scholarly journals Low-Voltage-Driven Large-Amplitude Soft Actuators Based on Phase Transition

Soft Robotics ◽  
2020 ◽  
Vol 7 (6) ◽  
pp. 688-699 ◽  
Author(s):  
Ragesh Chellattoan ◽  
Arief Yudhanto ◽  
Gilles Lubineau
2018 ◽  
Vol 4 (2) ◽  
pp. 1800535 ◽  
Author(s):  
Chengtian Shen ◽  
Qiujie Zhao ◽  
Christopher M. Evans

Author(s):  
Yoshitaka Naka ◽  
Masaki Fuchiwaki ◽  
Kazuhiro Tanaka

Micro pumps with various driving systems have been developed and they have been carried out with experimental and numerical approaches so far. The authors propose a micro pump with soft actuators by conducting polymers as a driving source. The purpose of the present study is to develop the micro pump driven by conducting polymer soft actuator based on polypyrrole and to clarify the basic characteristics of the micro pump. Especially, we measure the flow rates, delivery heads and energy consumption of the micro pump driven by conducting polymer soft actuators and compare these results with those of the conventional micro pumps. The micro pump driven by a conducting polymer soft actuator can transport fluids in one direction without backflow by two soft actuators with opening and closing movement. Furthermore, wider ranges of flow rates are obtained with this micro pump and greater maximum delivery heads are obtained by them Moreover, the influence of the viscosity of the transport fluid was small and the micro pump driven by the conducting polymer soft actuator can transport fluid even with the viscosity that is 400 times as great as that of water in addition. The energy consumption rates of our micro pump are dramatically lower than those of the conventional micro pumps. This is because a conducting polymer soft actuator drives with a low voltage and a micro pump with low energy consumption is realized here.


2011 ◽  
Vol 1312 ◽  
Author(s):  
Ching-Mao Wu ◽  
Szu-Yin Lin ◽  
Kuo-Tung Huang

ABSTRACTThermo-responsive actuation (thermomechanical effects) based on nematic liquid crystal elastomers (LCEs) have become a research priority in the preparation of soft actuators. Nematic LCEs combine the anisotropic features of liquid crystal phases with the rubber elasticity of polymer network. When heated at nematic to isotropic phase transition temperature (N-to-I temp.), a uniaxial thermomechanical deformation of LCEs will undergo at nearly constant volume due to a change of LC director order. Recently, an array of the micro-sized LCE pillars related to such thermomechanical effects have been successfully constructed through a soft lithography technology (i.e., replica molding). The prepared LCE pillars are mono-dispersive and micro-sized. They also possess N-to-I temp. higher than 100°C, largely limiting the available application. By contrast, the present study will report a hexagonal array of nano-sized thermo-responsive pillar actuators that are able to contract and expand in response to temperature changes around a lower N-to-I temp. is manufactured via using reactive rod-like liquid crystal and ultraviolet nanoimprinting technology. According to atomic force microscope (AFM) observation, a hexagonal array of pillars can be easily constructed by nanoimprinting and a responsive surface with a thermo-stimuli-driven roughness change is achieved. The room-temperature AFM scans quantitatively represent the single pillar shows a diameter of ca. 270 nm and 140 nm in depth, and the pitch meaning the averaged inter-pillar distance is measured as ca. 425 nm, thus lying in a nano-sized range. Furthermore, temperature-variable AFM is also utilized to demonstrate the pillar behaves as a thermally-stimulated nano-sized actuator. In our case, when heated above N-to-I phase transition temperature (ca. 65°C), it is clearly observed that the pillar diameter is expanded in the order of over 12-15 % and then reversibly contracted in response to temperature drop.


1964 ◽  
Vol 207 (1) ◽  
pp. 260-264 ◽  
Author(s):  
Joseph J. Peters ◽  
Alphonse R. Vonderahe ◽  
John J. McDonough

As the body temperature of chicks between the day of hatching and the 3rd week after hatching was raised from normal to approximately 44.5 C, the eye was subjected to periodic photic stimulation while electrical recordings were taken from the eye and cerebral and optic lobes. As body temperature rose, the cerebrum showed an increased percentage of low-voltage fast waves mainly in the older birds, then sequences of slow waves of large amplitude, and finally a disappearance of spontaneous electrical activity, even though an electrocardiogram persisted for several minutes longer. During photic stimulation and hyperthermia, at the optic lobes the "flash-for-flash" response disappeared first, and then the "on" response, followed by a loss of the electroretinogram at the eye. Under the influence of hyperthermia, electrical activity of brain and eye persisted longest in the newly hatched chicks, and in them there appeared a slow spike and wave pattern probably associated with brain damage.


2015 ◽  
Vol 719-720 ◽  
pp. 630-634 ◽  
Author(s):  
Yan Chun Xu ◽  
Guo Xun Chen

It is difficult to detect and judge a weak electric shock signals in the leakage current accurate in the low-voltage power grid .A novel chaotic detection of the electric shock current and Lyapunov exponent is introduced in this paper .Electric shock current component is extracted according to the characteristics that chaotic system’s bifurcation action from chaotic state is sensitive to the weak signals and immune to noise .The largest Lyapunov exponent is proposed as the judgment criterion of phase transition of chaotic system. It can automatically recognize the critical state before and after electric shock.


2021 ◽  
pp. 2101121
Author(s):  
Francesco Visentin ◽  
Saravana Prashanth Murali Babu ◽  
Fabian Meder ◽  
Barbara Mazzolai

2019 ◽  
Vol 1 (8) ◽  
pp. 1970080 ◽  
Author(s):  
Jie Han ◽  
Weitao Jiang ◽  
Dong Niu ◽  
Yiding Li ◽  
Yajun Zhang ◽  
...  

1990 ◽  
Vol 45 (3-4) ◽  
pp. 343-348 ◽  
Author(s):  
Hiromitsu Terao ◽  
Tsutomu Okuda

Abstract The 81Br and 127I NQR spectra were recorded in CH3NH3 HgBr3 and CH3NH HgI3 , respectively. In addition to a phase transition at 338 K, successive phase transitions take place at 127 ± 1, 184±1 and 243±5 K in CH3NH3 HgBr3. On heating, the resonance lines of CH3NH3HgI3 disappear near a phase transition at 328 K and one line appears above this temperature. The temperature variations of the resonance frequencies of the terminal halogen atoms in both crystals are extraordinarily steep. This indicates the large amplitude molecular motions expected for the CH3NH3 cations which are linked to the terminal halogen atoms through N-H ··· X type H-bonding.


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