supplementary materials


Acta Cryst. (2007). E63, m2355    [ doi:10.1107/S1600536807039608 ]

Morpholinium tetraoxidorhenate(VII)

M. S. Grigoriev, K. E. German and A. Y. Maruk

Abstract top

The title salt, (C4H10NO)[ReO4], contains slightly distorted tetrahedral [ReO4]- anions [Re-O = 1.7224 (11)-1.7361 (11) Å]. The structure consists of alternating cationic and anionic layers parallel to (100). The cations and anions are linked by N-H...O hydrogen bonds into chains along [100].

Comment top

The title compound, (I) (Fig. 1), contains slightly distorted tetrahedral ReO4 anions with Re—O distances from 1.7224 (11) to 1.7361 (11) Å (Table 1). Morpholinium cations have chair conformation.

The structure of (I) can be described as alternating cationic and anionic layers parallel to the (100) plane (Fig. 2). Morpholinium cations act as proton donors in two hydrogen bonds with O atoms of two ReO4 anions from different anionic layers (Table 2). The hydrogen bonds link cations and anions into chains in the [100] direction (Fig. 2).

Related literature top

See Grigoriev et al. (2007) for the structure of guanidinium tetraoxidorhenate.

Experimental top

Synthesis of (I) was carried out as a neutralization reaction by dissolution of morpholine under intensive stirring in 0.2 M water solution of HReO4 at room temperature to achieve pH = 7, followed by evaporation of the resulting solution over concentrated H2SO4. The compound was recrystallized from ethanol.

Refinement top

The H atoms of NH2 and CH2 groups were refined in idealized geometrical positions with displacement parameters being equal to 1.2 times Ueq of the attached N or C atoms.

Computing details top

Data collection: APEX2 (Bruker, 2006); cell refinement: SAINT-Plus (Bruker, 1998); data reduction: SAINT-Plus (Bruker, 1998); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997a); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997a); molecular graphics: SHELXTL (Sheldrick, 1997b); software used to prepare material for publication: SHELXTL (Sheldrick, 1997b).

Figures top
[Figure 1] Fig. 1. A view of (I), showing the atom-labelling scheme. Displacement ellipsoids are drawn at the 50% probability level and H atoms are represented by circles of arbitrary size. Dashed line indicates the hydrogen-bonding interaction.
[Figure 2] Fig. 2. The packing of (I) showing chains of hydrogen bonds.
Morpholinium tetraoxidorhenate(VII) top
Crystal data top
(C4H10NO)[Re1O4]F000 = 624
Mr = 338.33Dx = 2.838 Mg m3
Orthorhombic, Pca21Mo Kα radiation
λ = 0.71073 Å
Hall symbol: P 2c -2acCell parameters from 7854 reflections
a = 12.4401 (3) Åθ = 3.3–35.0º
b = 5.7480 (2) ŵ = 15.37 mm1
c = 11.0420 (3) ÅT = 100 (2) K
V = 789.57 (4) Å3Fragment, colourless
Z = 40.16 × 0.12 × 0.10 mm
Data collection top
Bruker Kappa APEX II area-detector
diffractometer
3460 independent reflections
Radiation source: fine-focus sealed tube3315 reflections with I > 2α(I)
Monochromator: graphiteRint = 0.021
T = 100(2) Kθmax = 35.0º
ω and φ scansθmin = 3.3º
Absorption correction: multi-scan
(SADABS; Sheldrick, 2004)
h = 20→19
Tmin = 0.239, Tmax = 0.309k = 9→9
21183 measured reflectionsl = 17→17
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.010  w = 1/[σ2(Fo2)]
where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.020(Δ/σ)max = 0.001
S = 0.94Δρmax = 0.70 e Å3
3460 reflectionsΔρmin = 0.60 e Å3
101 parametersExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
1 restraintExtinction coefficient: 0.00092 (6)
Primary atom site location: structure-invariant direct methodsAbsolute structure: Flack (1983), with 1650 Friedel pairs
Secondary atom site location: difference Fourier mapFlack parameter: 0.004 (4)
Crystal data top
(C4H10NO)[Re1O4]V = 789.57 (4) Å3
Mr = 338.33Z = 4
Orthorhombic, Pca21Mo Kα
a = 12.4401 (3) ŵ = 15.37 mm1
b = 5.7480 (2) ÅT = 100 (2) K
c = 11.0420 (3) Å0.16 × 0.12 × 0.10 mm
Data collection top
Bruker Kappa APEX II area-detector
diffractometer
3460 independent reflections
Absorption correction: multi-scan
(SADABS; Sheldrick, 2004)
3315 reflections with I > 2α(I)
Tmin = 0.239, Tmax = 0.309Rint = 0.021
21183 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.010H-atom parameters constrained
wR(F2) = 0.020Δρmax = 0.70 e Å3
S = 0.94Δρmin = 0.60 e Å3
3460 reflectionsAbsolute structure: Flack (1983), with 1650 Friedel pairs
101 parametersFlack parameter: 0.004 (4)
1 restraint
Special details top

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 > 2sigma(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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Re10.733624 (3)0.804729 (7)0.201310 (9)0.00950 (2)
O10.62050 (9)0.9089 (2)0.27573 (10)0.0162 (2)
O20.75192 (9)0.5155 (2)0.24128 (12)0.0166 (2)
O30.84512 (9)0.9655 (2)0.24066 (10)0.0169 (2)
O40.71429 (11)0.8243 (2)0.04689 (12)0.0174 (2)
O50.53574 (10)0.5438 (2)0.59191 (10)0.0182 (2)
N10.45216 (10)0.5969 (2)0.35282 (12)0.0115 (2)
H1A0.40040.56150.29630.014*
H1B0.50060.69720.31770.014*
C10.48749 (16)0.7571 (3)0.55316 (16)0.0192 (3)
H1C0.54330.85960.51800.023*
H1D0.45570.83780.62380.023*
C20.40096 (14)0.7119 (3)0.45982 (14)0.0151 (3)
H2A0.34460.60990.49430.018*
H2B0.36710.86030.43500.018*
C30.50859 (13)0.3794 (3)0.39090 (15)0.0141 (3)
H3A0.54760.31230.32100.017*
H3B0.45530.26350.41910.017*
C40.58711 (12)0.4327 (3)0.49177 (14)0.0138 (3)
H4A0.62080.28610.51960.017*
H4B0.64470.53500.46030.017*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Re10.00842 (2)0.01046 (2)0.00962 (2)0.00157 (1)0.00002 (7)0.00069 (7)
O10.0140 (5)0.0163 (5)0.0182 (5)0.0030 (4)0.0045 (4)0.0027 (4)
O20.0157 (5)0.0128 (5)0.0213 (5)0.0040 (4)0.0013 (4)0.0046 (4)
O30.0130 (5)0.0193 (6)0.0183 (5)0.0017 (4)0.0005 (4)0.0049 (4)
O40.0184 (6)0.0208 (6)0.0129 (5)0.0022 (4)0.0027 (4)0.0009 (4)
O50.0269 (6)0.0186 (6)0.0092 (5)0.0108 (5)0.0016 (4)0.0001 (4)
N10.0126 (5)0.0139 (6)0.0080 (5)0.0006 (5)0.0014 (4)0.0015 (5)
C10.0298 (9)0.0169 (7)0.0109 (7)0.0106 (6)0.0049 (6)0.0034 (6)
C20.0170 (7)0.0175 (7)0.0109 (7)0.0061 (6)0.0017 (5)0.0021 (6)
C30.0157 (7)0.0118 (7)0.0148 (6)0.0014 (5)0.0021 (5)0.0046 (6)
C40.0131 (6)0.0152 (7)0.0130 (6)0.0031 (5)0.0019 (5)0.0025 (5)
Geometric parameters (Å, °) top
Re1—O11.7361 (11)C1—C21.513 (2)
Re1—O21.7349 (13)C1—H1C0.9900
Re1—O31.7224 (11)C1—H1D0.9900
Re1—O41.7256 (13)C2—H2A0.9900
O5—C41.4279 (19)C2—H2B0.9900
O5—C11.430 (2)C3—C41.513 (2)
N1—C31.494 (2)C3—H3A0.9900
N1—C21.496 (2)C3—H3B0.9900
N1—H1A0.9200C4—H4A0.9900
N1—H1B0.9200C4—H4B0.9900
O1—Re1—O2108.44 (6)N1—C2—C1108.11 (14)
O1—Re1—O3110.39 (6)N1—C2—H2A110.1
O1—Re1—O4109.41 (6)C1—C2—H2A110.1
O2—Re1—O3110.14 (6)N1—C2—H2B110.1
O2—Re1—O4109.39 (6)C1—C2—H2B110.1
O3—Re1—O4109.06 (6)H2A—C2—H2B108.4
C4—O5—C1109.84 (12)N1—C3—C4109.94 (13)
C3—N1—C2110.34 (12)N1—C3—H3A109.7
C3—N1—H1A109.6C4—C3—H3A109.7
C2—N1—H1A109.6N1—C3—H3B109.7
C3—N1—H1B109.6C4—C3—H3B109.7
C2—N1—H1B109.6H3A—C3—H3B108.2
H1A—N1—H1B108.1O5—C4—C3111.83 (12)
O5—C1—C2110.81 (15)O5—C4—H4A109.3
O5—C1—H1C109.5C3—C4—H4A109.3
C2—C1—H1C109.5O5—C4—H4B109.3
O5—C1—H1D109.5C3—C4—H4B109.3
C2—C1—H1D109.5H4A—C4—H4B107.9
H1C—C1—H1D108.1
C4—O5—C1—C262.46 (19)C2—N1—C3—C454.28 (17)
C3—N1—C2—C156.60 (17)C1—O5—C4—C359.46 (19)
O5—C1—C2—N160.92 (18)N1—C3—C4—O555.57 (17)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
N1—H1A···O2i0.921.992.8529 (17)155
N1—H1B···O10.921.982.8855 (18)168
Symmetry codes: (i) x−1/2, −y+1, z.
Selected geometric parameters (Å, °) top
Re1—O11.7361 (11)Re1—O31.7224 (11)
Re1—O21.7349 (13)Re1—O41.7256 (13)
O1—Re1—O2108.44 (6)O2—Re1—O3110.14 (6)
O1—Re1—O3110.39 (6)O2—Re1—O4109.39 (6)
O1—Re1—O4109.41 (6)O3—Re1—O4109.06 (6)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
N1—H1A···O2i0.921.992.8529 (17)155
N1—H1B···O10.921.982.8855 (18)168
Symmetry codes: (i) x−1/2, −y+1, z.
references
References top

Bruker (1998). SAINT-Plus. Version 6.01. Bruker AXS Inc., Madison, Wisconsin, USA.

Bruker (2006). APEX2. Bruker AXS Inc., Madison, Wisconsin, USA.

Flack, H. D. (1983). Acta Cryst. A39, 876–881.

Grigoriev, M. S., German, K. E. & Maruk, A. Ya. (2007). Acta Cryst. E63, m2061–?.

Sheldrick, G. M. (1997a). SHELXS97 and SHELXL97. University of Göttingen, Germany.

Sheldrick, G. M. (1997b). SHELXTL. Version 5.10. Bruker AXS Inc., Madison, Wisconsin, USA.

Sheldrick, G. M. (2004). SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.