Literature DB >> 21202225

Bis-(2-amino-6-methyl-pyridinium) tetra-bromido-cuprate(II).

Rawhi H Al-Far, Basem Fares Ali, Salim F Haddad.   

Abstract

In the crystal structure of the title compound, (C(6)H(9)N(2))(2)[CuBr(4)], the geometry around the Cu atom is inter-mediate between tetra-hedral (T(d)) and square planar (D(4h)). Each [CuBr(4)](2-) anion is connected non-symmetrically to four surrounding cations through N-H⋯X (pyridine and amine proton) hydrogen bonds, forming chains of the ladder-type running parallel to the crystallographic b axis. These layers are further connected by means of offset face-to-face inter-actions (parallel to the a axis), giving a three-dimensional network. Cation π-π stacking [centroid separations of 3.69 (9) and 3.71 (1) Å] and Br⋯aryl inter-actions [3.72 (2) and 4.04 (6) Å] are present in the crystal structure. There are no inter-molecular Br⋯Br inter-actions.

Entities:  

Year:  2008        PMID: 21202225      PMCID: PMC2961314          DOI: 10.1107/S1600536808010647

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


Related literature

For related literature, see: Al-Far & Ali (2007a ▶,b ▶); Ali & Al-Far (2007 ▶, 2008 ▶); Allen et al. (1987 ▶, 1997 ▶); Desiraju & Steiner (1999 ▶); Dolling et al. (2001 ▶); Haddad et al. (2006 ▶); Hunter (1994 ▶); Panunto et al. (1987 ▶); Raithby et al. (2000 ▶); Robinson et al. (2000 ▶); Luque et al. (2001 ▶).

Experimental

Crystal data

(C6H9N2)2[CuBr4] M = 601.45 Triclinic, a = 7.9238 (9) Å b = 8.2521 (11) Å c = 15.2916 (18) Å α = 78.472 (11)° β = 82.839 (10)° γ = 89.947 (14)° V = 971.8 (2) Å3 Z = 2 Mo Kα radiation μ = 9.35 mm−1 T = 293 (2) K 0.20 × 0.15 × 0.10 mm

Data collection

Bruker P4 diffractometer Absorption correction: ψ scan (XSCANS; Bruker, 1996 ▶)T min = 0.199, T max = 0.392 4381 measured reflections 3567 independent reflections 2018 reflections with I > 2σ(I) R int = 0.053

Refinement

R[F 2 > 2σ(F 2)] = 0.058 wR(F 2) = 0.153 S = 1.00 3567 reflections 190 parameters H-atom parameters constrained Δρmax = 0.57 e Å−3 Δρmin = −0.65 e Å−3 Data collection: XSCANS (Bruker, 1996 ▶); cell refinement: XSCANS; data reduction: SHELXTL (Sheldrick, 2008 ▶); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL. Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536808010647/at2561sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536808010647/at2561Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
(C6H9N2)2[CuBr4]Z = 2
Mr = 601.45F000 = 574
Triclinic, P1Dx = 2.056 Mg m3
Hall symbol: -P 1Mo Kα radiation λ = 0.71073 Å
a = 7.9238 (9) ÅCell parameters from 298 reflections
b = 8.2521 (11) Åθ = 2.2–27.5º
c = 15.2916 (18) ŵ = 9.35 mm1
α = 78.472 (11)ºT = 293 (2) K
β = 82.839 (10)ºBlock, blue
γ = 89.947 (14)º0.20 × 0.15 × 0.10 mm
V = 971.8 (2) Å3
Bruker P4 diffractometer3567 independent reflections
Radiation source: fine-focus sealed tube2018 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.053
Detector resolution: 3 pixels mm-1θmax = 25.5º
T = 293(2) Kθmin = 2.5º
ω scansh = −9→1
Absorption correction: ψ scan(PROGRAM; REF (YEAR)k = −9→9
Tmin = 0.199, Tmax = 0.392l = −18→18
4381 measured reflections
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.058H-atom parameters constrained
wR(F2) = 0.153  w = 1/[σ2(Fo2) + (0.0724P)2] where P = (Fo2 + 2Fc2)/3
S = 1.00(Δ/σ)max < 0.001
3567 reflectionsΔρmax = 0.57 e Å3
190 parametersΔρmin = −0.65 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
Br10.18757 (14)0.94944 (11)0.69574 (7)0.0597 (3)
Cu10.32354 (14)0.69646 (13)0.74711 (8)0.0442 (3)
N10.6876 (10)1.0718 (9)1.0416 (6)0.052 (2)
H10.62921.11201.08320.062*
Br20.08231 (15)0.54289 (13)0.82710 (9)0.0745 (4)
N20.6864 (13)0.8282 (10)1.1440 (6)0.074 (3)
H2A0.62680.87501.18250.089*
H2B0.71430.72661.15910.089*
C20.7347 (13)0.9116 (12)1.0624 (7)0.052 (3)
Br30.56567 (13)0.80573 (15)0.79499 (8)0.0679 (4)
C30.8257 (13)0.8462 (13)0.9938 (8)0.060 (3)
H30.85940.73681.00490.072*
Br40.45192 (14)0.50445 (13)0.66438 (8)0.0650 (4)
C40.8653 (14)0.9439 (17)0.9100 (8)0.073 (4)
H40.92390.90060.86360.087*
C50.8171 (15)1.1093 (15)0.8947 (7)0.070 (3)
H50.84871.17610.83840.084*
C60.7270 (14)1.1742 (12)0.9585 (7)0.058 (3)
C70.6683 (17)1.3493 (13)0.9503 (9)0.089 (4)
H7C0.70281.40970.89020.134*
H7B0.71801.40070.99230.134*
H7A0.54651.34910.96300.134*
N80.0896 (10)0.7845 (9)0.5235 (5)0.049 (2)
H80.12790.82420.56530.059*
C9−0.0722 (12)0.7230 (11)0.5402 (7)0.049 (2)
N9−0.1600 (12)0.7226 (11)0.6204 (7)0.080 (3)
H9A−0.11370.76080.66030.095*
H9B−0.26290.68410.63220.095*
C10−0.1360 (13)0.6650 (11)0.4711 (8)0.057 (3)
H10−0.24730.62390.47880.068*
C11−0.0343 (14)0.6690 (12)0.3923 (8)0.057 (3)
H11−0.07710.63020.34610.069*
C120.1301 (15)0.7289 (12)0.3794 (7)0.062 (3)
H120.19680.72900.32490.074*
C130.1985 (13)0.7888 (11)0.4451 (7)0.052 (3)
C140.3706 (14)0.8601 (14)0.4410 (8)0.075 (3)
H14A0.38230.89230.49690.112*
H14B0.38780.95530.39290.112*
H14C0.45380.77920.43060.112*
U11U22U33U12U13U23
Br10.0758 (8)0.0456 (6)0.0583 (7)0.0137 (5)−0.0121 (6)−0.0101 (5)
Cu10.0410 (7)0.0451 (6)0.0453 (7)0.0029 (5)0.0001 (5)−0.0096 (5)
N10.049 (5)0.058 (5)0.050 (6)−0.003 (4)0.005 (4)−0.023 (4)
Br20.0557 (7)0.0607 (7)0.0916 (10)−0.0022 (5)0.0223 (7)0.0021 (6)
N20.116 (9)0.060 (5)0.045 (6)0.010 (5)−0.009 (6)−0.003 (5)
C20.067 (7)0.050 (6)0.046 (7)0.015 (5)−0.013 (6)−0.018 (5)
Br30.0443 (6)0.1028 (9)0.0670 (8)−0.0010 (6)−0.0037 (6)−0.0441 (7)
C30.052 (7)0.067 (7)0.071 (9)0.000 (5)−0.013 (6)−0.034 (7)
Br40.0553 (7)0.0640 (7)0.0793 (9)0.0006 (5)0.0101 (6)−0.0345 (6)
C40.050 (7)0.125 (11)0.061 (9)0.010 (7)−0.010 (6)−0.060 (8)
C50.076 (8)0.100 (9)0.035 (7)0.001 (7)−0.010 (6)−0.013 (6)
C60.063 (7)0.063 (6)0.044 (7)−0.002 (5)−0.010 (6)−0.003 (5)
C70.091 (10)0.069 (8)0.098 (11)0.009 (7)0.000 (8)0.001 (7)
N80.050 (5)0.055 (5)0.045 (5)0.008 (4)−0.009 (4)−0.014 (4)
C90.037 (6)0.049 (5)0.059 (7)0.009 (4)−0.002 (5)−0.010 (5)
N90.058 (6)0.108 (8)0.080 (8)−0.007 (5)0.009 (6)−0.048 (6)
C100.048 (6)0.053 (6)0.069 (8)0.010 (5)−0.020 (6)−0.001 (6)
C110.057 (7)0.070 (7)0.049 (7)0.007 (6)−0.022 (6)−0.011 (5)
C120.079 (9)0.070 (7)0.035 (6)0.017 (6)−0.005 (6)−0.005 (5)
C130.055 (6)0.042 (5)0.053 (7)0.003 (5)0.002 (6)0.001 (5)
C140.050 (7)0.091 (8)0.075 (9)−0.006 (6)0.008 (6)−0.006 (7)
Br1—Cu12.3848 (14)C7—H7B0.9600
Cu1—Br22.3575 (16)C7—H7A0.9600
Cu1—Br42.3713 (14)N8—C91.355 (12)
Cu1—Br32.3765 (16)N8—C131.382 (12)
N1—C21.360 (11)N8—H80.8600
N1—C61.377 (13)C9—N91.331 (13)
N1—H10.8600C9—C101.391 (14)
N2—C21.310 (13)N9—H9A0.8600
N2—H2A0.8600N9—H9B0.8600
N2—H2B0.8600C10—C111.359 (14)
C2—C31.396 (13)C10—H100.9300
C3—C41.371 (16)C11—C121.370 (15)
C3—H30.9300C11—H110.9300
C4—C51.399 (15)C12—C131.371 (14)
C4—H40.9300C12—H120.9300
C5—C61.335 (14)C13—C141.475 (14)
C5—H50.9300C14—H14A0.9600
C6—C71.504 (13)C14—H14B0.9600
C7—H7C0.9600C14—H14C0.9600
Br2—Cu1—Br4101.27 (6)C6—C7—H7A109.5
Br2—Cu1—Br3132.23 (7)H7C—C7—H7A109.5
Br4—Cu1—Br3100.99 (6)H7B—C7—H7A109.5
Br2—Cu1—Br198.36 (6)C9—N8—C13125.5 (9)
Br4—Cu1—Br1129.74 (7)C9—N8—H8117.2
Br3—Cu1—Br198.93 (6)C13—N8—H8117.2
C2—N1—C6124.6 (8)N9—C9—N8118.6 (10)
C2—N1—H1117.7N9—C9—C10124.3 (10)
C6—N1—H1117.7N8—C9—C10117.1 (9)
C2—N2—H2A120.0C9—N9—H9A120.0
C2—N2—H2B120.0C9—N9—H9B120.0
H2A—N2—H2B120.0H9A—N9—H9B120.0
N2—C2—N1117.9 (9)C11—C10—C9119.4 (10)
N2—C2—C3124.8 (9)C11—C10—H10120.3
N1—C2—C3117.3 (10)C9—C10—H10120.3
C4—C3—C2119.8 (10)C10—C11—C12121.3 (10)
C4—C3—H3120.1C10—C11—H11119.4
C2—C3—H3120.1C12—C11—H11119.4
C3—C4—C5119.5 (10)C11—C12—C13121.6 (10)
C3—C4—H4120.3C11—C12—H12119.2
C5—C4—H4120.3C13—C12—H12119.2
C6—C5—C4122.0 (11)C12—C13—N8115.1 (10)
C6—C5—H5119.0C12—C13—C14128.1 (11)
C4—C5—H5119.0N8—C13—C14116.8 (10)
C5—C6—N1116.8 (10)C13—C14—H14A109.5
C5—C6—C7126.9 (11)C13—C14—H14B109.5
N1—C6—C7116.3 (9)H14A—C14—H14B109.5
C6—C7—H7C109.5C13—C14—H14C109.5
C6—C7—H7B109.5H14A—C14—H14C109.5
H7C—C7—H7B109.5H14B—C14—H14C109.5
C6—N1—C2—N2−179.2 (10)C13—N8—C9—N9177.8 (9)
C6—N1—C2—C3−1.6 (15)C13—N8—C9—C10−2.5 (13)
N2—C2—C3—C4178.1 (11)N9—C9—C10—C11−179.0 (10)
N1—C2—C3—C40.7 (15)N8—C9—C10—C111.4 (13)
C2—C3—C4—C51.4 (16)C9—C10—C11—C120.1 (15)
C3—C4—C5—C6−2.8 (17)C10—C11—C12—C13−0.6 (16)
C4—C5—C6—N11.9 (17)C11—C12—C13—N8−0.3 (14)
C4—C5—C6—C7179.9 (11)C11—C12—C13—C14−178.6 (10)
C2—N1—C6—C50.3 (16)C9—N8—C13—C122.0 (14)
C2—N1—C6—C7−177.9 (9)C9—N8—C13—C14−179.5 (9)
D—H···AD—HH···AD···AD—H···A
N1—H1···Br3i0.862.473.324 (7)172
N8—H8···Br10.862.523.367 (8)170
N9—H9B···Br4ii0.862.643.487 (10)168
N2—H2B···Br2iii0.862.733.547 (9)158
Br1—Cu12.3848 (14)
Cu1—Br22.3575 (16)
Cu1—Br42.3713 (14)
Cu1—Br32.3765 (16)
Br2—Cu1—Br4101.27 (6)
Br2—Cu1—Br3132.23 (7)
Br4—Cu1—Br3100.99 (6)
Br2—Cu1—Br198.36 (6)
Br4—Cu1—Br1129.74 (7)
Br3—Cu1—Br198.93 (6)
Table 2

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
N1—H1⋯Br3i0.862.473.324 (7)172
N8—H8⋯Br10.862.523.367 (8)170
N9—H9B⋯Br4ii0.862.643.487 (10)168
N2—H2B⋯Br2iii0.862.733.547 (9)158

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

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