inorganic compounds
Redetermination of the cubic struvite analogue Cs[Mg(OH2)6](AsO4)
aInstitute for Chemical Technologies and Analytics, Division of Structural Chemistry, Vienna University of Technology, Getreidemarkt 9/164-SC, A-1060 Vienna, Austria
*Correspondence e-mail: mweil@mail.zserv.tuwien.ac.at
In contrast to the previous et al. (1955). Gazz. Chim. Ital. 84, 169–174], the present redetermination of the title compound, caesium hexaaquamagnesium arsenate(V), revealed the Cs atom to be on 4d instead of 4b of F3m. The structure can be derived from the halite structure. The centres of the complex [Mg(OH2)6] octahedra and the AsO4 tetrahedra (both with 3m symmetry) are on the respective Na and Cl positions. The building units are connected to each other by O—H⋯O hydrogen bonds. The Cs+ cations (3m symmetry) are located in the voids of this arrangement and exhibit a regular cuboctahedral 12-coordination to the O atoms of the water molecules. The O atom bonded to As has 2mm (Wyckoff position 24f) and the water-molecule O atom has m (Wyckoff position 48h).
from photographic data [FerrariRelated literature
The 4[Mg(OH2)6](PO4), was reported by Whitaker & Jeffery (1970a,b). Crystal growth of struvite-type compounds using the gel diffusion technique was reported by Banks et al. (1975). For isotypic structures, see: Carver et al. (2006) for Cs[Fe(OH2)6](PO4) and Massa et al. (2003) for the cubic form of dimorphic Cs[Mg(OH2)6](PO4). Isotypic struvite-type phases as well as analogues were recently surveyed by Weil (2008).
of struvite, NHExperimental
Crystal data
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Data collection: CAD-4 Software (Enraf–Nonius, 1989); cell CAD-4 Software; data reduction: HELENA implemented in PLATON (Spek, 2003); method used to solve structure: coordinates taken from an isotypic compound; program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ATOMS (Dowty, 2004); software used to prepare material for publication: SHELXL97.
Supporting information
10.1107/S1600536808043171/hb2885sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536808043171/hb2885Isup2.hkl
Colourless octahedral crystals of Cs[Mg(OH2)6](AsO4) with an edge-length up to 1 mm were grown by means of the gel diffusion technique, following a slightly modified procedure as that given by Banks et al. (1975). Aqueous solutions of 0.025 M MgSO4 and 0.02 M Na4edta (edta = ethylenediaminetetraacetate) were adjusted to pH 10 with NaOH. Commercially available gelatine foils (5 g) were dissolved in the hot resulting 100 ml solution and allowed to form a gel inside a large test tube overnight. When the gel had set, an equivalent amount of a solution of 0.025 M CsH2AsO4 (50 ml) was carefully poured over the gel. This solution was then adjusted to pH 9 with NaOH. The test tube was covered with parafilm and the crystal growth proceeded at the gel-liquid interface and into the gel. Crystals large enough for conventional x-ray analysis grew within one week at room temperature. They were separated mechanically from the gel and were washed with a water/ethanol/acetone (1/3/1) mixture.
The coordinates of the isotypic compound Cs[Fe(OH2)6](PO4) (Carver et al., 2006) were taken as starting parameters. The Cs atom in the original
(Ferrari et al., 1955) was positioned on Wyckoff site 4b (1/2, 1/2, 1/2), whereas in the present Cs is on position 4d (3/4, 3/4, 3/4). The position of the H atom was found from difference Fourier maps and was refined with a soft distance restraint of O—H = 0.85 (3) Å.Data collection: CAD-4 Software (Enraf–Nonius, 1989); cell
CAD-4 Software (Enraf–Nonius, 1989); data reduction: HELENA implemented in PLATON (Spek, 2003); program(s) used to solve structure: coordinates taken from an isotypic compound; program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ATOMS (Dowty, 2004); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).Cs[Mg(H2O)6](AsO4) | Dx = 2.559 Mg m−3 |
Mr = 404.24 | Mo Kα radiation, λ = 0.71073 Å |
Cubic, F43m | Cell parameters from 25 reflections |
Hall symbol: F -4 2 3 | θ = 11.4–12.7° |
a = 10.1609 (5) Å | µ = 6.75 mm−1 |
V = 1049.05 (9) Å3 | T = 293 K |
Z = 4 | Octahedron, colourless |
F(000) = 768 | 0.18 × 0.18 × 0.18 mm |
Enraf–Nonius CAD-4 diffractometer | 207 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.037 |
Graphite monochromator | θmax = 30.9°, θmin = 3.5° |
ω/2θ scans | h = −14→14 |
Absorption correction: integration (SHELXTL; Sheldrick, 2008) | k = −14→14 |
Tmin = 0.341, Tmax = 0.382 | l = −14→14 |
3332 measured reflections | 3 standard reflections every 200 min |
208 independent reflections | intensity decay: none |
Refinement on F2 | H atoms treated by a mixture of independent and constrained refinement |
Least-squares matrix: full | w = 1/[σ2(Fo2) + 5.0469P] where P = (Fo2 + 2Fc2)/3 |
R[F2 > 2σ(F2)] = 0.016 | (Δ/σ)max < 0.001 |
wR(F2) = 0.038 | Δρmax = 0.50 e Å−3 |
S = 1.14 | Δρmin = −0.48 e Å−3 |
208 reflections | Extinction correction: SHELXL, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
15 parameters | Extinction coefficient: 0.00144 (17) |
1 restraint | Absolute structure: Flack (1983), 90 Friedel pairs |
Primary atom site location: isomorphous structure methods | Absolute structure parameter: 0.01 (4) |
Cs[Mg(H2O)6](AsO4) | Z = 4 |
Mr = 404.24 | Mo Kα radiation |
Cubic, F43m | µ = 6.75 mm−1 |
a = 10.1609 (5) Å | T = 293 K |
V = 1049.05 (9) Å3 | 0.18 × 0.18 × 0.18 mm |
Enraf–Nonius CAD-4 diffractometer | 207 reflections with I > 2σ(I) |
Absorption correction: integration (SHELXTL; Sheldrick, 2008) | Rint = 0.037 |
Tmin = 0.341, Tmax = 0.382 | 3 standard reflections every 200 min |
3332 measured reflections | intensity decay: none |
208 independent reflections |
R[F2 > 2σ(F2)] = 0.016 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.038 | Δρmax = 0.50 e Å−3 |
S = 1.14 | Δρmin = −0.48 e Å−3 |
208 reflections | Absolute structure: Flack (1983), 90 Friedel pairs |
15 parameters | Absolute structure parameter: 0.01 (4) |
1 restraint |
Geometry. All e.s.d.'s (except the e.s.d. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell e.s.d.'s are taken into account individually in the estimation of e.s.d.'s in distances, angles and torsion angles; correlations between e.s.d.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell e.s.d.'s is used for estimating e.s.d.'s involving l.s. planes. |
Refinement. Refinement of F2 against ALL reflections. The weighted R-factor wR and goodness of fit S are based on F2, conventional R-factors R are based on F, with F set to zero for negative F2. The threshold expression of F2 > σ(F2) is used only for calculating R-factors(gt) etc. and is not relevant to the choice of reflections for refinement. R-factors based on F2 are statistically about twice as large as those based on F, and R- factors based on ALL data will be even larger. |
x | y | z | Uiso*/Ueq | ||
Cs1 | 0.7500 | 0.7500 | 0.7500 | 0.0599 (3) | |
Mg1 | 0.0000 | 0.0000 | 0.0000 | 0.0250 (6) | |
As1 | 0.2500 | 0.2500 | 0.2500 | 0.0201 (2) | |
O1 | 0.2031 (3) | 0.0000 | 0.0000 | 0.0508 (8) | |
O2 | 0.34550 (19) | 0.34550 (19) | 0.34550 (19) | 0.0269 (7) | |
H1 | 0.249 (3) | 0.045 (2) | 0.045 (2) | 0.053 (12)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cs1 | 0.0599 (3) | 0.0599 (3) | 0.0599 (3) | 0.000 | 0.000 | 0.000 |
Mg1 | 0.0250 (6) | 0.0250 (6) | 0.0250 (6) | 0.000 | 0.000 | 0.000 |
As1 | 0.0201 (2) | 0.0201 (2) | 0.0201 (2) | 0.000 | 0.000 | 0.000 |
O1 | 0.0259 (13) | 0.0632 (13) | 0.0632 (13) | 0.000 | 0.000 | −0.033 (2) |
O2 | 0.0269 (7) | 0.0269 (7) | 0.0269 (7) | −0.0036 (7) | −0.0036 (7) | −0.0036 (7) |
Cs1—O1i | 3.6239 (5) | Mg1—O1xiii | 2.064 (3) |
Cs1—O1ii | 3.6239 (5) | Mg1—O1xiv | 2.064 (3) |
Cs1—O1iii | 3.6239 (5) | Mg1—O1xv | 2.064 (3) |
Cs1—O1iv | 3.6239 (5) | Mg1—O1xvi | 2.064 (3) |
Cs1—O1v | 3.6239 (5) | Mg1—O1xvii | 2.064 (3) |
Cs1—O1vi | 3.6239 (5) | Mg1—O1 | 2.064 (3) |
Cs1—O1vii | 3.6239 (5) | As1—O2 | 1.681 (3) |
Cs1—O1viii | 3.6239 (5) | As1—O2xviii | 1.681 (3) |
Cs1—O1ix | 3.6239 (5) | As1—O2xix | 1.681 (3) |
Cs1—O1x | 3.6239 (5) | As1—O2xx | 1.681 (3) |
Cs1—O1xi | 3.6239 (5) | O1—H1 | 0.79 (2) |
Cs1—O1xii | 3.6239 (5) | ||
O1i—Cs1—O1ii | 47.49 (8) | O1iii—Cs1—O1xi | 72.12 (8) |
O1i—Cs1—O1iii | 47.49 (8) | O1iv—Cs1—O1xi | 47.49 (8) |
O1ii—Cs1—O1iii | 47.49 (8) | O1v—Cs1—O1xi | 90.991 (13) |
O1i—Cs1—O1iv | 164.89 (10) | O1vi—Cs1—O1xi | 119.429 (8) |
O1ii—Cs1—O1iv | 119.430 (7) | O1vii—Cs1—O1xi | 72.12 (8) |
O1iii—Cs1—O1iv | 119.429 (7) | O1viii—Cs1—O1xi | 119.429 (7) |
O1i—Cs1—O1v | 119.429 (8) | O1ix—Cs1—O1xi | 47.49 (8) |
O1ii—Cs1—O1v | 164.89 (10) | O1x—Cs1—O1xi | 164.89 (10) |
O1iii—Cs1—O1v | 119.429 (7) | O1i—Cs1—O1xii | 72.12 (8) |
O1iv—Cs1—O1v | 72.12 (8) | O1ii—Cs1—O1xii | 119.429 (7) |
O1i—Cs1—O1vi | 119.429 (8) | O1iii—Cs1—O1xii | 90.991 (13) |
O1ii—Cs1—O1vi | 119.429 (8) | O1iv—Cs1—O1xii | 119.429 (8) |
O1iii—Cs1—O1vi | 164.89 (10) | O1v—Cs1—O1xii | 47.49 (8) |
O1iv—Cs1—O1vi | 72.12 (8) | O1vi—Cs1—O1xii | 90.991 (13) |
O1v—Cs1—O1vi | 72.12 (8) | O1vii—Cs1—O1xii | 47.49 (8) |
O1i—Cs1—O1vii | 90.991 (13) | O1viii—Cs1—O1xii | 119.429 (7) |
O1ii—Cs1—O1vii | 119.430 (7) | O1ix—Cs1—O1xii | 164.89 (10) |
O1iii—Cs1—O1vii | 72.12 (8) | O1x—Cs1—O1xii | 72.12 (8) |
O1iv—Cs1—O1vii | 90.991 (13) | O1xi—Cs1—O1xii | 119.429 (8) |
O1v—Cs1—O1vii | 47.49 (8) | O1xiii—Mg1—O1xiv | 180.0 |
O1vi—Cs1—O1vii | 119.429 (8) | O1xiii—Mg1—O1xv | 90.0 |
O1i—Cs1—O1viii | 90.991 (13) | O1xiv—Mg1—O1xv | 90.0 |
O1ii—Cs1—O1viii | 72.12 (8) | O1xiii—Mg1—O1xvi | 90.0 |
O1iii—Cs1—O1viii | 119.430 (7) | O1xiv—Mg1—O1xvi | 90.0 |
O1iv—Cs1—O1viii | 90.991 (13) | O1xv—Mg1—O1xvi | 180.0 |
O1v—Cs1—O1viii | 119.429 (8) | O1xiii—Mg1—O1xvii | 90.0 |
O1vi—Cs1—O1viii | 47.49 (8) | O1xiv—Mg1—O1xvii | 90.0 |
O1vii—Cs1—O1viii | 164.89 (10) | O1xv—Mg1—O1xvii | 90.0 |
O1i—Cs1—O1ix | 119.429 (7) | O1xvi—Mg1—O1xvii | 90.0 |
O1ii—Cs1—O1ix | 72.12 (8) | O1xiii—Mg1—O1 | 90.0 |
O1iii—Cs1—O1ix | 90.991 (13) | O1xiv—Mg1—O1 | 90.0 |
O1iv—Cs1—O1ix | 47.49 (8) | O1xv—Mg1—O1 | 90.0 |
O1v—Cs1—O1ix | 119.429 (8) | O1xvi—Mg1—O1 | 90.0 |
O1vi—Cs1—O1ix | 90.991 (13) | O1xvii—Mg1—O1 | 180.0 |
O1vii—Cs1—O1ix | 119.429 (8) | O2—As1—O2xviii | 109.5 |
O1viii—Cs1—O1ix | 72.12 (8) | O2—As1—O2xix | 109.471 (1) |
O1i—Cs1—O1x | 72.12 (8) | O2xviii—As1—O2xix | 109.5 |
O1ii—Cs1—O1x | 90.991 (13) | O2—As1—O2xx | 109.5 |
O1iii—Cs1—O1x | 119.430 (7) | O2xviii—As1—O2xx | 109.5 |
O1iv—Cs1—O1x | 119.429 (8) | O2xix—As1—O2xx | 109.5 |
O1v—Cs1—O1x | 90.991 (13) | Mg1—O1—Cs1xxi | 97.56 (5) |
O1vi—Cs1—O1x | 47.49 (8) | Mg1—O1—Cs1xxii | 97.56 (5) |
O1vii—Cs1—O1x | 119.429 (7) | Cs1xxi—O1—Cs1xxii | 164.89 (10) |
O1viii—Cs1—O1x | 47.49 (8) | Mg1—O1—H1 | 126 (3) |
O1ix—Cs1—O1x | 119.429 (7) | Cs1xxi—O1—H1 | 85.6 (3) |
O1i—Cs1—O1xi | 119.430 (7) | Cs1xxii—O1—H1 | 85.6 (3) |
O1ii—Cs1—O1xi | 90.991 (13) |
Symmetry codes: (i) −y+1, z+1, −x+1; (ii) z+1, −x+1, −y+1; (iii) −x+1, −y+1, z+1; (iv) −y+1/2, z+1/2, −x+1; (v) z+1/2, −x+1, −y+1/2; (vi) −x+1, −y+1/2, z+1/2; (vii) y+1/2, z+1, x+1/2; (viii) y+1, z+1/2, x+1/2; (ix) x+1/2, y+1/2, z+1; (x) z+1, x+1/2, y+1/2; (xi) z+1/2, x+1/2, y+1; (xii) x+1/2, y+1, z+1/2; (xiii) −y, z, −x; (xiv) y, z, x; (xv) z, −x, −y; (xvi) z, x, y; (xvii) −x, −y, z; (xviii) −x+1/2, y, −z+1/2; (xix) x, −y+1/2, −z+1/2; (xx) −x+1/2, −y+1/2, z; (xxi) x−1/2, y−1/2, z−1; (xxii) x−1/2, y−1, z−1/2. |
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H1···O2xix | 0.79 (2) | 1.86 (2) | 2.650 (2) | 176 (4) |
Symmetry code: (xix) x, −y+1/2, −z+1/2. |
Experimental details
Crystal data | |
Chemical formula | Cs[Mg(H2O)6](AsO4) |
Mr | 404.24 |
Crystal system, space group | Cubic, F43m |
Temperature (K) | 293 |
a (Å) | 10.1609 (5) |
V (Å3) | 1049.05 (9) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 6.75 |
Crystal size (mm) | 0.18 × 0.18 × 0.18 |
Data collection | |
Diffractometer | Enraf–Nonius CAD-4 diffractometer |
Absorption correction | Integration (SHELXTL; Sheldrick, 2008) |
Tmin, Tmax | 0.341, 0.382 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 3332, 208, 207 |
Rint | 0.037 |
(sin θ/λ)max (Å−1) | 0.723 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.016, 0.038, 1.14 |
No. of reflections | 208 |
No. of parameters | 15 |
No. of restraints | 1 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.50, −0.48 |
Absolute structure | Flack (1983), 90 Friedel pairs |
Absolute structure parameter | 0.01 (4) |
Computer programs: CAD-4 Software (Enraf–Nonius, 1989), HELENA implemented in PLATON (Spek, 2003), coordinates taken from an isotypic compound, SHELXL97 (Sheldrick, 2008), ATOMS (Dowty, 2004).
Cs1—O1i | 3.6239 (5) | As1—O2 | 1.681 (3) |
Mg1—O1 | 2.064 (3) |
Symmetry code: (i) −x+1, −y+1, z+1. |
D—H···A | D—H | H···A | D···A | D—H···A |
O1—H1···O2ii | 0.79 (2) | 1.86 (2) | 2.650 (2) | 176 (4) |
Symmetry code: (ii) x, −y+1/2, −z+1/2. |
References
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Numerous compounds with general formula A[B(OH2)6]XO4, where A = alkali metal, NH4 or Tl, B = Mg or first row transition metal, and X = P or As, are known to crystallize in the orthorhombic struvite (NH4[Mg(OH2)6](PO4)) structure in space group Pmn21 (Whitaker & Jeffrey, 1970a, b). The title compound, (I), Cs[Mg(OH2)6](AsO4), is an isoformular analogue of struvite, but crystallizes in the cubic crystal system. All these structures can be described in terms of closed-packed layers with different stacking sequences (Massa et al., 2003). Phases that are isotypes of struvite, as well as struvite analogues were recently surveyed by Weil (2008). In comparison with the previous refinement from photographic data (Ferrari et al., 1955), the present redetermination of Cs[Mg(OH2)6](AsO4) revealed a different location of the Cs atom, the localization of the H atom and anisotropic displacement parameters for all non H-atoms.
The structure can be described as a derivative of the NaCl structure type (Massa et al., 2003). The centres of the regular complex [Mg(H2O)6] octahedra are situated on the respective Na positions, and the centres of the regular AsO4 tetrahedra are situated on the Cl positions (Fig. 1). Thus one [Mg(H2O)6] octahedron is surrounded by six AsO4 tetrahedra in an octahedral arrangement, and vice versa. The corresponding Mg—O and As—O distances are in the normal range (Table 1). These building units are linked via medium-strong hydrogen bonds (Table 2). Details and differences of the hydrogen bonding schemes in cubic, hexagonal and orthorhombic struvite-type structures were discussed in detail by Massa et al. (2003). The Cs+ cations are located in the voids of this arrangement and exhibit a regular cuboctahedral 12-coordination to the oxygen atoms of the water molecules (Table 1).