Literature DB >> 24046573

Poly[di-methyl-ammonium [(μ2-benzene-1,2-di-carboxyl-ato-κ(2) O (1):O (3))[μ2-3-(pyri-din-4-yl)-1H-pyrazol-1-ido-κ(2) N (1):N (3)]cuprate(II)]].

Liu Na1.   

Abstract

In the title complex, {(C2H8N)[Cu(C8H4O4)(C8H6N3)]} n , there are two Cu(II) cations (each located on a centre of inversion), one benzene-1,2-di-carboxyl-ate dianion, one 3-(pyridin-4-yl)-1H-pyrazol-1-ide anion and one di-methyl-ammonium cation in the asymmetric unit. The di-methyl-ammonium cation was highly disordered and was treated with the SQUEEZE routine in PLATON [Spek (2009 ▶). Acta Cryst. D65, 148-155]; the crystallographic data takes into account the presence of the cation. Each Cu(II) cation exhibits a square-planar coordination geometry. A benzene-1,2-di-carboxyl-ate dianion bridges two Cu(II) cations, building a linear chain along [001]. The chains are connected by 3-(pyridin-4-yl)-1H-pyrazol-1-ide anions, constructing a layer parallel to (101). The layers are assembled into a three-dimensional supra-molecular network through C-H⋯π inter-actions.

Entities:  

Year:  2013        PMID: 24046573      PMCID: PMC3772430          DOI: 10.1107/S1600536813016334

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


Related literature

For background to complexes derived from 4-(1H-pyrazol-3-yl)pyridine, see: Davies et al. (2005 ▶); Tan et al. (2011 ▶); For background to complexes derived from benzene-1,2-di­carb­oxy­lic acid, see: Guo (2010 ▶); Yan et al. (2012 ▶).

Experimental

Crystal data

(C2H8N)[Cu(C8H4O4)(C8H6N3)] M = 417.91 Triclinic, a = 8.0978 (16) Å b = 9.7244 (19) Å c = 11.694 (2) Å α = 89.26 (3)° β = 89.12 (3)° γ = 89.64 (3)° V = 920.7 (3) Å3 Z = 2 Mo Kα radiation μ = 1.22 mm−1 T = 293 K 0.24 × 0.22 × 0.21 mm

Data collection

Rigaku SCXmini diffractometer Absorption correction: multi-scan (ABSCOR; Higashi, 1995 ▶) T min = 0.759, T max = 0.784 8051 measured reflections 3236 independent reflections 2486 reflections with I > 2σ(I) R int = 0.044

Refinement

R[F 2 > 2σ(F 2)] = 0.046 wR(F 2) = 0.124 S = 1.06 3236 reflections 220 parameters H-atom parameters constrained Δρmax = 0.50 e Å−3 Δρmin = −0.30 e Å−3 Data collection: CrystalClear (Rigaku, 2005 ▶); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEPII (Johnson, 1976 ▶) and DIAMOND (Brandenburg, 1999 ▶); software used to prepare material for publication: SHELXL97. Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536813016334/tk5232sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813016334/tk5232Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
(C2H8N)[Cu(C8H4O4)(C8H6N3)]Z = 2
Mr = 417.91F(000) = 430
Triclinic, P1Dx = 1.507 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 8.0978 (16) ÅCell parameters from 8598 reflections
b = 9.7244 (19) Åθ = 3.0–27.6°
c = 11.694 (2) ŵ = 1.22 mm1
α = 89.26 (3)°T = 293 K
β = 89.12 (3)°Block, blue
γ = 89.64 (3)°0.24 × 0.22 × 0.21 mm
V = 920.7 (3) Å3
Rigaku SCXmini diffractometer3236 independent reflections
Radiation source: fine-focus sealed tube2486 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.044
ω scansθmax = 25.0°, θmin = 3.0°
Absorption correction: multi-scan (ABSCOR; Higashi, 1995)h = −9→9
Tmin = 0.759, Tmax = 0.784k = −11→11
8051 measured reflectionsl = −13→13
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.046Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.124H-atom parameters constrained
S = 1.06w = 1/[σ2(Fo2) + (0.0557P)2 + 0.9233P] where P = (Fo2 + 2Fc2)/3
3236 reflections(Δ/σ)max < 0.001
220 parametersΔρmax = 0.50 e Å3
0 restraintsΔρmin = −0.30 e Å3
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
Cu11.00000.50000.50000.0276 (2)
Cu21.00000.50000.00000.0269 (2)
O10.9981 (3)0.6272 (3)0.3683 (2)0.0309 (6)
O20.8655 (4)0.7485 (3)0.4981 (3)0.0519 (9)
O30.8239 (3)0.5948 (3)0.1664 (2)0.0329 (6)
O41.0087 (3)0.6914 (3)0.0509 (2)0.0318 (6)
N10.1845 (4)0.4575 (3)0.1055 (3)0.0304 (8)
N20.7841 (4)0.4230 (3)0.4546 (3)0.0310 (8)
N30.7012 (4)0.4575 (3)0.3568 (3)0.0284 (7)
C10.9180 (5)0.7341 (4)0.3997 (3)0.0320 (9)
C20.8933 (5)0.8487 (4)0.3141 (3)0.0299 (9)
C30.8962 (5)0.8307 (4)0.1954 (3)0.0287 (9)
C40.9107 (5)0.6958 (4)0.1364 (3)0.0270 (8)
C50.8805 (5)0.9467 (4)0.1244 (4)0.0387 (10)
H50.88420.93620.04550.046*
C60.8600 (6)1.0754 (5)0.1688 (4)0.0504 (12)
H60.84881.15110.12000.061*
C70.8559 (7)1.0929 (5)0.2847 (4)0.0539 (13)
H70.84241.18030.31500.065*
C80.8719 (6)0.9800 (5)0.3561 (4)0.0445 (11)
H80.86830.99240.43490.053*
C90.6856 (5)0.3392 (4)0.5137 (3)0.0349 (10)
H90.71160.29920.58390.042*
C100.5388 (5)0.3190 (4)0.4571 (3)0.0357 (10)
H100.45020.26490.48120.043*
C110.5517 (5)0.3955 (4)0.3579 (3)0.0287 (9)
C120.4293 (4)0.4167 (4)0.2673 (3)0.0283 (9)
C130.2849 (5)0.3433 (5)0.2711 (4)0.0451 (12)
H130.26660.27810.32870.054*
C140.1682 (5)0.3670 (5)0.1896 (4)0.0447 (12)
H140.07150.31600.19390.054*
C150.3227 (6)0.5277 (6)0.1017 (4)0.0567 (14)
H150.33670.59350.04400.068*
C160.4478 (6)0.5087 (5)0.1790 (4)0.0566 (15)
H160.54500.55870.17100.068*
U11U22U33U12U13U23
Cu10.0263 (4)0.0308 (4)0.0260 (4)−0.0010 (3)−0.0127 (3)0.0035 (3)
Cu20.0247 (4)0.0338 (4)0.0226 (3)−0.0005 (3)−0.0098 (3)−0.0011 (3)
O10.0306 (14)0.0326 (16)0.0298 (14)0.0011 (12)−0.0102 (12)0.0046 (12)
O20.068 (2)0.055 (2)0.0314 (17)0.0063 (17)0.0068 (16)0.0069 (15)
O30.0355 (15)0.0350 (16)0.0283 (14)−0.0081 (12)−0.0066 (12)0.0024 (12)
O40.0318 (15)0.0367 (16)0.0271 (14)−0.0033 (12)−0.0019 (12)−0.0018 (12)
N10.0264 (17)0.038 (2)0.0272 (17)−0.0013 (14)−0.0066 (14)0.0004 (15)
N20.0301 (18)0.037 (2)0.0261 (17)−0.0010 (15)−0.0137 (14)0.0061 (15)
N30.0259 (17)0.0328 (19)0.0269 (17)0.0009 (14)−0.0125 (14)0.0000 (14)
C10.033 (2)0.037 (2)0.027 (2)−0.0043 (18)−0.0089 (18)0.0011 (18)
C20.033 (2)0.029 (2)0.028 (2)0.0001 (17)−0.0050 (17)0.0006 (17)
C30.027 (2)0.032 (2)0.027 (2)0.0014 (16)−0.0038 (16)0.0019 (17)
C40.0250 (19)0.032 (2)0.024 (2)0.0002 (17)−0.0112 (17)0.0000 (16)
C50.045 (3)0.042 (3)0.029 (2)0.001 (2)−0.0041 (19)0.0073 (19)
C60.070 (3)0.029 (3)0.052 (3)0.006 (2)0.000 (3)0.010 (2)
C70.081 (4)0.027 (2)0.054 (3)0.007 (2)−0.001 (3)−0.004 (2)
C80.059 (3)0.041 (3)0.033 (2)0.000 (2)−0.005 (2)−0.006 (2)
C90.036 (2)0.041 (3)0.028 (2)−0.0007 (19)−0.0116 (18)0.0113 (18)
C100.027 (2)0.047 (3)0.033 (2)−0.0069 (18)−0.0058 (18)0.0040 (19)
C110.024 (2)0.032 (2)0.030 (2)−0.0009 (16)−0.0063 (17)−0.0014 (17)
C120.024 (2)0.036 (2)0.0245 (19)−0.0001 (16)−0.0068 (16)−0.0030 (17)
C130.039 (3)0.062 (3)0.034 (2)−0.014 (2)−0.011 (2)0.019 (2)
C140.031 (2)0.062 (3)0.041 (3)−0.016 (2)−0.013 (2)0.015 (2)
C150.038 (3)0.076 (4)0.056 (3)−0.016 (2)−0.024 (2)0.036 (3)
C160.033 (2)0.073 (4)0.064 (3)−0.025 (2)−0.027 (2)0.036 (3)
Cu1—O11.963 (3)C3—C41.494 (5)
Cu1—O1i1.963 (3)C5—C61.370 (6)
Cu1—N2i1.989 (3)C5—H50.9300
Cu1—N21.989 (3)C6—C71.368 (7)
Cu2—O41.964 (3)C6—H60.9300
Cu2—O4ii1.964 (3)C7—C81.378 (6)
Cu2—N1iii1.990 (3)C7—H70.9300
Cu2—N1iv1.990 (3)C8—H80.9300
O1—C11.276 (5)C9—C101.387 (6)
O2—C11.230 (5)C9—H90.9300
O3—C41.254 (4)C10—C111.373 (5)
O4—C41.268 (4)C10—H100.9300
N1—C151.315 (5)C11—C121.474 (5)
N1—C141.317 (5)C12—C161.365 (6)
N1—Cu2v1.990 (3)C12—C131.373 (6)
N2—C91.324 (5)C13—C141.369 (6)
N2—N31.372 (4)C13—H130.9300
N3—C111.355 (5)C14—H140.9300
C1—C21.503 (5)C15—C161.378 (6)
C2—C81.384 (6)C15—H150.9300
C2—C31.400 (5)C16—H160.9300
C3—C51.399 (5)
O1—Cu1—O1i180.000 (1)C3—C5—H5119.3
O1—Cu1—N2i89.29 (12)C7—C6—C5120.1 (4)
O1i—Cu1—N2i90.71 (12)C7—C6—H6119.9
O1—Cu1—N290.71 (12)C5—C6—H6119.9
O1i—Cu1—N289.29 (12)C6—C7—C8119.4 (4)
N2i—Cu1—N2180.00 (17)C6—C7—H7120.3
O4—Cu2—O4ii180.00 (14)C8—C7—H7120.3
O4—Cu2—N1iii88.12 (12)C7—C8—C2121.9 (4)
O4ii—Cu2—N1iii91.88 (12)C7—C8—H8119.1
O4—Cu2—N1iv91.88 (12)C2—C8—H8119.1
O4ii—Cu2—N1iv88.12 (12)N2—C9—C10111.0 (3)
N1iii—Cu2—N1iv180.00 (19)N2—C9—H9124.5
C1—O1—Cu1106.8 (2)C10—C9—H9124.5
C4—O4—Cu2104.6 (2)C11—C10—C9105.5 (3)
C15—N1—C14116.5 (3)C11—C10—H10127.3
C15—N1—Cu2v121.6 (3)C9—C10—H10127.3
C14—N1—Cu2v121.6 (3)N3—C11—C10107.7 (3)
C9—N2—N3106.2 (3)N3—C11—C12123.1 (3)
C9—N2—Cu1128.4 (3)C10—C11—C12129.1 (3)
N3—N2—Cu1125.2 (2)C16—C12—C13116.6 (4)
C11—N3—N2109.6 (3)C16—C12—C11123.9 (3)
O2—C1—O1122.5 (4)C13—C12—C11119.5 (3)
O2—C1—C2119.0 (4)C14—C13—C12119.5 (4)
O1—C1—C2118.5 (3)C14—C13—H13120.2
C8—C2—C3118.7 (4)C12—C13—H13120.2
C8—C2—C1117.3 (4)N1—C14—C13124.0 (4)
C3—C2—C1124.0 (3)N1—C14—H14118.0
C5—C3—C2118.6 (4)C13—C14—H14118.0
C5—C3—C4116.0 (3)N1—C15—C16123.3 (4)
C2—C3—C4125.4 (3)N1—C15—H15118.4
O3—C4—O4122.1 (4)C16—C15—H15118.4
O3—C4—C3121.5 (3)C12—C16—C15120.1 (4)
O4—C4—C3116.3 (3)C12—C16—H16120.0
C6—C5—C3121.3 (4)C15—C16—H16120.0
C6—C5—H5119.3
D—H···AD—HH···AD···AD—H···A
C7—H7···Cg1vi0.932.853.698 (5)152
Table 1

Hydrogen-bond geometry (Å, °)

Cg1 is the centroid of the N2,N3,C9–C11 ring.

D—H⋯A D—HH⋯A DA D—H⋯A
C7—H7⋯Cg1i 0.932.853.698 (5)152

Symmetry code: (i) .

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