42 research outputs found
Polymer Actuators Using Ion-Gel Electrolytes Prepared by Self-Assembly of ABA-Triblock Copolymers
Well-defined ABA-triblock copolymers, polystyrene-<i>block</i>-polyÂ(methyl methacrylate)-<i>block-</i>polystyrene
(SMS),
which have two different polystyrene (PSt) weight fractions (<i>f</i><sub>PSt</sub>), were synthesized by successive atom-transfer
radical polymerizations. Ion gels consisting of SMS and an ionic liquid,
(1-ethyl-3-methylimidazolium bisÂ(trifluoromethanesulfonyl)Âamide [C<sub>2</sub>mim]Â[NTf<sub>2</sub>]), were prepared using the cosolvent
evaporation method with tetrahydrofuran. Atomic force microscope images
of the ion gels indicated that PSt is phase-separated to form sphere
domains that serve as physical cross-linking points because PSt is
not compatible with [C<sub>2</sub>mim]Â[NTf<sub>2</sub>], while a continuous
polyÂ(methyl methacrylate) (PMMA) phase with dissolved [C<sub>2</sub>mim]Â[NTf<sub>2</sub>] is formed to serve as ion conduction paths.
Accordingly, the ion gels are formed by the self-assembly of SMS and
the preferential dissolution of [C<sub>2</sub>mim]Â[NTf<sub>2</sub>] into the PMMA phase. The viscoelastic properties of the gels can
be easily controlled by changing <i>f</i><sub>PSt</sub> in
SMS and [C<sub>2</sub>mim]Â[NTf<sub>2</sub>] concentration in the ion
gels. The ion gels that exhibit high ionic conductivities (>10<sup>–3</sup> S cm<sup>–1</sup>) at room temperature were
used as an electrolyte of an ionic polymer actuator, which has a trilaminar
structure consisting of the ion-gel electrolyte sandwiched between
two composite carbon electrodes containing high-surface-area activated
carbon powders. By applying low voltages (<3.0 V) to the electrodes,
the actuator exhibited a soft bending motion toward the anodic side
Driving Mechanisms of Ionic Polymer Actuators Having Electric Double Layer Capacitor Structures
Two solid polymer electrolytes, composed of a polyether-segmented
polyurethaneurea (PEUU) and either a lithium salt (lithium bisÂ(trifluoromethanesulfonyl)Âamide:
LiÂ[NTf<sub>2</sub>]) or a nonvolatile ionic liquid (1-ethyl-3-methylimidazolium
bisÂ(trifluoromethanesulfonyl)Âamide: [C<sub>2</sub>mim]Â[NTf<sub>2</sub>]), were prepared in order to utilize them as ionic polymer actuators.
These salts were preferentially dissolved in the polyether phases.
The ionic transport mechanism of the polyethers was discussed in terms
of the diffusion coefficients and ionic transference numbers of the
incorporated ions, which were estimated by means of pulsed-field gradient
spin–echo (PGSE) NMR. There was a distinct difference in the
ionic transport properties of each polymer electrolyte owing to the
difference in the magnitude of interactions between the cations and
the polyether. The anionic diffusion coefficient was much faster than
that of the cation in the polyether/LiÂ[NTf<sub>2</sub>] electrolyte,
whereas the cation diffused faster than the anion in the polyether/[C<sub>2</sub>mim]Â[NTf<sub>2</sub>] electrolyte. Ionic polymer actuators,
which have a solid-state electric-double-layer-capacitor (EDLC) structure,
were prepared using these polymer electrolyte membranes and ubiquitous
carbon materials such as activated carbon and acetylene black. On
the basis of the difference in the motional direction of each actuator
against applied voltages, a simple model of the actuation mechanisms
was proposed by taking the difference in ionic transport properties
into consideration. This model discriminated the behavior of the actuators
in terms of the products of transference numbers and ionic volumes.
The experimentally observed behavior of the actuators was successfully
explained by this model
Ionic Liquid Electrolytes for Lithium–Sulfur Batteries
A variety
of binary mixtures of aprotic ionic liquids (ILs) and
lithium salts were thoroughly studied as electrolytes for rechargeable
lithium–sulfur (Li–S) batteries. The saturation solubility
of sulfur and lithium polysulfides (Li<sub>2</sub>S<sub><i>m</i></sub>), the active materials in the Li–S battery, in the
electrolytes was quantitatively determined, and the performance of
the Li–S battery using the electrolytes was also investigated.
Although the solubility of nonionic sulfur was low in all of the electrolytes
evaluated, the solubility of Li<sub>2</sub>S<sub><i>m</i></sub> in the IL-based electrolyte was strongly dependent on the
anionic structure, and the difference in the solubility could be rationalized
in terms of the donor ability of the IL solvent. Dissolution of Li<sub>2</sub>S<sub><i>m</i></sub> in the ILs with strong donor
ability was comparable to that achieved with typical organic electrolytes;
the strongly donating IL electrolyte did not prevent redox shuttle
reaction in the Li–S cells. The battery performance was also
influenced by unfavorable side reactions of the anions (such as tetrafluoroborate
(BF<sub>4</sub><sup>–</sup>) and bisÂ(fluorosulfonylamide) ([FSA]<sup>−</sup>)) with polysulfides and by slow mass transport in
viscous ILs, even though the dissolution of Li<sub>2</sub>S<sub><i>m</i></sub> into the IL electrolyte was greatly suppressed.
Among the IL-based electrolytes, the low-viscosity [TFSA]-based ILs
facilitated stable charge/discharge of the Li–S batteries with
high capacity and high Coulombic efficiency. The unique <i>solvent
effect</i> of the ILs can thus be exploited in the Li–S
battery by judicious selection of ILs that exhibit high lithium-ion-transport
ability and electrochemical stability in the presence of Li<sub>2</sub>S<sub><i>m</i></sub>
Effect of Variation in Anion Type and Glyme Length on the Nanostructure of the Solvate Ionic Liquid/Graphite Interface as a Function of Potential
Atomic force microscope (AFM) force
curves are used to probe the effect of anion species and glyme length
on the nanostructure of the solvate ionic liquid (SIL)/highly ordered
pyrolytic graphite (HOPG) interface as a function of applied potential.
At all potentials, the lithium tetraglyme bisÂ(trifluoromethylsulfonyl)Âimide
(LiÂ(G4)ÂTFSI)/HOPG is more structured than lithium tetraglyme bisÂ(perfluoroethylsulfonyl)Âimide
(LiÂ(G4)ÂBETI)/HOPG because [BETI]<sup>−</sup> has greater conformational
flexibility. The LiÂ(G3) trifluoroacetate (TFA)/HOPG interface is even
more disordered because [TFA]<sup>−</sup> coordinates strongly
to the lithium ion, leading to a high concentration of free glyme.
The LiÂ(G3)ÂTFSI/HOPG interface is more structured than the LiÂ(G4)ÂTFSI/HOPG
interface because the longer glyme increases the molecular flexibility
of the complex cation. The LiÂ(G1)<sub>2</sub>TFSI/HOPG interface has
weak interfacial structure because monoglyme is poorly coordinating
so the free glyme concentration is high. Despite LiÂ(G3)ÂTFSI, LiÂ(G4)ÂTFSI,
and LiÂ(G4)ÂBETI being good SILs (meaning the free glyme concentration
is low), application of a negative potential to the HOPG surface leads
to the desolvation of Li<sup>+</sup> from the glyme at the surface
Printable Polymer Actuators from Ionic Liquid, Soluble Polyimide, and Ubiquitous Carbon Materials
We
present here printable high-performance polymer actuators comprising
ionic liquid (IL), soluble polyimide, and ubiquitous carbon materials.
Polymer electrolytes with high ionic conductivity and reliable mechanical
strength are required for high-performance polymer actuators. The
developed polymer electrolytes comprised a soluble sulfonated polyimide
(SPI) and IL, 1-ethyl-3-methylimidazolium bisÂ(trifluoromethanesulfonyl)Âamide
([C<sub>2</sub>mim]Â[NTf<sub>2</sub>]), and they exhibited acceptable
ionic conductivity up to 1 × 10<sup>–3</sup> S cm<sup>–1</sup> and favorable mechanical properties (elastic modulus
>1 × 10<sup>7</sup> Pa). Polymer actuators based on SPI/[C<sub>2</sub>mim]Â[NTf<sub>2</sub>] electrolytes were prepared using inexpensive
activated carbon (AC) together with highly electron-conducting carbon
such as acetylene black (AB), vapor grown carbon fiber (VGCF), and
Ketjen black (KB). The resulting polymer actuators have a trilaminar
electric double-layer capacitor structure, consisting of a polymer
electrolyte layer sandwiched between carbon electrode layers. Displacement,
response speed, and durability of the actuators depended on the combination
of carbons. Especially the actuators with mixed AC/KB carbon electrodes
exhibited relatively large displacement and high-speed response, and
they kept 80% of the initial displacement even after more than 5000
cycles. The generated force of the actuators correlated with the elastic
modulus of SPI/[C<sub>2</sub>mim]Â[NTf<sub>2</sub>] electrolytes. The
displacement of the actuators was proportional to the accumulated
electric charge in the electrodes, regardless of carbon materials,
and agreed well with the previously proposed displacement model
Solubility of Poly(methyl methacrylate) in Ionic Liquids in Relation to Solvent Parameters
The solubility of
polyÂ(methyl methacrylate) (PMMA) in 1-alkyl-3-methylimidazolium
ionic liquids (ILs) with different anionic structures has been explored.
Nearly monodisperse PMMA-grafted silica nanoparticles (PMMA-<i>g</i>-NPs) were used as a measurement probe for evaluating the
PMMA solubility in ILs. The hydrodynamic radius (<i>R</i><sub>h</sub>) of PMMA-<i>g</i>-NPs was measured in the
ILs by dynamic light scattering (DLS). Changes in <i>R</i><sub>h</sub> and colloidal stability, that is, the PMMA-solubility
change in the ILs, were observed depending on the ionic structures
of the ILs. The solubility was mainly affected by the anionic structures
of the ILs rather than by the alkyl chain length of the cationic structure.
Solvent parameters, including Lewis basicity, solubility parameters,
and a hydrophobicity parameter, were used to discuss the change in
the PMMA solubility in ILs with different ionic structures. By considering
the PMMA solubility in the ILs using these parameters, it was found
that there is a good correlation between the PMMA solubility and the
hydrophobicity parameter of the anions. Although the change in the
PMMA solubility with different cationic structures was not remarkable,
the hydrophobicity of the cations also played a role in the solvation
of PMMA by providing a low-polarity environment adequate to dissolve
PMMA
Thermally Reversible Ion Gels with Photohealing Properties Based on Triblock Copolymer Self-Assembly
We
describe a functional soft material that can spontaneously repair
damage by straightforward application of light illumination. The composite
material is composed of a common ionic liquid (IL), 1-butyl-3-methylimidazolium
hexafluorophosphate ([C<sub>4</sub>mim]ÂPF<sub>6</sub>), and a well-defined
ABA triblock copolymer consisting of the IL-compatible polyÂ(ethylene
oxide) (PEO) middle block with thermo- and photosensitive random copolymers
combining <i>N</i>-isopropylacrylamide (NIPAm) and 4-phenylazophenyl
methacrylate (AzoMA) including azobenzene chromophore as terminal
A blocks. The composite shows a sol–gel transition under UV
light (366 nm, 8 mW cm<sup>–2</sup>) irradiation at 47 °C,
whereas that observed under visible light (437 nm, 4 mW cm<sup>–2</sup>) is 55 °C, due to the difference in photochromic states of
the azobenzene unit. The ABA triblock copolymer undergoes a reversible
gel–sol–gel transition cycle at the bistable temperature
(53 °C), with a reversible association/fragmentation of the polymer
network resulting from the photoinduced self-assembly of the ABA triblock
copolymer in [C<sub>4</sub>mim]ÂPF<sub>6</sub>. A damaged ABA ion gel
shows a remarkable photohealing ability based on drastic changes in
the fluidity of the polymer–IL composite triggered by light
illumination. The damaged part is successfully repaired by shining
UV light resulting in solubilization to fill the crack, followed by
gelation to fix the crack triggered by visible light illumination.
Tensile tests confirmed the excellent recovery efficiency of the resultant
photohealed ABA ion gel, which was as high as 81% fracture energy
relative to the original sample. The flexible, self-supported ABA
ion gel is designed for various applications to exhibit not only photohealing
ability to improve operating lifetime of the material but also specific
functionalities imparted by the IL, such as high ion conductivity,
thermal stability, and (electro)Âchemical stability
Enhancing Li–S Battery Performance with Limiting Li[N(SO<sub>2</sub>F)<sub>2</sub>] Content in a Sulfolane-Based Sparingly Solvating Electrolyte
By enhancing the stability of the
lithium metal anode and mitigating
the formation of lithium dendrites through electrolyte design, it
becomes feasible to extend the lifespan of lithium–sulfur (Li–S)
batteries. One widely accepted approach involves the utilization of
Li[N(SO2F)2] (Li[FSA]), which holds promise
in stabilizing the lithium anode by facilitating the formation of
an inorganic-dominant solid electrolyte interface (SEI) film. However,
the use of Li[FSA] encounters limitations due to inevitable side reactions
between lithium polysulfides (LiPSs) and [FSA] anions. In this study,
our focus lies in precisely controlling the composition of the SEI
film and the morphology of the deposited lithium, as these two critical
factors profoundly influence lithium reversibility. Specifically,
by subjecting an initial charging process to an elevated temperature,
we have achieved a significant enhancement in lithium reversibility.
This improvement is accomplished through the employment of a LiPS
sparingly solvating electrolyte with a restricted Li[FSA] content.
Notably, these optimized conditions have resulted in an enhanced cycling
performance in practical Li–S pouch cells. Our findings underscore
the potential for improving the cycling performance of Li–S
batteries, even when confronted with challenging constraints in electrolyte
design
Thermosensitive Phase Separation Behavior of Poly(benzyl methacrylate)/Solvate Ionic Liquid Solutions
We report a lower
critical solution temperature (LCST) behavior
of binary systems consisting of polyÂ(benzyl methacrylate) (PBnMA)
and solvate ionic liquids: equimolar mixtures of triglyme (G3) or
tetraglyme (G4) and lithium bisÂ(trifluoromethanesulfonyl)Âamide. We
evaluated the critical temperatures (<i>T</i><sub>c</sub>s) using transmittance measurements. The stability of the glyme–Li<sup>+</sup> complex ([LiÂ(G3 or G4)]<sup>+</sup>) in the presence of PBnMA
was confirmed using Raman spectroscopy, pulsed-field gradient spin–echo
NMR (PGSE-NMR), and thermogravimetric analysis to demonstrate that
the complex was not disrupted. The interaction between glyme–Li<sup>+</sup> complex and PBnMA was investigated via <sup>7</sup>Li NMR
chemical shifts. Upfield shifts originating from the ring-current
effect of the aromatic ring within PBnMA were observed with the addition
of PBnMA, indicating localization of the glyme–Li<sup>+</sup> complex above and below the benzyl group of PBnMA, which may be
a reason for negative mixing entropy, a key requirement of the LCST