inorganic compounds
of a natural cobaltian mansfieldite from synchrotron data
aMuseo di Storia Naturale – Sezione di Mineralogia, Universitá di Firenze, via La Pira 4, 50121 Firenze, Italy, and bDipartimento di Scienze della Terra, Universitá di Firenze, via La Pira 4, 50121 Firenze, Italy
*Correspondence e-mail: matteo.zoppi@unifi.it
A structural 4·2H2O [aluminium orthoarsenate(V) dihydrate], has been performed based on synchrotron powder diffraction data, with 5% of the octahedral Al sites replaced by Co. Mansfieldite is the aluminium analogue and an isotype of the mineral scorodite (FeAsO4·2H2O), with which it forms a The framework structure is based on AsO4 tetrahedra sharing their vertices with AlO4(H2O)2 octahedra. Three of the four H atoms belonging to the two water molecules in cis positions take part in O—H⋯O hydrogen bonding.
of a natural sample of a Co-bearing mansfieldite, AlAsORelated literature
Mansfieldite (AlAsO4·2H2O) was first described by Allen et al. (1948) and the synthetic analogue was structurally characterised by Harrison (2000). For the structures of isotypic minerals and synthetic compounds, see: Botelho et al. (1994), Tang et al. (2001) (yanomamite, InAsO4·2H2O); Kniep et al. (1977) (variscite, AlPO4·2H2O); Hawthorne (1976), Kitahama et al. (1975), Xu et al. (2007) (scorodite, FeAsO4·2H2O); Taxer & Bartl (2004) (strengite, FePO4·2H2O); Loiseau et al. (1998) (synthetic GaPO4·2H2O); Mooney-Slater (1961) (synthetic InPO4·2H2O and TlPO4·2H2O).
Experimental
Crystal data
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Data collection
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Refinement
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Data collection: local image plate reading software; cell GSAS (Larson & Von Dreele, 2004) and EXPGUI (Toby, 2001); data reduction: FIT2D (Hammersley, 1997); program(s) used to solve structure: atomic coordinates from Harrison (2000); program(s) used to refine structure: GSAS and EXPGUI; molecular graphics: VICS (Izumi & Dilanian, 2005); software used to prepare material for publication: publCIF (Westrip, 2009).
Supporting information
10.1107/S1600536808044127/wm2209sup1.cif
contains datablocks global, I. DOI:Rietveld powder data: contains datablock I. DOI: 10.1107/S1600536808044127/wm2209Isup2.rtv
The specimen used in this study is from the locality of Mt. Cobalt, Cloncurry District, Queensland, Australia. Preliminarily, some transparent single crystals were selected from massive, light purple coloured, mansfieldite associated with smolianinovite [(Co,Ni,Mg,Ca)3(Fe3+,Al)2(AsO4)4.11H2O]. The average elemental chemical composition, determined using electron microprobe analyses, yielded the empirical chemical formula, calculated on a total of two cations per formula unit, (Al0.944Co3+0.046Cu2+0.005 Fe3+0.003 Zn2+0.002)Σ=1 (As0.972Al0.022P0.006)Σ=1O3.975.2H2O resulting in the simplified formula AlAsO4.2H2O. The excess Al resulting from the calculation has been arbitrarily assigned to the tetrahedral site. X-ray data collections of some single crystals, with a CCD equipped diffractometer, revealed that all the samples were actually polycrystalline aggregates and showed irregular and broadened spots typical of materials with high mosaicity. Refinements from single-crystal X-ray diffraction data yielded, in the best case, a not satisfactorily RF index of 6.54%. Fragments of pure mansfieldite were then ground and used for synchrotron X-ray data collection.
Structural data were refined employing the
and starting from the atomic coordinates provided by Harrison (2000), except for the H atom parameters that were not refined but included in the model. The site occupancies were assigned according to the composition of the idealised chemical formula (Al0.95Co3+0.05)AsO4.2H2O, with 5% Co at the octahedral Al sites.Data collection: local image plate reading software; cell
GSAS (Larson & Von Dreele, 2004) and EXPGUI (Toby, 2001); data reduction: FIT2D (Hammersley, 1997); program(s) used to solve structure: atomic coordinates from Harrison (2000); program(s) used to refine structure: GSAS (Larson & Von Dreele, 2004) and EXPGUI (Toby, 2001); molecular graphics: VICS (Izumi & Dilanian, 2005); software used to prepare material for publication: publCIF (Westrip, 2009).Fig. 1. The observed, calculated, background and difference X-ray diffraction profile for natural mansfieldite. Bragg reflection positions are shown at the bottom. | |
Fig. 2. The crystal structure of mansfieldite, viewed along the b axis. The unit cell is outlined and the hydrogen bonds are represented by dashed lines. |
AlAsO4·2H2O | F(000) = 789 |
Mr = 203.53 | Dx = 3.112 Mg m−3 |
Orthorhombic, Pbca | Synchrotron radiation, λ = 0.68780 Å |
Hall symbol: -P 2ac 2ab | µ = 7.25 mm−1 |
a = 8.79263 (11) Å | T = 298 K |
b = 9.79795 (10) Å | Particle morphology: powder |
c = 10.08393 (11) Å | light pink |
V = 868.73 (2) Å3 | flat sheet, 5.0 × 5.0 mm |
Z = 8 |
ESRF BM08 Beamline diffractometer | Absorption correction: for a cylinder mounted on the ϕ axis Debye-Scherrer, Term (= MU.r/wave) = 2.4540. Correction is not refined. |
Data collection mode: transmission | Tmin = 0.072, Tmax = 0.095 |
Scan method: Stationary detector |
Refinement on Inet | Excluded region(s): none |
Least-squares matrix: full | Profile function: CW Pseudo-Voigt |
Rp = 0.039 | 60 parameters |
Rwp = 0.050 | no restraints |
Rexp = 0.039 | H-atom parameters not refined |
RBragg = 0.034 | w = 1/[Yi] |
R(F2) = 0.03400 | (Δ/σ)max = 0.01 |
χ2 = 1.716 | Background function: GSAS Background function number 1 with 14 terms. Shifted Chebyshev function of 1st kind |
? data points | Preferred orientation correction: Spherical Harmonics ODF |
AlAsO4·2H2O | V = 868.73 (2) Å3 |
Mr = 203.53 | Z = 8 |
Orthorhombic, Pbca | Synchrotron radiation, λ = 0.68780 Å |
a = 8.79263 (11) Å | µ = 7.25 mm−1 |
b = 9.79795 (10) Å | T = 298 K |
c = 10.08393 (11) Å | flat sheet, 5.0 × 5.0 mm |
ESRF BM08 Beamline diffractometer | Absorption correction: for a cylinder mounted on the ϕ axis Debye-Scherrer, Term (= MU.r/wave) = 2.4540. Correction is not refined. |
Data collection mode: transmission | Tmin = 0.072, Tmax = 0.095 |
Scan method: Stationary detector |
Rp = 0.039 | χ2 = 1.716 |
Rwp = 0.050 | ? data points |
Rexp = 0.039 | 60 parameters |
RBragg = 0.034 | no restraints |
R(F2) = 0.03400 | H-atom parameters not refined |
x | y | z | Uiso*/Ueq | Occ. (<1) | |
Al1 | 0.1478 (3) | 0.18068 (16) | 0.12682 (18) | 0.0087 (5)* | 0.95 |
Co1 | 0.1478 (3) | 0.18068 (16) | 0.12682 (18) | 0.0087 (5)* | 0.05 |
As2 | 0.03632 (9) | −0.13857 (6) | 0.15042 (6) | 0.00875 (18)* | |
O1 | 0.0106 (4) | 0.0308 (3) | 0.1440 (3) | 0.0055 (8)* | |
O2 | 0.0003 (5) | −0.1986 (3) | 0.3005 (3) | 0.0077 (12)* | |
O3 | 0.2208 (5) | −0.1729 (4) | 0.1105 (3) | 0.0086 (12)* | |
O4 | −0.0815 (5) | −0.2171 (3) | 0.0434 (4) | 0.0063 (11)* | |
O5w | 0.2296 (5) | 0.1244 (4) | 0.2939 (3) | 0.0182 (12)* | |
O6w | 0.3186 (4) | 0.0696 (4) | 0.0559 (3) | 0.0164 (12)* | |
H51 | 0.19 | 0.17 | 0.354 | 0.08* | |
H52 | 0.309 | 0.114 | 0.301 | 0.036* | |
H61 | 0.347 | 0.093 | −0.01 | 0.033* | |
H62 | 0.295 | −0.023 | 0.053 | 0.047* |
Al1—O1 | 1.908 (4) | As2—O4 | 1.682 (4) |
Al1—O2i | 1.906 (4) | O5W—H51 | 0.8295 |
Al1—O3ii | 1.850 (4) | O5W—H52 | 0.709 |
Al1—O4iii | 1.848 (4) | O6W—H61 | 0.746 |
Al1—O5w | 1.914 (4) | O6W—H62 | 0.931 |
Al1—O6w | 1.988 (4) | O1—H52iv | 2.028 |
As2—O1 | 1.676 (3) | O3—H62 | 1.709 |
As2—O2 | 1.654 (3) | O4—H51v | 1.790 |
As2—O3 | 1.704 (4) | ||
O1—Al1—O2vi | 90.64 (19) | O1—As2—O3 | 108.35 (18) |
O1—Al1—O3ii | 179.4743 (18) | O1—As2—O4 | 110.18 (18) |
O1—Al1—O4iii | 91.93 (18) | O2—As2—O3 | 109.2 (2) |
O1—Al1—O5w | 86.31 (15) | O2—As2—O4 | 107.83 (19) |
O1—Al1—O6w | 95.09 (18) | O3—As2—O4 | 110.13 (18) |
O2vi—Al1—O3ii | 88.84 (18) | Al1—O1—As2 | 132.9 (2) |
O2vi—Al1—O4iii | 91.28 (18) | Al1vii—O2—As2 | 134.7 (2) |
O2vi—Al1—O5w | 95.56 (17) | Al1viii—O3—As2 | 136.6 (2) |
O2vi—Al1—O6w | 173.9 (2) | Al1iii—O4—As2 | 134.6 (2) |
O3ii—Al1—O4iii | 87.99 (19) | Al1—O5w—H51 | 109.3 (3) |
O3ii—Al1—O5w | 93.84 (18) | Al1—O5w—H52 | 120.0 (3) |
O3ii—Al1—O6w | 85.4 (2) | H51—O5w—H52 | 114.6 |
O4iii—Al1—O5w | 172.94 (19) | Al1—O6w—H61 | 113.9 (4) |
O4iii—Al1—O6w | 90.54 (17) | Al1—O6w—H62 | 112.1 (3) |
O5w—Al1—O6w | 82.82 (17) | H61—O6w—H62 | 110.3 |
O1—As2—O2 | 111.20 (17) |
Symmetry codes: (i) −x, y+1/2, −z+1/2; (ii) −x+1/2, y+1/2, z; (iii) −x, −y, −z; (iv) x−1/2, y, −z+1/2; (v) −x, y−1/2, −z+1/2; (vi) −x, y+3/2, −z+3/2; (vii) −x−1, y+1/2, −z+1/2; (viii) −x+1/2, y−1/2, z. |
D—H···A | D—H | H···A | D···A | D—H···A |
O5w—H51···O4i | 0.83 | 1.78 | 2.607 (5) | 168 (1) |
O5w—H52···O1ix | 0.71 | 2.03 | 2.614 (5) | 161 (1) |
O6w—H62···O3 | 0.93 | 1.71 | 2.587 (5) | 156 (1) |
Symmetry codes: (i) −x, y+1/2, −z+1/2; (ix) x+3/2, y, −z+3/2. |
Experimental details
Crystal data | |
Chemical formula | AlAsO4·2H2O |
Mr | 203.53 |
Crystal system, space group | Orthorhombic, Pbca |
Temperature (K) | 298 |
a, b, c (Å) | 8.79263 (11), 9.79795 (10), 10.08393 (11) |
V (Å3) | 868.73 (2) |
Z | 8 |
Radiation type | Synchrotron, λ = 0.68780 Å |
µ (mm−1) | 7.25 |
Specimen shape, size (mm) | Flat sheet, 5.0 × 5.0 |
Data collection | |
Diffractometer | ESRF BM08 Beamline diffractometer |
Specimen mounting | ? |
Data collection mode | Transmission |
Scan method | Stationary detector |
Absorption correction | For a cylinder mounted on the ϕ axis Debye-Scherrer, Term (= MU.r/wave) = 2.4540. Correction is not refined. |
Tmin, Tmax | 0.072, 0.095 |
2θ values (°) | 2θfixed = ? |
Refinement | |
R factors and goodness of fit | Rp = 0.039, Rwp = 0.050, Rexp = 0.039, χ2 = 1.716 | Bragg = 0.034, R(F2) = 0.03400,
No. of data points | ? |
No. of parameters | 60 |
No. of restraints | no |
H-atom treatment | H-atom parameters not refined |
Computer programs: local image plate reading software, GSAS (Larson & Von Dreele, 2004) and EXPGUI (Toby, 2001), FIT2D (Hammersley, 1997), atomic coordinates from Harrison (2000), VICS (Izumi & Dilanian, 2005), publCIF (Westrip, 2009).
Al1—O1 | 1.908 (4) | Al1—O6w | 1.988 (4) |
Al1—O2i | 1.906 (4) | As2—O1 | 1.676 (3) |
Al1—O3ii | 1.850 (4) | As2—O2 | 1.654 (3) |
Al1—O4iii | 1.848 (4) | As2—O3 | 1.704 (4) |
Al1—O5w | 1.914 (4) | As2—O4 | 1.682 (4) |
Symmetry codes: (i) −x, y+1/2, −z+1/2; (ii) −x+1/2, y+1/2, z; (iii) −x, −y, −z. |
D—H···A | D—H | H···A | D···A | D—H···A |
O5w—H51···O4i | 0.8295 | 1.784 | 2.607 (5) | 168.19 (28) |
O5w—H52···O1iv | 0.709 | 2.028 | 2.614 (5) | 160.98 (27) |
O6w—H62···O3 | 0.931 | 1.709 | 2.587 (5) | 155.80 (26) |
Symmetry codes: (i) −x, y+1/2, −z+1/2; (iv) x+3/2, y, −z+3/2. |
Acknowledgements
This work was funded by the research grant No. 21403(296) of the University of Florence. We thank Steve Sorrel for supplying the specimen.
References
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The mineral mansfieldite belongs to the general group of hydrous arsenates, a structure subgroup of variscite (AlPO4.2H2O), and has been known since the discovery of Allen et al. (1948). It is of white to pale gray colour and has a vitreous luster. It often develops encrustations, crust-like or rounded aggregates on the matrix, and individual crystals are rarely observed. While the structural data of synthetic mansfieldite were reported recently by Harrison (2000), no data regarding natural samples have been provided in literature up to now, probably because of the rare occurrence of crystalline material suitable for structural investigations. Rietveld refinement of a natural sample of a Co-bearing mansfieldite has now been carried out using synchrotron powder diffraction data (Fig. 1).
Mansfieldite crystallizes in the Pbca space group and is isostructural with the the arsenate minerals scorodite [FeAsO4.2H2O] (Xu et al., 2007; Hawthorne, 1976; Kitahama et al., 1975), yanomamite [InAsO4.2H2O] (Tang et al., 2001; Botelho et al., 1994), TlAsO4.2H2O (Mooney-Slater, 1961), and the phosphate minerals variscite [AlPO4.2H2O] (Kniep et al., 1977), strengite [FePO4.2H2O] (Taxer & Bartl, 2004), InPO4.2H2O (Tang et al., 2001; Mooney-Slater, 1961), GaPO4.2H2O (Loiseau et al., 1998) and TlPO4.2H2O (Mooney-Slater, 1961). Correspondingly to the mentioned arsenates, the structure of mansfieldite is composed of AsO4 tetrahedra and AlO4(H2O)2 octahedra, each tetrahedron being connected to four octahedra and each octahedron being connected to four tetrahedra, as shown in Fig. 2. The interatomic distances Al—O and As—O resulting from the refinement of the structure are reported in Table 1. The two water molecules are located in cis position, but the O atoms O5W and O6W do not participate in the linkage with the As—O4 tetrahedra, while three of the hydrogen atoms (H1, H2 and H3) take part in D—H···A bonds that link O5W to O4, O5W to O1, and O6W to O3, respectively (Table 2). Such a structure framework displays channels along b. With respect to the synthetic mansfieldite (Harrison, 2000), the natural sample shows a slightly smaller unit cell volume, which is the effect of slightly smaller octahedral (9.110 versus 9.187 Å3) and tetrahedral (2.428 versus 2.450 Å3) volumes. Also the distortion index of both the polyhedra, 0.019 and 0.008 for the octahedral and tetrahedral site, respectively, is larger than that calculated for the synthetic material, viz. 0.014 and 0.002. A slight distortion of the structure is probably due to the small amount of incorporated Co and other elements present in the structure of the natural sample. Bond valence calculations show slightly overbonded values of 3.036 and 5.079 valence units for the cation in the octahedral site and in the tetrahedral site, respectively. The isotropic thermal parameters for O5W and O6W, 0.0182 (12) and 0.0164 (12) Å2, respectively, are slightly larger than those of the other oxygen atoms and reveal a certain degree of disorder of the water molecules along the channels, since they are not taking part in the metal-oxygen-metal chains of the structure.