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Report No xxxx - Instytut Fizyki Jądrowej PAN

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PHASE TRANSITIONS AND REORIENTATIONAL MOTIONS OF THE<br />

COMPLEX CATIONS AND NH 3 LIGANDS IN POLYCRYSTALLINES<br />

[Co(NH 3 ) 6 ](ClO 4 ) 3 AND [Zn(NH 3 ) 4 ](BF 4 ) 2<br />

Natalia Górska a , Łukasz Hetmańczyk a , Edward Mikuli a , Anna Migdał-Mikuli a , Krystyna<br />

Hołderna-Natkaniec b , Weronika Kasperkowiak b<br />

a Jagiellonian University, Faculty of Chemistry, Department of Chemical Physics,<br />

30-060 Kraków, ul. Ingardena 3, Poland; b A. Mickiewicz University, Institute of Physics,<br />

61-606 Poznań, ul. Umultowska 85, Poland<br />

Hexaaminecobal(III) chlorate(VII) and tetraaminezinck(II) tetrafluoroborate<br />

compounds (chemical formula: [Co(NH 3 ) 6 ](ClO 4 ) 3 and ([Zn(NH 3 ) 4 ](BF 4 ) 2 ), respectively) are<br />

particularly interesting molecular materials because of different reorientational motions of the<br />

complex cation and NH 3 ligands. In [Co(NH 3 ) 6 ] 2+ cation the Co 3+ ion occupies the center of<br />

an octahedron, while in [Zn(NH 3 ) 4 ] 2+ the Zn 2+ ion occupies the center of a tetrahedron of the<br />

NH 3 ligands. The ClO - 4 and BF - 4 anions have a tetrahedral structure and also perform fast<br />

reorientational motions. Both substances undergo a several solid-solid phase transitions which<br />

are attributed to the changes in the molecular groups arrangements as well as in their<br />

reorientational dynamics. The DSC measurements [1,2] performed in the temperature range<br />

90-300 K detected the phase transitions which thermodynamic parameters are presented in<br />

Table. 1.<br />

Table. 1. Thermodynamics parameters of the phase transitions on heating<br />

Compound T C [K] ∆H [J·mol -1 ]<br />

-1<br />

∆S [J·mol<br />

-1·K<br />

[Co(NH 3 ) 6 ](ClO 4 ) 3 103.2 137 1.4<br />

[Zn(NH 3 ) 4 ](BF 4 ) 2 179.4<br />

120.6<br />

106.5<br />

1370<br />

930<br />

80<br />

7.6<br />

7.7<br />

0.7<br />

1<br />

The proton magnetic resonance H NMR measurements were performed on a labmade<br />

spectrometer operating in the double modulation system at 25 MHz [3]. Fig. 1a and 1b<br />

show the temperature dependencies of the slope line width (δH) and the second moment (M 2)<br />

of NMR line in the studied compounds. In order to propose a model of internal dynamics, the<br />

second moment value was calculated from the van Vleck formula [4]. The onset of the<br />

following reorientations was taken into account during the heating of these compounds: the<br />

reorientation of NH 3 ligands about the M-N axis and the reorientation of octahedral or<br />

tetr ahedral cation, respectively. It was assumed that the N-H bond distances were of 1.00 Å<br />

and all the N-H bonds were tetrahedraly directed with respect to the Zn-N bonds, or<br />

octahedrally directed with respect to the Co-N bonds, and the distance Zn-N and Co-N takes<br />

the value of 2.01 and 2.28 Å, respectively. The M Rigid 2 obtained the value of 47.3 and 43.8 G 2 ,<br />

for [Zn(NH 3 ) 4 ](BF 4 ) 2 and [Co(NH 3 ) 6 ](ClO 4 ) 3 , respectively. The observed value of the second<br />

moment of 1 H NMR line for [Zn(NH 3 ) 4 ](BF 4 ) 2 close to 15 G 2 at 90 K can be interpreted as<br />

resulting from the NH 3 ligands reorientation. On heating at T C1 also the reorientations of<br />

tetrahedral [Zn(NH 3 ) 4 ] 2+ cation set on. The observed value of the second moment of 1 H NMR<br />

line for [Co(NH 3 ) 6 ](ClO 4 ) 3 close to 17 G 2 at 90 K can be interpreted also as resulting from the<br />

NH 3 ligands reorientation. On heating the reorientations of octahedral [Co(NH 3 ) 6 ] 3+ cation set<br />

on, too.<br />

108

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