Chemical structure and physicochemical property of IL .
Ionic-polymer based actuators have the advantages of low voltage and power requirements, being easily processable, flexibility, soft action and bio-mimetic activation, which are of considerable interests for applications in biomedical micro-devices and soft robotics. In this chapter, we firstly review the development of ionic polymer actuator and reveal the universal architecture and mechanism of ionic polymer actuators. We then introduce two kinds of typical polymer actuators: ionic polymer-metal composites (IPMC) and bucky gel actuator (BGA), including their basic principle, fabrication process and typical applications. The aim of this chapter is to give some perspectives on IPMC and BGA and provide a way and case in using this actuator for real applications.
- electroactive polymer
- ionic polymer
- carbon nanotube
- ionic liquid
Recently, as one typical electroactive polymers (EAP), ionic polymer actuators have gradually grown into an important smart material, which is mainly composed of the interlayer for mass transfer and conductive layers on both sides similar to the sandwich structure. When applied an electric field, local stress occurs due to the migration of ions bonded solvent molecules toward the electrode layers, which causes one side to swell and another side to shrink, resulting in bending deformation as shown in Figure 1. Due to large bending deformation by low driven voltage, much attention has been focused on ionic polymer actuators [1, 2, 3].
The origin of ionic polymer actuators can be traced back to the 1990s of last century. Adolf et al.  and Oguro et al.  introduced the initial prototype patent of ionic polymer actuators in early stage. They both claimed that an actuator comprises an ion exchange membrane and a pair of electrodes attached to opposite surfaces of the ionic polymer, which refers to the cation or anion exchange membrane. Adolf et al. even named the actuator electrically controlled polymeric gel actuators, which maybe is the first normal name of ionic polymer actuator. After that, many researchers were attributed themselves to explore the essential properties of this actuator. They give different names to this special actuator based on different understandings, such as ionic polymeric gel actuator , electrically controllable artificial muscle , ion-exchange membrane metal composites , Nafion-Pt composite actuators (ICPF)  and ionic polymer-metal composites (IPMC) , which is the most common names so far. At this stage, it is dominant to clarify the actuating mechanism of this kind of actuator. So several electromechanical and physical models were gradually developed by de Gennes et al. , Newbury and Leo [12, 13], Nemat-Nasser et al. , Tadokoro et al. , Zicai Zhu et al. [15, 16] and so on. Meanwhile, for this ionic polymer actuator, the ionomer layer and conductive layer are critical components. The substitutes of components are an important way to improve the electromechanical performance of the actuator. Generally, perfluorinated polymers, such as Nafion (sulfonated) or Flemion (carboxylated), are employed as ionomer layer. The actuation ability of the ionic polymer actuator seriously is dependent on fixed anions, mobile cations and nanochannels inside Nafion or Flemion. Based on this property, a lot of novel hydrocarbon ion-exchangeable membranes are introduced to replace the ionomer layer . These membranes include commercial products, blending and synthetics, some of which overcome the back-reversal problem and show much larger bending deformation compared to the Nafion- or Flemion-IPMC, such as poly(styrene-alt-maleimide) (PSMI)-incorporated poly(vinylidene fluoride) (PVDF) and chitosan/polyaniline interpenetrating polymer network. Likewise, the electrode layer plays an important role in IPMC actuation. It is considered to be easier to modify the electrode layer to optimize the IPMC property than the ionomer layer. Of all metals, gold and platinum with excellent conductivity and chemical stability are the most widely used electrode materials. Because of high cost, inexpensive electrode materials are still in need to replace gold and platinum. Palladium , silver  or their complex  has been considered as substitute.
With the development of new conductive materials, non-metallic materials, such as polyaniline (PANI), carbon nanotube (CNT) and grapheme etc., are also introduced as electrode materials of the actuator. On this basis, Fukushima et al.  proposed a novel kind of fully plastic actuator fabricated by layer-by-layer casting with ionic liquid based bucky gel, which also named bucky-gel actuator (BGA). The bucky-gel actuators composed of the conductive layers of the CNT blending ionic liquid and PVdF(HFP) and the interlayer made of the ionic liquid and PVdF(HFP). In contrast with IPMC, the fabrication process includes neither deposition of metallic layers nor actuating ion exchange. And the bucky-gel actuator can operates stably and quickly in air without back-reversal deformation under DC voltage.
In this chapter, we try to give an overview of two kinds of typical polymer actuators: ionic polymer- metal composites (IPMC) and bucky gel actuator (BGA), including their basic principle, fabrication process and typical applications. We put some results of previous works into more general perspective as well and provide insights of how these results have to be considered for the implementation of future applications. The study and development of polymer actuators are unfolding. This is no doubt that ionic actuators will show great potentials as alternatives for use in the application of precision micro-actuating technology in the future.
As we all know that charged particles will have a directional migration effect when put in the electric field. Generally, parallel plate capacitors would create a uniform electric field between the plates. Special dielectric is added into capacitor, which has unique property with solid–liquid two-phase microstructure. Charged particles (such as cations) do not exist alone in solution environment, and they tend to bind to a certain amount of solvent molecules forming solvated cations. Charged particles together with solvent molecules travel through the liquid-phase microstructure of dielectric from one side to another side when voltage is applied to the plates. This will result in mass plentiful on one side and exhausted on the other side. At this point, mechanical local strain will occur on both sides. These constitute the basic principle of ion polymer actuators.
As mentioned in Section 1, normally, an IPMC consists of an ionomer membrane plated on both sides with metal electrodes and neutralized with the necessary amount of mobile ions and fixed counterions. Metal electrodes form the outermost layers, followed by the intermediate layer. The intermediate layer comprises of metal particles dispersed inside the polymer matrix, which contains the ionomer, the counter ions and solvent molecules inside the membrane as shown in Figure 2. Nafion by DuPont or Flemion by Asahi Glass are most used as ionomer. The differences between them are in the functional groups (sulfonate and carboxylate groups respective) and ion-exchange capacities. The chemical structure of Nafion and Flemion are shown in Figure 2(a). The commonly used cations inside the membrane include the alkali metal cations, such as Li, Na, K, Rb and Cs while the solvent mainly refer to water and ionic liquid [21, 22]. For electrode layer, due to their corrosion resistance and high conductivity, platinum and gold are commonly used [1, 23]. In our lab, we developed palladium typed IPMC because of its relative low price and optimized its preparation process [17, 24].
Bucky gel actuators (BGAs) are composed by carbon nanotubes (CNTs), ionic liquid (IL), and base polymer (BP). Single-walled CNT (SWCNT) is one of good nanocarbons as conductive electrode material. Not only imidazolium-type ILs but also ammonium-type ILs can be used as electrolyte source. Polyvinylidene fluoride-co-hexafluoropropylene (PVDF-HFP) is used as a BP. BGAs have a three-layered structure as shown in Figure 3, that is, one electrolyte layer is laminated by two electrode layers. A gel like self-standing electrolyte film is made with IL and BP. Generally, the electrode films are made from CNTs, IL, and BP. Some additives such as conductive or non-conductive nanoparticles can be added in the electrode layers in order to tune the electrochemical and mechanical properties of electrode [25, 26].
In contrast to IPMC and BGA, we can see that they both have very similar structures, with the exception of the ingredient of the electrode layer and interlayer, separately. This, of course, will finally result in the difference in preparation process and electromechanical performance.
2.2. Bending mechanism
The working mechanism of IPMC can be explained through electromechanical transduction. When applying an electric field, the cations inside the base membrane move toward the cathode with water molecules. The asymmetric distributions of the concentration of cations and water cause the IPMCs to swell near the cathode and generates extensional stress in the polymer, which causes the IPMC to swell near the cathode and shrink beside the anode. Finally, a bending motion is generated toward the anode . Likewise, when an external stimuli was applied to the IPMC, the distributions of ions and water molecules inside IPMCs changes. Potential difference appears on both sides of the IPMC, which could be viewed as sensing signal. The properties of sensing and actuating of IPMC depend on the types of cation and solvent, surface resistant, interface morphology and temperature and humidity, etc.
In general, the current is generated by ion transport in BGAs and the three-layered BGAs show a bending motion to the anode side when voltages are applied. The electric charge is stored capacitively in BGAs during applying voltages . This implies that our BGA is a capacitor. Baughman et al. reported SWCNT sheets (bucky papers) show the expansion and contraction (actuation) in aqueous electrolyte solution against a counter electrode . They proposed the actuation mechanism in which C-C bond distance in SWCNT changes by charge injection originated from quantum and double-layer electrostatic effects. On the other hands, we consider the actuation mechanism of BGAs is due to C-C bond distance changing in CNTs [27, 28], volume change of the electrodes by sorption/desorption of ions , and electrostatic effect in the electrical double-layer . Kiyohara and Asaka theoretically investigated the actuation mechanism of BGAs by a method of Monte Carlo simulation [31, 32]. We also studied the actuation mechanism of BGAs by a combination of symmetrical analysis, elasticity theory, and experimental results in the bulk scale . As a result, it was found that the cathode expands and the anode contracts resulting in the bending motion of BGAs to the anode side.
3. Fabrication methods
The current IPMC preparation technique involves two distinct steps: initial pretreatment, impregnation–reduction (IR) and chemical deposition. In our lab, we improve the technique by combining impregnation electroplating (IEP) . The detailed process is as follows:
1) Nafion 117 was used as the interlayer roughened by sandblasting process. The diameter size of powders 200# is 0.0750 mm and the sandblasting time is 30 s. 2) Immerse the pre-treated Nafion in a 160 mL ammonia solution of [Pd (NH3)4]Cl2 with 140 mg Pd and 20 mL ammonia of 25% for 2 h with low-speed stirring. Then soak the pre-exchanged Nafion with the Pd complex cations in an alkaline solution of NaBH4 (2–5%, PH > 13) under an ultrasonic environment at a continuous raising temperature (i.e. from 30 to 50°C). Repeat the first two steps for 3 times. 3) The pretreated Nafion membrane was soaked in Pd complex solution again for over 2 h and then placed in the apparatus to electroplate for over 30 s for both sides. Repeat the third step for 3 times. Immerse the IPMC in an aqueous solution of NaOH (0.1–0.5 mol/L) for 2 h.
A typical preparation method to fabricate BGAs is described below. The electrode film was obtained from SWCNT (HiPco–SWCNT, purified grade), PVDF-HFP (Kynar FlexⓇ2801), and 1-ethyl-3-methylimidazolium tetrafluoroborate (EMIBF4) as an ionic liquid. 20 wt% of SWCNT, 32 wt% of PVDF-HFP, and 48 wt% of EMIBF4 were dissolved into 9 mL of N, N-dimethylacetamide (DMAC) and stirred for more than 1 day at room temperature, then sonicated for 24 hours in an ultrasonic bath. A gelatinous black solution was obtained after sonication. Obtained gelatinous solution was cast into a Teflon mold (25 × 25 mm2) and dried on a hotplate at 50°C for 12 hours and dried DMAC furthermore at 80°C in vacuo for 3 days. As a result, a black self-standing electrode film was obtained. The electrolyte film was obtained from similar procedure. 50 wt% of PVDF-HFP and 50 wt% of EMIBF4 were mixed into the solvent mixture of 4-methyl-2-pentanone and propylene carbonate anhydrous and cast into the mold. The solvents were dried on a hot-plate then an opaque self-standing gel electrolyte was obtained. One electrolyte film was sandwiched by two electrode films with a hot-pressing technique to obtain the three-layered BGA. Super-growth SWCNT is also good nanocarbon for the electrode of BGAs . The more detail fabrication process is described elsewhere [25, 26].
4. Electromechanical responses
To evaluate the effect of parameters, the responses of IPMC, mainly including current and deformation, are measured in fully hydrated state. The performances of strip sample were tested for comparison. Figure 4 shows the testing schematic. The strip sample with 40 mm in length and 5 mm in width is clamped by two copper disks. The displacement at the point 25 mm away from the fixed point is measured by a laser displacement sensor (Keyence, LK-G80). The applied voltage and current are simultaneously measured. The tip displacement w of samples can be calculated from the measured displacement
The currents and deformations under DC voltage were measured more than 20 s. The voltage range was set from 0.5 to 1.7 V with an interval of 0.3 V. For the electrochemical system composed of water, palladium, Nafion, and Na + cations, the electrolytic voltage of water is 1.75 V even higher . So the voltages higher than 1.7 V were not employed in order to avoid the electrolysis process of water. To facilitate the analysis, the averages and errors of the peak currents and maximum deformations of the samples, testing three times for each sample, were extracted and recorded as shown in Figure 5. It can be observed that the peak currents increase with the applied voltage increasing (Figure 5(a)). Under the voltage of 2 V, the current response fluctuates in some degree due to the electrolysis of water. From Figure 5(b), the maximum displacements of sample exhibit significant differences. With the applied voltages in an increase, the maximum displacements are increased.
To further investigate the relationship between the electrode morphologies, physical and electrical parameters and the electromechanical responses, an electrical component is introduced to explain the deformation behavior of IPMC as shown in Figure 6.
The interlayer of IPMC can be viewed as an ion conductive material and modeled by a capacitor and a resistor in parallel. The electrode can be modeled by two resistors. Then the peak current
It shows that the peak current depends on the electrode resistance, surface resistance, membrane resistance and the area of interface electrode closely related to dielectric modulus under the condition of constant voltage. Eq. (3) and (4) can be employed to interpret the deformation behaviors of IPMC. From the perspective of the fabrication process, different fabrication process will exert an important effect on the surface resistances of the samples. Roughening increases the surface resistance while chemical plating can reduce it. Meanwhile, the decrease of surface resistance largely increases the bending stiffness. Although the bending stiffness does not contribute to peak current directly, it is also a key factor to affect the deformation of IPMC as shown in Eq. (3). So it is necessary to optimize the roughening process and chemical plating process. The impregnation-reduction process mainly forms a penetration electrode to increase the area of interface electrode. But it is difficult to further improve the interface due to the blocking effect of previous plated layer.
As we described before, the capacitive current is generated in BGAs during applying voltages. This means that the electrolyte (ionic liquid (IL)) plays a very important role for the actuation of BGAs. So, we studied the influence of ILs on the actuation mechanism of BGAs. We investigated the electrochemical and electromechanical properties of BGAs by using seven kinds of ILs . The chemical structures of ILs are shown in Table 1. Some physicochemical properties, such as melting point (
The observed displacement (
The frequency dependence of strain (
The obtained parameters such as the double layer capacitance of the electrode (
5. Typical applications
Ionic polymer actuators have been expected to be used for some practical applications such as active microcatheters, micropumps, tactile displays, biomimetic microrobots, and so on [42, 43]. First commercial production with ionic EAP was produced by a Japanese company (Eamex Co.) in 2002 ( p. 2). They produced a fish robot which has a caudal fin made with ionic EAP. They can control the movement of the caudal fin by electromagnetic induction (wireless control).
Here, we introduce three examples of our application trials with IPMC and BGAs.
First sample is the prototype of developed micropump using inner petal-shaped IPMC actuator as shown in Figure 9. Micropumps capable of providing an appropriate flow rate and a reasonable back pressure are usually inevitable requirements for a self-contained microfluidic system. Since this is a prototype only, the pump was not made to be very small. The overall size is 70 × 40 × 15 mm (length × width × height). The pump chamber is a 15 mm in diameter, 2 mm in depth. It should be noted that, we only tested inner petal-shaped IPMC actuator with a diameter of 15 mm. The actuator used in this prototype is a Nafion 117-based IPMC actuator. A pair of copper plates as electrodes was used to clamp the two sides of the IPMC actuator, providing the stimulus electrical signal. In order to evaluate the performance of micropump, we carry out the experiment of the flow rate and the back pressure measurement in 1 Hz sine voltage input by changing the voltage amplitude from 0.5 to 3 V by the interval of 0.5 V. The experimental results show that the flow rate from 162 to 1611 μL/min can be obtained by changing the voltage amplitude from 0.5 to 3 V, respectively. And the back pressure on the micropump can be as high as 71 mm-H2O under the condition of 1 Hz and 3 V sine voltage input.
Second example is an ultra-thin and ultra-light refreshable Braille display with BGAs [41, 44]. There are more than 100 million visually impaired people in the world. This means there are a huge number of people who cannot access the internet because most information in the internet are shown with words and photos on the liquid crystal displays of mobile phones, laptop computers, and other tablet tools. Currently, the refreshable Braille displays with inorganic piezoelectric actuators are commercially available but they are not suitable for the mobile use because they are heavy (~kg) and large (266 (length) × 129 (width) × 40 mm (thickness) for a 32 Braille characters display). So, we had a motivation to produce an ultra-light and ultra-thin Braille display by using BGAs. The developed prototype Braille display with BGAs is shown in Figure 10 which has a size of 65 (length) × 30 (width) × 3 mm (thickness) with 6 refreshable Braille characters and the weight is only 5 g. This prototype Braille display was produce by collaborations with ALPS Electric Co., Ltd. Our Braille display was readable for most of visually impaired people but not readable for some visually impaired people who are not used to use Braille display. This is the reason why the dot force is not enough compared to commercial Braille displays. Improving the force and the durability is now in progress.
Third example is the application for micropipette and micropump. Recently, micropipettes and micropumps have been receiving a lot of attention for the microfluidic point-of-care (POC) diagnostic devices. So, we are willing to test the potential of BGAs as a micropipette. This project has been done by collaborations with Fraunhofer IPA (Stuttgart, Germany) . A BGA (black square film) was set into the printed circuit boards (PCBs) to apply voltages as shown in Figure 11. The pipette has a channel tip which has a size of 1 × 1 × 10 mm to suck and release liquid. The BGA showed an up-and-down motion in the PCBs like a diaphragm pump and can dispense
Ionic polymer actuator is a class of functional polymers that has great potential for application in soft robotics and micro-devices. In this chapter, two representative ionic polymer actuators are introduced: IPMC and BGA. Some fundamental characteristics and properties of the ionic polymer actuator have been clarified, and some recent applications in the micro pump, braille display and micropipette of IPMC and BGA as soft actuators have been presented.
This work is supported by the National Natural Science Foundation of China (NO.51505369 and 91748124), Jiangsu Key Laboratory of Special Robot Technology (NO. 2017B21114), and the Fundamental Research Funds for the Central Universities, P.R. China. The authors gratefully acknowledge the supports. The author T. S. thank to Sendai R&D center of Alps Electric Co. Ltd., Keio University (Prof. Nakano) and University of Tokyo (Prof. Someya) for their collaborations in the Braille project (the grant from Ministry of Health, Labor and Welfare of Japan in 2009 FY and 2010 FY).
The authors contributed equally to this work.
Tiwari R, Garcia E. The state of understanding of ionic polymer metal composite architecture: A review. Smart Materials and Structures. 2011; 20(8):083001
Jo C, Pugal D, Oh IK, et al. Recent advances in ionic polymer–metal composite actuators and their modeling and applications. Progress in Polymer Science. 2013; 38(7):1037-1066
Wang Y, Chen H, Liu J, et al. Aided manufacturing techniques and applications in optics and manipulation for ionic polymer-metal composites as soft sensors and actuators. Journal of Polymer Engineering. 2015; 35(7):611-626
Adolf D, Shahinpoor M, Segalman D, Witkowski W. Electrically Controlled Polymeric Gel Actuators, US Patent Number 5250167, October 1993
Oguro K, Takenaka H, Kawami Y. Actuator Element. US Patent Office, US patent no. 5268082, Issued December 7, 1993
Shahinpoor M. Continuum electromechanics of ionic polymeric gels as artificial muscles for robotic applications. Smart Materials and Structures. 1994; 3(3):367
Shahinpoor M. Micro-electro-mechanics of ionic polymeric gels as electrically controllable artificial muscles. Journal of Intelligent Material Systems and Structures. 1995; 6(3):307-314
Salehpoor K, Shahinpoor M, Mojarrad M. Linear and platform type robotic actuators made from ion-exchange membrane-metal composites. Proceedings of SPIE Smart Material Structure. 1997; 3040:192-198
Tadokoro S, Yamagami S, Takamori T, et al. Modeling of Nafion-Pt composite actuators (ICPF) by ionic motion[C]//smart structures and materials 2000: Electroactive polymer actuators and devices (EAPAD). International Society for Optics and Photonics. 2000; 3987:92-103
Shahinpoor M, Bar-Cohen Y, Simpson JO, et al. Ionic polymer-metal composites (IPMCs) as biomimetic sensors, actuators and artificial muscles-a review. Smart Materials and Structures. 1998; 7(6):R15
De Gennes PG, Okumura K, Shahinpoor M, et al. Mechanoelectric effects in ionic gels. EPL (Europhysics Letters). 2000; 50(4):513
Newbury KM, Leo DJ. Linear electromechanical model of ionic polymer transducers-part I: Model development. Journal of Intelligent Material Systems and Structures. 2003; 14(6):333-342
Newbury KM, Leo DJ. Linear electromechanical model of ionic polymer transducers-part II: Experimental validation. Journal of Intelligent Material Systems and Structures. 2003; 14(6):343-357
Nemat-Nasser S, Li JY. Electromechanical response of ionic polymer-metal composites. Journal of Applied Physics. 2000; 87(7):3321-3331
Zhu Z, Asaka K, Chang L, et al. Multiphysics of ionic polymer–metal composite actuator. Journal of Applied Physics. 2013; 114(8) 084902
Zhu Z, Wang Y, Liu Y, et al. Application-oriented simplification of actuation mechanism and physical model for ionic polymer-metal composites. Journal of Applied Physics. 2016; 120(3) 034901
Chang L, Chen H, Zhu Z, et al. Manufacturing process and electrode properties of palladium-electroded ionic polymer–metal composite. Smart Materials and Structures. 2012; 21(6) 065018
Chung CK, Fung PK, Hong YZ, et al. A novel fabrication of ionic polymer-metal composites (IPMC) actuator with silver nano-powders. Sensors and Actuators B: Chemical. 2006; 117(2):367-375
Wang Y, Liu J, Zhu Y, et al. Formation and characterization of dendritic interfacial electrodes inside an Ionomer. ACS Applied Materials & Interfaces. 2017; 9(36):30258-30262
Fukushima T, Asaka K, Kosaka A, et al. Fully plastic actuator through layer-by-layer casting with ionic-liquid-based Bucky gel. Angewandte Chemie International Edition. 2005; 44(16):2410-2413
Nemat-Nasser S, Wu Y. Comparative experimental study of ionic polymer–metal composites with different backbone ionomers and in various cation forms. Journal of Applied Physics. 2003; 93(9):5255-5267
Zhu Z, Chang L, Takagi K, et al. Water content criterion for relaxation deformation of Nafion based ionic polymer metal composites doped with alkali cations. Applied Physics Letters. 2014; 105(5) 054103
Wang Y, Chen H, Wang Y, et al. Effect of dehydration on the mechanical and physicochemical properties of gold-and palladium-ionomeric polymer-metal composite (IPMC) actuators. Electrochimica Acta. 2014; 129:450-458
Wang Y, Zhu Z, Liu J, et al. Effects of surface roughening of Nafion 117 on the mechanical and physicochemical properties of ionic polymer–metal composite (IPMC) actuators. Smart Materials and Structures. 2016; 25(8) 085012
Sugino T, Kiyohara K, Takeuchi I, Mukai K, Asaka K. Actuator properties of the complexes composed by carbon nanotube and ionic liquid: The effect of additives. Sensors and Actuators B. 2009; 141:179-186. DOI: 10.1016/j.snb.2009.06.002
Sugino T, Kiyohara K, Takeuchi I, Mukai K, Asaka K. Improving the actuating response of carbon anotube/ionic liquid composites by the addition of conductive nanoparticles. Carbon. 2011; 49:3560-3570. DOI: 10.1016/j.carbon.2011.04.056
Baughman RH, Cui C, Zakhidov AA, Iqbal Z, Barisci JN, Spinks GM, Wallace GG, Mazzordi A, Rossi DD, Rinzler AG, Jaschinski O, Roth S, Kertesz M. Carbon nanotube actuators. Science. 1999; 284:1340-1344. DOI: 10.1126/science.284.5418.1340
Chan CT, Kamitakahara WA, Ho KM. Charge-transfer effects in graphite intercalates: Ab initio calculations and neutron-diffraction experiment. Physical Review Letters. 1987; 58:1528-1531. DOI: 10.1103/PhysRevLett.58.1528
Hahn M, Barbieri O, Campana FP, Kötz R, Gallay R. Carbon based double layer capacitors with aprotic electrolyte solutions: The possible role of intercalation/insertion processes. Applied Physics A: Materials Science & Processing. 2006; 82:633-638. DOI: 10.1007/s00339-005-3403-1
Oren Y, Glatt I, Livnat A, Kafri O, Soffer A. The electrical double layer charge and associated dimensional changes of high surface area electrodes as detected by moire deflectometry. Journal of Electroanalytical Chemistry. 1985; 187:59-71. DOI: 10.1016/0368-1874(85)85575-1
Kiyohara K, Asaka K. Monte Carlo simulation of electrolytes in the constant voltage ensemble. The Journal of Chemical Physics. 2007; 126:214704-214714. DOI: 10.1063/1.2736371
Kiyohara K, Asaka K. Monte Carlo simulation of porous electrodes in the constant voltage ensemble. Journal of Physical Chemistry C. 2007; 111:15903-15909. DOI: 10.1021/jp0736589
Kiyohara K, Sugino T, Takeuchi I, Mukai K, Asaka K. Expansion and contraction of polymer electrodes under applied voltage. Journal of Applied Physics. 2009; 105:063506-1-8 [Erratum: J Appl Phys 2009;105:119902-1 ] DOI: 10.1063/1.3078031 [Erratum: DOI: 10.1063/1.3141728]
Hata K, Futaba DN, Mizuno K, Namai T, Yumura M, Iijima S. Water-assisted highly efficient synthesis of impurity-free single walled carbon nanotubes. Science. 2004; 306:1362-1364. DOI: 10.1126/science.1104962
Zoulias E, Varkaraki E, Lymberopoulos N, Christodoulou CN, Karagiorgis GN. A review on water electrolysis. TCJST. 2004; 4(2):41-71
Takeuchi I, Asaka K, Kiyohara K, Sugino T, Terasawa N, Mukai K, Fukushima T, Aida T. Electromechanical behavior of fully plastic actuators based on buckey gel containing various internal inonic liquids. Electrochimica Acta. 2009; 54:1762-1768. DOI: 10.1016/j.electacta.2008.10.007
Ohno H, editor. Ionic Liquid II: Marvelous Developments and Colorful Near Future. Japan: CMC; 2006. 299 p. ISBN: 4-88231-557-2
Takeuchi I, Asaka K, Kiyohara K, Sugino T, Terasawa N, Mukai K, Shiraishi S. Electromechanical behavior of a fully plastic actuator based on dispersed nano-carbon/ionic-liquid-gel electrodes. Carbon. 2009; 47:1373-1380. DOI: 10.1016/j.carbon.2009.01.029
Takeuchi I, Asaka K, Kiyohara K, Sugino T, Mukai K, Randriamahazaka H. Electrochemical impedance spectroscopy and electromechanical behavior of bucky-gel actuators containing ionic liquids. Journal of Physical Chemistry C. 2010; 114:14627-14634. DOI: 10.1021/jp1018185
Randriamahazaka H, Asaka K. Electrochemical analysis by means of complex capacitance of bucky-gel actuators based on single-walled carbon nanotubes and an ionic liquid. Journal of Physical Chemistry C. 2010; 114:17982-17988. DOI: 10.1021/jp106232s
Asaka K, Mukai K, Sugino T, Kiyohara K. Ionic electroactive polymer actuators based on nano-carbon electrodes. Polymer International. 2013; 62:1263-1270. DOI: 10.1002/pi.4562
Bar-Cohen Y, editor. Electroactive Polymer (EAP) Actuators as Artificial Muscles: Reality, Potential, and Challenges. 2nd ed. Washington: SPIE; 2004. 765 p. DOI: 10.1117/3.547465
Carpi F, Smela E, editors. Biomedical Applications of Electroactive Polymer Actuators. West Sussex: Wiley; 2009. 476 p. DOI: 10.1002/9780470744697
Takahashi I, Takatsuka T, Abe M. Application of nano-carbon actuator to braille display. In: Asaka K, Okuzaki H, editors. Soft Actuators: Materials, Modeling, Applications, and Future Perspectives. Springer Japan: Springer; 2014. pp. 371-384. DOI: 10.1007/978-4-431-54767-9.ch27
Addinall R. Sugino T, Neuhaus R, Kosidlo U, Tonner F, Glanz C, Kolaric I, Bauerhansl T, Asaka K. Integration of CNT-based actuators for bio-medical applications-example printed circuit board CNT actuator pipette. In: Proceedings of 2014 IEEE/ASME international conference on advanced intelligent mechatronics (AIM); 8-11 July 2014; Besacon. France: IEEE; 2014. p. 1436-1441
Goya K, Fuchiwaki Y, Tanaka M, Addinall R, Ooie T, Sugino T, Asaka K. A micropipette system based on low driving voltage carbon nanotube actuator. Microsystem Technologies. 2017; 23:2657-2661. DOI: 10.1007/s00542-016-2943-y