Search engine for discovering works of Art, research articles, and books related to Art and Culture
ShareThis
Javascript must be enabled to continue!

The Influence of Sintering Time in High and Low Density Bi-2223 Superconductor

View through CrossRef
The effects of sintering time in high and low density Bi-2223 phase formation have been investigated. The samples were prepared by the solid-state reaction method at various sintering times ranging from 24, 48, 72 and 96 hours. Sucrose was added during palletization and after heated at 400°C for two hours the sucrose was removed and hence low density sample was created. The samples were characterized by X-ray diffraction (XRD), scanning electron microscopy (SEM) and critical current density. The transition temperature varies between 102 K and 96 K with increasing of sintering times. The optimal sintering time of the samples Bi-2223 system was found at 850°C for 72 hours. The critical current density, JC of high density and low density Bi-2223 was measured to be 7.547 A/cm2 and 8.333 A/cm2 respectively at 77 K under zero magnetic field. The critical current density, JC and superconductivity transition temperature, TC of low density were found to be higher than the pure samples. The critical transition temperature increased with a short gap between TConset and TC zero. The most intense peak in the XRD pattern of sample at sintering time 72 hours belong to the high-TC phase which also indicates an increase in the volume fraction of the high-TC phase with optimum sintering time.
Title: The Influence of Sintering Time in High and Low Density Bi-2223 Superconductor
Description:
The effects of sintering time in high and low density Bi-2223 phase formation have been investigated.
The samples were prepared by the solid-state reaction method at various sintering times ranging from 24, 48, 72 and 96 hours.
Sucrose was added during palletization and after heated at 400°C for two hours the sucrose was removed and hence low density sample was created.
The samples were characterized by X-ray diffraction (XRD), scanning electron microscopy (SEM) and critical current density.
The transition temperature varies between 102 K and 96 K with increasing of sintering times.
The optimal sintering time of the samples Bi-2223 system was found at 850°C for 72 hours.
The critical current density, JC of high density and low density Bi-2223 was measured to be 7.
547 A/cm2 and 8.
333 A/cm2 respectively at 77 K under zero magnetic field.
The critical current density, JC and superconductivity transition temperature, TC of low density were found to be higher than the pure samples.
The critical transition temperature increased with a short gap between TConset and TC zero.
The most intense peak in the XRD pattern of sample at sintering time 72 hours belong to the high-TC phase which also indicates an increase in the volume fraction of the high-TC phase with optimum sintering time.

Related Results

STRUCTURAL AND ELECTRICAL PROPERTIES OF HIGH AND LOW-DENSITY Yb-DOPED Bi(Pb)-2223 SUPERCONDUCTOR
STRUCTURAL AND ELECTRICAL PROPERTIES OF HIGH AND LOW-DENSITY Yb-DOPED Bi(Pb)-2223 SUPERCONDUCTOR
Ytterbium (Yb)-doped of Bi(Pb)-2223 with varying concentration was prepared by co-precipitation (COP) and solid state reaction (SSR) to produce high density and low density samples...
Effect of Eu Substitution in Low Density Bi (Pb)-2223 High Temperature Superconductors
Effect of Eu Substitution in Low Density Bi (Pb)-2223 High Temperature Superconductors
High temperature superconductor ceramic of low density Bi1.6Pb0.4Sr2(Ca2-xEux)Cu3Oy both doped and non-doped, have been produced by the method of conventional solid state reaction ...
Synthesis and Characterization of Low Density Bi-2223 Superconductors via Co-Precipitation Method
Synthesis and Characterization of Low Density Bi-2223 Superconductors via Co-Precipitation Method
High temperature Bi1.6Pb0.4Sr2Ca2Cu3Oδ of low density has been synthesized via co-precipitation method and its electrical and structural properties have been studied. The optimum p...
Fundamental Concepts and Methodology for the Analysis of Animal Population Dynamics, with Particular Reference to Univoltine Species
Fundamental Concepts and Methodology for the Analysis of Animal Population Dynamics, with Particular Reference to Univoltine Species
This paper presents some concepts and methodology essential for the analysis of population dynamics of univoltine species. Simple stochastic difference equations, comprised of endo...
Properties of Rare-Earth Substitution in Bi(Pb)-2223 Superconductor Prepared by Coprecipitation Method
Properties of Rare-Earth Substitution in Bi(Pb)-2223 Superconductor Prepared by Coprecipitation Method
The superconducting and structural properties of pure and rare-earth elements substituted in Bi (Pb)-2223 samples were investigated. All samples were fabricated by the oxalate copr...
Interplay of superconductivity and magnetism in the Fe1+yTe1‐xSex iron‐based superconductor: A theoretical study
Interplay of superconductivity and magnetism in the Fe1+yTe1‐xSex iron‐based superconductor: A theoretical study
AbstractThe competition between superconductivity and magnetism has been studied for the ongoing investigation of mechanisms in unconventional superconductors. Fe1+yTe1−xSex is dis...
The Effect of Sintering Conditions on the Microstructure and Electrical Properties of Pb(Zr0.52Ti0.48)O3 Ceramic
The Effect of Sintering Conditions on the Microstructure and Electrical Properties of Pb(Zr0.52Ti0.48)O3 Ceramic
Lead zirconatetitanate Pb(Zr0.52Ti0.48)O3, (PZT) from a mixture of commercial PbO, TiO2 and ZrO2 powders was successfully prepared using a planetary ball mill. The microstructure a...
Influence of Na, Mg and Yb Substitution for Ca in Bi(Pb)-2223 Superconductor
Influence of Na, Mg and Yb Substitution for Ca in Bi(Pb)-2223 Superconductor
The effect of Ca substitution by Na, Mg and Yb on the structural and transport properties of Bi1.6Pb0.4Sr2Ca2-xMxCu3Oy (M = Na, Mg and Yb) (x = 0.0 and 0.2) superconducting samples...

Back to Top