Literature DB >> 22058898

Bis(benzyl-trimethyl-ammonium) tetra-bromidocuprate(II).

Lei Jin1, Ning Liu, Yong-Jun Li, De-Hong Wu.   

Abstract

In the title mol-ecular salt, (C(10)H(16)N)(2)[CuBr(4)], the Cu(II) ion adopts a squashed tetra-hedral geometry with Br-Cu-Br angles varying between 99.29 (3) and 132.53 (3)°. In the crystal, the components are linked by C-H⋯Br inter-actions, thereby generating a three-dimensional network.

Entities:  

Year:  2011        PMID: 22058898      PMCID: PMC3200753          DOI: 10.1107/S1600536811034830

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


Related literature

For background to mol­ecular–ionic compounds, see: Coffey et al. (2000 ▶); Liu et al. (2001 ▶); Long et al. (1997 ▶); Luque et al. (1997 ▶); Woodward et al. (2001 ▶).

Experimental

Crystal data

(C10H16N)2[CuBr4] M = 683.66 Orthorhombic, a = 9.1908 (8) Å b = 9.6697 (19) Å c = 29.0243 (8) Å V = 2579.5 (6) Å3 Z = 4 Mo Kα radiation μ = 7.05 mm−1 T = 291 K 0.28 × 0.26 × 0.24 mm

Data collection

Rigaku Mercury2 diffractometer Absorption correction: multi-scan (CrystalClear; Rigaku, 2005 ▶) T min = 0.161, T max = 0.183 25511 measured reflections 5922 independent reflections 3769 reflections with I > 2σ(I) R int = 0.101

Refinement

R[F 2 > 2σ(F 2)] = 0.063 wR(F 2) = 0.172 S = 1.02 5922 reflections 250 parameters H-atom parameters constrained Δρmax = 0.89 e Å−3 Δρmin = −1.33 e Å−3 Absolute structure: Flack (1983 ▶), 2556 Friedel pairs Flack parameter: 0.06 (2) 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/S1600536811034830/hb6385sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536811034830/hb6385Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
(C10H16N)2[CuBr4]F(000) = 1340
Mr = 683.66Dx = 1.760 Mg m3
Orthorhombic, P212121Mo Kα radiation, λ = 0.71073 Å
Hall symbol: P 2ac 2abCell parameters from 20422 reflections
a = 9.1908 (8) Åθ = 3.1–27.8°
b = 9.6697 (19) ŵ = 7.05 mm1
c = 29.0243 (8) ÅT = 291 K
V = 2579.5 (6) Å3Block, purple
Z = 40.28 × 0.26 × 0.24 mm
Rigaku Mercury2 diffractometer5922 independent reflections
Radiation source: fine-focus sealed tube3769 reflections with I > 2σ(I)
graphiteRint = 0.101
Detector resolution: 13.6612 pixels mm-1θmax = 27.5°, θmin = 3.1°
CCD_Profile_fitting scansh = −11→11
Absorption correction: multi-scan (CrystalClear; Rigaku, 2005)k = −12→12
Tmin = 0.161, Tmax = 0.183l = −37→37
25511 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)] = 0.063H-atom parameters constrained
wR(F2) = 0.172w = 1/[σ2(Fo2) + (0.0838P)2] where P = (Fo2 + 2Fc2)/3
S = 1.02(Δ/σ)max < 0.001
5922 reflectionsΔρmax = 0.89 e Å3
250 parametersΔρmin = −1.33 e Å3
0 restraintsAbsolute structure: Flack (1983), 2556 Friedel pairs
Primary atom site location: structure-invariant direct methodsFlack parameter: 0.06 (2)
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
Br10.16703 (6)0.33426 (5)0.800673 (18)0.06775 (16)
Br20.49529 (5)0.46102 (5)0.855426 (17)0.05492 (13)
Br30.48651 (5)0.08709 (5)0.870934 (18)0.05845 (14)
Br40.15255 (6)0.21832 (6)0.91811 (2)0.07334 (17)
C10.5435 (5)0.2722 (7)0.73255 (16)0.077 (2)
H1A0.49860.33590.71150.115*
H1B0.50800.28890.76310.115*
H1C0.52030.17920.72360.115*
C20.7333 (6)0.4347 (5)0.74409 (16)0.0749 (18)
H2A0.67610.49590.72540.112*
H2B0.83480.45300.73910.112*
H2C0.71000.44930.77600.112*
C30.7683 (5)0.1951 (6)0.76459 (15)0.0680 (17)
H3A0.73920.21940.79530.102*
H3B0.87230.20050.76210.102*
H3C0.73710.10250.75790.102*
C40.7539 (4)0.2631 (4)0.68414 (13)0.0441 (12)
H4A0.69500.31580.66270.053*
H4B0.73870.16590.67750.053*
C50.9108 (4)0.2968 (4)0.67551 (13)0.0351 (11)
C60.9473 (5)0.4283 (5)0.65858 (15)0.0537 (14)
H60.87590.49390.65240.064*
C71.0959 (6)0.4577 (5)0.65128 (17)0.0684 (17)
H71.12350.54440.64050.082*
C81.1977 (5)0.3617 (6)0.65970 (15)0.0683 (17)
H81.29450.38520.65470.082*
C91.1682 (5)0.2327 (5)0.67503 (15)0.0569 (14)
H91.24200.16870.68030.068*
C101.0156 (4)0.1981 (4)0.68298 (14)0.0474 (12)
H100.98970.11010.69300.057*
C110.8707 (5)0.5105 (5)0.91952 (14)0.0533 (14)
H11A0.95180.45660.90890.080*
H11B0.90340.60160.92760.080*
H11C0.79920.51680.89550.080*
C120.9205 (5)0.4376 (6)0.99779 (15)0.0609 (16)
H12A0.87700.40721.02610.091*
H12B0.96170.52791.00200.091*
H12C0.99560.37400.98890.091*
C130.7555 (5)0.3076 (5)0.95072 (16)0.0596 (16)
H13A0.69320.30960.92420.089*
H13B0.70220.27280.97670.089*
H13C0.83720.24850.94470.089*
C140.6765 (5)0.5276 (4)0.97618 (16)0.0482 (13)
H14A0.62850.47851.00100.058*
H14B0.60800.53470.95090.058*
C150.7132 (4)0.6732 (4)0.99279 (15)0.0426 (12)
C160.7364 (5)0.6983 (5)1.03985 (15)0.0567 (15)
H160.72870.62801.06160.068*
C170.7715 (6)0.8337 (6)1.05265 (17)0.0758 (18)
H170.78460.85441.08370.091*
C180.7868 (5)0.9352 (5)1.0209 (2)0.0659 (17)
H180.81841.02221.03020.079*
C190.7564 (5)0.9120 (6)0.9752 (2)0.0732 (18)
H190.76130.98440.95420.088*
C200.7181 (5)0.7791 (5)0.96046 (16)0.0584 (15)
H200.69630.76200.92970.070*
Cu10.32377 (5)0.27605 (5)0.861735 (16)0.03655 (13)
N10.7012 (3)0.2913 (3)0.73160 (12)0.0441 (10)
N20.8055 (3)0.4434 (3)0.96042 (12)0.0401 (10)
U11U22U33U12U13U23
Br10.0715 (3)0.0703 (3)0.0614 (3)0.0008 (3)−0.0305 (3)0.0075 (3)
Br20.0561 (2)0.0591 (3)0.0496 (3)−0.0083 (2)0.0004 (2)−0.0010 (2)
Br30.0548 (2)0.0547 (2)0.0659 (3)0.0217 (2)0.0048 (2)−0.0025 (2)
Br40.0754 (3)0.0813 (3)0.0634 (3)0.0056 (3)0.0165 (3)−0.0031 (3)
C10.040 (2)0.150 (5)0.040 (3)−0.008 (3)0.004 (2)−0.014 (3)
C20.108 (4)0.060 (3)0.057 (3)−0.015 (3)0.033 (3)−0.026 (2)
C30.068 (3)0.096 (4)0.040 (3)0.007 (3)0.008 (3)0.006 (3)
C40.0396 (19)0.054 (2)0.039 (2)−0.002 (2)0.0012 (19)−0.012 (2)
C50.0446 (19)0.036 (2)0.025 (2)−0.0101 (18)0.0075 (17)−0.0088 (17)
C60.069 (3)0.054 (3)0.038 (3)−0.006 (2)0.015 (2)0.004 (2)
C70.104 (4)0.052 (3)0.050 (3)−0.021 (3)0.016 (3)0.004 (2)
C80.056 (3)0.109 (4)0.040 (3)−0.035 (3)0.010 (2)−0.009 (3)
C90.053 (2)0.082 (3)0.037 (3)−0.007 (3)−0.005 (2)0.000 (2)
C100.043 (2)0.053 (2)0.047 (2)−0.004 (2)0.019 (2)−0.003 (2)
C110.070 (3)0.056 (2)0.034 (2)−0.005 (2)0.003 (2)0.012 (2)
C120.059 (3)0.089 (3)0.035 (3)0.021 (3)−0.017 (2)−0.003 (3)
C130.061 (3)0.053 (3)0.065 (3)0.001 (2)0.000 (3)−0.002 (2)
C140.041 (2)0.059 (3)0.045 (3)−0.002 (2)−0.002 (2)−0.004 (2)
C150.036 (2)0.043 (2)0.048 (3)−0.0017 (19)−0.0012 (19)−0.005 (2)
C160.070 (3)0.062 (3)0.038 (3)0.003 (3)−0.002 (2)−0.004 (2)
C170.107 (4)0.074 (3)0.046 (3)0.024 (3)−0.010 (3)−0.021 (3)
C180.056 (3)0.045 (3)0.096 (4)0.001 (2)0.006 (3)−0.020 (3)
C190.084 (3)0.061 (3)0.075 (4)0.005 (3)0.024 (3)0.017 (3)
C200.078 (3)0.056 (3)0.041 (3)0.020 (3)0.003 (2)0.001 (2)
Cu10.0384 (2)0.0409 (2)0.0304 (3)0.0049 (2)−0.0006 (2)−0.0023 (2)
N10.0378 (17)0.0514 (19)0.043 (2)−0.0065 (17)0.0017 (15)−0.0093 (17)
N20.0329 (16)0.0449 (19)0.042 (2)−0.0031 (16)−0.0029 (15)−0.0020 (16)
Cu1—Br12.3522 (7)C9—H90.9300
Cu1—Br22.3912 (7)C10—H100.9300
Cu1—Br32.3764 (7)C11—N21.480 (5)
Cu1—Br42.3378 (7)C11—H11A0.9600
C1—N11.461 (5)C11—H11B0.9600
C1—H1A0.9600C11—H11C0.9600
C1—H1B0.9600C12—N21.515 (5)
C1—H1C0.9600C12—H12A0.9600
C2—N11.463 (6)C12—H12B0.9600
C2—H2A0.9600C12—H12C0.9600
C2—H2B0.9600C13—N21.420 (6)
C2—H2C0.9600C13—H13A0.9600
C3—N11.471 (6)C13—H13B0.9600
C3—H3A0.9600C13—H13C0.9600
C3—H3B0.9600C14—N21.509 (5)
C3—H3C0.9600C14—C151.525 (6)
C4—N11.485 (5)C14—H14A0.9700
C4—C51.499 (5)C14—H14B0.9700
C4—H4A0.9700C15—C201.390 (6)
C4—H4B0.9700C15—C161.403 (6)
C5—C101.374 (5)C16—C171.398 (7)
C5—C61.404 (6)C16—H160.9300
C6—C71.411 (7)C17—C181.353 (7)
C6—H60.9300C17—H170.9300
C7—C81.340 (7)C18—C191.373 (8)
C7—H70.9300C18—H180.9300
C8—C91.352 (7)C19—C201.400 (7)
C8—H80.9300C19—H190.9300
C9—C101.460 (6)C20—H200.9300
Br4—Cu1—Br199.92 (3)N2—C11—H11C109.5
Br4—Cu1—Br399.29 (3)H11A—C11—H11C109.5
Br1—Cu1—Br3130.85 (3)H11B—C11—H11C109.5
Br4—Cu1—Br2132.53 (3)N2—C12—H12A109.5
Br1—Cu1—Br299.62 (3)N2—C12—H12B109.5
Br3—Cu1—Br299.72 (3)H12A—C12—H12B109.5
N1—C1—H1A109.5N2—C12—H12C109.5
N1—C1—H1B109.5H12A—C12—H12C109.5
H1A—C1—H1B109.5H12B—C12—H12C109.5
N1—C1—H1C109.5N2—C13—H13A109.5
H1A—C1—H1C109.5N2—C13—H13B109.5
H1B—C1—H1C109.5H13A—C13—H13B109.5
N1—C2—H2A109.5N2—C13—H13C109.5
N1—C2—H2B109.5H13A—C13—H13C109.5
H2A—C2—H2B109.5H13B—C13—H13C109.5
N1—C2—H2C109.5N2—C14—C15114.8 (3)
H2A—C2—H2C109.5N2—C14—H14A108.6
H2B—C2—H2C109.5C15—C14—H14A108.6
N1—C3—H3A109.5N2—C14—H14B108.6
N1—C3—H3B109.5C15—C14—H14B108.6
H3A—C3—H3B109.5H14A—C14—H14B107.5
N1—C3—H3C109.5C20—C15—C16121.6 (4)
H3A—C3—H3C109.5C20—C15—C14118.3 (4)
H3B—C3—H3C109.5C16—C15—C14120.1 (4)
N1—C4—C5115.4 (3)C17—C16—C15117.1 (4)
N1—C4—H4A108.4C17—C16—H16121.4
C5—C4—H4A108.4C15—C16—H16121.4
N1—C4—H4B108.4C18—C17—C16121.5 (5)
C5—C4—H4B108.4C18—C17—H17119.3
H4A—C4—H4B107.5C16—C17—H17119.3
C10—C5—C6121.1 (4)C17—C18—C19121.2 (5)
C10—C5—C4119.8 (4)C17—C18—H18119.4
C6—C5—C4119.0 (4)C19—C18—H18119.4
C5—C6—C7117.8 (4)C18—C19—C20119.8 (5)
C5—C6—H6121.1C18—C19—H19120.1
C7—C6—H6121.1C20—C19—H19120.1
C8—C7—C6120.6 (5)C15—C20—C19118.5 (4)
C8—C7—H7119.7C15—C20—H20120.7
C6—C7—H7119.7C19—C20—H20120.7
C7—C8—C9124.1 (5)C1—N1—C2108.4 (4)
C7—C8—H8118.0C1—N1—C3108.9 (4)
C9—C8—H8118.0C2—N1—C3110.7 (4)
C8—C9—C10117.1 (4)C1—N1—C4108.6 (3)
C8—C9—H9121.4C2—N1—C4109.7 (3)
C10—C9—H9121.4C3—N1—C4110.5 (3)
C5—C10—C9119.3 (4)C13—N2—C11112.2 (3)
C5—C10—H10120.3C13—N2—C14107.8 (3)
C9—C10—H10120.3C11—N2—C14108.9 (3)
N2—C11—H11A109.5C13—N2—C12109.5 (3)
N2—C11—H11B109.5C11—N2—C12107.9 (3)
H11A—C11—H11B109.5C14—N2—C12110.5 (3)
D—H···AD—HH···AD···AD—H···A
C8—H8···Br3i0.932.903.737 (5)150
C12—H12A···Br4ii0.962.893.781 (5)155
C12—H12C···Br4iii0.962.933.794 (5)151
Table 1

Selected bond lengths (Å)

Cu1—Br12.3522 (7)
Cu1—Br22.3912 (7)
Cu1—Br32.3764 (7)
Cu1—Br42.3378 (7)
Table 2

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
C8—H8⋯Br3i0.932.903.737 (5)150
C12—H12A⋯Br4ii0.962.893.781 (5)155
C12—H12C⋯Br4iii0.962.933.794 (5)151

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

  3 in total

1.  Synthesis and crystal structures of (C(5)H(7)N(3)Br)(3)CuBr(4) and (C(5)H(8)N(3))CuBr(2): an isolated tetrahedral CuBr(4)(3-) anion.

Authors:  S H Liu; J D Chen; L S Liou; J C Wang
Journal:  Inorg Chem       Date:  2001-12-03       Impact factor: 5.165

2.  Crystal Structures and Magnetic Properties of a Novel Layer Perovskite System: (3-Picoliniumylammonium)CuX(4) (X = Cl, Br).

Authors:  Greg S. Long; Mingyi Wei; Roger D. Willett
Journal:  Inorg Chem       Date:  1997-07-02       Impact factor: 5.165

3.  A short history of SHELX.

Authors:  George M Sheldrick
Journal:  Acta Crystallogr A       Date:  2007-12-21       Impact factor: 2.290

  3 in total
  3 in total

1.  Benzyl-triethyl-ammonium aqua-trichlorido-zincate.

Authors:  Lei Jin
Journal:  Acta Crystallogr Sect E Struct Rep Online       Date:  2011-11-19

2.  Bis(benzyl-trimethyl-ammonium) dichromate(VI).

Authors:  Lei Jin; Ning Liu
Journal:  Acta Crystallogr Sect E Struct Rep Online       Date:  2011-10-22

3.  Tetrabromidocuprates(II)-Synthesis, Structure and EPR.

Authors:  André Zabel; Alette Winter; Alexandra Kelling; Uwe Schilde; Peter Strauch
Journal:  Int J Mol Sci       Date:  2016-04-20       Impact factor: 5.923

  3 in total

北京卡尤迪生物科技股份有限公司 © 2022-2023.