Effect of B2O3 on Structure and Properties of CaO–MgO–B2O3–Al2O3–SiO2 Glasses
xB 2 O 3 -(1 − x) (60SiO 2 –15Al 2 O 3 –15MgO–10CaO) glasses with various x around 5–30 mol% at the step of 5 mol% are prepared by the melting-quenching method at 1,450 °C for 3 h. The IR data indicate that replacing other components by B 2 O 3 levels up the amount of [BO 4 ] tetrahedron and boron-o...
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Veröffentlicht in: | Journal of inorganic and organometallic polymers and materials 2015-07, Vol.25 (4), p.816-822 |
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Hauptverfasser: | , , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
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Zusammenfassung: | xB
2
O
3
-(1 − x) (60SiO
2
–15Al
2
O
3
–15MgO–10CaO) glasses with various x around 5–30 mol% at the step of 5 mol% are prepared by the melting-quenching method at 1,450 °C for 3 h. The IR data indicate that replacing other components by B
2
O
3
levels up the amount of [BO
4
] tetrahedron and boron-oxygen rings, forcing [AlO
4
] tetrahedron to drop gradually. The glass transition temperature (T
g
), crystallization temperature (T
c
) and thermal stability (∆T) rise when B
2
O
3
is present in lower concentrations (≤20 mol%); accordingly the glass network enhances. However, further increase in concentration of B
2
O
3
(>20 mol%) reduces the T
g
, T
c
and ∆T. We utilize temperature-gradient furnace to measure the G6 glass, while the re-melt sample and crystallized phase are observed from polarizing microscope destroying microstructure. As B
2
O
3
content move up, falls in dielectric constant (ε
r
) and loss (tanδ) can be associated with drop of cations polarizability as well as concentration, along with glass network rigidity ascending. |
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ISSN: | 1574-1443 1574-1451 |
DOI: | 10.1007/s10904-015-0164-y |