−1). (D) Rate capability for PIL binders and PVDF. The rate capability data of PVDF (the black line in (A), (B) and (C)) was taken from ref. 29 (active materials loading 2.5 mg). |
Further investigations on the PIL binders were executed by a higher current density of 5C (=850 mA g−1), which is harsh and provides accelerated ageing of all involved materials (Fig. 2C). The cathodes using PVDF, P1, P2 and P3 show at these high currents initial discharge capacities of 85, 90, 96 and 101 mA h g−1, respectively. P1 exhibits the lowest specific capacity, while P3 presents both a highest specific capacity and the best cycling stability, with around 86% retention of the initial specific capacity after 1000 cycles (Fig. 3C). This is the highest value of the tested binders in this work. Also the rate capability suggests that P3 is the best structure among the three tested PIL binders (Fig. 3D).
To track the chemical alterations being potentially responsible for the different behaviors of these binders in the electrode operation, 1H-NMR (Fig. 3) and FT-IR (Fig. S5†) spectroscopies were employed to analyze the chemical structure for all binders before and after a 2 week corrosion test at 4.0 V vs. Li/Li+ (see ESI† for details). In Fig. 3A, the 1H-NMR spectra of PVDF appear identical before and after the test, indicating that PVDF is inert during this well-define process. In comparison in Fig. 3B of P1, peaks between 7 and 9.5 ppm assigned to the imidazolium protons have changed significantly. The protic α-H (marked in red) at C2 position vanished after the test. It is known that the α-H due to its acidity may become invisible due to proton exchange with protic NMR solvents. In the current case, a non-protic NMR solvent, DMSO-d6 was used for these two samples under identical conditions, and the signal of α-H in P1 disappeared only in the sample after the corrosion test. This comparison thus supports unambiguously the occurrence of side reactions at the C2 position. Additionally, in the FT-IR spectrum of the P1 binder, the bands at 2950 cm−1 assigned to –CH3 stretching models (Fig. S5B†) disappeared completely at their original position and a set of new bands were observed at 3150 cm−1, implying that the α-H elimination may form the imidazol-2-ylidene persistent carbene under the electrochemical condition.33 Furthermore, the appearance of multiple peaks from 1600 to 1725 cm−1 in P1 after the corrosion test is indicative of the oxidation of the ethyl substituent into several types of carbonyl functions, such as aldehyde, ketone or carboxylic acids, which cannot be specifically distinguished at present. Bearing this observation in mind, we concluded that P1, though delivers a high specific capacity in the initial runs (Fig. 2B), is intrinsically unstable during the long term charging–recharging process. In the case of P2 (Fig. 3C), less changes were observed in the 1H-NMR spectra. The change in α-H signal was nevertheless spotted by a slight shift from 9.2 to 9.5 ppm, a sign that α-H elimination takes place only partially. Affected by this side reaction, the other 2 imidazolium protons deform their signals around 7.5 ppm. The two FTIR spectra did not present detectable variation before and after the corrosion tests. A close view on the chemical structures of P1 and P2 implies that the large phenyl ring attached to the imidazolium unit via a methylene bridge exerts a positive effect, which is possibly related to the sterical hindrance that minimizes the attack to the imidazolium ring. In the case of P3, the basic C2 position was blocked by a methyl group. No change was identified at all in both 1H-NMR and FTIR spectra (Fig. 3D and S5C and D†). P3 is intrinsically the most inert among the three PILs in a harsh electrochemical environment and maintains its glueing and conducting power.
Further investigations were carried out to explain the exact functions of PIL binders to deliver higher specific capacities than PVDF. In our previous report, the PIL nanoparticle binders were discussed to reduce the interfacial charge transfer resistance, being a major part of resistance in Li+ intercalation mechanism.29 In order to give a deeper insight in this phenomenon of the current linear PIL system, we build up the cathodes made of only binders (the cell configuration is PIL/liquid electrolyte/Li) and measured cyclic voltammograms (CVs) and electrochemical impedance spectra (EIS) at room temperature (Fig. 4). We applied an equivalent circuit based on half-blocking cell to fit the EIS which is constituted of an electrolyte resistance (Rs), charge transfer resistance (R1 and R2), constant phase element (CPE1 and CPE2), and capacitance at the blocking electrode (C1). For PVDF, P2, and P3, the CVs exhibited similar specific capacitance and showed no redox peak for all samples, which means that there is no electrochemical transition/energy storage function for the PIL binders (Fig. 4A). Only P1 shows small anodic peak suggesting formation of decomposition as shown by the 1H-NMR spectrum (Fig. 3B). However, the EIS show that the PIL binders are Li+ conductors in the presence of electrolyte (LiPF6 in EC/DMC) while PVDF is not (Fig. 4B and S6, and Table S1†). A high Li+ conductivity of PILs is found in general in the presence of Li salts, which was also well studied by Ohno and other researchers.23,34,35 The pristine PIL phase doesn't contain any Li+ and is not a Li+ conductor. The Li+ conductivity in the cell occurred after a formation of PIL/liquid electrolyte swollen layer phase, where the lithium salt starts to diffuse into the PIL phase and turns it into a Li+ conductor. Worth mentioning, the binder P3 outperforms all other systems already in this short term experiment, i.e. it provides the lowest ion and current flux resistance.
Fig. 4 Electrochemical characterization for the PIL binders and PVDF. (A) Cyclic voltammograms, and (B) electrochemical impedance spectra at room temperature. |
Considering these results, we can propose an overall mechanism for high electrochemical performance where the PIL binders do not only glue the particles, but actively contribute to the high ion conductivity in a two-phase nano-heterojunction system.36,37 The PIL binders absorb the organic electrolyte in their chain structures, building up a nanometer thick layer with a higher concentration of Li+ at the interface to the active battery material (here LiFePO4) of PIL binder and bulk electrolyte (Fig. 5). It must be underlined that the build-up of an (inhibitive) Maxwell–Wagner polarization sensitively depends on the charge concentrations at the interface. The applied equivalent circuit model for the Li+-cathode containing two semi-circles to fit the experimentally obtained impedance signal (Fig. 4B inset): the first semi-circle is related to Li+ transfer resistance from a bulk liquid electrolyte to the heterophase associated with the desolvation process (R1), and the second semi-circle described the Li+ transfer resistance in the LiFePO4 heterophase (R2).38–40 From a view of chemistry, the data describe an enhanced electrochemical reactions via high ion conductivity and high electrochemical stability of an enriched electrolyte nanophase, as the concentration of Li+ in the PIL-stabilization layer is higher than in the bulk because the PILs are favorably polarized media.
In the EIS measurements P3 showed both the lowest R1 and R2 among the three PILs (Fig. 4B and Table S1†). We can only speculate why P3 is most favourable, but it is to be assumed that the 3 solvophilic substituents on the charged imidazolium ring prohibit the known interface packing41 and thereby give the space to embed mobile Li-ions. From this point of view, PVDF is in any case an undesired choice, as it forms an insulation layer, independent of the presence of electrolyte (Fig. 5 and S6†).
Also for interaction with the conductive carbon additive, the formation of interfacial space Li+ charging layer will promote ionic character and conduction. The well-known charge transfer interaction between PILs to carbons making them perfect nanocarbon stabilizers42,43 is not only creating a favourable structural electron pathway due to a strong interaction between carbon and PILs, but at the same time will also increase the number of charge carriers by charge transfer effects.
Footnotes |
† Electronic supplementary information (ESI) available. See DOI: 10.1039/c5ra16535k |
‡ Present address: Chosun University, Department of Bio-chemical and polymer engineering, 309 Pilmun-daero, Dong-gu, Gwangju 501-759, Korea. |
This journal is © The Royal Society of Chemistry 2015 |