Literature DB >> 21584033

1-(3-Bromo-prop-yl)-4-(2-pyrid-yl)-1H-1,2,3-triazole.

James D Crowley1, Pauline H Bandeen, Lyall R Hanton.   

Abstract

In the structure of the title compound, C(10)H(11)BrN(4), the plane of the substituted n class="Chemical">1,2,3-triazole ring is tilted by 14.84 (10)° with respect to the mean plane of the pyridine ring. The pyridine and closest triazole N atoms adopt an anti arrangement which removes any lone pair-lone pair repulsions between the N atoms. This conformation is further stabilized by weak intermolecular C-H⋯N inter-actions. There are two mol-ecules in the unit cell, which form a centrosymmetric head-to-tail dimer. The dimers are stabilized through π-π inter-actions [centroid-centroid distance = 3.733 (4) Å and mean inter-planar distance = 3.806 (12) Å] between the substituted 1,2,3-triazole ring and the pyridine rings in adjacent mol-ecules. Each dimer inter-acts with two neighbouring dimers above and below, forming a slipped stack of dimers through the crystal. The 3-bromo-propyl chain sits over the pyridine ring of a neighbouring mol-ecule and the triazole rings of nearby mol-ecules are adjacent.

Entities:  

Year:  2009        PMID: 21584033      PMCID: PMC2977690          DOI: 10.1107/S1600536809012148

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


Related literature

For details of the Cu(I)-catalysed 1,3-cyclo­addition of organic n class="Chemical">azides with terminal alkynes, see: Rostovtsev et al. (2002 ▶); Tornoe et al. (2002 ▶); Meldal & Tornoe (2008 ▶). For applications of pyridyl-functionalized 1,2,3-triazoles, see: Li & Flood (2008 ▶); Meudtner & Hecht (2008 ▶); Krivopalov & Shkurko (2005 ▶); Li et al. (2007 ▶); Richardson et al. (2008 ▶). For related structures, see Schweinfurth et al. (2008 ▶); Obata et al. (2008 ▶).

Experimental

Crystal data

C10H11BrN4 M = 267.14 Triclinic, a = 5.658 (2) Å b = 9.688 (4) Å c = 10.191 (4) Å α = 84.498 (3)° β = 85.663 (2)° γ = 83.854 (2)° V = 551.6 (4) Å3 Z = 2 Mo Kα radiation μ = 3.70 mm−1 T = 90 K 0.53 × 0.23 × 0.11 mm

Data collection

Bruker APEXII CCD area-detector diffractometer Absorption correction: multi-scan (SADABS; Bruker, 2004 ▶) T min = 0.358, T max = 0.66 8776 measured reflections 1879 independent reflections 1759 reflections with I > 2σ(I) R int = 0.043

Refinement

R[F 2 > 2σ(F 2)] = 0.027 wR(F 2) = 0.071 S = 0.97 1879 reflections 136 parameters H-atom parameters constrained Δρmax = 0.64 e Å−3 Δρmin = −0.61 e Å−3 Data collection: APEX2 (Bruker, 2004 ▶); cell refinement: APEX2 and SAINT (Bruker, 2004 ▶); data reduction: SAIn class="Chemical">NT; program(s) used to solve structure: SIR97 (Altomare et al., 1999 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶) and Mercury (Bruno et al., 2002 ▶); software used to prepare material for publication: SHELXTL (Sheldrick, 2008 ▶) and enCIFer (Allen et al., 2004 ▶). Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809012148/fj2204sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536809012148/fj2204Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C10H11BrN4Z = 2
Mr = 267.14F(000) = 268
Triclinic, P1Dx = 1.608 Mg m3
Hall symbol: -P 1Melting point: 362 K
a = 5.658 (2) ÅMo Kα radiation, λ = 0.71073 Å
b = 9.688 (4) ÅCell parameters from 5048 reflections
c = 10.191 (4) Åθ = 3.1–33.3°
α = 84.498 (3)°µ = 3.70 mm1
β = 85.663 (2)°T = 90 K
γ = 83.854 (2)°Irregular, colourless
V = 551.6 (4) Å30.53 × 0.23 × 0.11 mm
Bruker APEXII CCD area-detector diffractometer1879 independent reflections
Radiation source: fine-focus sealed tube1759 reflections with I > 2σ(I)
graphiteRint = 0.043
φ and ω scansθmax = 25.0°, θmin = 4.0°
Absorption correction: multi-scan (SADABS; Bruker, 2004)h = −6→6
Tmin = 0.358, Tmax = 0.66k = −11→11
8776 measured reflectionsl = −12→12
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.027Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.071H-atom parameters constrained
S = 0.97w = 1/[σ2(Fo2) + (0.0372P)2 + 0.5592P] where P = (Fo2 + 2Fc2)/3
1879 reflections(Δ/σ)max = 0.001
136 parametersΔρmax = 0.64 e Å3
0 restraintsΔρmin = −0.61 e Å3
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
Br10.84285 (5)−0.19395 (3)0.97535 (3)0.03839 (13)
N30.3211 (3)0.1602 (2)0.6731 (2)0.0243 (4)
C60.4287 (4)0.2879 (2)0.4946 (2)0.0177 (5)
N20.2396 (4)0.2401 (2)0.5713 (2)0.0236 (4)
N10.6005 (4)0.4000 (2)0.2965 (2)0.0230 (4)
N40.5611 (3)0.15753 (19)0.66118 (19)0.0188 (4)
C50.3999 (4)0.3838 (2)0.3747 (2)0.0179 (5)
C70.6350 (4)0.2341 (2)0.5518 (2)0.0185 (5)
H70.79080.24760.52150.022*
C40.1805 (4)0.4545 (2)0.3468 (2)0.0216 (5)
H40.04470.43850.40100.026*
C80.7073 (4)0.0790 (2)0.7608 (2)0.0212 (5)
H8A0.60750.05760.84030.025*
H8B0.82670.13600.78320.025*
C20.3717 (5)0.5674 (2)0.1552 (2)0.0244 (5)
H20.36770.63020.08020.029*
C10.5814 (4)0.4892 (2)0.1884 (2)0.0249 (5)
H10.71700.49930.13220.030*
C90.8298 (5)−0.0555 (3)0.7124 (2)0.0291 (6)
H9A0.7101−0.11680.70020.035*
H9B0.9133−0.03490.62730.035*
C30.1681 (4)0.5495 (2)0.2364 (2)0.0242 (5)
H30.02450.60080.21720.029*
C101.0035 (5)−0.1294 (3)0.8062 (3)0.0309 (6)
H10A1.1188−0.06670.82220.037*
H10B1.0890−0.20870.76630.037*
U11U22U33U12U13U23
Br10.04089 (19)0.03674 (19)0.03195 (18)0.00206 (12)0.00069 (13)0.01657 (12)
N30.0180 (10)0.0273 (11)0.0260 (11)−0.0011 (8)−0.0002 (9)0.0033 (9)
C60.0187 (11)0.0154 (10)0.0191 (11)−0.0011 (9)−0.0003 (9)−0.0032 (9)
N20.0191 (10)0.0265 (10)0.0241 (11)−0.0024 (8)−0.0010 (8)0.0032 (9)
N10.0214 (10)0.0240 (10)0.0227 (10)−0.0008 (8)0.0001 (9)−0.0013 (8)
N40.0171 (9)0.0191 (9)0.0194 (10)0.0001 (8)−0.0017 (8)0.0001 (8)
C50.0187 (11)0.0152 (10)0.0200 (11)−0.0024 (9)−0.0012 (9)−0.0028 (9)
C70.0159 (11)0.0181 (10)0.0212 (11)−0.0013 (9)−0.0002 (9)−0.0014 (9)
C40.0170 (11)0.0229 (11)0.0246 (12)−0.0011 (9)−0.0006 (10)−0.0021 (10)
C80.0240 (12)0.0200 (11)0.0187 (11)0.0020 (9)−0.0037 (10)−0.0007 (9)
C20.0344 (14)0.0183 (11)0.0208 (12)−0.0028 (10)−0.0075 (11)0.0015 (9)
C10.0251 (12)0.0266 (12)0.0220 (12)−0.0039 (10)0.0024 (10)0.0015 (10)
C90.0424 (15)0.0230 (12)0.0198 (12)0.0072 (11)−0.0026 (11)−0.0027 (10)
C30.0239 (12)0.0204 (11)0.0281 (13)0.0029 (10)−0.0067 (11)−0.0030 (10)
C100.0357 (15)0.0261 (13)0.0264 (13)0.0093 (11)0.0030 (12)0.0028 (10)
Br1—C101.966 (3)C8—C91.516 (3)
N3—N21.315 (3)C8—H8A0.9700
N3—N41.352 (3)C8—H8B0.9700
C6—N21.371 (3)C2—C31.383 (4)
C6—C71.373 (3)C2—C11.384 (4)
C6—C51.471 (3)C2—H20.9300
N1—C11.337 (3)C1—H10.9300
N1—C51.351 (3)C9—C101.501 (4)
N4—C71.344 (3)C9—H9A0.9700
N4—C81.463 (3)C9—H9B0.9700
C5—C41.388 (3)C3—H30.9300
C7—H70.9300C10—H10A0.9700
C4—C31.384 (3)C10—H10B0.9700
C4—H40.9300
N2—N3—N4106.83 (18)H8A—C8—H8B107.9
N2—C6—C7108.4 (2)C3—C2—C1118.2 (2)
N2—C6—C5122.9 (2)C3—C2—H2120.9
C7—C6—C5128.7 (2)C1—C2—H2120.9
N3—N2—C6108.78 (19)N1—C1—C2123.8 (2)
C1—N1—C5117.1 (2)N1—C1—H1118.1
C7—N4—N3111.53 (18)C2—C1—H1118.1
C7—N4—C8127.7 (2)C10—C9—C8112.8 (2)
N3—N4—C8120.73 (19)C10—C9—H9A109.0
N1—C5—C4122.9 (2)C8—C9—H9A109.0
N1—C5—C6115.7 (2)C10—C9—H9B109.0
C4—C5—C6121.4 (2)C8—C9—H9B109.0
N4—C7—C6104.5 (2)H9A—C9—H9B107.8
N4—C7—H7127.8C2—C3—C4119.3 (2)
C6—C7—H7127.8C2—C3—H3120.4
C3—C4—C5118.6 (2)C4—C3—H3120.4
C3—C4—H4120.7C9—C10—Br1111.7 (2)
C5—C4—H4120.7C9—C10—H10A109.3
N4—C8—C9111.80 (19)Br1—C10—H10A109.3
N4—C8—H8A109.3C9—C10—H10B109.3
C9—C8—H8A109.3Br1—C10—H10B109.3
N4—C8—H8B109.3H10A—C10—H10B107.9
C9—C8—H8B109.3
D—H···AD—HH···AD···AD—H···A
C7—H7···N2i0.932.623.449 (4)149
C10—H10B···N1ii0.972.513.450 (4)164
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
C7—H7⋯N2i0.932.623.449 (4)149
C10—H10B⋯N1ii0.972.513.450 (4)164

Symmetry codes: (i) ; (ii) .

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