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Dispersion of antimony doped tin oxide nanopowders for preparing transparent thermal insulation water-based coatings

Published online by Cambridge University Press:  13 June 2017

Hao Sun*
Affiliation:
School of Chemistry and Chemical Engineering, Guangxi University, Nanning 530004, People’s Republic of China; and Guangxi NaterTech Co., Ltd., Nanning 530007, People’s Republic of China
Bingshan Liu
Affiliation:
Guangxi NaterTech Co., Ltd., Nanning 530007, People’s Republic of China
Xu Liu
Affiliation:
School of Chemistry and Chemical Engineering, Guangxi University, Nanning 530004, People’s Republic of China
Zuodong Yin*
Affiliation:
School of Chemistry and Chemical Engineering, Guangxi University, Nanning 530004, People’s Republic of China
*
a) Address all correspondence to these authors. e-mail: s1024h@163.com

Abstract

Antimony doped tin oxide (ATO) is an ideal material for thermal insulation. To obtain the stable performance of ATO nanodispersions and measure the transparent and thermal insulation properties of the ATO coatings, we investigated how a dispersant and sand milling affect the stability of ATO dispersion, which has come to the results that adding an appropriate dispersant and sand milling for 2.0 h were beneficial to the ATO dispersion. We characterized the morphology, nanostructure, particle size distribution, zeta potential, and optical properties of the ATO dispersions by a transmission electron microscope (TEM), a laser particle size analyzer, and a spectrometer. The results show that the average particle size of the dispersions is about 50 nm and their absolute values of all zeta potentials are more than 40 mV. We coated the thermal insulation water-based coatings on quartz glasses by spin coating method, the effect of thermal insulation is evident with the increase of the ATO content, and there exists approximately 10 °C difference between the ATO sample and blank sample with the condition for maintaining high transmittance of visual light.

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Articles
Copyright
Copyright © Materials Research Society 2017 
Figure 0

FIG. 1. Zeta potential versus pH value of ATO dispersion.

Figure 1

TABLE I. The effect of different dispersants on ATO stability.

Figure 2

FIG. 2. (a) Effect of different dispersants on ATO average particle diameter by sand milling in deionized water with the same amount of dispersant (2%). (b) Effect of sand milling on ATO average particle diameter by sand milling in deionized water with the same amount of dispersant (5%).

Figure 3

TABLE II. The effect of the dispersant concentration on the ATO average particle diameter.

Figure 4

FIG. 3. (a) TEM images of the ATO dispersions by sand milling in deionized water with dispersant (PVP). (b) TEM images of the ATO dispersions by sand milling in deionized water with dispersant (PEG1000). (c) TEM images of the ATO dispersions by sand milling in deionized water with dispersant (TEA). (d) TEM images of the ATO dispersions by sand milling in deionized water with dispersant (NaOH).

Figure 5

FIG. 4. (a) Particle size distribution range of the ATO dispersions by sand milling in deionized water with dispersant (PVP). The inset images are test results of the zeta potential and ATO dispersions with 30 wt% content. (b) Particle size distribution range of the ATO dispersions by sand milling in deionized water with dispersant (PEG1000). The inset images are test results of the zeta potential and ATO dispersions with 30 wt% content. (c) Particle size distribution range of the ATO dispersions by sand milling in deionized water with dispersant (TEA). The inset images are test results of the zeta potential and ATO dispersions with 30 wt% content. (d) Particle size distribution range of the ATO dispersions by sand milling in deionized water with dispersant (NaOH). The inset images are test results of the zeta potential and ATO dispersions with 30 wt% content.

Figure 6

FIG. 5. Transmittance spectra of the ATO dispersion by sand milling in deionized water with dispersant (PVP). The inset images are test results of the reflectance of ATO dispersion.

Figure 7

FIG. 6. (a) The transmittance of ATO/PU thin films coated on the surface of quartz glasses (the center wavelength of UV is 365 nm; the wavelength of Vis is from 380 to 760 nm; the center wavelength of NIR is 1400 nm). (b) The transmittance of ATO/PA thin films coated on the surface of quartz glasses (the center wavelength of UV is 365 nm; the wavelength of Vis is from 380 to 760 nm; the center wavelength of NIR is 1400 nm).

Figure 8

FIG. 7. Schematic illustration of simulated experiment.

Figure 9

FIG. 8. (a) Temperature versus irradiation time of ATO/PU thin films. (b) Temperature versus irradiation time of ATO/PA thin films. (c) The images of the sample glasses of S0. (d) The images of the sample glasses of ATO/PU-S50. (e) The images of the sample glasses of ATO/PA-S50.