Controllable synthesis of ZnO with different morphologies and their morphology-dependent infrared emissivity in high temperature conditions

Nowadays, the high temperature low infrared emissivity problem has been of increasing significance and attracting more attention owing to the widespread applications for high temperature conditions. One key solution for this problem is to study the mechanism of high temperature low infrared emissivi...

Full description

Saved in:
Bibliographic Details
Published inJournal of alloys and compounds Vol. 804; pp. 503 - 510
Main Authors Guo, Tengchao, Xu, Guoyue, Tan, Shujuan, Yang, Zhihong, Bu, Honghan, Fang, Gang, Hou, Haili, Li, Jing, Pan, Lingyu
Format Journal Article
LanguageEnglish
Published Lausanne Elsevier B.V 05.10.2019
Elsevier BV
Subjects
Online AccessGet full text

Cover

Loading…
More Information
Summary:Nowadays, the high temperature low infrared emissivity problem has been of increasing significance and attracting more attention owing to the widespread applications for high temperature conditions. One key solution for this problem is to study the mechanism of high temperature low infrared emissivity and then design the materials with low infrared emissivity at elevated temperature. This paper gives an introduction to the infrared emissivity of ZnO powders in 3∼5 μm waveband at elevated temperature with various well-defined morphologies, e.g. needle-, pencil-, flower-, and flat-like. Among these morphologies, flat-like ZnO powders exhibit the lowest infrared emissivity because they have the largest real part of the dielectric function. Additionally, the variation of electrons average scattering time and lattice vibration at various temperature determine the variation tendency of infrared emissivity with temperature. [Display omitted] •ZnO powders with various morphologies are prepared by facile wet chemistry method.•Flat-like ZnO exhibits the lowest emissivity because of its highest real part of dielectric function.•The emissivity vs. temperature presents a U-shaped curve, and it reaches to the lowest value of 0.41 at 500 °C.•The decrease of emissivity with temperature is originated from the decrease of electrons scattering time.•The increase of emissivity with temperature higher than 500 °C is attributed to the strong lattice vibration absorption.
ISSN:0925-8388
1873-4669
DOI:10.1016/j.jallcom.2019.07.011