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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2011 Apr 29;67(Pt 5):o1224. doi: 10.1107/S1600536811014735

3-(2,6-Dimethyl­anilino)imidazo[1,2-a]pyridin-1-ium perchlorate

Gary S Nichol a,*, Anuj Sharma b, Hong-Yu Li b
PMCID: PMC3089197  PMID: 21754522

Abstract

The structure of the organic cation in the title compound, C15H16N3 +·ClO4 , contains two essentially planar rings. Mean planes fitted through all non-H atoms of each ring system have an r.m.s. deviation of 0.019 Å for the imidazole-based ring and 0.016 Å for the 2,6-dimethyl­phenyl ring. The angle between the two planes is 86.76 (2)°. In the crystal structure, N—H⋯O inter­actions form a one-dimensional chain, which propagates in the b-axis direction. C—H⋯O inter­actions are also found in the crystal packing.

Related literature

For background information on the Groebke–Blackburn synthesis, see: Bienaymé & Bouzid (1998); Blackburn et al. (1998); Groebke et al. (1998). For details of the chemical synthesis, see: Nichol et al. (2011); Sharma & Li (2011). For information on graph-set notation to describe hydrogen-bonding motifs, see: Bernstein et al. (1995).graphic file with name e-67-o1224-scheme1.jpg

Experimental

Crystal data

  • C15H16N3 +·ClO4

  • M r = 337.76

  • Triclinic, Inline graphic

  • a = 8.6347 (3) Å

  • b = 8.7663 (3) Å

  • c = 11.5155 (4) Å

  • α = 70.668 (2)°

  • β = 73.131 (2)°

  • γ = 72.679 (2)°

  • V = 767.24 (5) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.27 mm−1

  • T = 100 K

  • 0.26 × 0.16 × 0.16 mm

Data collection

  • Bruker Kappa APEXII DUO CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 1996) T min = 0.932, T max = 0.957

  • 27864 measured reflections

  • 8640 independent reflections

  • 6871 reflections with I > 2σ(I)

  • R int = 0.031

Refinement

  • R[F 2 > 2σ(F 2)] = 0.038

  • wR(F 2) = 0.111

  • S = 1.05

  • 8640 reflections

  • 272 parameters

  • All H-atom parameters refined

  • Δρmax = 0.61 e Å−3

  • Δρmin = −0.51 e Å−3

Data collection: APEX2 (Bruker, 2007); cell refinement: SAINT (Bruker, 2007); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; molecular graphics: ORTEP-3 for Windows (Farrugia, 1997) and Mercury (Macrae et al., 2008); software used to prepare material for publication: SHELXTL and publCIF (Westrip, 2010).

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811014735/kj2175sup1.cif

e-67-o1224-sup1.cif (24.9KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811014735/kj2175Isup2.hkl

e-67-o1224-Isup2.hkl (422.6KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811014735/kj2175Isup3.cdx

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
N2—H2N⋯O1i 0.869 (16) 1.955 (17) 2.8169 (10) 170.8 (15)
N3—H3N⋯O3 0.832 (16) 2.216 (15) 2.8899 (10) 138.3 (14)
C2—H2⋯O2ii 0.911 (14) 2.547 (14) 3.3826 (11) 152.8 (12)
C3—H3⋯O4ii 0.971 (15) 2.559 (15) 3.2893 (12) 132.0 (11)

Symmetry codes: (i) Inline graphic; (ii) Inline graphic.

Acknowledgments

The diffractometer was purchased with funding from NSF grant No. CHE-0741837.

supplementary crystallographic information

Comment

The Groebke–Blackburn reaction is the most popular way to prepare imidazo-azines from 2-aminoazines in a single-step (Groebke et al., 1998; Bienaymé & Bouzid, 1998; Blackburn et al., 1998). We have recently reported developments on this synthetic method (Nichol et al., 2011; Sharma & Li, 2011) and present here the crystal structure of the title compound, determined as part of a larger study.

The asymmetric unit of the title compound is shown in Fig. 1. Molecular dimensions are unexceptional. Both ring systems are essentially planar (a mean plane fitted through atoms N1, N2, N3 C1 > C7 has an r.m.s. deviation of 0.019 Å; a mean plane fitted through atoms N3, C8 > C15 has an r.m.s. deviation of 0.016 Å) and the angle between both planes is 86.76 (2)°.

In the crystal, N—H···O interactions form a one-dimensional C22(9) chain (Bernstein et al. 1995), which propagates in the b-axis direction (Fig. 2). C—H···O interactions are also found in the crystal packing.

Experimental

The synthesis is described in Sharma & Li (2011).

Refinement

All H atoms were located from a difference Fourier map and are freely refined. N—H distances are 0.869 (16) and 0.832 (16) Å; C—H distances lie in the range 0.911 (4)–1.033 (17) Å.

Figures

Fig. 1.

Fig. 1.

The asymmetric unit of the title compound with displacement ellipsoids at the 50% probability level.

Fig. 2.

Fig. 2.

N—H···O interactions (dotted blue lines; dotted red lines indicate continuation) in the title compound.

Crystal data

C15H16N3+·ClO4 Z = 2
Mr = 337.76 F(000) = 352
Triclinic, P1 Dx = 1.462 Mg m3
Hall symbol: -P 1 Mo Kα radiation, λ = 0.71073 Å
a = 8.6347 (3) Å Cell parameters from 8544 reflections
b = 8.7663 (3) Å θ = 2.5–39.0°
c = 11.5155 (4) Å µ = 0.27 mm1
α = 70.668 (2)° T = 100 K
β = 73.131 (2)° Block, colourless
γ = 72.679 (2)° 0.26 × 0.16 × 0.16 mm
V = 767.24 (5) Å3

Data collection

Bruker Kappa APEXII DUO CCD diffractometer 8640 independent reflections
Radiation source: fine-focus sealed tube with Miracol optics 6871 reflections with I > 2σ(I)
graphite Rint = 0.031
φ and ω scans θmax = 38.6°, θmin = 1.9°
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) h = −13→15
Tmin = 0.932, Tmax = 0.957 k = −15→15
27864 measured reflections l = −20→20

Refinement

Refinement on F2 Primary atom site location: structure-invariant direct methods
Least-squares matrix: full Secondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.038 Hydrogen site location: difference Fourier map
wR(F2) = 0.111 All H-atom parameters refined
S = 1.05 w = 1/[σ2(Fo2) + (0.0581P)2 + 0.1118P] where P = (Fo2 + 2Fc2)/3
8640 reflections (Δ/σ)max = 0.001
272 parameters Δρmax = 0.61 e Å3
0 restraints Δρmin = −0.51 e Å3

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
N1 0.98956 (8) 0.60185 (8) 0.27803 (6) 0.01285 (10)
N2 0.85450 (9) 0.82744 (9) 0.33586 (7) 0.01631 (12)
H2N 0.825 (2) 0.904 (2) 0.3751 (15) 0.032 (4)*
N3 0.82987 (9) 0.59792 (9) 0.13756 (7) 0.01541 (11)
H3N 0.782 (2) 0.5193 (19) 0.1717 (14) 0.030 (4)*
C1 1.10989 (10) 0.45913 (10) 0.27281 (8) 0.01559 (13)
H1 1.1040 (18) 0.3970 (17) 0.2222 (13) 0.021 (3)*
C2 1.22970 (11) 0.41819 (11) 0.33968 (8) 0.01768 (14)
H2 1.3107 (17) 0.3243 (17) 0.3371 (13) 0.021 (3)*
C3 1.23050 (11) 0.52108 (11) 0.41221 (8) 0.01805 (14)
H3 1.3177 (18) 0.4918 (18) 0.4584 (14) 0.026 (3)*
C4 1.11017 (11) 0.66267 (11) 0.41743 (8) 0.01665 (13)
H4 1.1091 (17) 0.7333 (17) 0.4609 (13) 0.022 (3)*
C5 0.98717 (10) 0.70098 (9) 0.34900 (7) 0.01399 (12)
C6 0.77067 (10) 0.80959 (10) 0.25805 (8) 0.01618 (13)
H6 0.6720 (18) 0.8831 (18) 0.2376 (14) 0.025 (3)*
C7 0.85317 (10) 0.66985 (9) 0.22032 (7) 0.01359 (12)
C8 0.77759 (10) 0.70835 (9) 0.02641 (7) 0.01420 (12)
C9 0.62087 (11) 0.72027 (11) 0.00791 (8) 0.01716 (13)
C10 0.57589 (12) 0.82519 (12) −0.10399 (9) 0.02081 (15)
H10 0.4688 (18) 0.8271 (17) −0.1195 (13) 0.023 (3)*
C11 0.68217 (13) 0.91810 (12) −0.19433 (9) 0.02220 (16)
H11 0.657 (2) 0.9887 (19) −0.2776 (15) 0.033 (4)*
C12 0.83699 (12) 0.90525 (11) −0.17397 (8) 0.02083 (15)
H12 0.915 (2) 0.9649 (19) −0.2370 (15) 0.032 (4)*
C13 0.88820 (11) 0.79974 (10) −0.06457 (8) 0.01662 (13)
C14 0.50193 (13) 0.62394 (14) 0.10725 (10) 0.02599 (19)
H14A 0.549 (2) 0.498 (2) 0.1225 (15) 0.035 (4)*
H14B 0.483 (2) 0.655 (2) 0.1867 (16) 0.037 (4)*
H14C 0.394 (2) 0.652 (2) 0.0884 (16) 0.037 (4)*
C15 1.05888 (12) 0.78164 (13) −0.04629 (9) 0.02178 (16)
H15A 1.0548 (18) 0.8453 (18) 0.0085 (14) 0.027 (4)*
H15B 1.135 (2) 0.819 (2) −0.1279 (16) 0.036 (4)*
H15C 1.1063 (19) 0.6657 (19) −0.0109 (14) 0.028 (4)*
Cl 0.65990 (2) 0.20252 (2) 0.419315 (17) 0.01454 (5)
O1 0.79691 (9) 0.07166 (9) 0.46174 (7) 0.02290 (13)
O2 0.60990 (9) 0.15985 (9) 0.32753 (7) 0.02488 (14)
O3 0.71409 (13) 0.35550 (10) 0.36274 (8) 0.03427 (19)
O4 0.52640 (10) 0.21967 (12) 0.52460 (7) 0.03483 (19)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
N1 0.0136 (3) 0.0125 (2) 0.0123 (2) −0.0019 (2) −0.0038 (2) −0.0031 (2)
N2 0.0182 (3) 0.0136 (3) 0.0171 (3) −0.0008 (2) −0.0050 (2) −0.0054 (2)
N3 0.0204 (3) 0.0135 (3) 0.0136 (3) −0.0049 (2) −0.0072 (2) −0.0011 (2)
C1 0.0161 (3) 0.0143 (3) 0.0155 (3) −0.0001 (2) −0.0046 (2) −0.0047 (2)
C2 0.0157 (3) 0.0180 (3) 0.0183 (3) 0.0004 (3) −0.0061 (3) −0.0049 (3)
C3 0.0164 (3) 0.0210 (3) 0.0175 (3) −0.0037 (3) −0.0065 (3) −0.0042 (3)
C4 0.0184 (3) 0.0180 (3) 0.0156 (3) −0.0050 (3) −0.0055 (3) −0.0047 (3)
C5 0.0153 (3) 0.0135 (3) 0.0133 (3) −0.0030 (2) −0.0035 (2) −0.0037 (2)
C6 0.0163 (3) 0.0144 (3) 0.0167 (3) −0.0006 (2) −0.0054 (2) −0.0037 (2)
C7 0.0141 (3) 0.0132 (3) 0.0131 (3) −0.0020 (2) −0.0047 (2) −0.0024 (2)
C8 0.0166 (3) 0.0133 (3) 0.0125 (3) −0.0031 (2) −0.0051 (2) −0.0018 (2)
C9 0.0175 (3) 0.0185 (3) 0.0154 (3) −0.0046 (3) −0.0059 (3) −0.0018 (3)
C10 0.0213 (4) 0.0218 (4) 0.0188 (3) −0.0018 (3) −0.0104 (3) −0.0020 (3)
C11 0.0290 (4) 0.0189 (3) 0.0161 (3) −0.0023 (3) −0.0094 (3) 0.0000 (3)
C12 0.0270 (4) 0.0178 (3) 0.0149 (3) −0.0072 (3) −0.0039 (3) 0.0006 (3)
C13 0.0187 (3) 0.0157 (3) 0.0148 (3) −0.0048 (3) −0.0028 (2) −0.0030 (2)
C14 0.0204 (4) 0.0336 (5) 0.0227 (4) −0.0128 (4) −0.0065 (3) 0.0016 (4)
C15 0.0186 (4) 0.0249 (4) 0.0222 (4) −0.0087 (3) −0.0026 (3) −0.0048 (3)
Cl 0.01653 (8) 0.01267 (7) 0.01320 (7) −0.00157 (5) −0.00390 (6) −0.00279 (5)
O1 0.0223 (3) 0.0221 (3) 0.0274 (3) 0.0056 (2) −0.0147 (3) −0.0118 (3)
O2 0.0258 (3) 0.0247 (3) 0.0311 (4) 0.0006 (3) −0.0171 (3) −0.0124 (3)
O3 0.0591 (6) 0.0231 (3) 0.0265 (4) −0.0231 (4) −0.0188 (4) 0.0067 (3)
O4 0.0263 (4) 0.0410 (5) 0.0207 (3) 0.0058 (3) 0.0040 (3) −0.0066 (3)

Geometric parameters (Å, °)

N1—C1 1.3741 (10) C8—C13 1.4039 (11)
N1—C5 1.3687 (10) C9—C10 1.3966 (12)
N1—C7 1.3992 (10) C9—C14 1.5071 (13)
N2—H2N 0.869 (16) C10—H10 0.985 (14)
N2—C5 1.3408 (11) C10—C11 1.3849 (14)
N2—C6 1.3740 (11) C11—H11 0.999 (16)
N3—H3N 0.832 (16) C11—C12 1.3891 (14)
N3—C7 1.3896 (10) C12—H12 0.966 (16)
N3—C8 1.4262 (10) C12—C13 1.3951 (12)
C1—H1 0.939 (14) C13—C15 1.5034 (13)
C1—C2 1.3602 (12) C14—H14A 1.033 (17)
C2—H2 0.911 (14) C14—H14B 0.994 (17)
C2—C3 1.4203 (12) C14—H14C 0.958 (17)
C3—H3 0.971 (15) C15—H15A 0.958 (15)
C3—C4 1.3671 (12) C15—H15B 0.994 (16)
C4—H4 0.912 (14) C15—H15C 0.971 (15)
C4—C5 1.3999 (11) Cl—O1 1.4528 (7)
C6—H6 0.941 (15) Cl—O2 1.4375 (7)
C6—C7 1.3601 (11) Cl—O3 1.4353 (8)
C8—C9 1.3985 (11) Cl—O4 1.4239 (8)
C1—N1—C5 121.77 (7) C8—C9—C10 118.57 (8)
C1—N1—C7 129.50 (7) C8—C9—C14 120.81 (7)
C5—N1—C7 108.71 (6) C10—C9—C14 120.61 (8)
H2N—N2—C5 123.8 (11) C9—C10—H10 118.3 (8)
H2N—N2—C6 126.6 (11) C9—C10—C11 121.14 (8)
C5—N2—C6 109.48 (7) H10—C10—C11 120.4 (8)
H3N—N3—C7 114.8 (11) C10—C11—H11 123.1 (9)
H3N—N3—C8 114.5 (11) C10—C11—C12 119.44 (8)
C7—N3—C8 116.63 (7) H11—C11—C12 117.3 (9)
N1—C1—H1 117.3 (9) C11—C12—H12 121.1 (9)
N1—C1—C2 118.21 (7) C11—C12—C13 121.33 (8)
H1—C1—C2 124.5 (9) H12—C12—C13 117.5 (9)
C1—C2—H2 119.5 (9) C8—C13—C12 118.23 (8)
C1—C2—C3 120.71 (8) C8—C13—C15 121.02 (7)
H2—C2—C3 119.8 (9) C12—C13—C15 120.74 (8)
C2—C3—H3 120.1 (9) C9—C14—H14A 111.5 (9)
C2—C3—C4 120.84 (7) C9—C14—H14B 108.0 (10)
H3—C3—C4 119.1 (9) C9—C14—H14C 113.1 (10)
C3—C4—H4 123.1 (9) H14A—C14—H14B 109.3 (13)
C3—C4—C5 117.33 (8) H14A—C14—H14C 109.5 (14)
H4—C4—C5 119.6 (9) H14B—C14—H14C 105.1 (14)
N1—C5—N2 107.30 (7) C13—C15—H15A 110.8 (9)
N1—C5—C4 121.11 (7) C13—C15—H15B 111.2 (10)
N2—C5—C4 131.58 (8) C13—C15—H15C 109.7 (9)
N2—C6—H6 123.8 (9) H15A—C15—H15B 108.4 (13)
N2—C6—C7 108.34 (7) H15A—C15—H15C 109.6 (12)
H6—C6—C7 127.8 (9) H15B—C15—H15C 107.1 (13)
N1—C7—N3 120.77 (7) O1—Cl—O2 108.58 (4)
N1—C7—C6 106.16 (7) O1—Cl—O3 109.13 (5)
N3—C7—C6 132.97 (7) O1—Cl—O4 109.21 (5)
N3—C8—C9 120.05 (7) O2—Cl—O3 109.54 (5)
N3—C8—C13 118.66 (7) O2—Cl—O4 110.96 (6)
C9—C8—C13 121.27 (7) O3—Cl—O4 109.39 (6)
C5—N1—C1—C2 −0.63 (12) C1—N1—C7—C6 178.53 (8)
C7—N1—C1—C2 −179.04 (8) C5—N1—C7—N3 176.88 (7)
N1—C1—C2—C3 −0.38 (13) C5—N1—C7—C6 −0.04 (9)
C1—C2—C3—C4 0.61 (13) C7—N3—C8—C9 −114.31 (9)
C2—C3—C4—C5 0.16 (13) C7—N3—C8—C13 67.62 (10)
C6—N2—C5—N1 0.59 (9) N3—C8—C9—C10 −177.75 (8)
C6—N2—C5—C4 −179.96 (9) N3—C8—C9—C14 3.10 (13)
C1—N1—C5—N2 −179.04 (7) C13—C8—C9—C10 0.27 (13)
C1—N1—C5—C4 1.44 (12) C13—C8—C9—C14 −178.88 (9)
C7—N1—C5—N2 −0.34 (9) C8—C9—C10—C11 −1.10 (14)
C7—N1—C5—C4 −179.86 (7) C14—C9—C10—C11 178.05 (10)
C3—C4—C5—N1 −1.16 (12) C9—C10—C11—C12 0.78 (15)
C3—C4—C5—N2 179.45 (9) C10—C11—C12—C13 0.40 (15)
C5—N2—C6—C7 −0.62 (10) C11—C12—C13—C8 −1.19 (14)
N2—C6—C7—N1 0.39 (9) C11—C12—C13—C15 177.38 (9)
N2—C6—C7—N3 −175.99 (8) N3—C8—C13—C12 178.90 (8)
C8—N3—C7—N1 −138.11 (8) N3—C8—C13—C15 0.33 (12)
C8—N3—C7—C6 37.84 (13) C9—C8—C13—C12 0.85 (13)
C1—N1—C7—N3 −4.55 (12) C9—C8—C13—C15 −177.71 (8)

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N2—H2N···O1i 0.869 (16) 1.955 (17) 2.8169 (10) 170.8 (15)
N3—H3N···O3 0.832 (16) 2.216 (15) 2.8899 (10) 138.3 (14)
C2—H2···O2ii 0.911 (14) 2.547 (14) 3.3826 (11) 152.8 (12)
C3—H3···O4ii 0.971 (15) 2.559 (15) 3.2893 (12) 132.0 (11)

Symmetry codes: (i) x, y+1, z; (ii) x+1, y, z.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: KJ2175).

References

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  5. Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.
  6. Groebke, K., Weber, L. & Mehlin, F. (1998). Synlett, pp. 661–663.
  7. Macrae, C. F., Bruno, I. J., Chisholm, J. A., Edgington, P. R., McCabe, P., Pidcock, E., Rodriguez-Monge, L., Taylor, R., van de Streek, J. & Wood, P. A. (2008). J. Appl. Cryst. 41, 466–470.
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  12. Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.

Associated Data

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

Supplementary Materials

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536811014735/kj2175sup1.cif

e-67-o1224-sup1.cif (24.9KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536811014735/kj2175Isup2.hkl

e-67-o1224-Isup2.hkl (422.6KB, hkl)

Supplementary material file. DOI: 10.1107/S1600536811014735/kj2175Isup3.cdx

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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