[
Zn(NH ) ][PtCl ] AND [Cd(NH ) ][PtCl ] AS PRECURSORS
501
3
4
6
3 4
6
–
1
4
00–4000 cm . Assignment was done with reference
T, °C
800
to work [4]. The assignment results are displayed in
Table 1.
2
4
2.5/48.12
7
00
00
Chlorine was determined routinely according to
Schoniger. Separate analyses of complexes and metal
solid solutions for the metals were carried out by
atomic absorption spectrometry (AAS) Zeeman back-
ground correction on a Hitachi Z 8000 spectrometer
with after solubilizing the solid phases with aqua regia.
Element interference was eliminated by buffering the
solutions with LaCl3.
6
~
70/48.12
500
00
300
~
62/48.12
3
4
6
4
4.0/48.12
4
1
47.8/48.12
2
1
00
00
0
For [Zn(NH ) ][PtCl ] anal. calcd., %: Cl, 39.30;
Zn, 12.08; Pt, 36.04.
5
3
4
6
4
8.9/48.12
Found, %: Cl, 39.1; Zn, 12.2; Pt, 36.1.
0
0.5
1.0
1.5
2.0
2.5
3.0
τ, h
For [Cd(NH ) ][PtCl ] anal. calcd., %: Cl, 36.16;
3
4
6
Cd, 19.11; Pt, 33.16.
Fig. 1. Thermolysis of [Zn(NH ) ][PtCl ] in hydrogen.
The weight of the residue (in percent of the starting weight)
as a function of heating schedule (obs./calcd.).
3
4
6
Found, %: Cl, 36.3; Cd, 19.3; Pt, 33.0.
Metal powders were prepared by reducing samples
of the complexes (~100 mg) in flowing hydrogen at var-
ious temperatures and hearing rates. Figure 1 displays
the weight of the residue (in percent of the starting
weight) as a function of heating schedule for
[
4]) in the spectra of the DCSs in question provides cir-
cumstantial evidence in favor of the individuality of the
compounds.
[
Zn(NH ) ][PtCl ].
3 4 6
Powder X-ray diffraction. We failed to grow DCS
crystals suitable for a single-crystal X-ray diffraction
experiment. We also failed to find compounds isostruc-
tural to our synthesized complexes in the JCPDS data-
base [6]. The X-ray diffraction pattern for a polycrys-
talline sample of the complex was indexed assuming a
monoclinic unit cell with the parameters a = 12.134(3)
Å, b = 7.813(2) Å, c = 7.787(2) Å, β= 119.4(2)°. The
positions and intensities of X-ray diffraction reflections
for this complex repeat from synthesis to synthesis.
Reflections other than pertaining to the chosen unit cell
were not found.
Thermoanalytical curves (Figs. 2, 3) were obtained
on a Q-1000 derivatograph modified to operate in dif-
ferent gas atmospheres.
Powder X-ray diffraction analysis of polycrystal-
line samples of the complex salts and their thermolysis
products was carried out on a DRON-Seifert RM4 dif-
fractometer (CuK radiation, graphite monochromator
α
on a diffracted beam, scintillation detector with ampli-
tude discrimination). Test samples were prepared by
spilling an ethanol suspension onto the polished side
of a fused silica cell. A polycrystalline silicon sample
a = 5.4309 Å) prepared in the same manner was used
as an external reference. The X-ray diffraction patterns
(
The X-ray diffraction pattern of the complex
were recorded in a discrete mode in the 2θ range from [Cd(NH ) ][PtCl ] differs strongly from that of the
3
4
6
5
° to 60° for the complex salts and from 5° to 135° for
thermolysis products.
complex [Zn(NH ) ][PtCl ] in both the positions and
3
4
6
intensities of the reflections. Broad, poorly resolved
reflections did not allow us to index the unit cell.
RESULTS AND DISCUSSION
Thermolysis in helium. The thermolysis of the
DCSs under a helium atmosphere involves three
stages. The weight loss at the first stage corresponds
to ~17 amu in both cases. Powder X-ray diffraction
shows that the intermediate produced at this stage is
amorphous. There are low-intensity reflections, which
are assigned to the (NH ) [PtCl ] phase. This stage is
accompanied by a noticeable exotherm in the DTA curve,
which is characteristic of ligand exchange between the
inner spheres of the complex ions in the DCS.
IR spectra. In the IR spectra of the DCSs, the
bands of the bending vibrations of coordinated ammo-
nia molecules shift toward higher wavenumbers com-
pared to simple salts of zinc and cadmium tetraam-
mines. The δ (NH ) bands are split in both compounds.
d
3
4
2
6
The δ (NH ) and δ (NH ) bands are split for the zinc
s
3
r
3
compound. We observed split and shifted modes of
coordinated ammonia molecules in DCSs in our previ-
ous work [5]; this was due to the distortion of the sym-
metry of complex ions in the crystal structure of DCSs.
The nonappearance of the vibrations intrinsic to the
ammonium ion and other complex cations
The second stage also produces a hygroscopic inter-
mediate, which contains metallic platinum and zinc or
cadmium chloride hydrates as shown by powder X-ray
2+
–1
(
[Cd(NH ) ] with the following wavenumbers (cm ): diffraction. Weight losses at this stage well match the sto-
3 6
δ (NH ), 1091; δ (NH ) 1585; ρ (NH ) 613; νMN, 298 ichiometry of the PtMCl residue, where M = Zn or Cd.
s
3
d
3
r
3
2
RUSSIAN JOURNAL OF INORGANIC CHEMISTRY Vol. 52 No. 4 2007