Layer-by-layer carbon nanotube bio-templates for in situ monitoring of the metabolic activity of nitrifying bacteria

2009 ◽  
Author(s):  
Kenneth J. Loh ◽  
Jeremy S. Guest ◽  
Genevieve Ho ◽  
Jerome P. Lynch ◽  
Nancy G. Love
2020 ◽  
Vol 54 (23) ◽  
pp. 3447-3456
Author(s):  
Dongouk Kim ◽  
Sang-Eui Lee ◽  
Yoonchul Sohn

Polymer composites with a high electrical conductivity ( σ) to thermal conductivity ( k) ratio have been intensively investigated in recent years. While highly conductive materials, such as metallic fillers or conducting polymers, were used to enhance σ, microstructural engineering was used to decrease k by forming porous structures, such as aerogels or 3D networks. These structures, however, were mechanically vulnerable and could only have limited applications. In this study, multiwalled carbon nanotube /silicone composites with a high σ/k ratio were developed by forming a double-segregated multiwalled carbon nanotube network in the porous body of the composites. The unique microstructure of the composites was created by a novel fabrication process: layer-by-layer deposition with in-situ polymerization of silicone emulsion particles dispersed in a water solvent. This novel process yielded very thick films, >200 µm, with high σ/k values, ∼2 × 104 (S/m)/(W/m·K). These high σ/k composites can be used for various applications, such as resistive heating elements, thermoelectric materials, and wearable thermotherapy.


2002 ◽  
Author(s):  
Yoshishige Tsuchiya ◽  
Masato Endoh ◽  
Masatoshi Kurosawa ◽  
Raymond T. Tung ◽  
Takeo Hattori ◽  
...  

RSC Advances ◽  
2021 ◽  
Vol 11 (12) ◽  
pp. 6655-6661
Author(s):  
Qiang Qiang Shi ◽  
Hang Zhan ◽  
Yu Zhang ◽  
Jian Nong Wang

A carbon nanotube-hollow carbon nanocage hybrid film is fabricated via a facile layer-by-layer strategy. The in situ addition of hollow carbon nanocages to the film is beneficial for preventing CNT stacking and thus promoting electrolyte transport.


Carbon ◽  
2003 ◽  
Vol 41 (3) ◽  
pp. 583-585 ◽  
Author(s):  
Do-Hyung Kim ◽  
Hoon-Sik Jang ◽  
Chang-Duk Kim ◽  
Dong-Soo Cho ◽  
Hee-Dong Kang ◽  
...  

1995 ◽  
Vol 401 ◽  
Author(s):  
Hitoshi Tabata ◽  
Masakazu Hamada ◽  
Tomoji Kawai

AbstractBismuth based artificial superlattices have been formed by a layer-by-layer laser deposition with in-situ monitoring of RHEED. The Bi2O2/WO6, Bi2O2/SrTa2O9, Bi2O2/SrTa2O9 /SrTiO3 and Bi2O2/SrTa2O9/BaTiO3 are constructed epitaxially by a single, double and triple perovskite layers sandwiched by Bi2O2 layers, respectively. The dielectric constant increases with increasing the number of perovskite layers. And the D-E hysteresis loop (ferroelectric properties) appears along the c-axis direction in odd perovskite layers (n=l and 3). We have also formed the SrTiO3/BiWO6/SrTiO3 multi layers. With this combination, the STO layers are isolated by the BWO layers. The dimensionality of STO layer can be controlled by changing the thickness of BWO layers. Below the BWO thickness of 500 Å, the εr increases monotonously with decreasing the BWO thickness. Therefore, the the coulomb force, which is in proportion to inverse of the distance, plays an essential role for the dielectric constant. The formation of “artificially constructed ferroelectric films” by a layer-by-layer deposition method will be discussed ad an essential approach to elucidate the mechanism of ferroelectricity.


Author(s):  
Hisayoshi Oshima ◽  
katsunori iwase ◽  
Yutaka Ohno

Abstract In floating catalyst chemical vapor deposition (FCCVD), when a carbon nanotube (CNT) network film is produced by filter collection, the film thickness is adjusted by controlling the collection time. However, even with consistent synthesis parameters, the synthesis condition in FCCVD changes constantly depending on the carbon and catalyst adhesion to the inner wall of the reaction tube. Thus, the rate of synthesis changes, making it difficult to obtain the target film thickness repeatedly and stably. We propose a method of monitoring CNT film thickness and percolation threshold by the in situ measurement of the electrical impedance during the deposition. The time evolution of the measured impedance is reproducible by an equivalent electrical circuit simulation.


Sign in / Sign up

Export Citation Format

Share Document