Literature DB >> 21753970

Poly[aqua(μ-vinyl-phospho-nato)cadmium].

Laura K Byington Congiardo, Joel T Mague, Aaron R Funk, Ria Yngard, D Andrew Knight.   

Abstract

The title compound, [Cd(C(2)H(3)O(3)P)(H(2)O)](n), was obtained from vinyl-phospho-nic acid and cadmium nitrate. The vinyl groups project into the inter-lamellar space and the structure is held together via van der Waals forces. The Cd(2+) ion is six-coordinate and the geometry is best described as distorted octa-hedral, with O-Cd-O angles falling within the range 61.72 (13)-101.82 (14)°. Five of the coordinated oxygen atoms originate from the phospho-nate group and the sixth from a bound water molecule. Cd-O distances lie between 2.220 (3) and 2.394 (2) Å. The water mol-ecule is hydrogen bonded to a phospho-nate oxygen atom.

Entities:  

Year:  2011        PMID: 21753970      PMCID: PMC3099788          DOI: 10.1107/S160053681100780X

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


Related literature

For the isotypic structure of [Zn(C2H3PO3)]·H2O, see: Menaa et al. (2002 ▶). For other cadmium organo­phospho­nates, see: Cao et al. (1993 ▶); Hou et al. (2008 ▶); Bauer et al. (2007 ▶). For other metal phospho­nates, see: Brody et al. (1984 ▶); Bujoli et al. (2001 ▶, 2007 ▶); Butcher et al. (2002 ▶); Cheetham et al. (1999 ▶); Clearfield et al. (1997 ▶); Clearfiled & Wang (2002 ▶); Fan et al. (2007 ▶); Hu et al. (2003 ▶).

Experimental

Crystal data

[Cd(C2H3O3P)(H2O)] M = 236.43 Orthorhombic, a = 5.9020 (7) Å b = 9.7792 (12) Å c = 4.9901 (6) Å V = 288.01 (6) Å3 Z = 2 Mo Kα radiation μ = 3.99 mm−1 T = 100 K 0.12 × 0.11 × 0.01 mm

Data collection

Bruker APEX CCD area detector diffractometer Absorption correction: multi-scan (SADABS; Sheldrick, 2008a ▶) T min = 0.656, T max = 0.956 2412 measured reflections 726 independent reflections 717 reflections with I > 2σ(I) R int = 0.021

Refinement

R[F 2 > 2σ(F 2)] = 0.020 wR(F 2) = 0.053 S = 1.16 726 reflections 46 parameters 7 restraints H-atom parameters constrained Δρmax = 1.50 e Å−3 Δρmin = −0.50 e Å−3 Absolute structure: Flack (1983 ▶), 303 Friedel pairs Flack parameter: 0.05 (5) Data collection: SMART (Bruker, 2000 ▶); cell refinement: SAINT-Plus (Bruker, 2004 ▶); data reduction: SAINT-Plus; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008b ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008b ▶); molecular graphics: XP in SHELXTL (Sheldrick, 2008b ▶) and CrystalMaker (CrystalMaker, 2010 ▶); software used to prepare material for publication: publCIF (Westrip, 2010 ▶). Crystal structure: contains datablocks I, global. DOI: 10.1107/S160053681100780X/pk2298sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S160053681100780X/pk2298Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
[Cd(C2H3O3P)(H2O)]F(000) = 224
Mr = 236.43Dx = 2.726 Mg m3
Orthorhombic, Pmn21Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ac -2Cell parameters from 2302 reflections
a = 5.9020 (7) Åθ = 4.0–28.2°
b = 9.7792 (12) ŵ = 3.99 mm1
c = 4.9901 (6) ÅT = 100 K
V = 288.01 (6) Å3Plate, colourless
Z = 20.12 × 0.11 × 0.01 mm
Bruker APEX CCD area detector diffractometer726 independent reflections
Radiation source: fine-focus sealed tube717 reflections with I > 2σ(I)
graphiteRint = 0.021
φ and ω scansθmax = 28.0°, θmin = 2.1°
Absorption correction: multi-scan (SADABS; Sheldrick, 2008a)h = −7→7
Tmin = 0.656, Tmax = 0.956k = −12→12
2412 measured reflectionsl = −6→6
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.020H-atom parameters constrained
wR(F2) = 0.053w = 1/[σ2(Fo2) + (0.0351P)2 + 0.0408P] where P = (Fo2 + 2Fc2)/3
S = 1.16(Δ/σ)max = 0.001
726 reflectionsΔρmax = 1.50 e Å3
46 parametersΔρmin = −0.49 e Å3
7 restraintsAbsolute structure: Flack (1983), 303 Friedel pairs
Primary atom site location: heavy-atom methodFlack parameter: 0.05 (5)
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 > 2 s(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. Atom C2 appears disordered across the mirror on the basis of its value for Uiso which is noticeably larger than that of C1. However, no satisfactory 2-site model could be devised. CCDC-784849 contains the supplementary crystallographic data for this article. These data can be obtained free of charge at http://www.ccdc.cam.ac.uk/conts/retrieving.html [or from the Cambridge Crystallographic Data Center (CCDC), 12 Union Road, Cambridge CB2 1EZ, UK; fax: +44 (0)1223–336033; email: deposit@ccdc.cam.ac.uk].
xyzUiso*/Ueq
Cd10.00001.02972 (3)0.10825 (10)0.01148 (12)
P20.00000.81874 (14)0.6776 (2)0.0107 (2)
O10.00001.1926 (4)−0.2266 (7)0.0152 (7)
H1O0.10181.1927−0.34430.018*
O20.00000.8471 (4)0.3805 (7)0.0164 (8)
O30.2081 (4)0.8782 (3)0.8230 (5)0.0132 (5)
C10.00000.6369 (6)0.7329 (12)0.0220 (12)
H10.00000.61820.94330.026*
C20.00000.5472 (8)0.550 (3)0.067 (4)
H2A0.00000.45400.60520.080*
H2B0.00000.57290.36680.080*
U11U22U33U12U13U23
Cd10.01300 (17)0.01407 (18)0.00737 (16)0.0000.000−0.00103 (15)
P20.0131 (5)0.0110 (5)0.0080 (6)0.0000.0000.0007 (4)
O10.0150 (18)0.0198 (18)0.0109 (17)0.0000.0000.0009 (14)
O20.025 (2)0.0153 (19)0.0088 (19)0.0000.000−0.0009 (15)
O30.0121 (12)0.0167 (12)0.0110 (10)0.0003 (9)0.0020 (10)−0.0003 (8)
C10.030 (3)0.013 (2)0.023 (3)0.0000.0000.001 (2)
C20.087 (7)0.034 (4)0.079 (8)0.0000.0000.000 (4)
Cd1—O3i2.220 (3)P2—Cd1iv2.9791 (13)
Cd1—O22.244 (4)O1—H1O0.8400
Cd1—O12.309 (4)O3—Cd1v2.220 (3)
Cd1—O3ii2.394 (2)O3—Cd1iv2.394 (2)
Cd1—P2iii2.9791 (13)C1—C21.265 (14)
P2—O21.508 (4)C1—H11.0659
P2—O31.540 (3)C2—H2A0.9509
P2—C11.799 (6)C2—H2B0.9500
O3i—Cd1—O3vi101.82 (14)O2—P2—C1109.4 (3)
O3i—Cd1—O291.76 (9)O3—P2—C1107.50 (16)
O3i—Cd1—O193.98 (9)O2—P2—Cd1iv125.58 (17)
O2—Cd1—O1170.89 (13)O3—P2—Cd1iv53.05 (10)
O3i—Cd1—O3ii159.44 (11)C1—P2—Cd1iv125.0 (2)
O3vi—Cd1—O3ii98.05 (6)Cd1—O1—H1O120.4
O2—Cd1—O3ii82.37 (10)P2—O2—Cd1137.8 (2)
O1—Cd1—O3ii89.82 (11)P2—O3—Cd1v123.01 (15)
O3vi—Cd1—O3iii159.44 (11)P2—O3—Cd1iv96.01 (12)
O3ii—Cd1—O3iii61.72 (13)Cd1v—O3—Cd1iv115.72 (11)
O3i—Cd1—P2iii128.99 (7)C2—C1—P2125.1 (7)
O2—Cd1—P2iii83.42 (10)C2—C1—H1126.2
O1—Cd1—P2iii87.47 (10)P2—C1—H1108.7
O3ii—Cd1—P2iii30.94 (6)C1—C2—H2A117.2
O2—P2—O3113.18 (14)C1—C2—H2B120.7
O3—P2—O3vii105.8 (2)H2A—C2—H2B122.1
O3—P2—O2—Cd1−60.15 (14)C1—P2—O3—Cd1v112.9 (2)
O3vii—P2—O2—Cd160.15 (14)Cd1iv—P2—O3—Cd1v−126.1 (2)
O3i—Cd1—O2—P250.94 (7)O2—P2—O3—Cd1iv118.03 (17)
O3vi—Cd1—O2—P2−50.94 (7)O3vii—P2—O3—Cd1iv−6.4 (2)
O3ii—Cd1—O2—P2−148.83 (7)C1—P2—O3—Cd1iv−121.04 (19)
O3iii—Cd1—O2—P2148.83 (7)O3—P2—C1—C2−123.27 (12)
O2—P2—O3—Cd1v−8.0 (3)O3vii—P2—C1—C2123.27 (12)
O3vii—P2—O3—Cd1v−132.49 (11)
D—H···AD—HH···AD···AD—H···A
O1—H1O···O3viii0.842.122.916 (4)158
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
O1—H1O⋯O3i0.842.122.916 (4)158

Symmetry code: (i) .

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