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In the title compound, C14H10N4, all the atoms are close to being coplanar (r.m.s. deviation 0.0098 Å) except for the imino H atoms. The mol­ecule forms a one-dimensional chain through intermolecular N-H...N hydrogen bonds.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270100014761/qa0384sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270100014761/qa0384Isup2.hkl
Contains datablock I

CCDC reference: 156221

Comment top

The title compound, (I), is well known to act as a bridging ligand in transition metal compounds (Fieselmann et al., 1978; Haga et al., 1987). The asymmetric unit contains one quarter of the molecule and the other parts are twofold-rotation and mirror related. The rotation axis passes through the centre of the C1—C1' bond, while the mirror contains this bond. The occupancy of the imino H1 atom was set at 0.5 due to the mirror symmetry operation. The average bond distances and angles for the benzimidazole moiety are in good agreement with those of other substituted bis-benzimidazole compounds (Matthews et al., 1996; Ozbey et al., 1998; Bei et al., 2000). \scheme

The C1—C1' bond length of 1.435 (5) Å is close to the value for a single-bond length between trigonally linked C atoms (Cruickshank & Sparks, 1960; Bei et al., 2000). The molecule forms a one-dimensional chain through N1—H1···N1(x, −y, −1/2 − z) intermolecular hydrogen bonds.

Experimental top

The title compound was prepared from 1,2-diaminobenzene and oxamide according to the method of Fieselmann et al. (1978). Single crystals suitable for X-ray measurement were obtained by slow evaporation at room temperature from an ethylene glycol solution.

Refinement top

All the H atoms were located from the difference Fourier map and refined isotropically. The C—H range is 0.92 (3)–1.01 (2) Å and the N—H distance is 0.94 (4) Å.

Computing details top

Data collection: MSC/AFC Diffractometer Control Software (Molecular Structure Corporation, 1990); cell refinement: MSC/AFC Diffractometer Control Software; data reduction: TEXSAN (Molecular Structure Corporation and Rigaku Corporation, 1999); program(s) used to solve structure: SIR92 (Altomare et al., 1993); program(s) used to refine structure: TEXSAN; software used to prepare material for publication: TEXSAN.

(I) top
Crystal data top
C14H10N4Dx = 1.354 Mg m3
Mr = 234.26Mo Kα radiation, λ = 0.7107 Å
Orthorhombic, IbamCell parameters from 25 reflections
Hall symbol: -I 2 2cθ = 12.4–14.9°
a = 11.331 (3) ŵ = 0.09 mm1
b = 10.183 (2) ÅT = 296 K
c = 9.962 (2) ÅPrismatic, yellow
V = 1149.4 (4) Å30.30 × 0.10 × 0.10 mm
Z = 4
Data collection top
Rigaku AFC-5R
diffractometer
Rint = 0.015
ω–2θ scansθmax = 27.5°
Absorption correction: ψ scan
(North et al., 1968)
h = 114
Tmin = 0.937, Tmax = 0.996k = 113
985 measured reflectionsl = 112
703 independent reflections3 standard reflections every 150 reflections
321 reflections with I > 2σ(I) intensity decay: 0.6%
Refinement top
Refinement on F2All H-atom parameters refined
R[F2 > 2σ(F2)] = 0.043 w = 1/[σ2(Fo2) + (0.045(Max(Fo2,0) + 2Fc2)/3)2]
wR(F2) = 0.127(Δ/σ)max = 0.004
S = 1.06Δρmax = 0.48 e Å3
703 reflectionsΔρmin = 0.43 e Å3
55 parameters
Crystal data top
C14H10N4V = 1149.4 (4) Å3
Mr = 234.26Z = 4
Orthorhombic, IbamMo Kα radiation
a = 11.331 (3) ŵ = 0.09 mm1
b = 10.183 (2) ÅT = 296 K
c = 9.962 (2) Å0.30 × 0.10 × 0.10 mm
Data collection top
Rigaku AFC-5R
diffractometer
321 reflections with I > 2σ(I)
Absorption correction: ψ scan
(North et al., 1968)
Rint = 0.015
Tmin = 0.937, Tmax = 0.9963 standard reflections every 150 reflections
985 measured reflections intensity decay: 0.6%
703 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.04355 parameters
wR(F2) = 0.127All H-atom parameters refined
S = 1.06Δρmax = 0.48 e Å3
703 reflectionsΔρmin = 0.43 e Å3
Special details top

Refinement. Refinement using reflections with F2 > 0.0 σ(F2). The weighted R-factor (wR) and goodness of fit (S) are based on F2. R-factor (gt) are based on F. The threshold expression of F2 > 2.0 σ(F2) is used only for calculating R-factor (gt).

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/UeqOcc. (<1)
N10.8799 (1)0.0477 (2)0.1130 (2)0.0569 (6)
C10.9404 (2)0.0241 (3)0.00000.0504 (10)
C20.7704 (2)0.0931 (2)0.0694 (2)0.0513 (6)
C30.6723 (2)0.1345 (3)0.1406 (3)0.0743 (9)
C40.5757 (2)0.1744 (3)0.0691 (3)0.0669 (8)
H10.897 (3)0.008 (4)0.196 (4)0.046 (10)*0.50
H20.674 (2)0.137 (3)0.233 (3)0.102 (9)*
H30.503 (2)0.205 (2)0.119 (2)0.076 (7)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.045 (1)0.082 (2)0.045 (1)0.009 (1)0.0070 (9)0.000 (1)
C10.042 (2)0.052 (2)0.057 (2)0.006 (1)0.00000.0000
C20.045 (1)0.057 (1)0.052 (1)0.003 (1)0.001 (1)0.000 (1)
C30.060 (1)0.105 (2)0.058 (2)0.022 (1)0.008 (1)0.005 (2)
C40.050 (1)0.077 (2)0.074 (2)0.017 (1)0.007 (1)0.001 (1)
Geometric parameters (Å, º) top
N1—C11.339 (2)C2—C31.385 (3)
N1—C21.394 (3)C3—C41.367 (4)
N1—H10.94 (4)C3—H20.92 (3)
C1—C1i1.436 (6)C4—C4ii1.377 (5)
C2—C2ii1.382 (4)C4—H31.01 (2)
N1···H3iii2.88 (2)C2···H3iii3.38 (2)
N1···N1iv2.898 (4)C2···H2xii3.44 (3)
N1···H1v3.19 (3)C3···H2iv3.04 (3)
N1···H2iv3.37 (3)C3···H2xii3.17 (3)
C1···H1vi2.70 (3)C3···H3xiii3.20 (2)
C1···H3vii3.09 (2)C3···H1iv3.36 (3)
C1···H3iii3.09 (2)C3···C3iv3.501 (6)
C1···H1iv3.09 (4)C4···H3xiii3.25 (2)
C1···H1viii3.09 (4)C4···H2xiii3.47 (3)
C1···C4vii3.500 (4)H1···H1v2.56 (6)
C1···C4iii3.500 (4)H1···H2iv3.02 (4)
C1···H3ix3.52 (2)H1···H3iii3.25 (5)
C1···H3x3.52 (2)H1···H3x3.37 (5)
C1···H1v3.55 (4)H2···H3xiii2.59 (4)
C1···H1xi3.55 (4)H2···H2iv2.81 (5)
C1···C2vi3.555 (4)H2···H2xii2.89 (5)
C2···H1iv2.93 (3)H3···H3xiii2.61 (4)
C2···H2iv3.25 (3)
C1—N1—C2104.7 (2)C2ii—C2—C3120.8 (1)
C1—N1—H1123 (2)C2—C3—C4117.8 (2)
C2—N1—H1127 (1)C2—C3—H2120 (1)
N1—C1—N1ii114.3 (3)C4—C3—H2121 (1)
N1—C1—C1i122.8 (1)C3—C4—C4ii121.4 (2)
N1—C1ii—C1i122.8 (1)C3—C4—H3119 (1)
N1—C2—C2ii108.2 (1)C4ii—C4—H3119 (1)
N1—C2—C3131.0 (2)
N1—C1—N1ii—C2ii1.1 (3)C1—N1—C2—C3179.0 (3)
N1—C1—C1i—N1i0.9 (7)C1—N1ii—C2ii—C20.6 (2)
N1—C1—C1i—N1vi180.0C1—N1ii—C2ii—C3ii179.0 (3)
N1—C2—C2ii—N1ii0.0C2—C2ii—C3ii—C4ii0.4 (3)
N1—C2—C2ii—C3ii179.6 (3)C2—C3—C4—C4ii0.4 (3)
N1—C2—C3—C4179.9 (2)C3—C2—C2ii—C3ii0.0
C1—N1—C2—C2ii0.6 (2)C3—C4—C4ii—C3ii0.0
Symmetry codes: (i) x+2, y, z; (ii) x, y, z; (iii) x+1/2, y+1/2, z; (iv) x, y, z1/2; (v) x+2, y, z1/2; (vi) x+2, y, z; (vii) x+1/2, y+1/2, z; (viii) x, y, z+1/2; (ix) x+3/2, y1/2, z; (x) x+3/2, y1/2, z; (xi) x+2, y, z+1/2; (xii) x+3/2, y+1/2, z1/2; (xiii) x+1, y, z1/2.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···N1iv0.94 (4)1.99 (4)2.897 (3)160 (3)
Symmetry code: (iv) x, y, z1/2.

Experimental details

Crystal data
Chemical formulaC14H10N4
Mr234.26
Crystal system, space groupOrthorhombic, Ibam
Temperature (K)296
a, b, c (Å)11.331 (3), 10.183 (2), 9.962 (2)
V3)1149.4 (4)
Z4
Radiation typeMo Kα
µ (mm1)0.09
Crystal size (mm)0.30 × 0.10 × 0.10
Data collection
DiffractometerRigaku AFC-5R
diffractometer
Absorption correctionψ scan
(North et al., 1968)
Tmin, Tmax0.937, 0.996
No. of measured, independent and
observed [I > 2σ(I)] reflections
985, 703, 321
Rint0.015
(sin θ/λ)max1)0.650
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.043, 0.127, 1.06
No. of reflections703
No. of parameters55
No. of restraints?
H-atom treatmentAll H-atom parameters refined
Δρmax, Δρmin (e Å3)0.48, 0.43

Computer programs: MSC/AFC Diffractometer Control Software (Molecular Structure Corporation, 1990), MSC/AFC Diffractometer Control Software, TEXSAN (Molecular Structure Corporation and Rigaku Corporation, 1999), SIR92 (Altomare et al., 1993), TEXSAN.

Selected geometric parameters (Å, º) top
N1—C11.339 (2)C2—C31.385 (3)
N1—C21.394 (3)C3—C41.367 (4)
C1—C1i1.436 (6)C4—C4ii1.377 (5)
C2—C2ii1.382 (4)
C1—N1—C2104.7 (2)N1—C1—C1i122.8 (1)
N1—C1—N1ii114.3 (3)N1—C1ii—C1i122.8 (1)
Symmetry codes: (i) x+2, y, z; (ii) x, y, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1···N1iii0.94 (4)1.99 (4)2.897 (3)160 (3)
Symmetry code: (iii) x, y, z1/2.
 

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