intermediate electrode
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Energies ◽  
2020 ◽  
Vol 13 (23) ◽  
pp. 6404
Author(s):  
Yongqing Wang ◽  
Bo An ◽  
Ke Wang ◽  
Yan Cao ◽  
Fan Gao

To identify critical parameters upon variable operational temperatures in a planar SOFC, an experimentally agreeable model was established. The significance of temperature effect on the performance of SOFC components was investigated, and the effect of activation energy during the development of intermediate electrode materials was evaluated. It is found the ionic conductivity of electrolytes is identified to be unavoidably concerned in the development of the intermediate-temperature SOFC. The drop of the ionic conductivity of the electrolyte decreases the overall current density 63% and 80% at temperatures reducing to 700 °C and 650 °C from 800 °C. However, there exists a critical value on the defined ratio between the electric resistance of the electrolyte in the overall internal resistance of SOFC, above which the further increase in the ionic conductivity would not significantly improve the performance. The lower the operational temperature, the higher critical ratio of the electrical resistance in the overall internal resistance of the cell. The minimal decrease in the activation energy during the development of intermediate electrode materials can significantly enhance the overall performance. Considering the development trend toward the intermediate temperature SOFC, advanced electrode material with the decreased activation energy should be primarily focused. The result provides a guidance reference for developing SOFC with the operational temperature toward the intermediate temperature.


Proceedings ◽  
2018 ◽  
Vol 2 (13) ◽  
pp. 928
Author(s):  
Yu Zhou ◽  
Cyrus Shafai ◽  
Lot Shafai ◽  
Greg Burley

Employing a tri-electrode topology for electrostatic actuators can significantly reduce needed control voltages. The tri-electrode topology employs a perforated intermediate electrode between the MEMS structure and pull-down electrode, and provides a low voltage control for the MEMS structure. Simulations of a spring supported MEMS in a conventional electrostatic actuator offering ~4.5 µm displacement with 20 V on the pull-down electrode, were compared to the tri-electrode actuator. This study showed that the intermediate electrode can act to provide similar controlled displacement with only 1/3 and 1/4 the voltage for the cases with the pull-down electrode held fixed at 20 V and 40 V respectively. A fabricated prototype experimentally showed that the intermediate electrode can provide similar displacement control with only 1/6 the normal control voltage of an electrostatic actuator.


2017 ◽  
Vol 157 ◽  
pp. 200-208 ◽  
Author(s):  
Bokkyu Choi ◽  
Dhruba Panthi ◽  
Masateru Nakoji ◽  
Toshiki Kabutomori ◽  
Kaduo Tsutsumi ◽  
...  

ACS Nano ◽  
2014 ◽  
Vol 8 (12) ◽  
pp. 12632-12640 ◽  
Author(s):  
Fei Guo ◽  
Peter Kubis ◽  
Ning Li ◽  
Thomas Przybilla ◽  
Gebhard Matt ◽  
...  

2014 ◽  
Vol 22 (S6) ◽  
pp. A1400 ◽  
Author(s):  
Xuanru Zhang ◽  
Qiuping Huang ◽  
Jigang Hu ◽  
Randy J. Knize ◽  
Yalin Lu

Author(s):  
Kento Masuyama ◽  
Steven R. H. Barrett

Partially ionized fluids can gain net momentum under an electric field, as charged particles undergo momentum-transfer collisions with neutral molecules in a phenomenon termed an ionic wind. Electrohydrodynamic (EHD) thrusters generate thrust by using two or more electrodes to ionize the ambient fluid and create an electric field. We characterize the performance of EHD thrusters of single- (SS) and dual-stage (DS) configurations. SS thrusters refer to a geometry using one emitter electrode, an air gap and a collector electrode with large radius of curvature relative to the emitter. DS thrusters add a collinear intermediate electrode. SS thruster performance was shown to be consistent with a one-dimensional theory. Increasing the gap length requires a higher voltage for thrust onset, generates less thrust per input voltage, generates more thrust per input current and most importantly generates more thrust per input power. A thrust-to-power ratio as high as approximately 100 N kW −1 was obtained. DS thrusters were shown to be more effective than their SS counterparts at producing current, leading to a smaller total voltage necessary for producing equal thrust. However, losses involving ion collection at the intermediate electrode led to reduced thrust-per-power compared with the SS thruster of equal length.


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