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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2012 Apr 28;68(Pt 5):o1553. doi: 10.1107/S1600536812016728

1,4-Bis[4-(meth­oxy­carbon­yl)benz­yl]-1H-1,2,4-triazol-4-ium bromide

Wen-Jiao Guo a, Hua-Rong Huang a,*, Zhi-Yun Du a, Yan-Xiong Fang a, Kun Zhang a
PMCID: PMC3344652  PMID: 22590414

Abstract

In the title salt, C20H20N3O4 +·Br, the dihedral angle between the benzene rings is 8.69 (16)°, and those between the benzene rings and the triazole ring are 69.98 (18) and 72.17 (18)°. In the crystal, C—H⋯Br hydrogen bonds link the cations and anions into chains along the c axis.

Related literature  

For general background to triazole derivatives, see: Zanardi et al. (2011). For a related structure, see: Huang et al. (2010).graphic file with name e-68-o1553-scheme1.jpg

Experimental  

Crystal data  

  • C20H20N3O4 +·Br

  • M r = 446.30

  • Orthorhombic, Inline graphic

  • a = 33.6880 (15) Å

  • b = 4.7962 (3) Å

  • c = 12.3337 (6) Å

  • V = 1992.81 (18) Å3

  • Z = 4

  • Cu Kα radiation

  • μ = 3.08 mm−1

  • T = 173 K

  • 0.40 × 0.32 × 0.31 mm

Data collection  

  • Oxford Diffraction Xcalibur Atlas Gemini Ultra diffractometer

  • Absorption correction: multi-scan (ABSPACK in CrysAlis PRO; Oxford Diffraction, 2006) T min = 0.372, T max = 0.449

  • 6375 measured reflections

  • 2709 independent reflections

  • 2541 reflections with I > 2σ(I)

  • R int = 0.027

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.027

  • wR(F 2) = 0.069

  • S = 1.05

  • 2709 reflections

  • 255 parameters

  • 1 restraint

  • H-atom parameters constrained

  • Δρmax = 0.37 e Å−3

  • Δρmin = −0.24 e Å−3

  • Absolute structure: Flack (1983), 840 Friedel pairs

  • Flack parameter: 0.021 (18)

Data collection: CrysAlis PRO (Oxford Diffraction, 2006); cell refinement: CrysAlis PRO; data reduction: CrysAlis PRO; 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: WinGX (Farrugia, 1999) and PLATON (Spek, 2009).

Supplementary Material

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812016728/ng5263sup1.cif

e-68-o1553-sup1.cif (21.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812016728/ng5263Isup2.hkl

e-68-o1553-Isup2.hkl (133KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812016728/ng5263Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
C1—H1⋯Br1 0.95 2.61 3.461 (3) 149
C3—H3A⋯Br1 0.99 2.91 3.795 (4) 149
C2—H2⋯Br1i 0.95 2.75 3.657 (3) 161

Symmetry code: (i) Inline graphic.

Acknowledgments

This work was funded by the 211 Project of Guangdong Province.

supplementary crystallographic information

Comment

1H-1,2,4-Triazole, like imidazole and benzimidazole, can be N-alkylated to form N-heterocyclic carbine (Zanardi et al., 2011).

In an earlier report, we presented a N-heterocyclic benzimidazole derivative. The crystal structure consists of infinite chains connected via C—H···Br and C—H···O hydrogen bonds; it also shows π···π stacking interactions (Huang et al., 2010).

In this work, we report the structure of a triazole-based N-heterocyclic carbene, 1,4-bis[4-(methoxycarbonyl)benzyl]-1H-1,2,4-triazolium bromide (Fig. 1).

In the crystal structure, the dihedral angles between the triazole ring system and the two (C4–C9) and (C13–C18) benzene rings are 69.98 (18) ° and 72.17 (18) °, respectively; the dihedral angle between the two benzene rings is 8.69 (16) °.

The bromide anions and cations form infinite hydrogen bonding chains along the c-axis via C—H···Br hydrogen bonds between the bromide anions and carbineen atoms of triazole ring and ethylene linkage (Fig. 2, Table 1).

Experimental

4-(Methoxycarbonyl)benzyl bromide (2.28 g, 10.0 mmol) was slowly added to a solution of 1H-1,2,4-triazole (0.35 g, 5.0 mmol) in acetonitrile (25 ml) and the resulting mixture was stirred under reflux for 8 h.

The solvent was evaporated under reduced pressure. The solid residue was recrystallized in methanol, and colorless block crystals were obtained after few days, yield 1.42 g, 63.5%.

Elemental analysis, calcd (%) for C20H20N3BrO4: C 53.82, H 4.52, N 9.42; found(%): C 53.80, H 4.60, N 9.41.

The FAB mass spectrum showed tje ions at 447.

Refinement

The C-bound H atoms were positioned geometrically and were included in the refinement in the riding-model approximation, with distances 0.98 (CH3), 0.99 (CH2) and 0.95 Å (aromatic and triazole); Uiso(H) = xUeq(attached atom), where x = 1.5 for methyl C and 1.2 for all other C.

Figures

Fig. 1.

Fig. 1.

Perspective view showing 30% probability displacement ellipsoids and the atom-numbering scheme.

Fig. 2.

Fig. 2.

Crystal packing of the title compound. Dashed lines indicate hydrogen bonds. Symmetry: I = -x + 1, -y + 1, z + 1/2; II = -x + 1, -y + 2, z + 1/2. H atoms not involved in the hydrogen bond interactions have been omitted.

Crystal data

C20H20N3O4+·Br Dx = 1.488 Mg m3
Mr = 446.30 Cu Kα radiation, λ = 1.5418 Å
Orthorhombic, Pca21 Cell parameters from 3691 reflections
a = 33.6880 (15) Å θ = 3.6–66.9°
b = 4.7962 (3) Å µ = 3.08 mm1
c = 12.3337 (6) Å T = 173 K
V = 1992.81 (18) Å3 Block, colorless
Z = 4 0.40 × 0.32 × 0.31 mm
F(000) = 912

Data collection

Oxford Diffraction Xcalibur Atlas Gemini Ultra diffractometer 2709 independent reflections
Radiation source: Enhance Ultra (Cu) X-ray Source 2541 reflections with I > 2σ(I)
Mirror monochromator Rint = 0.027
Detector resolution: 10.5058 pixels mm-1 θmax = 66.9°, θmin = 4.4°
φ and ω scans h = −40→39
Absorption correction: multi-scan (ABSPACK in CrysAlis PRO; Oxford Diffraction, 2006) k = −5→4
Tmin = 0.372, Tmax = 0.449 l = −11→14
6375 measured reflections

Refinement

Refinement on F2 Secondary atom site location: difference Fourier map
Least-squares matrix: full Hydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.027 H-atom parameters constrained
wR(F2) = 0.069 w = 1/[σ2(Fo2) + (0.0373P)2 + 0.0837P] where P = (Fo2 + 2Fc2)/3
S = 1.05 (Δ/σ)max < 0.001
2709 reflections Δρmax = 0.37 e Å3
255 parameters Δρmin = −0.24 e Å3
1 restraint Absolute structure: Flack (1983), 840 Friedel pairs
Primary atom site location: structure-invariant direct methods Flack parameter: 0.021 (18)

Special details

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)

x y z Uiso*/Ueq
C1 0.47864 (8) 0.6564 (6) 0.2417 (3) 0.0375 (7)
H1 0.4887 0.7596 0.1819 0.045*
C2 0.47240 (9) 0.3718 (7) 0.3756 (3) 0.0452 (7)
H2 0.4788 0.2350 0.4285 0.054*
C3 0.40894 (9) 0.8422 (7) 0.2458 (3) 0.0480 (8)
H3A 0.4184 0.9793 0.1917 0.058*
H3B 0.3980 0.9465 0.3083 0.058*
C4 0.37667 (8) 0.6644 (6) 0.1961 (3) 0.0441 (7)
C5 0.34867 (10) 0.5364 (9) 0.2611 (3) 0.0554 (9)
H5 0.3490 0.5665 0.3373 0.067*
C6 0.32036 (11) 0.3655 (9) 0.2160 (3) 0.0599 (10)
H6 0.3017 0.2741 0.2616 0.072*
C7 0.31867 (9) 0.3249 (7) 0.1051 (3) 0.0450 (7)
C8 0.34607 (8) 0.4583 (7) 0.0390 (4) 0.0538 (7)
H8 0.3449 0.4351 −0.0374 0.065*
C9 0.37509 (10) 0.6255 (8) 0.0851 (3) 0.0533 (9)
H9 0.3941 0.7143 0.0399 0.064*
C10 0.28761 (9) 0.1331 (7) 0.0608 (4) 0.0518 (10)
C11 0.26013 (14) −0.0757 (11) −0.0946 (4) 0.0807 (13)
H11A 0.2335 −0.0263 −0.0690 0.121*
H11B 0.2662 −0.2681 −0.0735 0.121*
H11C 0.2612 −0.0592 −0.1737 0.121*
C12 0.53934 (10) 0.3639 (7) 0.2875 (3) 0.0456 (8)
H12A 0.5389 0.2054 0.2361 0.055*
H12B 0.5492 0.2936 0.3580 0.055*
C13 0.56784 (9) 0.5850 (7) 0.2453 (3) 0.0389 (7)
C14 0.59021 (9) 0.7440 (7) 0.3159 (3) 0.0421 (7)
H14 0.5868 0.7241 0.3919 0.051*
C15 0.61770 (9) 0.9330 (7) 0.2758 (3) 0.0454 (7)
H15 0.6334 1.0398 0.3246 0.054*
C16 0.62246 (8) 0.9668 (7) 0.1643 (3) 0.0428 (7)
C17 0.59997 (10) 0.8069 (8) 0.0951 (3) 0.0521 (8)
H17 0.6030 0.8288 0.0190 0.063*
C18 0.57294 (9) 0.6139 (8) 0.1348 (3) 0.0475 (7)
H18 0.5580 0.5021 0.0861 0.057*
C19 0.65221 (11) 1.1610 (8) 0.1181 (4) 0.0541 (10)
C20 0.70101 (11) 1.5049 (8) 0.1569 (5) 0.0781 (14)
H20A 0.7055 1.6461 0.2130 0.117*
H20B 0.6921 1.5960 0.0901 0.117*
H20C 0.7258 1.4045 0.1429 0.117*
N1 0.44256 (8) 0.6675 (5) 0.2823 (2) 0.0398 (6)
N2 0.43770 (8) 0.4859 (7) 0.3659 (2) 0.0497 (8)
N3 0.49824 (8) 0.4702 (6) 0.3018 (2) 0.0345 (5)
O1 0.26382 (8) 0.0139 (6) 0.1165 (3) 0.0724 (8)
O2 0.28892 (9) 0.1106 (6) −0.0466 (3) 0.0679 (7)
O3 0.65877 (9) 1.1836 (7) 0.0219 (3) 0.0767 (10)
O4 0.67098 (7) 1.3101 (5) 0.1933 (3) 0.0648 (7)
Br1 0.479859 (9) 1.16298 (6) 0.04187 (3) 0.04923 (11)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
C1 0.0373 (15) 0.0360 (17) 0.0391 (17) −0.0023 (11) 0.0009 (12) 0.0032 (13)
C2 0.0461 (17) 0.051 (2) 0.0381 (17) −0.0054 (13) −0.0026 (13) 0.0080 (14)
C3 0.0408 (15) 0.0435 (19) 0.060 (2) 0.0051 (13) −0.0021 (15) −0.0033 (15)
C4 0.0349 (14) 0.0423 (18) 0.0550 (19) 0.0042 (11) −0.0035 (14) −0.0035 (15)
C5 0.0490 (18) 0.073 (3) 0.0444 (19) −0.0087 (16) 0.0028 (15) −0.0006 (17)
C6 0.0504 (18) 0.080 (3) 0.050 (2) −0.0217 (17) 0.0059 (16) 0.0001 (18)
C7 0.0335 (14) 0.049 (2) 0.0527 (19) 0.0010 (12) 0.0005 (13) −0.0019 (15)
C8 0.0473 (15) 0.070 (2) 0.0442 (15) −0.0054 (13) 0.006 (2) −0.003 (2)
C9 0.0431 (16) 0.066 (2) 0.0507 (18) −0.0115 (15) 0.0083 (14) 0.0001 (16)
C10 0.0411 (14) 0.0516 (18) 0.063 (3) 0.0008 (13) −0.0052 (17) −0.0019 (19)
C11 0.083 (3) 0.087 (3) 0.072 (3) −0.020 (2) −0.022 (3) −0.009 (3)
C12 0.0394 (16) 0.0411 (18) 0.056 (2) 0.0024 (13) −0.0035 (16) 0.0029 (15)
C13 0.0333 (14) 0.0384 (17) 0.0450 (18) 0.0048 (12) −0.0016 (13) 0.0034 (15)
C14 0.0405 (15) 0.0466 (17) 0.0392 (16) 0.0031 (12) −0.0009 (13) 0.0001 (14)
C15 0.0393 (15) 0.0486 (19) 0.0483 (18) −0.0006 (12) −0.0026 (13) −0.0061 (15)
C16 0.0367 (14) 0.0421 (18) 0.0494 (17) 0.0055 (12) 0.0017 (13) 0.0057 (14)
C17 0.0513 (18) 0.066 (3) 0.0386 (16) −0.0032 (16) −0.0007 (15) 0.0064 (16)
C18 0.0474 (17) 0.055 (2) 0.0405 (17) −0.0066 (13) −0.0061 (14) −0.0029 (15)
C19 0.0439 (17) 0.051 (2) 0.068 (3) 0.0036 (14) 0.0061 (18) 0.0162 (19)
C20 0.0489 (19) 0.049 (2) 0.137 (4) −0.0081 (16) 0.016 (2) 0.009 (2)
N1 0.0370 (12) 0.0420 (16) 0.0402 (14) −0.0050 (10) −0.0018 (12) −0.0007 (11)
N2 0.0437 (14) 0.064 (2) 0.0408 (16) −0.0075 (13) 0.0009 (12) 0.0105 (14)
N3 0.0365 (11) 0.0365 (14) 0.0304 (12) −0.0044 (9) 0.0003 (9) 0.0020 (11)
O1 0.0623 (16) 0.082 (2) 0.0729 (19) −0.0267 (15) 0.0071 (14) −0.0048 (16)
O2 0.0654 (16) 0.0780 (19) 0.0603 (16) −0.0199 (14) −0.0075 (14) −0.0071 (15)
O3 0.0720 (17) 0.087 (2) 0.071 (3) −0.0134 (14) 0.0174 (17) 0.0213 (16)
O4 0.0499 (13) 0.0555 (16) 0.089 (2) −0.0115 (10) 0.0067 (14) 0.0025 (15)
Br1 0.06480 (19) 0.04233 (17) 0.04057 (16) −0.00337 (13) −0.0031 (2) 0.0041 (2)

Geometric parameters (Å, º)

C1—N1 1.316 (4) C11—H11B 0.9800
C1—N3 1.335 (4) C11—H11C 0.9800
C1—H1 0.9500 C12—N3 1.486 (5)
C2—N2 1.296 (4) C12—C13 1.522 (5)
C2—N3 1.345 (4) C12—H12A 0.9900
C2—H2 0.9500 C12—H12B 0.9900
C3—N1 1.479 (4) C13—C18 1.381 (5)
C3—C4 1.512 (4) C13—C14 1.381 (5)
C3—H3A 0.9900 C14—C15 1.387 (5)
C3—H3B 0.9900 C14—H14 0.9500
C4—C5 1.382 (5) C15—C16 1.394 (5)
C4—C9 1.383 (5) C15—H15 0.9500
C5—C6 1.376 (5) C16—C17 1.376 (5)
C5—H5 0.9500 C16—C19 1.482 (5)
C6—C7 1.382 (5) C17—C18 1.388 (5)
C6—H6 0.9500 C17—H17 0.9500
C7—C8 1.388 (5) C18—H18 0.9500
C7—C10 1.497 (5) C19—O3 1.212 (6)
C8—C9 1.386 (5) C19—O4 1.331 (5)
C8—H8 0.9500 C20—O4 1.449 (4)
C9—H9 0.9500 C20—H20A 0.9800
C10—O1 1.200 (5) C20—H20B 0.9800
C10—O2 1.331 (6) C20—H20C 0.9800
C11—O2 1.445 (5) N1—N2 1.359 (4)
C11—H11A 0.9800
N1—C1—N3 105.8 (3) C13—C12—H12A 109.0
N1—C1—H1 127.1 N3—C12—H12B 109.0
N3—C1—H1 127.1 C13—C12—H12B 109.0
N2—C2—N3 111.9 (3) H12A—C12—H12B 107.8
N2—C2—H2 124.1 C18—C13—C14 119.9 (3)
N3—C2—H2 124.1 C18—C13—C12 119.1 (3)
N1—C3—C4 110.8 (3) C14—C13—C12 120.9 (3)
N1—C3—H3A 109.5 C13—C14—C15 120.1 (3)
C4—C3—H3A 109.5 C13—C14—H14 120.0
N1—C3—H3B 109.5 C15—C14—H14 120.0
C4—C3—H3B 109.5 C14—C15—C16 120.3 (3)
H3A—C3—H3B 108.1 C14—C15—H15 119.9
C5—C4—C9 119.3 (3) C16—C15—H15 119.9
C5—C4—C3 120.4 (3) C17—C16—C15 119.0 (3)
C9—C4—C3 120.3 (3) C17—C16—C19 118.9 (3)
C6—C5—C4 120.2 (3) C15—C16—C19 122.0 (3)
C6—C5—H5 119.9 C16—C17—C18 120.9 (3)
C4—C5—H5 119.9 C16—C17—H17 119.5
C5—C6—C7 120.9 (3) C18—C17—H17 119.5
C5—C6—H6 119.6 C13—C18—C17 119.8 (3)
C7—C6—H6 119.6 C13—C18—H18 120.1
C6—C7—C8 119.3 (3) C17—C18—H18 120.1
C6—C7—C10 118.4 (3) O3—C19—O4 123.2 (4)
C8—C7—C10 122.3 (3) O3—C19—C16 123.8 (4)
C9—C8—C7 119.7 (4) O4—C19—C16 113.0 (3)
C9—C8—H8 120.2 O4—C20—H20A 109.5
C7—C8—H8 120.2 O4—C20—H20B 109.5
C4—C9—C8 120.7 (3) H20A—C20—H20B 109.5
C4—C9—H9 119.6 O4—C20—H20C 109.5
C8—C9—H9 119.6 H20A—C20—H20C 109.5
O1—C10—O2 123.6 (4) H20B—C20—H20C 109.5
O1—C10—C7 123.4 (4) C1—N1—N2 112.0 (3)
O2—C10—C7 113.0 (3) C1—N1—C3 127.9 (3)
O2—C11—H11A 109.5 N2—N1—C3 120.1 (3)
O2—C11—H11B 109.5 C2—N2—N1 103.4 (3)
H11A—C11—H11B 109.5 C1—N3—C2 106.9 (3)
O2—C11—H11C 109.5 C1—N3—C12 128.6 (3)
H11A—C11—H11C 109.5 C2—N3—C12 124.2 (3)
H11B—C11—H11C 109.5 C10—O2—C11 115.8 (4)
N3—C12—C13 112.9 (3) C19—O4—C20 117.5 (4)
N3—C12—H12A 109.0
N1—C3—C4—C5 84.0 (4) C14—C13—C18—C17 −1.3 (5)
N1—C3—C4—C9 −95.3 (4) C12—C13—C18—C17 −177.5 (3)
C9—C4—C5—C6 2.0 (6) C16—C17—C18—C13 1.3 (5)
C3—C4—C5—C6 −177.3 (3) C17—C16—C19—O3 −1.9 (6)
C4—C5—C6—C7 −1.8 (6) C15—C16—C19—O3 175.5 (4)
C5—C6—C7—C8 0.2 (6) C17—C16—C19—O4 177.8 (3)
C5—C6—C7—C10 179.1 (3) C15—C16—C19—O4 −4.9 (5)
C6—C7—C8—C9 1.2 (5) N3—C1—N1—N2 −1.9 (4)
C10—C7—C8—C9 −177.6 (3) N3—C1—N1—C3 179.8 (3)
C5—C4—C9—C8 −0.6 (6) C4—C3—N1—C1 111.4 (4)
C3—C4—C9—C8 178.7 (3) C4—C3—N1—N2 −66.8 (4)
C7—C8—C9—C4 −1.0 (5) N3—C2—N2—N1 −0.8 (4)
C6—C7—C10—O1 0.6 (5) C1—N1—N2—C2 1.7 (4)
C8—C7—C10—O1 179.4 (3) C3—N1—N2—C2 −179.8 (3)
C6—C7—C10—O2 −180.0 (4) N1—C1—N3—C2 1.3 (4)
C8—C7—C10—O2 −1.1 (5) N1—C1—N3—C12 175.9 (3)
N3—C12—C13—C18 −90.6 (4) N2—C2—N3—C1 −0.3 (4)
N3—C12—C13—C14 93.2 (4) N2—C2—N3—C12 −175.2 (3)
C18—C13—C14—C15 0.1 (5) C13—C12—N3—C1 35.4 (5)
C12—C13—C14—C15 176.2 (3) C13—C12—N3—C2 −150.9 (3)
C13—C14—C15—C16 1.1 (5) O1—C10—O2—C11 −1.6 (6)
C14—C15—C16—C17 −1.1 (5) C7—C10—O2—C11 178.9 (3)
C14—C15—C16—C19 −178.4 (3) O3—C19—O4—C20 −0.9 (5)
C15—C16—C17—C18 −0.1 (5) C16—C19—O4—C20 179.4 (3)
C19—C16—C17—C18 177.3 (3)

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
C1—H1···Br1 0.95 2.61 3.461 (3) 149
C3—H3A···Br1 0.99 2.91 3.795 (4) 149
C2—H2···Br1i 0.95 2.75 3.657 (3) 161

Symmetry code: (i) −x+1, −y+1, z+1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: NG5263).

References

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Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) global, I. DOI: 10.1107/S1600536812016728/ng5263sup1.cif

e-68-o1553-sup1.cif (21.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536812016728/ng5263Isup2.hkl

e-68-o1553-Isup2.hkl (133KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536812016728/ng5263Isup3.cml

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


Articles from Acta Crystallographica Section E: Structure Reports Online are provided here courtesy of International Union of Crystallography

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