Die Kristallstruktur (Pc, Z = 2) von NiH3IO6 · 6 H2O wurde mittels Röntgen‐Einkristallmessungen auf der Basis von 4169 symmetrieunabhängigen Reflexen bestimmt (R = 1,96%). IR‐ und Raman‐Spektren von NiH3IO6 · 6 H2O und der isotypen Verbindung MgH3IO6 · 6 H2O sowie von deuterierten Präparaten werden mitgeteilt. Die Spektren isotypenverdünnter Proben zeigen bis zu 14 OH(OD)‐Streckschwingungen entsprechend den 15 verschiedenen Wasserstoff‐Positionen der Struktur. Die meridionalen H3IO62−‐Ionen (Pseudosymmetrie C2v) besitzen wegen der T‐förmigen Anordnung der je 3 IO‐und IOH‐Gruppen nur je 2 IO‐, IO(H)‐ und OH‐Streckschwingungen in den IR‐ und Raman‐Spektren und können daher schwingungsspektroskopisch nicht von H3IO62−‐Ionen mit facialer Struktur (C3v) unterschieden werden.
The thermal decompositions of Ba(OH)2.8H20, Ba(OH)z.8D20, Ba(OH)2.H20 and Ba(OH)2. D20 were studied and the phase transitions were identified by DSC and DTA methods. The corresponding enthalpy changes were determined and compared with those calculated from the thermodynamic data. A decrease of the thermal stability was demonstrated for the deuterated crystal hydrates in comparison with the normal ones.The utilization of phase transitions in crystal hydrates as a kind of heat-energy storage explains the particular recent interest in this type of compounds. Specially, barium hydroxide and its crystal hydrates are of great interest both for the abovementioned purpose and for electronics applications.The thermal behaviour of Ba(OH) 2-8H20 has been studied by differential thermal analysis (DTA) [1][2][3][4][5], but the data obtained for the lower crystal hydrates and for the transition temperatures were contradictory. There are no corresponding data on Ba(OH)2-nD20.The object of the present work was to examine the thermal dissociations of Ba(OH)2.8H20 , Ba(OH)z. H20 , Ba(OH)2.8D20 and Ba(OH) z'D20 by two different methods, DTA and differential scanning calorimetry (DSC), in order to enrich the information available on the thermal behaviours of the above compounds and on the differences between normal and deuterated analogues, as well as to determine the enthalpy changes in the most important phase transitions.
Crystal data: 86(103)2 • 2HIO3 • 6H2O, A/, = 818.73, orthorhombic, Pnam. a = 7.842(1), b = 8.613(1), c = 24.407(2) Ä, F= 1648.5(5) Ä^ Z = 4, Z), = 3.299g-cmMo^a, A = 0.70930 Ä, /i = 75.7cm"', F(000) = 1496, r=292K, Ä = 0.030 for 3018 observed reHections with /> 3CT (7). The iodic acid and iodate groups are arranged in along the baxis cornigated slabs with the HIO3 molecules at the crests and troughs. The Channels between them are extended along the a-axis and filled with Be(H20)4^ cations and water molecules. All the structural fragments take part in a H-bonding scheme.
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