Literature DB >> 24109254

Redetermination of MgCrO4·5H2O.

Matthias Weil1.   

Abstract

The CCD-data based redetermination of the crystal structure of the title compound, magnesium chromate(VI) penta-hydrate, confirms in principle the previous study based on precession film data [Bertrand et al. (1971 ▶). C. R. Hebd. Seances Acad. Sci. Serie C, 272, 530-533.], but with all atoms refined with anisotropic displacement parameters and with all H atoms localized. This allowed an unambiguous assignment of the hydrogen-bonding pattern. MgCrO4·5H2O adopts the MgSO4·5H2O structure type. It contains two Mg(2+) sites on special positions with site symmetry -1, one tetra-hedral CrO4 group and five water mol-ecules. Four of them coordinate to the Mg(2+) cation, and one is an uncoordinating lattice water mol-ecule. The octa-hedral environment of the Mg(2+) cation is completed by two axial O atoms of CrO4 tetra-hedra. This arrangement leads to the formation of chains parallel to [011]. Adjacent chains are linked through O-H⋯O hydrogen bonds (one of them bifurcated), involving both the coordi-nating and lattice water mol-ecules, into a three-dimensional network.

Entities:  

Year:  2013        PMID: 24109254      PMCID: PMC3793667          DOI: 10.1107/S1600536813018588

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For the original structure determination of the title compound, see: Bertrand et al. (1971 ▶). For hydrogen-bonding pattern in the structures of MXO4·5H2O compounds (M = Mg, Cu; X = S, Cr), see: Baur & Rolin (1972 ▶). For Cr—O bond length distributions in chromates(VI), see: Pressprich et al. (1988 ▶). For bond lengths and angles in the related structure of MgCrO4·11H2O, see: Fortes et al. (2013 ▶). For standardization of structure data, see: Gelato & Parthé (1987 ▶).

Experimental

Crystal data

MgCrO4·5H2O M = 230.39 Triclinic, a = 6.1467 (3) Å b = 6.3742 (4) Å c = 10.7048 (6) Å α = 75.919 (4)° β = 81.603 (3)° γ = 71.134 (3)° V = 383.92 (4) Å3 Z = 2 Mo Kα radiation μ = 1.59 mm−1 T = 296 K 0.10 × 0.08 × 0.01 mm

Data collection

Bruker APEXII CCD diffractometer Absorption correction: multi-scan (SADABS; Bruker, 2011 ▶) T min = 0.594, T max = 0.748 10569 measured reflections 4019 independent reflections 3340 reflections with I > 2σ(I) R int = 0.031

Refinement

R[F 2 > 2σ(F 2)] = 0.031 wR(F 2) = 0.069 S = 1.02 4019 reflections 143 parameters 10 restraints H atoms treated by a mixture of independent and constrained refinement Δρmax = 1.17 e Å−3 Δρmin = −0.72 e Å−3 Data collection: APEX2 (Bruker, 2011 ▶); cell refinement: SAINT (Bruker, 2011 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ATOMS for Windows (Dowty, 2008 ▶); software used to prepare material for publication: publCIF (Westrip, 2010 ▶). Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536813018588/br2229sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813018588/br2229Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
MgCrO4·5H2OZ = 2
Mr = 230.39F(000) = 236
Triclinic, P1Dx = 1.993 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 6.1467 (3) ÅCell parameters from 3623 reflections
b = 6.3742 (4) Åθ = 3.5–39.7°
c = 10.7048 (6) ŵ = 1.59 mm1
α = 75.919 (4)°T = 296 K
β = 81.603 (3)°Plate, yellow
γ = 71.134 (3)°0.10 × 0.08 × 0.01 mm
V = 383.92 (4) Å3
Bruker APEXII CCD diffractometer4019 independent reflections
Radiation source: fine-focus sealed tube3340 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.031
ω– and φ–scansθmax = 37.5°, θmin = 3.5°
Absorption correction: multi-scan (SADABS; Bruker, 2011)h = −10→10
Tmin = 0.594, Tmax = 0.748k = −10→10
10569 measured reflectionsl = −17→18
Refinement on F2Primary atom site location: isomorphous structure methods
Least-squares matrix: fullHydrogen site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.031H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.069w = 1/[σ2(Fo2) + (0.0263P)2 + 0.1663P] where P = (Fo2 + 2Fc2)/3
S = 1.02(Δ/σ)max < 0.001
4019 reflectionsΔρmax = 1.17 e Å3
143 parametersΔρmin = −0.72 e Å3
10 restraints
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.
xyzUiso*/Ueq
Mg10.00000.00000.00000.00672 (11)
Mg20.00000.50000.50000.00587 (10)
Cr10.35414 (3)0.02843 (3)0.709355 (18)0.00508 (4)
O10.17472 (14)0.28496 (15)0.66131 (9)0.00919 (15)
O20.61762 (13)0.04795 (15)0.70554 (9)0.00825 (15)
O30.64389 (14)0.14163 (16)0.38351 (9)0.00978 (16)
O40.72867 (14)0.07678 (16)0.14081 (9)0.00919 (15)
OW10.30276 (14)0.54057 (17)0.40541 (10)0.01038 (16)
HW1A0.331 (4)0.660 (3)0.378 (2)0.029 (6)*
HW1B0.413 (3)0.435 (3)0.397 (2)0.032 (6)*
OW20.16925 (14)0.70426 (17)0.12175 (9)0.01025 (16)
HW2A0.118 (4)0.675 (4)0.1938 (16)0.027 (6)*
HW2B0.305 (3)0.669 (4)0.130 (2)0.026 (5)*
OW30.16025 (16)0.18082 (17)0.06898 (10)0.01161 (17)
HW3A0.240 (3)0.115 (3)0.1307 (17)0.024 (5)*
HW3B0.221 (4)0.263 (4)0.016 (2)0.038 (7)*
OW40.65171 (16)0.54576 (17)0.13300 (10)0.01237 (17)
HW4A0.689 (4)0.414 (3)0.130 (2)0.036 (7)*
HW4B0.714 (4)0.560 (4)0.1924 (18)0.030 (6)*
OW50.03331 (14)0.23596 (17)0.41734 (10)0.01081 (16)
HW5A−0.076 (3)0.201 (4)0.413 (2)0.023 (5)*
HW5B0.143 (3)0.156 (3)0.384 (2)0.029 (6)*
U11U22U33U12U13U23
Mg10.0071 (2)0.0069 (3)0.0059 (3)−0.00218 (18)−0.00012 (17)−0.0010 (2)
Mg20.0065 (2)0.0051 (3)0.0058 (3)−0.00195 (18)−0.00013 (17)−0.0007 (2)
Cr10.00505 (6)0.00478 (8)0.00506 (8)−0.00132 (5)−0.00015 (5)−0.00072 (6)
O10.0101 (3)0.0067 (4)0.0085 (4)−0.0003 (3)−0.0012 (3)−0.0001 (3)
O20.0072 (3)0.0092 (4)0.0093 (4)−0.0038 (3)−0.0002 (3)−0.0021 (3)
O30.0102 (3)0.0092 (4)0.0113 (4)−0.0021 (3)−0.0015 (3)−0.0054 (3)
O40.0100 (3)0.0084 (4)0.0071 (4)−0.0023 (3)0.0017 (3)0.0004 (3)
OW10.0078 (3)0.0071 (4)0.0147 (4)−0.0024 (3)0.0022 (3)−0.0010 (3)
OW20.0094 (3)0.0116 (4)0.0074 (4)−0.0020 (3)−0.0003 (3)0.0006 (3)
OW30.0143 (4)0.0125 (4)0.0099 (4)−0.0075 (3)−0.0038 (3)0.0007 (3)
OW40.0140 (4)0.0081 (4)0.0141 (5)−0.0029 (3)0.0001 (3)−0.0018 (3)
OW50.0078 (3)0.0105 (4)0.0162 (5)−0.0024 (3)0.0002 (3)−0.0075 (3)
Mg1—OW3i2.0505 (9)Mg2—OW12.0467 (8)
Mg1—OW32.0505 (9)Mg2—OW1vi2.0467 (8)
Mg1—OW2ii2.0656 (9)Mg2—O12.1099 (9)
Mg1—OW2iii2.0656 (9)Mg2—O1vi2.1099 (9)
Mg1—O4iv2.0952 (9)Cr1—O3vii1.6357 (9)
Mg1—O4v2.0952 (9)Cr1—O4vii1.6554 (9)
Mg2—OW52.0265 (10)Cr1—O11.6568 (9)
Mg2—OW5vi2.0265 (10)Cr1—O21.6579 (8)
OW3i—Mg1—OW3180.00 (5)OW5vi—Mg2—O1vi92.35 (4)
OW3i—Mg1—OW2ii90.97 (4)OW1—Mg2—O1vi88.90 (4)
OW3—Mg1—OW2ii89.03 (4)OW1vi—Mg2—O1vi91.10 (4)
OW3i—Mg1—OW2iii89.03 (4)O1—Mg2—O1vi180.00 (3)
OW3—Mg1—OW2iii90.97 (4)O3vii—Cr1—O4vii109.01 (5)
OW2ii—Mg1—OW2iii180.00 (7)O3vii—Cr1—O1111.25 (5)
OW3i—Mg1—O4iv91.55 (4)O4vii—Cr1—O1108.90 (5)
OW3—Mg1—O4iv88.45 (4)O3vii—Cr1—O2109.30 (4)
OW2ii—Mg1—O4iv88.19 (4)O4vii—Cr1—O2109.31 (4)
OW2iii—Mg1—O4iv91.81 (4)O1—Cr1—O2109.05 (4)
OW3i—Mg1—O4v88.45 (4)Cr1—O1—Mg2142.08 (6)
OW3—Mg1—O4v91.55 (4)Cr1vii—O4—Mg1viii140.12 (5)
OW2ii—Mg1—O4v91.81 (4)Mg2—OW1—HW1A126.4 (16)
OW2iii—Mg1—O4v88.19 (4)Mg2—OW1—HW1B121.9 (17)
O4iv—Mg1—O4v180.00 (5)HW1A—OW1—HW1B111 (2)
OW5—Mg2—OW5vi180.00 (5)Mg1ix—OW2—HW2A119.3 (16)
OW5—Mg2—OW190.91 (4)Mg1ix—OW2—HW2B122.2 (15)
OW5vi—Mg2—OW189.09 (4)HW2A—OW2—HW2B102 (2)
OW5—Mg2—OW1vi89.09 (4)Mg1—OW3—HW3A118.2 (15)
OW5vi—Mg2—OW1vi90.91 (4)Mg1—OW3—HW3B117.0 (18)
OW1—Mg2—OW1vi180.0HW3A—OW3—HW3B111 (2)
OW5—Mg2—O192.35 (4)HW4A—OW4—HW4B109 (2)
OW5vi—Mg2—O187.65 (4)Mg2—OW5—HW5A119.5 (16)
OW1—Mg2—O191.10 (4)Mg2—OW5—HW5B131.6 (16)
OW1vi—Mg2—O188.90 (4)HW5A—OW5—HW5B109 (2)
OW5—Mg2—O1vi87.65 (4)
D—H···AD—HH···AD···AD—H···A
OW1—HW1A···O2x0.81 (2)1.96 (2)2.7702 (13)174 (2)
OW1—HW1B···O30.80 (2)1.97 (2)2.7598 (13)169 (2)
OW2—HW2A···O1vi0.79 (2)2.19 (2)2.9014 (13)150 (2)
OW2—HW2A···OW10.79 (2)2.52 (2)3.1008 (14)132 (2)
OW2—HW2B···OW40.80 (2)2.02 (2)2.8173 (12)171 (2)
OW3—HW3A···O2vii0.82 (2)1.97 (2)2.7891 (13)170 (2)
OW3—HW3B···OW4xi0.81 (2)1.99 (2)2.7906 (14)172 (2)
OW4—HW4B···O1x0.83 (2)2.32 (2)3.1205 (14)163 (2)
OW4—HW4A···O40.80 (2)2.06 (2)2.8535 (14)170 (2)
OW5—HW5B···O2vii0.80 (2)1.93 (2)2.7262 (13)173 (2)
OW5—HW5A···O3iv0.79 (2)1.96 (2)2.7409 (12)174 (2)
Table 1

Selected bond lengths (Å)

Mg1—OW32.0505 (9)
Mg1—OW2i 2.0656 (9)
Mg1—O4ii 2.0952 (9)
Mg2—OW52.0265 (10)
Mg2—OW12.0467 (8)
Mg2—O12.1099 (9)
Cr1—O3iii 1.6357 (9)
Cr1—O4iii 1.6554 (9)
Cr1—O11.6568 (9)
Cr1—O21.6579 (8)

Symmetry codes: (i) ; (ii) ; (iii) .

Table 2

Hydrogen-bond geometry (Å, °)

D—H⋯A D—HH⋯A DA D—H⋯A
OW1—HW1A⋯O2iv 0.81 (2)1.96 (2)2.7702 (13)174 (2)
OW1—HW1B⋯O30.80 (2)1.97 (2)2.7598 (13)169 (2)
OW2—HW2A⋯O1v 0.79 (2)2.19 (2)2.9014 (13)150 (2)
OW2—HW2A⋯OW10.79 (2)2.52 (2)3.1008 (14)132 (2)
OW2—HW2B⋯OW40.80 (2)2.02 (2)2.8173 (12)171 (2)
OW3—HW3A⋯O2iii 0.82 (2)1.97 (2)2.7891 (13)170 (2)
OW3—HW3B⋯OW4vi 0.81 (2)1.99 (2)2.7906 (14)172 (2)
OW4—HW4B⋯O1iv 0.83 (2)2.32 (2)3.1205 (14)163 (2)
OW4—HW4A⋯O40.80 (2)2.06 (2)2.8535 (14)170 (2)
OW5—HW5B⋯O2iii 0.80 (2)1.93 (2)2.7262 (13)173 (2)
OW5—HW5A⋯O3vii 0.79 (2)1.96 (2)2.7409 (12)174 (2)

Symmetry codes: (iii) ; (iv) ; (v) ; (vi) ; (vii) .

  2 in total

1.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

2.  MgSO4·11H2O and MgCrO4·11H2O based on time-of-flight neutron single-crystal Laue data.

Authors:  A Dominic Fortes; Ian G Wood; Matthias J Gutmann
Journal:  Acta Crystallogr C       Date:  2013-03-12       Impact factor: 1.172

  2 in total

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