Literature DB >> 23468672

catena-Poly[[[dichlorido(pyridin-1-ium-3-yl)arsenic(III)]-μ-chlorido] mono-hydrate].

Lukas Reck1, Wolfgang Schmitt.   

Abstract

The crystal structure of the title compound, {[AsCl3(C5H5n class="Chemical">N)]·H2O} n , is characterized by polymeric chains consisting of alternating arsenic and chlorine atoms running parallel to the a axis. O-H⋯Cl and N-H⋯O hydrogen bonds mediated by non-coordinating water mol-ecules assemble these chains into a three-dimensional framework. The As(III) atom, the atoms of the pyridinium ring and the water O atom have m site symmetry and the bridging Cl atom has site symmetry 2. This is the first reported organotrichloro-arsenate(III) in which arsenic adopts a ψ-octa-hedral fivefold coordination.

Entities:  

Year:  2012        PMID: 23468672      PMCID: PMC3588707          DOI: 10.1107/S1600536812042882

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


Related literature

For the synthesis, see: Binz & von Schickh (1936 ▶). For mono­meric and oligomeric monon class="Chemical">organohaloarsenates(III) with tetra­coordinate arsenic, see: Grewe et al. (1998 ▶). For homologous monoorganohaloanti­monate(III)/-bis­muth­ate(III) structures, see: Althaus et al. (1999 ▶); Breunig et al. (1992 ▶, 1999 ▶, 2010 ▶); Hall & Sowerby (1988 ▶); James et al. (1999 ▶); Preut et al. (1987 ▶); Sheldrick & Martin (1992 ▶); von Seyerl et al. (1986 ▶). For organoarsenic functionalized metal oxide clusters, see: Breen, Clérac et al. (2012 ▶); Breen, Zhang et al. (2012 ▶); Onet et al. (2011 ▶); Zhang et al. (2012 ▶).

Experimental

Crystal data

[AsCl3(C5H5N)]·H2O M = 278.39 Orthorhombic, a = 8.2107 (9) Å b = 8.5812 (9) Å c = 13.2046 (14) Å V = 930.37 (17) Å3 Z = 4 Mo Kα radiation μ = 4.46 mm−1 T = 200 K 0.5 × 0.2 × 0.2 mm

Data collection

Bruker SMART APEX CCD diffractometer Absorption correction: multi-scan (SADABS; Bruker, 1997 ▶) T min = 0.341, T max = 0.469 3423 measured reflections 1184 independent reflections 1167 reflections with I > 2σ(I) R int = 0.068

Refinement

R[F 2 > 2σ(F 2)] = 0.032 wR(F 2) = 0.078 S = 1.10 1184 reflections 66 parameters 3 restraints H atoms treated by a mixture of independent and constrained refinement Δρmax = 1.14 e Å−3 Δρmin = −1.28 e Å−3 Absolute structure: Flack (1983 ▶), 529 Friedel pairs Flack parameter: 0.006 (12) Data collection: SMART (Bruker, 1997 ▶); cell refinement: SAINT (Bruker, 1997 ▶); data reduction: SAIn class="Chemical">NT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: OLEX2 (Dolomanov et al., 2009 ▶); software used to prepare material for publication: OLEX2. Click here for additional data file. Crystal structure: contains datablock(s) global. DOI: 10.1107/S1600536812042882/nk2180sup1.cif Click here for additional data file. Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812042882/nk2180Isup2.hkl Click here for additional data file. Supplementary material file. DOI: 10.1107/S1600536812042882/nk2180Isup3.cdx Additional supplementary materials: crystallographic information; 3D view; checkCIF report
[AsCl3(C5H5N)]·H2ODx = 1.987 Mg m3
Mr = 278.39Mo Kα radiation, λ = 0.71073 Å
Orthorhombic, Im2aCell parameters from 2911 reflections
a = 8.2107 (9) Åθ = 2.8–28.2°
b = 8.5812 (9) ŵ = 4.46 mm1
c = 13.2046 (14) ÅT = 200 K
V = 930.37 (17) Å3Block, colourless
Z = 40.5 × 0.2 × 0.2 mm
F(000) = 544
Bruker SMART APEX CCD diffractometer1184 independent reflections
Radiation source: fine-focus sealed tube1167 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.068
φ and ω scansθmax = 28.2°, θmin = 2.8°
Absorption correction: multi-scan (SADABS; Bruker, 1997)h = −10→10
Tmin = 0.341, Tmax = 0.469k = −11→9
3423 measured reflectionsl = −13→17
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.032H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.078w = 1/[σ2(Fo2) + (0.0554P)2] where P = (Fo2 + 2Fc2)/3
S = 1.10(Δ/σ)max < 0.001
1184 reflectionsΔρmax = 1.14 e Å3
66 parametersΔρmin = −1.28 e Å3
3 restraintsAbsolute structure: Flack (1983), 529 Friedel pairs
Primary atom site location: structure-invariant direct methodsFlack parameter: 0.006 (12)
Experimental. R(int) was 0.0767 before and 0.0385 after correction. The Ratio of minimum to maximum transmission is 0.7260. The λ/2 correction factor is 0.0015.
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
As10.75000.27357 (4)0.63175 (3)0.01702 (14)
Cl10.55187 (9)0.36810 (11)0.73375 (6)0.0270 (2)
Cl20.50000.15046 (13)0.50000.0229 (2)
N30.75000.5797 (5)0.3838 (3)0.0215 (8)
H30.75000.56900.31750.026*
C10.75000.4632 (5)0.5450 (3)0.0187 (8)
C20.75000.4508 (5)0.4411 (3)0.0201 (8)
H20.75000.35090.41000.024*
C40.75000.7237 (6)0.4225 (4)0.0291 (11)
H40.75000.81170.37880.035*
C50.75000.7435 (6)0.5249 (4)0.0402 (14)
H50.75000.84500.55360.048*
C60.75000.6127 (6)0.5865 (4)0.0333 (12)
H60.75000.62500.65800.040*
O10.75000.0724 (4)0.3215 (2)0.0242 (7)
H10.672 (2)0.093 (6)0.358 (2)0.036*
U11U22U33U12U13U23
As10.0145 (2)0.0197 (2)0.0169 (2)0.0000.0000.00251 (18)
Cl10.0210 (3)0.0386 (5)0.0213 (4)0.0061 (3)0.0042 (3)0.0002 (3)
Cl20.0192 (5)0.0278 (6)0.0219 (5)0.0000.0024 (4)0.000
N30.0224 (19)0.025 (2)0.0172 (15)0.0000.0000.0015 (14)
C10.0204 (19)0.018 (2)0.0173 (19)0.0000.000−0.0001 (16)
C20.0194 (19)0.017 (2)0.024 (2)0.0000.000−0.0017 (16)
C40.034 (3)0.021 (2)0.032 (2)0.0000.0000.0019 (18)
C50.072 (4)0.014 (3)0.034 (3)0.0000.000−0.003 (2)
C60.058 (4)0.025 (3)0.017 (2)0.0000.000−0.0035 (18)
O10.0180 (15)0.0329 (19)0.0218 (15)0.0000.000−0.0053 (14)
As1—C11.990 (4)C2—H20.9500
As1—Cl12.2624 (8)C4—C51.363 (7)
As1—Cl22.8907 (5)C4—H40.9500
N3—C41.337 (7)C5—C61.386 (7)
N3—C21.340 (6)C5—H50.9500
N3—H30.8800C6—H60.9500
C1—C21.377 (6)O1—H10.818 (17)
C1—C61.395 (7)
C1—As1—Cl192.83 (9)N3—C2—C1119.9 (4)
C1—As1—Cl287.28 (9)N3—C2—H2120.0
Cl1—As1—Cl1i91.95 (4)C1—C2—H2120.0
Cl1—As1—Cl2ii179.25 (3)N3—C4—C5119.6 (5)
Cl1—As1—Cl288.78 (2)N3—C4—H4120.2
Cl2ii—As1—Cl290.49 (2)C5—C4—H4120.2
As1iii—Cl2—As1137.13 (5)C4—C5—C6118.7 (4)
C4—N3—C2123.2 (4)C4—C5—H5120.6
C4—N3—H3118.4C6—C5—H5120.6
C2—N3—H3118.4C5—C6—C1121.0 (4)
C2—C1—C6117.5 (4)C5—C6—H6119.5
C2—C1—As1120.7 (3)C1—C6—H6119.5
C6—C1—As1121.8 (3)
C1—As1—Cl2—As1iii−26.08 (9)C6—C1—C2—N30.000 (2)
Cl1—As1—Cl2—As1iii66.82 (2)As1—C1—C2—N3180.000 (1)
Cl2ii—As1—Cl2—As1iii−113.33 (2)C2—N3—C4—C50.000 (2)
Cl1—As1—C1—C2−133.95 (2)N3—C4—C5—C60.000 (2)
Cl2—As1—C1—C2−45.308 (11)C4—C5—C6—C10.000 (2)
Cl1—As1—C1—C646.05 (2)C2—C1—C6—C50.000 (2)
Cl2—As1—C1—C6134.692 (12)As1—C1—C6—C5180.000 (2)
C4—N3—C2—C10.000 (2)
D—H···AD—HH···AD···AD—H···A
O1—H1···Cl20.82 (2)2.40 (2)3.197 (2)165 (3)
N3—H3···O1iv0.881.842.711173
Table 1

Selected bond lengths (Å)

As1—Cl12.2624 (8)
As1—Cl22.8907 (5)
Table 2

Hydrogen-bond geometry (Å, °)

D—H⋯A D—HH⋯A DA D—H⋯A
O1—H1⋯Cl20.82 (2)2.40 (2)3.197 (2)165 (3)
N3—H3⋯O1i 0.881.842.711173

Symmetry code: (i) .

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4.  A short history of SHELX.

Authors:  George M Sheldrick
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5.  Self-assembly of hybrid organic-inorganic polyoxomolybdates: solid-state structures and investigation of formation and core rearrangements in solution.

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