Literature DB >> 21836953

Bis(1-methyl-piperazine-1,4-diium) tetra-chloridocuprate(II).

Cong-Hu Peng1.   

Abstract

The title compound, (C(5)H(14)N(2))[CuCl(4)], was synthesized by hydro-thermal reaction of CuCl(2) with 1-methyl-piperazine in an HCl/water solution. Both amine N atoms are protonated. The piperazine ring adopts a chair conformation. The Cu-Cl distances in the tetrahedral anion are in the range 2.2360 (7)-2.2732 (7) Å. In the crystal, moderately strong and weak inter-molecular N-H⋯Cl hydrogen bonds link the anion and cation units into an infinite two-dimensional network parallel to the ab plane.

Entities:  

Year:  2011        PMID: 21836953      PMCID: PMC3152076          DOI: 10.1107/S1600536811024354

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


Related literature

For related amino coordination compounds, see: Fu et al. (2009 ▶); Aminabhavi et al. (1986 ▶); Dai & Fu (2008a ▶,b ▶). For halogen atoms as hydrogen-bond acceptors, see: Brammer et al. (2001 ▶). For the bromide analogue of the title compound, see: Peng (2011 ▶).

Experimental

Crystal data

(C5H14N2)[CuCl4] M = 307.52 Orthorhombic, a = 8.9717 (18) Å b = 9.945 (2) Å c = 13.753 (3) Å V = 1227.1 (4) Å3 Z = 4 Mo Kα radiation μ = 2.61 mm−1 T = 298 K 0.20 × 0.05 × 0.05 mm

Data collection

Rigaku Mercury2 diffractometer Absorption correction: multi-scan (CrystalClear; Rigaku, 2005 ▶) T min = 0.89, T max = 1.00 12813 measured reflections 2808 independent reflections 2616 reflections with I > 2σ(I) R int = 0.036

Refinement

R[F 2 > 2σ(F 2)] = 0.025 wR(F 2) = 0.059 S = 1.11 2808 reflections 111 parameters H-atom parameters constrained Δρmax = 0.35 e Å−3 Δρmin = −0.30 e Å−3 Absolute structure: Flack (1983 ▶), 1185 Friedel pairs Flack parameter: 0.010 (11) 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: SHELXTL (Sheldrick, 2008 ▶); software used to prepare material for publication: SHELXTL. Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536811024354/vn2015sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811024354/vn2015Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
(C5H14N2)[CuCl4]F(000) = 620
Mr = 307.52Dx = 1.665 Mg m3
Orthorhombic, P212121Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ac 2abCell parameters from 2808 reflections
a = 8.9717 (18) Åθ = 3.1–27.5°
b = 9.945 (2) ŵ = 2.61 mm1
c = 13.753 (3) ÅT = 298 K
V = 1227.1 (4) Å3Block, blue
Z = 40.20 × 0.05 × 0.05 mm
Rigaku Mercury2 diffractometer2808 independent reflections
Radiation source: fine-focus sealed tube2616 reflections with I > 2σ(I)
graphiteRint = 0.036
Detector resolution: 13.6612 pixels mm-1θmax = 27.5°, θmin = 3.1°
profile data from φ scansh = −11→11
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005)k = −12→12
Tmin = 0.89, Tmax = 1.00l = −17→17
12813 measured reflections
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-atom parameters constrained
R[F2 > 2σ(F2)] = 0.025w = 1/[σ2(Fo2) + (0.022P)2 + 0.1621P] where P = (Fo2 + 2Fc2)/3
wR(F2) = 0.059(Δ/σ)max < 0.001
S = 1.11Δρmax = 0.35 e Å3
2808 reflectionsΔρmin = −0.30 e Å3
111 parametersExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.0271 (9)
Primary atom site location: structure-invariant direct methodsAbsolute structure: Flack (1983), 1185 Friedel pairs
Secondary atom site location: difference Fourier mapFlack parameter: 0.010 (11)
Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds 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.
xyzUiso*/Ueq
Cu10.78864 (3)0.56811 (3)0.60180 (2)0.03632 (10)
Cl20.98061 (8)0.41919 (7)0.59536 (5)0.05205 (19)
Cl30.71852 (8)0.71379 (6)0.71940 (5)0.04349 (16)
N20.6621 (2)−0.0291 (2)0.58707 (15)0.0377 (5)
H2A0.6784−0.11160.61180.045*
H2B0.6166−0.05380.53160.045*
Cl40.60364 (7)0.41742 (6)0.61497 (6)0.04956 (18)
N10.7864 (2)0.17565 (17)0.70981 (13)0.0304 (4)
H10.75170.24660.67610.037*
Cl10.88660 (8)0.71628 (6)0.49755 (5)0.04457 (17)
C40.7962 (3)0.0489 (2)0.55755 (18)0.0401 (5)
H4A0.76580.12770.52110.048*
H4B0.8585−0.00600.51580.048*
C50.8834 (3)0.0914 (2)0.64550 (18)0.0361 (5)
H5A0.91740.01260.68080.043*
H5B0.97020.14260.62560.043*
C10.8693 (3)0.2304 (3)0.79610 (19)0.0491 (7)
H1A0.80800.29480.82920.074*
H1B0.95940.27310.77460.074*
H1C0.89350.15810.83960.074*
C20.6547 (3)0.0954 (3)0.74224 (18)0.0383 (6)
H2C0.59190.15020.78380.046*
H2D0.68820.01840.77960.046*
C30.5663 (3)0.0481 (3)0.65572 (18)0.0397 (6)
H3A0.4848−0.00830.67760.048*
H3B0.52410.12520.62240.048*
U11U22U33U12U13U23
Cu10.03892 (17)0.02711 (15)0.04294 (17)0.00232 (13)0.00213 (13)0.00148 (13)
Cl20.0549 (4)0.0356 (3)0.0656 (4)0.0155 (3)0.0214 (3)0.0148 (4)
Cl30.0472 (3)0.0367 (3)0.0466 (3)−0.0003 (3)0.0106 (3)−0.0032 (3)
N20.0397 (11)0.0306 (10)0.0428 (12)−0.0029 (8)−0.0008 (9)−0.0038 (9)
Cl40.0380 (3)0.0328 (3)0.0779 (5)−0.0016 (3)−0.0067 (3)0.0037 (3)
N10.0304 (9)0.0270 (9)0.0340 (10)0.0017 (8)−0.0019 (9)−0.0003 (8)
Cl10.0558 (4)0.0348 (3)0.0431 (3)0.0093 (3)0.0080 (3)0.0093 (3)
C40.0483 (14)0.0315 (12)0.0403 (13)−0.0010 (12)0.0147 (11)−0.0016 (11)
C50.0288 (12)0.0280 (12)0.0516 (14)0.0007 (10)0.0079 (10)0.0019 (11)
C10.0456 (15)0.0592 (17)0.0424 (14)−0.0092 (13)−0.0093 (12)−0.0046 (13)
C20.0324 (13)0.0435 (14)0.0391 (13)−0.0042 (10)0.0070 (10)−0.0004 (11)
C30.0316 (12)0.0422 (14)0.0454 (14)−0.0038 (11)−0.0004 (10)−0.0057 (13)
Cu1—Cl12.2360 (7)C4—H4A0.9700
Cu1—Cl42.2435 (8)C4—H4B0.9700
Cu1—Cl32.2606 (7)C5—H5A0.9700
Cu1—Cl22.2732 (7)C5—H5B0.9700
N2—C41.488 (3)C1—H1A0.9600
N2—C31.490 (3)C1—H1B0.9600
N2—H2A0.9001C1—H1C0.9600
N2—H2B0.8999C2—C31.505 (3)
N1—C21.494 (3)C2—H2C0.9700
N1—C51.497 (3)C2—H2D0.9700
N1—C11.502 (3)C3—H3A0.9700
N1—H10.8998C3—H3B0.9700
C4—C51.502 (4)
Cl1—Cu1—Cl4141.52 (3)N1—C5—C4109.30 (19)
Cl1—Cu1—Cl398.38 (3)N1—C5—H5A109.8
Cl4—Cu1—Cl399.47 (3)C4—C5—H5A109.8
Cl1—Cu1—Cl296.12 (3)N1—C5—H5B109.8
Cl4—Cu1—Cl297.38 (3)C4—C5—H5B109.8
Cl3—Cu1—Cl2131.02 (3)H5A—C5—H5B108.3
C4—N2—C3111.74 (19)N1—C1—H1A109.5
C4—N2—H2A116.6N1—C1—H1B109.5
C3—N2—H2A108.9H1A—C1—H1B109.5
C4—N2—H2B106.1N1—C1—H1C109.5
C3—N2—H2B114.6H1A—C1—H1C109.5
H2A—N2—H2B98.4H1B—C1—H1C109.5
C2—N1—C5109.69 (17)N1—C2—C3110.34 (19)
C2—N1—C1110.44 (19)N1—C2—H2C109.6
C5—N1—C1112.44 (19)C3—C2—H2C109.6
C2—N1—H1107.4N1—C2—H2D109.6
C5—N1—H1109.6C3—C2—H2D109.6
C1—N1—H1107.1H2C—C2—H2D108.1
N2—C4—C5110.40 (19)N2—C3—C2110.97 (19)
N2—C4—H4A109.6N2—C3—H3A109.4
C5—C4—H4A109.6C2—C3—H3A109.4
N2—C4—H4B109.6N2—C3—H3B109.4
C5—C4—H4B109.6C2—C3—H3B109.4
H4A—C4—H4B108.1H3A—C3—H3B108.0
D—H···AD—HH···AD···AD—H···A
N2—H2A···Cl3i0.902.313.179 (2)162
N2—H2B···Cl2ii0.902.523.185 (2)132
N2—H2B···Cl1ii0.902.653.306 (2)130
N1—H1···Cl40.902.313.1895 (19)164
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
N2—H2A⋯Cl3i0.902.313.179 (2)162
N2—H2B⋯Cl2ii0.902.523.185 (2)132
N2—H2B⋯Cl1ii0.902.653.306 (2)130
N1—H1⋯Cl40.902.313.1895 (19)164

Symmetry codes: (i) ; (ii) .

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