Thermal Emission of Alkali Metal Ions from Al 30 -Pillared Montmorillonite Studied by Mass Spectrometric Method
The thermal emission of alkali metal ions from Al -pillared montmorillonite in comparison with its natural form was studied by mass spectrometry in the temperature range 770-930 K. The measurements were carried out on a magnetic mass spectrometer MI-1201. For natural montmorillonite, the densities o...
Gespeichert in:
Veröffentlicht in: | Journal of analytical methods in chemistry 2017, Vol.2017, p.4984151-6 |
---|---|
Hauptverfasser: | , , , |
Format: | Artikel |
Sprache: | eng |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
Zusammenfassung: | The thermal emission of alkali metal ions from Al
-pillared montmorillonite in comparison with its natural form was studied by mass spectrometry in the temperature range 770-930 K. The measurements were carried out on a magnetic mass spectrometer MI-1201. For natural montmorillonite, the densities of the emission currents (
) decrease in the mass spectrum in the following sequence (T = 805 K, A/cm
): K
(4.55 · 10
), Cs
(9.72 · 10
), Rb
(1.13 · 10
), Na
(1.75 · 10
), Li
(3.37 · 10
). For Al
-pillared montmorillonite, thermionic emission undergoes temperature-time changes. In the low-temperature section of the investigated range (770-805 K), the value of
increases substantially for all ions in comparison with natural montmorillonite (T = 805 K, A/cm
): Cs
(6.47 · 10
), K
(9.44 · 10
), Na
(3.34 · 10
), Rb
(1.77 · 10
), and Li
(4.59 · 10
). A reversible anomaly is observed in the temperature range 805-832 K: with increasing temperature, the value of
of alkaline ions falls abruptly. This effect increases with increasing ionic radius of M
. After a long heating-up period, this anomaly disappears and the ln
- 1/
dependence acquires a classical linear form. The results are interpreted from the point of view of the dependence of the efficiency of thermionic emission on the phase transformations of pillars. |
---|---|
ISSN: | 2090-8865 2090-8873 |
DOI: | 10.1155/2017/4984151 |