porous electrode
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2022 ◽  
Vol 609 ◽  
pp. 179-187
Author(s):  
Huiling Li ◽  
Lihua Cao ◽  
Huijun Zhang ◽  
Zhiwei Tian ◽  
Qian Zhang ◽  
...  

2022 ◽  
Vol 307 ◽  
pp. 118278
Author(s):  
Yang Yang ◽  
Jun Li ◽  
Yingrui Yang ◽  
Linghan Lan ◽  
Run Liu ◽  
...  

2022 ◽  
Author(s):  
Beatrise Berzina ◽  
Sungu Kim ◽  
Umesha Peramune ◽  
Kumar Saurabh ◽  
Baskar Ganapathysubramanian ◽  
...  

Ion concentration polarization (ICP) accomplishes preconcentration for bioanalysis by localized depletion of electrolyte ions, thereby generating a gradient in electric field strength that facilitates electrokinetic focusing of charged analytes by their electromigration against opposing fluid flow. Such ICP focusing has been shown to accomplish up to a million-fold enrichment of nucleic acids and proteins in single-stage preconcentrators. However, the rate at which the sample volume is swept is limited, requiring several hours to achieve these high enrichment factors. This limitation is caused by two factors. First, an ion depleted zone (IDZ) formed at a planar membrane or electrode may not extend across the full channel cross section under the flow rate employed for focusing, thereby allowing the analyte “leak” past the IDZ. Second, within the IDZ, large fluid vortices lead to mixing, which decreases the efficiency of analyte enrichment and worsens with increased channel dimensions. Here, we address these challenges with faradaic ICP (fICP) at a three-dimensional (3D) electrode comprising metallic microbeads. This 3D-electrode distributes the IDZ, and therefore, the electric field gradient utilized for counter-flow focusing across the full height of the fluidic channel, and its large area, microstructured surface supports smaller vortices. An additional bed of insulating microbeads restricts flow patterns and supplies a large area for surface conduction of ions through the IDZ. Finally, the resistance of this secondary bed enhances focusing by locally strengthening sequestering forces. This easy-to-build platform lays a foundation for the integration of enrichment with user-defined packed bed and electrode materials.


2022 ◽  
Author(s):  
Shouguang Yao ◽  
Jianguo Luo ◽  
Rui Liu ◽  
Xiaoyu Shen ◽  
Xinyu Huang

The desalting process of desalting battery includes ion transport in pores, diffusion in active particles and electrochemical reaction at the interface between solution and active particles. In this paper, quartet...


Lab on a Chip ◽  
2022 ◽  
Author(s):  
Beatrise Berzina ◽  
Sungu Kim ◽  
Umesha Peramune ◽  
Kumar Saurabh ◽  
Baskar Ganapathysubramanian ◽  
...  

Ion concentration polarization (ICP) accomplishes preconcentration for bioanalysis by localized depletion of electrolyte ions, thereby generating a gradient in electric field strength that facilitates electrokinetic focusing of charged analytes by...


Materials ◽  
2021 ◽  
Vol 15 (1) ◽  
pp. 278
Author(s):  
Bernardo F. Serôdio Costa ◽  
Blanca I. Arias-Serrano ◽  
Aleksey A. Yaremchenko

A series of strontium titanates-vanadates (STVN) with nominal cation composition Sr1-xTi1-y-zVyNizO3-δ (x = 0–0.04, y = 0.20–0.40 and z = 0.02–0.12) were prepared by a solid-state reaction route in 10% H2–N2 atmosphere and characterized under reducing conditions as potential fuel electrode materials for solid oxide fuel cells. Detailed phase evolution studies using XRD and SEM/EDS demonstrated that firing at temperatures as high as 1200 °C is required to eliminate undesirable secondary phases. Under such conditions, nickel tends to segregate as a metallic phase and is unlikely to incorporate into the perovskite lattice. Ceramic samples sintered at 1500 °C exhibited temperature-activated electrical conductivity that showed a weak p(O2) dependence and increased with vanadium content, reaching a maximum of ~17 S/cm at 1000 °C. STVN ceramics showed moderate thermal expansion coefficients (12.5–14.3 ppm/K at 25–1100 °C) compatible with that of yttria-stabilized zirconia (8YSZ). Porous STVN electrodes on 8YSZ solid electrolytes were fabricated at 1100 °C and studied using electrochemical impedance spectroscopy at 700–900 °C in an atmosphere of diluted humidified H2 under zero DC conditions. As-prepared STVN electrodes demonstrated comparatively poor electrochemical performance, which was attributed to insufficient intrinsic electrocatalytic activity and agglomeration of metallic nickel during the high-temperature synthetic procedure. Incorporation of an oxygen-ion-conducting Ce0.9Gd0.1O2-δ phase (20–30 wt.%) and nano-sized Ni as electrocatalyst (≥1 wt.%) into the porous electrode structure via infiltration resulted in a substantial improvement in electrochemical activity and reduction of electrode polarization resistance by 6–8 times at 900 °C and ≥ one order of magnitude at 800 °C.


Author(s):  
Brian T Heligman ◽  
Kevin P Scanlan ◽  
Arumugam Manthiram

Abstract Tin foils have an impressive lithium-storage capacity more than triple that of graphite anodes, and their adoption could facilitate a drastic improvement in battery energy density. However, implementation of a dense foil electrode architecture represents a significant departure from the standard blade-cast geometry with a distinct electrochemical environment, and this has led to confusion with regards to the first cycle efficiency of the system. In this work, we investigate the unique behavior of a tin active material in a foil architecture to understand its performance as an anode. We find shallow cycling of the foil results in an irreversible formation (< 40 %) due to diffusional trapping, but intermediate and complete utilization allows for a remarkably reversible formation reaction (> 90 %). This striking nonlinearity stems from an in-situ transformation from bulk metal to porous electrode that occurs during formation cycles and defines electrode-level lithium-transport on subsequent cycles. An alternative cycling procedure for assessing the stability of foils is proposed to account for this chemomechanical effect.


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