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Analysis of tiles produced from a schist material and their ultraviolet, near-infrared, mid-infrared, longwave-infrared and far-infrared spectra

Published online by Cambridge University Press:  16 March 2022

Hulya Kuru Mutlu*
Affiliation:
Eskisehir Osmangazi University, Vocational School of Health Services, Opticianry Program, 26040, Eskisehir, Turkey
Atakan Mutlu
Affiliation:
Hatipoglu Gunes Tile and Brick Industry, Inc., 43030, Kutahya, Turkey
*
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Abstract

Clays are used in the general production of earthen tiles. In this study, the production and characterization of earthen tiles from schist, a clayey rock formed by metamorphism of mudstone or shale, was investigated. The impact of tiles on atmospheric temperature through their absorption of the visible, near-infrared and far-infrared wavelength regions is evaluated. In particular, the absorption of ultraviolet and infrared radiation by the tiles was evaluated, as this could have beneficial applications for human health and the environment. UV-A radiation (320–400 nm) is not absorbed by the atmosphere, but schist materials absorb UV-A, which can contribute to melanoma formation (i.e. cancer). Field-emission scanning electron microscopy, X-ray fluorescence spectrometry and X-ray diffraction were used for the analysis of the schist materials. The tile-production stages of schist materials (drying, firing, water absorption rate, etc.) were tested at Hatipoglu Gunes Tile and Brick Industry, Inc. (Turkey). The tiles fired at 950°C and 1000°C comply with the industry standard compressive strength values for fired tiles (when converted to industry production conditions) and were 156.15 and 123.20 kg cm–2, respectively.

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Article
Copyright
Copyright © The Author(s), 2022. Published by Cambridge University Press on behalf of The Mineralogical Society of Great Britain and Ireland
Figure 0

Fig. 1. XRD trace of the Rızapasa schist. Ac = actinolite; Al = albite; Chl = chlorite; M = mica; Q = quartz; T = Al-rich titanite; V = Mg-vermiculite.

Figure 1

Table 1. Chemical composition of the Rızapasa schist determined using XRF spectroscopy.

Figure 2

Table 2. Particle-size distribution of the Rızapasa schist.

Figure 3

Fig. 2. FESEM images of the Rızapasa schist at (a) 150× magnification, (b) 500× magnification, (c) 30,000× magnification and (d) 100,000× magnification.

Figure 4

Fig. 3. Photographs of the schist samples after drying. (c) All samples were dried at 80°C.

Figure 5

Fig. 4. Photographs of the schist samples after firing at (a) 900°C, (b) 950°C and (c) 1000°C.

Figure 6

Table 3. Shrinkage values of the Rızapasa schist samples after drying and firing.

Figure 7

Table 4. Average shrinkage values of the Rızapasa schist samples after drying and firing.

Figure 8

Table 5. Temperature-dependent and converted industry compressive strength values of the Rızapasa schist samples (kg cm–2).

Figure 9

Fig. 5. Absorption of IR radiation by the schist in the UV wavelength region.

Figure 10

Fig. 6. Absorption of IR radiation by the schist in the NIR wavelength region.

Figure 11

Fig. 7. Absorption of IR radiation by the schist in the MWIR, LWIR and FIR wavelength regions.