Optical Properties of Soda-Lime-Silica Glasses Doped with Eggshell Powder

• Authors: B. Aktas , M. Albaskara , S. Yalcin , K. Dogru
• Languages of publication: EN

Abstracts

EN

The optical properties of soda-lime-silica glasses doped with eggshell powder were investigated using UV-visible and the Fourier transform infrared spectroscopies. Pure soda-lime-silica glass, which is colorless and transparent, turned dark green after the addition of the eggshell powder. When the eggshell powder content was ≥ 3 wt%, the glass became translucent. The maximum wavelengths in the UV spectra of the soda-lime-silica glasses doped with 0.5, 1, 3, and 5 wt% eggshell powder were observed at 300.20, 277.40, 284.40, and 312.40 nm, respectively. The Fourier transform infrared spectra of the eggshell-doped soda-lime-silica glass samples were very similar to that of the base undoped glass. The bands at approximately 770-820 cm¯¹ could be attributed to the Si-O-Si symmetric stretching of the bridging oxygen between the tetrahedra, while the bands at approximately 970 cm¯¹ were related to the Si-O-Si antisymmetric stretching of the bridging oxygen within the tetrahedra.

Keywords

EN

soda-lime-silica glass; eggshell powder; optical properties; FTIR spectra

• Publisher: Institute of Physics, Polish Academy of Sciences
• Journal: Acta Physica Polonica A
• Year: 2017
• Volume: 132
• Issue: 3
• Pages: 442-444

Dates

published

2017-09

Contributors

author

B. Aktas

• Harran University, Mechanical Engineering Department, Sanliurfa, Turkey

author

M. Albaskara

• Harran University, Mechanical Engineering Department, Sanliurfa, Turkey

author

S. Yalcin

• Harran University, Physics Department, Sanliurfa, Turkey

author

K. Dogru

• Harran University, Institute of Natural and Applied Sciences, Sanliurfa, Turkey

References

• [1] R.H. Doremus, Glass Science, Wiley, New York 1973, p. 319
• [2] H. Rawson, Properties and Applications of Glasses, Elsevier, Amsterdam 1980, p. 156
• [3] B. Aktas, M. Albaskara, S. Yalcin, K. Dogru, Archiv. Mater. Sci. Eng. 82, 57 (2016)
• [4] B. Kiris, O. Bingol, R. Senol, A. Altintas, Acta. Phys. Pol. A 130, 55 (2016), doi: 10.12693/APhysPolA.130.55
• [5] M. Ustundag, B.G. Yalcin, M. Aslan, S. Bagci, Acta. Phys. Pol. A 130, 98 (2016), doi: 10.12693/APhysPolA.130.98
• [6] I.A. Kariper, O. Baglayan, F. Gode, Acta. Phys. Pol. A 128, B-219 (2015), doi: 10.12693/APhysPolA.128.B-219
• [7] A.A. Barzinjy, M.M. Zankana, Acta. Phys. Pol. A 130, 239 (2016), doi: 10.12693/APhysPolA.130.239
• [8] H. Lin, E.Y.B. Pun, X.R. Liu, J. Non-Cryst. Solids 283, 27 (2001), doi: 10.1016/S0022-3093(01)00488-4
• [9] S.A. Boussaa, A. Kheloufi, N.B. Zaourar, F. Kerkar, Acta. Phys. Pol. A 130, 133 (2016), doi: 10.12693/APhysPolA.130.133
• [10] M.A. Ouis, H.A. El Batal, M.A. Azooz, A.M. Abdelghany, Indian J. Pure Appl. Phys. 51, 11 (2013)
• [11] M.M. Ibrahim, M.A. Fanny, M.Y. Hassaan, H.A. ElBatal, Silicon 8, 443 (2016), doi: 10.1007/s12633-015-9362-z
• [12] Y.K. Lee, Y.L. Peng, M. Tomozawa, J. Non-Cryst. Solids 222, 125 (1997), doi: 10.1016/S0022-3093(97)90104-6

Identifiers

DOI

10.12693/APhysPolA.132.442