scholarly journals Effect of Layer Thickness and Temperature Difference on Oxygen Diffusion Behavior in Thin Solution Layer Formed on Metal

2021 ◽  
Vol 107 (12) ◽  
pp. 1029-1035
Author(s):  
Masatoshi Sakairi ◽  
Masaya Taniguchi
2009 ◽  
Vol 421-422 ◽  
pp. 197-200 ◽  
Author(s):  
Tsubasa Nakagawa ◽  
Isao Sakaguchi ◽  
Kenji Matsumoto ◽  
Masashi Uematsu ◽  
Hajime Haneda ◽  
...  

Diffusion behaviors of aluminum (Al) in zinc-oxide (ZnO) single crystals were measured by means of ion implantation technique and SIMS depth profiling. It was found that Al concentration profile had a peculiar shape with a constant-concentration region and a steep tail, which was also found in profiles of other donors such as Ga and In. Detailed analysis of the profiles revealed that the diffusivity of Al was proportional to the square of Al concentration and its intrinsic diffusivity was much smaller than previously reported values. Oxygen diffusion experiments were also performed and the implantation of Al ions enhanced the oxygen diffusion coefficients by about 20 times. This result indicates that oxygen interstitial diffusion occurs in n-type ZnO.


2016 ◽  
Vol 176 ◽  
pp. 253-256 ◽  
Author(s):  
Guoling Li ◽  
Li Li ◽  
Jialong Hao ◽  
Jie Zheng ◽  
Wenhuai Tian ◽  
...  

1980 ◽  
Vol 51 (1) ◽  
pp. 392-396
Author(s):  
Nobuyuki Toyoda ◽  
Minoru Mihara ◽  
Tohru Hara

1984 ◽  
Vol 56 (12) ◽  
pp. 2263-2265 ◽  
Author(s):  
Marc D. Porter ◽  
Shaojung. Dong ◽  
Yupeng. Gui ◽  
Theodore. Kuwana

1988 ◽  
Vol 196 ◽  
pp. 135-156 ◽  
Author(s):  
J. Tanny ◽  
A. B. Tsinober

The dynamics and structure of double-diffusive layers were studied experimentally by heating a linear stable solute gradient from a sidewall in a wide tank. The formation and subsequent development of the layers were investigated by various flow-visualization techniques, namely fluorescent dye, fluorescent particles and shadowgraph. Experiments were performed in order to determine the stability diagram of the flow, following in each experiment the phase trajectory of the system in the phase plane of thermal and solute Rayleigh numbers. The experimentally obtained stability diagram appears to be similar to that obtained numerically by Thangam et al. (1981) and by Hart (1971) for a vertical narrow slot and a steady basic flow. It is shown that if the temperature of the sidewall rises slowly to its prescribed value, the thickness of the initial layers, formed at the onset of instability, is a function of the ambient density gradient and fluid properties only. On the other hand, if the wall temperature rises quickly (almost impulsive heating), the thickness of the initial layers is proportional to the imposed temperature difference, provided that the Rayleigh number, based on this difference, is larger than some critical value which is associated with the first merging of the layers. A criterion for the first merging of the initial layers is obtained, and it is suggested that this merging is due to subsequent instability of the system. The subsequent merging process, following the first merging, is not a simple successive doubling of the layer thickness and in each of five nearly identical experiments a different dependence of the average layer thickness on the instantaneous Rayleigh number is obtained. This indicates that the system of layers behaves chaotically after the first merging. The final thickness of the layers depends on the prescribed lateral temperature difference, and the ratio between the final and the initial thickness of the layers is a linear function of the final Rayleigh number. Flow-visualization experiments indicate that the layers consist of vortices with vertical scale of the layer thickness and various horizontal scales.


2012 ◽  
Vol 4 (3) ◽  
pp. 665-674 ◽  
Author(s):  
M. M. Alam ◽  
M. Z. Bin Mukhlish ◽  
S. Uddin ◽  
S. Das ◽  
K. Ferdous ◽  
...  

Titanium dioxide (TiO2) has been used as photo-catalyst for the degradation of reactive yellow (RY) in batch and continuous mode under UV irradiation. Titanium dioxide (TiO2) was immobilized onto the ceramic plate using cement as binder. The effects of various parameters such as initial dye concentration, solution layer thickness, presence of catalyst, residence time, and catalyst loading on degradation have been investigated. The results showed that without catalyst no degradation was achieved. The maximum sorption capacity of TiO2 was found to be 0.01447 kg/kg. The degradation of RY followed pseudo-first order kinetics with rate constant k = 0.001 min-1. A decrease in degradation of RY was observed with an increase in initial concentration and solution layer thickness. A comparison of photocatalytic performance between batch and continuous mode was performed and the batch mode provided better degradation performance. About 60% degradation of dye was achieved at 360 min for 200 ppm RY solution in batch mode.© 2012 JSR Publications. ISSN: 2070-0237 (Print); 2070-0245 (Online). All rights reserved.doi: http://dx.doi.org/10.3329/jsr.v4i3.8654 J. Sci. Res. 4 (3), 665-674 (2012)


2006 ◽  
Vol 301 ◽  
pp. 257-260
Author(s):  
Naoki Wakiya ◽  
Akinori Higuchi ◽  
Haruki Ryoken ◽  
Hajime Haneda ◽  
Keiichi Fukunaga ◽  
...  

Diffusion behavior at the interface of (001)-epitaxially grown (Ba,Sr)TiO3(BST)/electrode/buffer layer/Si thin films was examined by use of secondary ion-microprobe mass spectrometer (SIMS) and transmission electron microscope (TEM) attached with energy dispersive X-ray fluorescence spectrometer (EDX). As the (001)-epitaxially grown film, following three kinds of structure was grown; (1)BST/(La,Sr)CoO3(LSCO)/CeO2/yttria-stabilized zirconia(YSZ)/Si, (2)BST/PLD-deposited Pt/SrTiO3(ST)/LSCO/CeO2/YSZ/Si and (3)BST/sputter-deposited Pt/ST/LSCO/CeO2/YSZ/Si. For sample (1), uphill diffusion of Sr and Ti was observed at the interface of YSZ and SiO2. Diffusion of Co into CeO2 layer was also detected. These tendencies of diffusion were also observed for samples (2) and (3). In addition to these tendencies, apparent uphill diffusion of Co at the Pt layer was observed for sample (2). However, this diffusion was not observed for sample (3). It was also observed that oxygen diffusion was prevented for sputter-deposited Pt. On the other hand, oxygen diffusion was observed for PLD-deposited Pt.


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