Literature DB >> 24046647

4-{5-[(2-Bromo-benz-yl)sulfan-yl]-1H-tetra-zol-1-yl}benzoic acid.

Ana C Mafud1, Yvonne P Mascarenhas, Alessandro S Nascimento.   

Abstract

In the title compound, C15H11BrN4O2S, the tetra-zole ring makes dihedral angles of 45.97 (10) and 75.41 (1)°, respectively, with the benzoyl and bromo-benzene rings while the dihedral angle between the benzene rings is 73.77 (1)°. In the crystal, mol-ecules are linked through O-H⋯ N and C-H⋯ O hydrogen bonds, giving infinite chains in both the [110] and [1-10] directions. These chains are further connected by C-Br⋯π and C-O⋯π inter-actions and also by π-π stacking between tetra-zole rings [centroid-centroid distance = 3.312 (1) Å], generating a three-dimensional network.

Entities:  

Year:  2013        PMID: 24046647      PMCID: PMC3770362          DOI: 10.1107/S1600536813014840

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


Related literature

For details of the ZINC database, see: Irwin et al. (2012 ▶). For biological properties of tetra­zoles, see: Kees et al. (1989 ▶); Nolte et al. (1998 ▶); Mafud et al. (2013 ▶).

Experimental

Crystal data

C15H11BrN4O2S M = 391.25 Monoclinic, a = 7.4570 (5) Å b = 8.3500 (5) Å c = 25.3680 (14) Å β = 97.626 (3)° V = 1565.59 (17) Å3 Z = 4 Mo Kα radiation μ = 2.77 mm−1 T = 290 K 0.1 x 0.1 (radius) mm

Data collection

Nonius KappaCCD diffractometer Absorption correction: for a cylinder mounted on the ϕ axis (modified Dwiggins, 1975 ▶) T min = 0.604, T max = 0.608 24464 measured reflections 2889 independent reflections 2388 reflections with I > 2σ(I) R int = 0.069

Refinement

R[F 2 > 2σ(F 2)] = 0.041 wR(F 2) = 0.114 S = 1.06 2889 reflections 213 parameters H atoms treated by a mixture of independent and constrained refinement Δρmax = 0.38 e Å−3 Δρmin = −0.47 e Å−3 Data collection: COLLECT (Nonius, 1999 ▶); cell refinement: SCALEPACK (Otwinowski & Minor, 1997 ▶); data reduction: DENZO (Otwinowski & Minor, 1997 ▶) and SCALEPACK; program(s) used to solve structure: SIR92 (Altomare et al., 1994 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 for Windows (Farrugia, 2012 ▶) and Mercury (Macrae et al., 2008 ▶); software used to prepare material for publication: WinGX (Farrugia, 2012 ▶). Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536813014840/lr2105sup1.cif Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813014840/lr2105Isup2.hkl Click here for additional data file. Supplementary material file. DOI: 10.1107/S1600536813014840/lr2105Isup3.cml Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C15H11BrN4O2SF(000) = 784
Mr = 391.25Dx = 1.66 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 3980 reflections
a = 7.4570 (5) Åθ = 12.0–18.1°
b = 8.3500 (5) ŵ = 2.77 mm1
c = 25.3680 (14) ÅT = 290 K
β = 97.626 (3)°Prism, colourless
V = 1565.59 (17) Å30.1 × 0.1 × 0.1 × 0.1 (radius) mm
Z = 4
Nonius KappaCCD diffractometer2889 independent reflections
Graphite monochromator2388 reflections with I > 2σ(I)
Detector resolution: 9 pixels mm-1Rint = 0.069
CCD scansθmax = 25.7°, θmin = 2.9°
Absorption correction: for a cylinder mounted on the φ axis (Dwiggins, 1975)h = −9→9
Tmin = 0.604, Tmax = 0.608k = −10→10
24464 measured reflectionsl = −30→30
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.041Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.114H atoms treated by a mixture of independent and constrained refinement
S = 1.06w = 1/[σ2(Fo2) + (0.0623P)2 + 0.5855P] where P = (Fo2 + 2Fc2)/3
2889 reflections(Δ/σ)max < 0.001
213 parametersΔρmax = 0.38 e Å3
0 restraintsΔρmin = −0.47 e Å3
Experimental. Absorption correction: interpolation using Int.Tab. Vol. C (1992) p. 523,Tab. 6.3.3.3 for values of muR in the range 0-2.5, and Int.Tab. Vol.II (1959) p.302; Table 5.3.6 B for muR in the range 2.6-10.0. The interpolation procedure of (Dwiggins, 1975) is used with some modification
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
Br10.16110 (5)−0.03469 (5)0.285194 (14)0.07850 (19)
S10.11800 (10)0.09831 (9)0.14388 (3)0.0586 (2)
O1−0.4811 (3)0.7429 (2)0.08768 (9)0.0684 (6)
O2−0.7294 (3)0.5931 (3)0.06893 (9)0.0644 (6)
H1−0.769 (6)0.671 (5)0.0724 (17)0.097*
N1−0.1430 (3)0.0490 (2)0.05969 (8)0.0424 (5)
N2−0.1946 (3)−0.0608 (2)0.02100 (9)0.0482 (5)
N3−0.0817 (3)−0.1770 (3)0.02891 (9)0.0514 (5)
N40.0451 (3)−0.1480 (2)0.07213 (8)0.0484 (5)
C1−0.5529 (4)0.6156 (3)0.07638 (10)0.0506 (6)
C2−0.4489 (3)0.4647 (3)0.07046 (10)0.0462 (6)
C3−0.5338 (3)0.3184 (3)0.06132 (11)0.0515 (6)
H3−0.65940.31240.05770.062*
C4−0.4328 (3)0.1809 (3)0.05749 (10)0.0496 (6)
H4−0.48910.08190.05150.059*
C5−0.2460 (3)0.1937 (3)0.06285 (9)0.0421 (5)
C6−0.1586 (3)0.3385 (3)0.07012 (11)0.0495 (6)
H6−0.03340.34460.07220.059*
C7−0.2614 (4)0.4750 (3)0.07421 (11)0.0507 (6)
H7−0.20480.57410.07950.061*
C80.0051 (3)−0.0061 (3)0.09069 (10)0.0442 (5)
C90.2832 (4)−0.0542 (4)0.16947 (12)0.0618 (8)
H9A0.2221−0.14350.18380.074*
H9B0.3459−0.09380.1410.074*
C100.4163 (4)0.0194 (3)0.21228 (11)0.0568 (7)
C110.3845 (4)0.0329 (3)0.26468 (11)0.0567 (7)
C120.5133 (4)0.0977 (4)0.30333 (13)0.0699 (8)
H120.49020.10310.33840.084*
C130.6728 (5)0.1533 (5)0.29027 (15)0.0862 (11)
H130.75820.1970.31640.103*
C140.7079 (5)0.1450 (6)0.23877 (17)0.0932 (12)
H140.81590.18520.22970.112*
C150.5817 (4)0.0764 (5)0.20012 (14)0.0781 (10)
H150.60810.06840.16540.094*
U11U22U33U12U13U23
Br10.0729 (3)0.0918 (3)0.0707 (3)−0.00307 (17)0.00932 (18)0.00600 (16)
S10.0576 (4)0.0567 (4)0.0563 (4)0.0182 (3)−0.0120 (3)−0.0109 (3)
O10.0681 (12)0.0486 (11)0.0884 (15)0.0129 (10)0.0105 (10)−0.0114 (10)
O20.0531 (12)0.0549 (12)0.0823 (14)0.0223 (9)−0.0014 (10)−0.0076 (10)
N10.0388 (10)0.0404 (11)0.0466 (11)0.0060 (8)0.0005 (8)−0.0039 (8)
N20.0435 (11)0.0446 (11)0.0550 (12)0.0048 (9)0.0011 (9)−0.0070 (9)
N30.0468 (11)0.0477 (12)0.0583 (13)0.0048 (9)0.0018 (9)−0.0063 (10)
N40.0445 (11)0.0464 (12)0.0532 (12)0.0101 (9)0.0027 (9)−0.0019 (9)
C10.0530 (15)0.0498 (16)0.0480 (14)0.0154 (12)0.0030 (11)−0.0014 (11)
C20.0472 (14)0.0459 (14)0.0442 (13)0.0136 (11)0.0013 (10)0.0011 (10)
C30.0391 (12)0.0516 (14)0.0623 (15)0.0094 (11)0.0007 (11)−0.0028 (12)
C40.0414 (13)0.0442 (13)0.0610 (15)0.0043 (10)−0.0010 (11)−0.0028 (11)
C50.0409 (12)0.0413 (12)0.0429 (12)0.0101 (10)0.0012 (9)−0.0009 (9)
C60.0391 (12)0.0458 (14)0.0624 (15)0.0063 (10)0.0026 (11)−0.0007 (11)
C70.0500 (14)0.0413 (13)0.0589 (15)0.0015 (11)0.0009 (12)−0.0023 (11)
C80.0406 (12)0.0457 (13)0.0456 (13)0.0090 (10)0.0037 (10)0.0001 (10)
C90.0615 (17)0.0648 (18)0.0545 (16)0.0235 (14)−0.0098 (13)−0.0083 (13)
C100.0516 (16)0.0634 (17)0.0519 (15)0.0204 (13)−0.0066 (12)−0.0011 (12)
C110.0564 (16)0.0570 (16)0.0538 (16)0.0134 (12)−0.0038 (12)0.0022 (12)
C120.0649 (19)0.080 (2)0.0589 (17)0.0110 (16)−0.0149 (14)−0.0054 (15)
C130.066 (2)0.105 (3)0.079 (2)−0.0006 (19)−0.0213 (18)−0.0040 (19)
C140.0483 (18)0.129 (3)0.098 (3)0.0027 (19)−0.0050 (17)0.013 (2)
C150.0581 (18)0.113 (3)0.0615 (19)0.0226 (19)0.0036 (15)0.0099 (18)
Br1—C111.896 (3)C4—H40.93
S1—C81.728 (3)C5—C61.374 (4)
S1—C91.830 (3)C6—C71.386 (3)
O1—C11.208 (3)C6—H60.93
O2—C11.318 (3)C7—H70.93
O2—H10.72 (4)C9—C101.502 (4)
N1—C81.349 (3)C9—H9A0.97
N1—N21.361 (3)C9—H9B0.97
N1—C51.440 (3)C10—C111.386 (4)
N2—N31.283 (3)C10—C151.394 (5)
N3—N41.371 (3)C11—C121.388 (4)
N4—C81.324 (3)C12—C131.358 (5)
C1—C21.498 (3)C12—H120.93
C2—C31.381 (4)C13—C141.368 (6)
C2—C71.392 (4)C13—H130.93
C3—C41.384 (4)C14—C151.389 (5)
C3—H30.93C14—H140.93
C4—C51.386 (3)C15—H150.93
C8—S1—C999.29 (12)C2—C7—H7119.9
C1—O2—H1106 (4)N4—C8—N1107.7 (2)
C8—N1—N2108.81 (18)N4—C8—S1128.29 (19)
C8—N1—C5130.9 (2)N1—C8—S1124.04 (18)
N2—N1—C5120.24 (19)C10—C9—S1108.74 (19)
N3—N2—N1106.25 (19)C10—C9—H9A109.9
N2—N3—N4111.12 (19)S1—C9—H9A109.9
C8—N4—N3106.15 (19)C10—C9—H9B109.9
O1—C1—O2124.2 (2)S1—C9—H9B109.9
O1—C1—C2123.1 (2)H9A—C9—H9B108.3
O2—C1—C2112.7 (2)C11—C10—C15117.0 (3)
C3—C2—C7120.1 (2)C11—C10—C9123.1 (3)
C3—C2—C1121.9 (2)C15—C10—C9119.9 (3)
C7—C2—C1118.0 (2)C10—C11—C12121.3 (3)
C2—C3—C4120.3 (2)C10—C11—Br1120.5 (2)
C2—C3—H3119.9C12—C11—Br1118.2 (2)
C4—C3—H3119.9C13—C12—C11120.5 (3)
C3—C4—C5118.6 (2)C13—C12—H12119.8
C3—C4—H4120.7C11—C12—H12119.8
C5—C4—H4120.7C12—C13—C14120.0 (3)
C6—C5—C4122.3 (2)C12—C13—H13120
C6—C5—N1119.9 (2)C14—C13—H13120
C4—C5—N1117.8 (2)C13—C14—C15119.9 (4)
C5—C6—C7118.5 (2)C13—C14—H14120.1
C5—C6—H6120.8C15—C14—H14120.1
C7—C6—H6120.8C14—C15—C10121.4 (3)
C6—C7—C2120.3 (2)C14—C15—H15119.3
C6—C7—H7119.9C10—C15—H15119.3
D—H···AD—HH···AD···AD—H···A
C9—H9B···O1i0.972.413.351 (4)163
O2—H1···N4ii0.73 (4)2.05 (4)2.746 (3)161 (5)
C1—O1···Cg1iii1.21 (1)3.62 (1)4.534 (1)133 (2)
C11—Br1···Cg2iv1.90 (1)3.58 (1)4.895 (2)124 (1)
Table 1

Hydrogen-bond geometry (Å, °)

Cg1 and Cg2 are the centroids of the N1–N4/C8 tetra­zole ring and the C10–C15 benzene ring, respectively.

D—H⋯A D—HH⋯A DA D—H⋯A
C9—H9B⋯O1i 0.972.413.351 (4)163
O2—H1⋯N4ii 0.73 (4)2.05 (4)2.746 (3)161 (5)
C1—O1⋯Cg1iii 1.21 (1)3.62 (1)4.534 (1)133 (2)
C11—Br1⋯Cg2iv 1.90 (1)3.58 (1)4.895 (2)124 (1)

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

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