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bv2140 scheme

Acta Cryst. (2010). E66, o1060    [ doi:10.1107/S1600536810012511 ]

Biphenyl-3,3',4,4'-tetraamine

H.-F. Qian and W. Huang

Abstract top

The title compound, C12H14N4, has a crystallographically imposed centre of symmetry. Intermolecular N-H...N hydrogen bonds between amino groups link adjacent molecules into a three-dimensional network where ten-membered hydrogen-bonded rings are observed.

Comment top

The crystal structure of 3,3',4,4'-tetrammoniobiphenyl tetrachloride dihydrate (Dobrzycki & Wozniak, 2007) has been reported in literature. In this paper, we report the X-ray single-crystal structure of 3,3',4,4'-tetrammoniobiphenyl (I).

The molecular structure of (I) is illustrated in Fig. 1. Two amino groups in the 3-position lie in the opposite sides of the molecular plane. The dihedral angle between phenyl rings of adjacent molecules is 86.3 (2)°. Intermolecular N—H···N hydrogen bonds between amino groups link adjacent molecules into a three-dimensional network, where ten-membered hydrogen-bonded rings are observed (Fig. 2).

Related literature top

For a related compound, see: Dobrzycki & Wozniak (2007).

Experimental top

The title compound was purchased directly from TCI. Single crystals suitable for X-ray diffraction were grown from a methanol solution by slow evaporation in air at room temperature for one week.

Refinement top

H atoms were placed in geometrically idealized positions and refined as riding, with C—H = 0.93 Å and N—H = 0.86–0.90 Å, and with Uiso(H) = 1.2Ueq(C,N).

Computing details top

Data collection: SMART (Bruker, 2000); cell refinement: SMART (Bruker, 2000); data reduction: SAINT (Bruker, 2000); program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. The molecular structure of the title compound with the atom-numbering scheme. Displacement ellipsoids are drawn at the 30% probability level.
[Figure 2] Fig. 2. Perspective view of the hydrogen bonding interactions in the crystal packing of (I), where the hydrogen bonds are shown as dashed lines. [Symmetry codes: (i) -x, -y + 2, -z; (ii) -x, y - 1/2, -z + 1/2.]
Biphenyl-3,3',4,4'-tetraamine top
Crystal data top
C12H14N4F(000) = 228
Mr = 214.27Dx = 1.280 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 931 reflections
a = 9.646 (4) Åθ = 2.5–27.0°
b = 7.476 (3) ŵ = 0.08 mm1
c = 7.751 (3) ÅT = 291 K
β = 95.773 (5)°Block, colourless
V = 556.1 (4) Å30.14 × 0.12 × 0.10 mm
Z = 2
Data collection top
Bruker SMART 1K CCD area-detector
diffractometer
979 independent reflections
Radiation source: fine-focus sealed tube724 reflections with I > 2σ(I)
graphiteRint = 0.075
ω scansθmax = 25.0°, θmin = 2.1°
Absorption correction: multi-scan
(SADABS; Bruker, 2000)
h = 911
Tmin = 0.989, Tmax = 0.992k = 68
2698 measured reflectionsl = 89
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.051Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.156H-atom parameters constrained
S = 1.09 w = 1/[σ2(Fo2) + (0.0926P)2 + 0.0016P]
where P = (Fo2 + 2Fc2)/3
979 reflections(Δ/σ)max < 0.001
73 parametersΔρmax = 0.18 e Å3
0 restraintsΔρmin = 0.30 e Å3
Crystal data top
C12H14N4V = 556.1 (4) Å3
Mr = 214.27Z = 2
Monoclinic, P21/cMo Kα radiation
a = 9.646 (4) ŵ = 0.08 mm1
b = 7.476 (3) ÅT = 291 K
c = 7.751 (3) Å0.14 × 0.12 × 0.10 mm
β = 95.773 (5)°
Data collection top
Bruker SMART 1K CCD area-detector
diffractometer
979 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2000)
724 reflections with I > 2σ(I)
Tmin = 0.989, Tmax = 0.992Rint = 0.075
2698 measured reflectionsθmax = 25.0°
Refinement top
R[F2 > 2σ(F2)] = 0.051H-atom parameters constrained
wR(F2) = 0.156Δρmax = 0.18 e Å3
S = 1.09Δρmin = 0.30 e Å3
979 reflectionsAbsolute structure: ?
73 parametersFlack parameter: ?
0 restraintsRogers parameter: ?
Special details top

Experimental. The structure was solved by direct methods (Bruker, 2000) and successive difference Fourier syntheses.

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.42719 (17)0.9895 (2)0.4590 (2)0.0335 (5)
C20.37707 (18)1.0872 (2)0.3125 (2)0.0356 (5)
H20.43781.16390.26290.043*
C30.24074 (18)1.0749 (2)0.2378 (2)0.0336 (5)
C40.14684 (18)0.9615 (2)0.3120 (2)0.0341 (5)
C50.1965 (2)0.8586 (2)0.4523 (2)0.0391 (6)
H50.13670.77850.49910.047*
C60.3330 (2)0.8714 (3)0.5255 (2)0.0421 (6)
H60.36290.80030.62050.051*
N10.18955 (16)1.1838 (2)0.0986 (2)0.0442 (5)
H1A0.15151.11300.01270.053*
H1B0.24371.26000.05620.053*
N20.00747 (15)0.9522 (2)0.23637 (19)0.0418 (5)
H2A0.04840.91670.31610.050*
H2B0.01301.06510.20250.050*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0327 (11)0.0338 (10)0.0336 (10)0.0017 (8)0.0013 (8)0.0006 (8)
C20.0326 (11)0.0381 (11)0.0362 (10)0.0008 (8)0.0043 (8)0.0023 (8)
C30.0355 (11)0.0348 (10)0.0300 (9)0.0026 (8)0.0004 (8)0.0012 (7)
C40.0327 (11)0.0353 (10)0.0337 (10)0.0013 (8)0.0007 (8)0.0053 (8)
C50.0376 (12)0.0392 (11)0.0397 (11)0.0082 (8)0.0003 (9)0.0049 (8)
C60.0422 (12)0.0420 (11)0.0404 (11)0.0036 (9)0.0046 (9)0.0092 (8)
N10.0434 (11)0.0480 (10)0.0396 (10)0.0045 (7)0.0033 (8)0.0113 (7)
N20.0324 (10)0.0493 (11)0.0424 (10)0.0036 (7)0.0026 (7)0.0017 (7)
Geometric parameters (Å, °) top
C1—C21.395 (3)C4—N21.413 (2)
C1—C61.401 (3)C5—C61.384 (3)
C1—C1i1.491 (3)C5—H50.9300
C2—C31.386 (2)C6—H60.9300
C2—H20.9300N1—H1A0.8999
C3—N11.401 (2)N1—H1B0.8600
C3—C41.405 (2)N2—H2A0.9000
C4—C51.379 (3)N2—H2B0.9000
C2—C1—C6116.41 (17)C4—C5—C6121.72 (17)
C2—C1—C1i121.8 (2)C4—C5—H5119.1
C6—C1—C1i121.8 (2)C6—C5—H5119.1
C3—C2—C1122.83 (17)C5—C6—C1121.21 (18)
C3—C2—H2118.6C5—C6—H6119.4
C1—C2—H2118.6C1—C6—H6119.4
C2—C3—N1121.97 (16)C3—N1—H1A108.3
C2—C3—C4119.50 (16)C3—N1—H1B119.9
N1—C3—C4118.29 (16)H1A—N1—H1B108.9
C5—C4—C3118.20 (17)C4—N2—H2A109.9
C5—C4—N2122.70 (16)C4—N2—H2B104.2
C3—C4—N2119.05 (16)H2A—N2—H2B110.4
C6—C1—C2—C32.1 (3)N1—C3—C4—N24.4 (2)
C1i—C1—C2—C3177.55 (18)C3—C4—C5—C63.2 (3)
C1—C2—C3—N1175.14 (17)N2—C4—C5—C6179.28 (17)
C1—C2—C3—C40.8 (3)C4—C5—C6—C10.3 (3)
C2—C3—C4—C53.4 (3)C2—C1—C6—C52.3 (3)
N1—C3—C4—C5177.99 (15)C1i—C1—C6—C5177.30 (19)
C2—C3—C4—N2178.99 (15)
Symmetry codes: (i) −x+1, −y+2, −z+1.
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
N1—H1A···N2ii0.902.393.224 (2)154
N2—H2A···N1iii0.902.353.124 (2)145
Symmetry codes: (ii) −x, −y+2, −z; (iii) −x, y−1/2, −z+1/2.
Table 1
Selected geometric parameters (Å)
top
C3—N11.401 (2)C4—N21.413 (2)
Table 2
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
N1—H1A···N2i0.902.393.224 (2)154
N2—H2A···N1ii0.902.353.124 (2)145
Symmetry codes: (i) −x, −y+2, −z; (ii) −x, y−1/2, −z+1/2.
Acknowledgements top

WH acknowledges the National Natural Science Foundation of China (grant No. 20871065) and the Jiangsu Province Department of Science and Technology (grant No. BK2009226) for financial aid.

references
References top

Bruker (2000). SMART, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.

Dobrzycki, L. & Wozniak, K. (2007). CrystEngComm, 9, 1029–1040.

Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.