Literature DB >> 21201846

Poly[μ(4)-succinato-μ(2)-succinato-bis[diamminecopper(II)]].

Shouwen Jin, Daqi Wang, Yan-Lin Yu, Guan-Min Luo, Yan-Yan Ye.   

Abstract

In the title compound, [Cu(C(4)H(4)O(4))(NH(3))(2)](n), the Cu atom is coordinated by the N atoms of two ammonia mol-ecules and four O atoms from three different succinate ligands in a highly distorted octa-hedral geometry. The Cu atom and the C and O atoms of the succinate ligands lie on a mirror plane. Two adjacent CuO(4)N(2) octa-hedra share one common O-O edge, forming a Cu(2)O(6)N(4) biocta-hedron with a CuCu separation of 3.524 (2) Å. Neighboring biocta-hedra are connected by bis-unidentate succinate anions in the a-axis direction, while in the c-axis direction biocta-hedra are connected by bis-bidentate succinate anions, leading to an infinite two-dimensional network structure. These networks are further connected along the a-axis direction by hydrogen bonds between ammonia ligands and carboxyl-ate O atoms of neighboring network layers, forming a three-dimensional lamellar structure.

Entities:  

Year:  2008        PMID: 21201846      PMCID: PMC2960840          DOI: 10.1107/S1600536808002493

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


Related literature

For related literature, see: Halcrow (2001 ▶); Holm et al. (1996 ▶); Jin & Chen (2007a ▶,b ▶); Jin et al. (2007 ▶); Kato & Muto (1988 ▶); Lassahn et al. (2004 ▶); Mehrotra & Bohra (1983 ▶); Park et al. (2001 ▶); Rao et al. (2004 ▶); Zheng et al. (2000 ▶, 2001 ▶).

Experimental

Crystal data

[Cu(C4H4O4)(NH3)2] M = 213.68 Monoclinic, a = 13.761 (6) Å b = 7.374 (3) Å c = 8.709 (4) Å β = 124.515 (4)° V = 728.2 (5) Å3 Z = 4 Mo Kα radiation μ = 2.97 mm−1 T = 293 (2) K 0.27 × 0.15 × 0.09 mm

Data collection

Bruker SMART APEX CCD diffractometer Absorption correction: multi-scan (SADABS; Sheldrick, 1996 ▶) T min = 0.501, T max = 0.776 1874 measured reflections 694 independent reflections 641 reflections with I > 2σ(I) R int = 0.036

Refinement

R[F 2 > 2σ(F 2)] = 0.026 wR(F 2) = 0.072 S = 1.14 694 reflections 64 parameters H-atom parameters constrained Δρmax = 0.37 e Å−3 Δρmin = −0.58 e Å−3 Data collection: SMART (Bruker, 1997 ▶); cell refinement: SAINT (Bruker, 1997 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXTL. Crystal structure: contains datablocks global, I. DOI: 10.1107/S1600536808002493/im2043sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536808002493/im2043Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
[Cu(C4H4O4)(NH3)2]F000 = 436
Mr = 213.68Dx = 1.949 Mg m3
Monoclinic, C2/mMo Kα radiation λ = 0.71073 Å
Hall symbol: -C 2yCell parameters from 1618 reflections
a = 13.761 (6) Åθ = 2.8–28.2º
b = 7.374 (3) ŵ = 2.97 mm1
c = 8.709 (4) ÅT = 293 (2) K
β = 124.515 (4)ºBlock, blue
V = 728.2 (5) Å30.27 × 0.15 × 0.09 mm
Z = 4
Bruker SMART APEX CCD diffractometer694 independent reflections
Radiation source: fine-focus sealed tube641 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.036
T = 293(2) Kθmax = 25.0º
φ and ω scansθmin = 2.8º
Absorption correction: multi-scan(SADABS; Sheldrick, 1996)h = −15→16
Tmin = 0.501, Tmax = 0.776k = −8→8
1874 measured reflectionsl = −9→10
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.026H-atom parameters constrained
wR(F2) = 0.072  w = 1/[σ2(Fo2) + (0.0361P)2 + 0.9127P] where P = (Fo2 + 2Fc2)/3
S = 1.14(Δ/σ)max = 0.001
694 reflectionsΔρmax = 0.37 e Å3
64 parametersΔρmin = −0.58 e Å3
Primary atom site location: structure-invariant direct methodsExtinction correction: none
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
Cu10.84469 (3)0.50000.85475 (5)0.0211 (2)
O10.9788 (2)0.50000.8255 (3)0.0239 (6)
O20.8291 (2)0.50000.5275 (4)0.0387 (8)
O30.7184 (2)0.50000.8984 (4)0.0280 (6)
O40.5330 (2)0.50000.8099 (4)0.0381 (7)
N10.83799 (18)0.7693 (4)0.8316 (3)0.0280 (5)
H10.83350.82630.91340.042*
H20.77970.80730.72510.042*
H30.89900.81310.84070.042*
C10.9363 (3)0.50000.6510 (5)0.0223 (8)
C21.0265 (3)0.50000.6041 (5)0.0275 (9)
H2A1.07630.39390.65990.033*
C30.6069 (3)0.50000.7718 (5)0.0241 (8)
C40.5663 (3)0.50000.5694 (5)0.0261 (8)
H40.59870.39390.54800.031*
U11U22U33U12U13U23
Cu10.0203 (3)0.0245 (3)0.0180 (3)0.0000.0106 (2)0.000
O10.0217 (13)0.0359 (16)0.0144 (12)0.0000.0104 (11)0.000
O20.0267 (15)0.068 (2)0.0187 (13)0.0000.0111 (12)0.000
O30.0188 (13)0.0446 (17)0.0191 (12)0.0000.0097 (11)0.000
O40.0252 (15)0.066 (2)0.0255 (14)0.0000.0159 (12)0.000
N10.0283 (12)0.0266 (14)0.0233 (11)0.0018 (10)0.0111 (10)−0.0004 (10)
C10.0249 (18)0.024 (2)0.0183 (16)0.0000.0127 (15)0.000
C20.0256 (19)0.039 (2)0.0200 (19)0.0000.0139 (16)0.000
C30.0256 (19)0.0239 (19)0.0215 (17)0.0000.0126 (16)0.000
C40.028 (2)0.031 (2)0.0179 (17)0.0000.0118 (17)0.000
Cu1—O31.978 (3)N1—H20.8599
Cu1—N1i1.993 (3)N1—H30.8599
Cu1—N11.993 (3)C1—C21.510 (5)
Cu1—O12.001 (3)C2—C2ii1.524 (7)
O1—C11.282 (4)C2—H2A0.9698
O2—C11.240 (5)C3—C41.517 (5)
O3—C31.286 (5)C4—C4iii1.514 (7)
O4—C31.236 (5)C4—H40.9696
N1—H10.8599
O3—Cu1—N1i91.38 (6)H2—N1—H3104.0
O3—Cu1—N191.38 (6)O2—C1—O1123.2 (3)
N1i—Cu1—N1170.34 (12)O2—C1—C2121.5 (3)
O3—Cu1—O1176.92 (9)O1—C1—C2115.3 (3)
N1i—Cu1—O188.87 (6)C1—C2—C2ii114.1 (4)
N1—Cu1—O188.87 (6)C1—C2—H2A108.7
C1—O1—Cu1108.5 (2)C2ii—C2—H2A108.8
C3—O3—Cu1125.9 (2)O4—C3—O3122.2 (3)
Cu1—N1—H1115.1O4—C3—C4119.7 (3)
Cu1—N1—H2113.3O3—C3—C4118.1 (3)
H1—N1—H2105.8C4iii—C4—C3114.3 (4)
Cu1—N1—H3112.2C4iii—C4—H4108.9
H1—N1—H3105.4C3—C4—H4108.5
O3—Cu1—O1—C1180.000 (10)Cu1—O1—C1—C2180.000 (1)
N1i—Cu1—O1—C185.31 (6)O2—C1—C2—C2ii0.000 (1)
N1—Cu1—O1—C1−85.31 (6)O1—C1—C2—C2ii180.000 (2)
N1i—Cu1—O3—C3−85.37 (6)Cu1—O3—C3—O4180.000 (1)
N1—Cu1—O3—C385.37 (6)Cu1—O3—C3—C40.000 (2)
O1—Cu1—O3—C3180.000 (12)O4—C3—C4—C4iii0.0
Cu1—O1—C1—O20.0O3—C3—C4—C4iii180.000 (2)
D—H···AD—HH···AD···AD—H···A
N1—H3···O4iv0.862.443.272 (3)164
N1—H2···O2v0.862.323.133 (3)159
N1—H1···O3vi0.862.483.331 (3)169
N1—H1···O4vi0.862.413.085 (3)136
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
N1—H3⋯O4i0.862.443.272 (3)164
N1—H2⋯O2ii0.862.323.133 (3)159
N1—H1⋯O3iii0.862.483.331 (3)169
N1—H1⋯O4iii0.862.413.085 (3)136

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

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