supplementary materials


Acta Cryst. (2007). E63, i153-i154    [ doi:10.1107/S1600536807027705 ]

K2(SO4)0.63(SeO4)0.37·Te(OH)6

M. Abdelhedi, L. Ktari, M. Dammak, A. Cousson and A. Kolsi

Abstract top

The title compound, dipotassium sulfate selenate/telluric acid adduct, K2(SO4)0.63(SeO4)0.47·Te(OH)6, is a solid solution in the series K2SO4·Te(OH)6/K2SeO4·Te(OH)6. It crystallizes in the same structure as the end member K2SO4·Te(OH)6 in the space group P\overline{1}, whereas the other end-member K2SeO4·Te(OH)6 crystallizes in the space group C2/c. The structure of the solid solution consists of planes of Te(OH)6 octahedra alternating with planes of statistically occupied XO4 tetrahedra (X = S and Se), and with K+ cations situated between the planes. The structure is stabilized by interplanar O-H...O hydrogen bonds involving all the H atoms that belong to the OH groups of the Te(OH)6 octahedra. Both Te atoms lie on inversion centres.

Comment top

Fig. 1 shows a projection of the title structure (I) on the ab plane. The structure consists of planes of Te(OH)6 octahedra alternating with planes of statistically occupied XO4 tetrahedra (X = S, Se). The Te(OH)6 layers extend parallel to the ac plane at y = 0, whereas the parallel XO4 layers are at y 0.5. The K+ cations are situated between the layers.

The two independent Te atoms in (I) occupy inversion centres (Fig. 2), with very similar Te—O distances between 1.900 (6) and 1.921 (6) Å and O—Te—O angles between 88.8 (3) and 91.20 (3)°. In the isostructural end-member K2SO4·Te(OH)6 (KSTe) (Zilber et al., 1980), the Te—O distances are nearly the same and vary from 1.914 (5) to 1.938 (5) Å, whilst in K2SeO4·Te(OH)6 (KSeTe) they are between 1.913 (2) and 1.919 (2) Å (Dammak et al., 2005).

The X—O distances of the slightly distorted XO4 tetrahedra vary from 1.460 (7) to 1.508 (6) Å, with O—X—O angles between 108.3 (4) and 111.0 (4)°. In the KSTe structure, the S—O distances range from 1.453 (5) to 1.503 (5) Å and in the KSeTe homologue, the Se—O distances vary from 1.627 (7) to 1.659 (7) Å.

The two K+ cations are both in eightfold coordination with distances ranging between 2.709 (6) and 3.267 (8) Å. K1+ is coordinated by three O atoms belonging to two XO4 tetrahedra, by one O atom of a Te1O6 octahedron, and by four O atoms of three Te2O6 octahedra. The environment of K2+ consists of three O atoms belonging to three XO4 tetrahedra, of one O atom from a Te2O6 octahedron, and of four O atoms from three Te1O6 octahedra.

Interplanar O—H···O hydrogen bonding between the Te(OH)6 octahedra and the XO4 tetrahedra helps to consolidate the structural set-up. In consequence, all H atoms of the hydroxyl groups participate in the formation of hydrogen bonding. In the XO4 group, two oxygen atoms are acceptors of one H atom, whereas the other O atoms are acceptors of two H atoms. The O···O distances vary from 2.654 (9) to 2.780 (9) Å and the O—H···O angles range from 164.3 (4) and 175.6 (5)° (Table 1, Fig. 3).

Related literature top

For the structures of the end-members of this solid solution series, see K2SO4·Te(OH)6 (Zilber et al., 1980) and K2SeO4·Te(OH)6 (Dammak et al., 2005).

Experimental top

Transparent, colorless single crystals of compound (I) were grown at room temperature by slow evaporation of an aqueous solution consisting of a mixture of Te(OH)6 (Aldrich, 99%), K2SeO4 (Aldrich, 99.99%) and K2SO4 (Aldrich, 99%) in the stoichiometric ratio 1:0.5:0.5.

Refinement top

Hydrogen atoms on Te(OH)6 groups were located in a difference map and were refined with restrained distances between 0.81 (1) and 0.86 (1) Å and a common Uiso parameter. For the refinement of the occupation factors for S and Se, their sum was constrained to be equal to 1. The highest peak and the deepest hole in the final Fourier map are located 0.04 and 0.57 Å, respectively, from the X site (X = S, Se).

Computing details top

Data collection: COLLECT (Nonius, 2001); cell refinement: DENZO/SCALEPACK; data reduction: DENZO/SCALEPACK (Otwinowski & Minor, 1997); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: CRYSTALS (Betteridge et al., 2003); molecular graphics: DIAMOND (Brandenburg & Berndt, 1999); software used to prepare material for publication: CRYSTALS.

Figures top
[Figure 1] Fig. 1. Projection of the K2(SO4)0.63(SeO4)0.37·Te(OH)6 crystal structure on the ab plane.
[Figure 2] Fig. 2. The asymmetric unit of K2(SO4)0.63(SeO4)0.37·Te(OH)6 (expanded by symmetry to give complete Te(OH)6 octahedra) with displacement ellipsoids drawn at the 50% probability level. [Symmetry codes:(a) −x, −y, −z; (b) −x + 1, −y, −z + 1].
[Figure 3] Fig. 3. The hydrogen bonding (dotted lines) in the crystal structure of K2(SO4)0.63(SeO4)0.37·Te(OH)6.
Dipotassium sulfate/selenate tellurate top
Crystal data top
K2(SO4)0.63(SeO4)0.37Te(OH)6Z = 2
Mr = 421.16F000 = 397.250
Triclinic, P1Dx = 2.961 Mg m3
Hall symbol: -P 1Mo Kα radiation
λ = 0.71073 Å
a = 6.2463 (2) ÅCell parameters from 7138 reflections
b = 6.6470 (2) Åθ = 2.7–30.1º
c = 13.1326 (4) ŵ = 5.63 mm1
α = 102.138 (2)ºT = 298 K
β = 90.073 (2)ºPrism, colourless
γ = 116.943 (1)º0.15 × 0.14 × 0.10 mm
V = 472.28 (3) Å3
Data collection top
Nonius KappaCCD
diffractometer
1719 reflections with I > 3σ(I)
Monochromator: graphiteRint = 0.038
T = 298 Kθmax = 30.2º
φ rotation scans with 2° widthθmin = 1.6º
Absorption correction: multi-scan
(MULABS in PLATON; Spek, 2003)
h = 8→8
Tmin = 0.447, Tmax = 0.569k = 9→9
69116 measured reflectionsl = 18→18
2787 independent reflections
Refinement top
Refinement on FPrimary atom site location: structure-invariant direct methods
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.045All H-atom parameters refined
wR(F2) = 0.051  Method, part 1, Chebychev polynomial, [Watkin (1994). Acta Cryst. A50, 411–437; Prince, (1982). Mathematical Techniques in Crystallography and Materials Science. Springer-Verlag: New York.] [weight] = 1.0/[A0*T0(x) + A1*T1(x) ··· + An-1]*Tn-1(x)]
where Ai are the Chebychev coefficients listed below and x = F /Fmax Method = Robust Weighting (Prince, 1982) W = [weight] * [1-(deltaF/6*sigmaF)2]2 Ai are: 4.11 -3.38 2.64
S = 1.09(Δ/σ)max = 0.002
1719 reflectionsΔρmax = 2.40 e Å3
114 parametersΔρmin = 2.99 e Å3
7 restraintsExtinction correction: None
Crystal data top
K2(SO4)0.63(SeO4)0.37Te(OH)6γ = 116.943 (1)º
Mr = 421.16V = 472.28 (3) Å3
Triclinic, P1Z = 2
a = 6.2463 (2) ÅMo Kα
b = 6.6470 (2) ŵ = 5.63 mm1
c = 13.1326 (4) ÅT = 298 K
α = 102.138 (2)º0.15 × 0.14 × 0.10 mm
β = 90.073 (2)º
Data collection top
Nonius KappaCCD
diffractometer
2787 independent reflections
Absorption correction: multi-scan
(MULABS in PLATON; Spek, 2003)
1719 reflections with I > 3σ(I)
Tmin = 0.447, Tmax = 0.569Rint = 0.038
69116 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0457 restraints
wR(F2) = 0.051All H-atom parameters refined
S = 1.09Δρmax = 2.40 e Å3
1719 reflectionsΔρmin = 2.99 e Å3
114 parameters
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
Te10.00000.00000.00000.0150
Te20.50000.00000.50000.0144
Se10.24991 (17)0.46625 (17)0.24814 (17)0.04390.368 (7)
S10.24991 (17)0.46625 (17)0.24814 (17)0.04390.632 (7)
K10.1921 (4)0.2576 (3)0.35079 (18)0.0274
K20.4207 (4)0.2342 (3)0.14873 (17)0.0254
O10.0604 (11)0.0373 (10)0.1399 (5)0.0232
O20.1770 (12)0.1704 (11)0.0061 (5)0.0251
O30.2905 (11)0.2817 (10)0.0548 (6)0.0269
O40.7680 (10)0.0037 (10)0.4321 (5)0.0250
O50.6055 (11)0.3137 (9)0.4891 (5)0.0215
O60.3083 (10)0.1107 (10)0.3668 (5)0.0233
O70.1044 (11)0.4714 (11)0.3412 (5)0.0260
O80.3641 (13)0.6150 (12)0.2807 (6)0.0281
O90.0842 (12)0.5509 (12)0.1687 (6)0.0312
O100.4411 (12)0.2270 (10)0.2057 (6)0.0301
H10.06930.16710.14520.0436*
H20.14190.27460.05890.0436*
H30.36570.24910.09370.0436*
H40.72290.13430.38960.0436*
H50.69850.33950.44040.0436*
H60.18750.23150.37020.0436*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Te10.01489 (9)0.01533 (9)0.01406 (9)0.00653 (9)0.00131 (9)0.00335 (9)
Te20.01472 (9)0.01349 (9)0.01512 (9)0.00649 (9)0.00155 (9)0.00350 (9)
Se10.03752 (17)0.04897 (17)0.03836 (17)0.01470 (17)0.00249 (17)0.00931 (17)
S10.03752 (17)0.04897 (17)0.03836 (17)0.01470 (17)0.00249 (17)0.00931 (17)
K10.0242 (8)0.0260 (8)0.0370 (11)0.0156 (7)0.0043 (7)0.0079 (7)
K20.0244 (8)0.0227 (8)0.0346 (10)0.0146 (7)0.0013 (7)0.0093 (7)
O10.033 (3)0.025 (3)0.016 (3)0.015 (2)0.007 (2)0.009 (2)
O20.031 (3)0.028 (3)0.024 (3)0.022 (3)0.000 (2)0.003 (2)
O30.025 (3)0.016 (2)0.035 (4)0.004 (2)0.007 (2)0.008 (2)
O40.019 (3)0.020 (3)0.032 (3)0.008 (2)0.008 (2)0.001 (2)
O50.026 (3)0.013 (2)0.026 (3)0.009 (2)0.006 (2)0.006 (2)
O60.024 (3)0.019 (3)0.020 (3)0.004 (2)0.004 (2)0.006 (2)
O70.023 (3)0.031 (3)0.028 (3)0.011 (2)0.000 (2)0.017 (3)
O80.036 (4)0.032 (3)0.029 (4)0.029 (3)0.006 (3)0.001 (3)
O90.032 (3)0.030 (3)0.033 (4)0.013 (3)0.006 (3)0.012 (3)
O100.031 (3)0.016 (3)0.038 (4)0.007 (2)0.005 (3)0.005 (2)
Geometric parameters (Å, °) top
Te1—O1i1.920 (6)O4—H40.848
Te1—O3i1.915 (6)O5—H50.856
Te1—O2i1.900 (6)O6—H60.826
Te1—O11.920 (6)K1—O4iii2.792 (6)
Te1—O21.900 (6)K1—O72.815 (6)
Te1—O31.915 (6)K1—O5iv2.889 (6)
Te2—O6ii1.921 (6)K1—O62.897 (6)
Te2—O5ii1.919 (5)K1—O12.984 (7)
Te2—O4ii1.905 (6)K1—O52.990 (6)
Te2—O41.905 (6)K1—O8v3.022 (8)
Te2—O51.919 (5)K1—O10v3.032 (8)
Te2—O61.921 (6)K2—O10v2.709 (6)
X1—O71.508 (6)K2—O2i2.751 (6)
X1—O81.460 (7)K2—O8vi2.786 (8)
X1—O91.482 (7)K2—O9vii2.852 (7)
X1—O101.473 (6)K2—O1v2.908 (7)
O1—H10.857K2—O3vii2.915 (6)
O2—H20.817K2—O62.984 (7)
O3—H30.817K2—O3viii3.267 (8)
O1i—Te1—O3i89.9 (3)O6ii—Te2—O590.4 (3)
O1i—Te1—O2i91.2 (3)O5ii—Te2—O5179.994
O3i—Te1—O2i90.4 (3)O4ii—Te2—O590.0 (3)
O1i—Te1—O1179.994O4—Te2—O590.0 (3)
O3i—Te1—O190.1 (3)O6ii—Te2—O6179.994
O2i—Te1—O188.8 (3)O5ii—Te2—O690.4 (3)
O1i—Te1—O288.8 (3)O4ii—Te2—O689.6 (3)
O3i—Te1—O289.6 (3)O4—Te2—O690.4 (3)
O2i—Te1—O2179.994O5—Te2—O689.6 (3)
O1—Te1—O291.2 (3)O7—X1—O8109.8 (4)
O1i—Te1—O390.1 (3)O7—X1—O9108.3 (4)
O3i—Te1—O3179.994O8—X1—O9110.1 (4)
O2i—Te1—O389.6 (3)O7—X1—O10109.3 (4)
O1—Te1—O389.9 (3)O8—X1—O10108.4 (4)
O2—Te1—O390.4 (3)O9—X1—O10111.0 (4)
O6ii—Te2—O5ii89.6 (3)Te1—O1—H1109.426
O6ii—Te2—O4ii90.4 (3)Te1—O2—H2114.986
O5ii—Te2—O4ii90.0 (3)Te1—O3—H3105.734
O6ii—Te2—O489.6 (3)Te2—O4—H4109.438
O5ii—Te2—O490.0 (3)Te2—O5—H5108.396
O4ii—Te2—O4179.994Te2—O6—H6106.016
Symmetry codes: (i) −x, −y, −z; (ii) −x+1, −y, −z+1; (iii) x−1, y, z; (iv) −x+1, −y+1, −z+1; (v) x+1, y, z; (vi) x+1, y−1, z; (vii) x, y−1, z; (viii) −x+1, −y, −z.
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
O1—H1···O9vii0.857 (6)1.924 (7)2.780 (9)175.6 (5)
O2—H2···O90.817 (6)1.967 (7)2.773 (10)168.7 (5)
O3—H3···O10v0.817 (6)1.972 (7)2.778 (9)169.1 (5)
O4—H4···O8vi0.848 (6)1.815 (7)2.654 (9)169.7 (5)
O5—H5···O7v0.856 (6)1.868 (6)2.701 (9)164.3 (4)
O6—H6···O7vii0.826 (6)1.946 (6)2.755 (8)166.0 (5)
Symmetry codes: (vii) x, y−1, z; (v) x+1, y, z; (vi) x+1, y−1, z.
Selected geometric parameters (Å) top
Te1—O1i1.920 (6)K1—O4iii2.792 (6)
Te1—O3i1.915 (6)K1—O72.815 (6)
Te1—O2i1.900 (6)K1—O5iv2.889 (6)
Te1—O11.920 (6)K1—O62.897 (6)
Te1—O21.900 (6)K1—O12.984 (7)
Te1—O31.915 (6)K1—O52.990 (6)
Te2—O6ii1.921 (6)K1—O8v3.022 (8)
Te2—O5ii1.919 (5)K1—O10v3.032 (8)
Te2—O4ii1.905 (6)K2—O10v2.709 (6)
Te2—O41.905 (6)K2—O2i2.751 (6)
Te2—O51.919 (5)K2—O8vi2.786 (8)
Te2—O61.921 (6)K2—O9vii2.852 (7)
X1—O71.508 (6)K2—O1v2.908 (7)
X1—O81.460 (7)K2—O3vii2.915 (6)
X1—O91.482 (7)K2—O62.984 (7)
X1—O101.473 (6)K2—O3viii3.267 (8)
Symmetry codes: (i) −x, −y, −z; (ii) −x+1, −y, −z+1; (iii) x−1, y, z; (iv) −x+1, −y+1, −z+1; (v) x+1, y, z; (vi) x+1, y−1, z; (vii) x, y−1, z; (viii) −x+1, −y, −z.
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
O1—H1···O9vii0.857 (6)1.924 (7)2.780 (9)175.6 (5)
O2—H2···O90.817 (6)1.967 (7)2.773 (10)168.7 (5)
O3—H3···O10v0.817 (6)1.972 (7)2.778 (9)169.1 (5)
O4—H4···O8vi0.848 (6)1.815 (7)2.654 (9)169.7 (5)
O5—H5···O7v0.856 (6)1.868 (6)2.701 (9)164.3 (4)
O6—H6···O7vii0.826 (6)1.946 (6)2.755 (8)166.0 (5)
Symmetry codes: (vii) x, y−1, z; (v) x+1, y, z; (vi) x+1, y−1, z.
Acknowledgements top

This project was supported by the French Ministry of Research & New Technologies and the French/Tunisian Twin Comity for University collaboration.

references
References top

Betteridge, P. W., Carruthers, J. R., Cooper, R. I., Prout, K. & Watkin, D. J. (2003). J. Appl. Cryst. 36, 1487–?.

Brandenburg, K. & Berndt, M. (1999). DIAMOND. Version 2.1.b. Crystal Impact GbR, Bonn, Germany.

Dammak, M., Cousson, A. & Nierlich, M. (2005). Acta Cryst. E61, i55–i57.

Nonius (2001). COLLECT. Nonius BV, Delft, The Netherlands.

Otwinowski, Z. & Minor, W. (1997). Methods in Enzymology, Vol. 276, Macromolecular Crystallography, Part A, edited by C. W. Carter Jr & R. M. Sweet, pp. 307–326. New York: Academic Press.

Sheldrick, G. M. (1997). SHELXS97. University of Göttingen, Germany.

Spek, A. L. (2003). J. Appl. Cryst. 36, 7–13.

Zilber, R., Tordjman, I. & Guitel, J. C. (1980). Acta Cryst. B36, 2741–2743.