supplementary materials


Acta Cryst. (2009). E65, o990-o991    [ doi:10.1107/S1600536809011908 ]

N-(2-Hydroxyethyl)-2-[3-(p-tolyl)triazen-1-yl]benzamide

F. Rocha-Alonzo, G. Aguirre and M. Parra-Hake

Abstract top

In the solid state, the structure of the title compound, C16H18N4O2, is stabilized by intermolecular N-H...O and O-H...O hydrogen bonds. These hydrogen bonds arrange the molecules into a double-layer supramolecular structure. The molecular conformation is is consolidated by an intramolecular N-H...N hydrogen bond. The dihedral angle between the aromatic rings is 8.01 (10)°

Comment top

The synthesis of alternative ligands to stabilize dinuclear complexes and control their reactivity is an area of great importance in coordination and organometallic chemistry (for recent literature see: Das et al., 2008; Estevan et al., 2006; Jie et al., 2007; Müller & Vogt, 2007; Schilling et al., 2008). In this context, we have focused our attention to the synthesis of 1,3-bis(aryl)triazenes as precursors for triazenido ligands bearing Lewis basic ortho substituents such as ester, methoxy and methylmercapto groups (Nuricumbo-Escobar et al., 2007; Ríos-Moreno et al., 2003; Rodríguez et al., 1999; Tejel et al., 2004); it has been found that the nature of the substituent produces a dramatic impact on their coordination chemistry and reactivity. As part of our ongoing research, we have synthesized the title compound (I, Fig. 1) using the diazonium salt N-coupling methodology.

The molecular structure of (I) shows the characteristic trans stereochemistry about NN of the diazoamino group of free triazenes. The N1N2 bond [1.264 (3) Å] is longer than the typical value for NN bond (1.222 Å), whereas the N2—N3 bond [1.320 (3) Å] is shorter than typical value for a Nsp3—Nsp2 single bond (1.420 Å) (Allen et al., 1987). In addition, the C7—N3 bond [1.395 (3) Å] is shorter than the characteristic Caryl—NH single bonds for secondary aromatic amines (1.419 Å) (Orpen, et al., 1989). An intramolecular N1—H···N4 hydrogen bond is observed (Fig. 1 and Table 1).

In the crystal structure, adjacent units are arranged into a two-dimensional network along the (100) plane via intermolecular N— H···O and O—H···O hydrogen bond interactions (Fig. 2 and Table 1). These layers are linked together via intermolecular N—H···O and O—H···O hydrogen bonds forming a zig-zag bilayered array along the [001] direction (Fig. 3).

Related literature top

The synthesis of alternative ligands to stabilize dinuclear complexes and control their reactivity is an area of great importance in coordination and organometallic chemistry, see: Das et al. (2008); Estevan et al. (2006); Jie et al. (2007); Müller & Vogt (2007); Schilling et al. (2008). For the synthesis of 1,3-bis(aryl)triazenes as precursors for triazenido ligands bearing Lewis basic ortho substituents such as ester, methoxy and methylmercapto groups, see: Nuricumbo-Escobar et al.(2007); Ríos-Moreno et al. (2003); Rodríguez et al. (1999); Tejel et al. (2004). The starting material 2-[4,5-dihydro-1,3-oxazol-2-yl]aniline was synthesized by a modification of the literature method of Gómez et al. (2005). For bond-length data, see: Allen et al. (1987); Orpen et al. (1989).

Experimental top

The synthesis of the title compound included reagents and solvents of reagent grade, which were used without further purification. As a starting material we synthesized 2-[4,5-dihydro-1,3-oxazol-2-yl]aniline by a modification of the Gómez and coworkers methodology (Gómez et al., 2005). 2-[4,5-Dihydro-1,3-oxazol-2-yl]aniline (1.00 g, 6.17 mmol) was dissolved in aqueous HCl 2 M (9.25 ml, 18.50 mmol) and cooled to 268 K. A sodium nitrite solution (0.51 g, 7.40 mmol) in water (6 ml) was slowly added with continuous stirring. A solution of p-toluidine (0.66 g, 6.17 mmol) in methanol (10 ml) was added slowly to the reaction mixture, and stirred for 30 m at 268 K. The resulting mixture was neutralised with a saturated aqueous solution of NaHCO3. A crude yellow-orange was separated by filtration and washed with small portions of water. The product was purified by flash chromatography on neutral alumina (hexane/ethyl acetate, 1:9), and recrystallized from an ethyl acetate/hexane mixture (9 : 1). Orange bar-shaped crystals of (I), suitable for X-ray analysis, were obtained by slow evaporation of the solvent mixture. Yield 47% (0.87 g, 2.90 mmol), based on 2-[4,5-dihydro-1,3-oxazol-2-yl]aniline; m.p., 111–113 °C. IR (KBr pellet, cm-1), 3278, 3233, 1625, 1538, 1269.1H NMR [(CD3)2CO, 200 MHz] δ 12.89 (s), 8.10 (s), 7.93–7.02 (m, 8H), 4.10 (s), 3.74 (dd J = 5.4, 11.0 Hz, 2H), 3.54 (dd, J = 5.4, 11.0 Hz, 2H), 2.35 (s, 3H).13C NMR [(C D3)2CO, 50 MHz] δ 135.4, 133.0, 130.1, 128.4, 121.7,114.9, 61.2, 43.2, 21.0. Anal. Calcd. for C16H18N4O2: C, 64.41; H, 6.08;N, 18.78%. Found C, 64.11; H, 6.44; N, 18.93%. HRESIMS Calcd. for [M+H]+299.1503. Found 299.1519.

Refinement top

Refinement for H atoms was carried out using a riding model, with distances constrained to: 0.93 Å for aromatic CH, 0.98 Å for methine CH. Isotropic U parameters were fixed to Uiso(H)=1.2Ueq(carrier atom) for aromatic CH.

Computing details top

Data collection: XSCANS (Siemens, 1996); cell refinement: XSCANS (Siemens, 1996); data reduction: XSCANS (Siemens, 1996); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: Mercury (Macrae et al., 2006); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. The title compound (I) with displacement ellipsoids drawn at the 30% probability level. Intramolecular H-bond is indicated by dashed lines.
[Figure 2] Fig. 2. Packing of I showing the H-bonds. The molecules are forming a two dimensional network in the (100) plane. H-bonds are indicated by dashed lines.
[Figure 3] Fig. 3. Packing of I showing the bilayer. The molecules are forming a zig-zag array along the [001] direction.
N-(2-Hydroxyethyl)-2-[3-(p-tolyl)triazen-1-yl]benzamide top
Crystal data top
C16H18N4O2F(000) = 632
Mr = 298.34Dx = 1.299 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 76 reflections
a = 16.846 (2) Åθ = 4.7–12.0°
b = 12.2053 (17) ŵ = 0.09 mm1
c = 7.4302 (11) ÅT = 298 K
β = 93.212 (13)°Neele, yellow
V = 1525.3 (4) Å30.40 × 0.22 × 0.14 mm
Z = 4
Data collection top
Bruker P4
diffractometer
Rint = 0.044
Radiation source: fine-focus sealed tubeθmax = 26.3°, θmin = 2.1°
graphiteh = 2020
2θ/ω scansk = 151
4153 measured reflectionsl = 91
3067 independent reflections3 standard reflections every 97 reflections
1778 reflections with I > 2σ(I) intensity decay: 2.8%
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.055H-atom parameters constrained
wR(F2) = 0.188 w = 1/[σ2(Fo2) + (0.1035P)2 + 0.0651P]
where P = (Fo2 + 2Fc2)/3
S = 1.04(Δ/σ)max < 0.001
3067 reflectionsΔρmax = 0.57 e Å3
201 parametersΔρmin = 0.22 e Å3
0 restraintsExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.008 (3)
Crystal data top
C16H18N4O2V = 1525.3 (4) Å3
Mr = 298.34Z = 4
Monoclinic, P21/cMo Kα radiation
a = 16.846 (2) ŵ = 0.09 mm1
b = 12.2053 (17) ÅT = 298 K
c = 7.4302 (11) Å0.40 × 0.22 × 0.14 mm
β = 93.212 (13)°
Data collection top
Bruker P4
diffractometer
Rint = 0.044
4153 measured reflectionsθmax = 26.3°
3067 independent reflections3 standard reflections every 97 reflections
1778 reflections with I > 2σ(I) intensity decay: 2.8%
Refinement top
R[F2 > 2σ(F2)] = 0.055H-atom parameters constrained
wR(F2) = 0.188Δρmax = 0.57 e Å3
S = 1.04Δρmin = 0.22 e Å3
3067 reflectionsAbsolute structure: ?
201 parametersFlack parameter: ?
0 restraintsRogers parameter: ?
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
N10.69940 (11)0.33793 (15)0.0017 (3)0.0484 (5)
N20.76320 (11)0.39013 (16)0.0332 (3)0.0481 (5)
N40.54570 (10)0.30472 (15)0.1084 (3)0.0456 (5)
H4A0.57900.34800.05250.055*
O10.51316 (10)0.13062 (14)0.1750 (2)0.0574 (5)
O20.39653 (10)0.39859 (16)0.0593 (3)0.0651 (6)
H2B0.43410.38340.12990.098*
N30.75322 (11)0.49670 (16)0.0124 (3)0.0521 (6)
H3A0.70660.52190.01750.063*
C10.70741 (13)0.22274 (19)0.0146 (3)0.0434 (6)
C20.64042 (13)0.15801 (18)0.0313 (3)0.0424 (6)
C30.64717 (15)0.0445 (2)0.0087 (4)0.0550 (7)
H3B0.60290.00060.03460.066*
C40.71719 (17)0.0036 (2)0.0504 (4)0.0646 (8)
H4B0.72000.07920.06510.078*
C50.78345 (15)0.0601 (2)0.0881 (4)0.0654 (8)
H5A0.83170.02750.12370.078*
C60.77816 (14)0.1716 (2)0.0729 (4)0.0577 (7)
H6A0.82280.21410.10220.069*
C70.81680 (13)0.56925 (19)0.0379 (3)0.0472 (6)
C80.80588 (14)0.6767 (2)0.0132 (4)0.0552 (7)
H8A0.75690.69930.06420.066*
C90.86733 (16)0.7513 (2)0.0109 (4)0.0608 (7)
H9A0.85880.82400.02270.073*
C100.94103 (16)0.7200 (3)0.0839 (4)0.0622 (8)
C110.95105 (16)0.6126 (3)0.1297 (4)0.0682 (8)
H11A1.00060.58960.17710.082*
C120.89054 (14)0.5364 (2)0.1086 (4)0.0608 (7)
H12A0.89940.46370.14160.073*
C130.56158 (13)0.19811 (19)0.1101 (3)0.0420 (5)
C140.47468 (13)0.3509 (2)0.1968 (3)0.0495 (6)
H14A0.46710.31860.31570.059*
H14B0.48290.42890.21260.059*
C150.40087 (15)0.3347 (2)0.0995 (4)0.0617 (8)
H15A0.35550.35230.18060.074*
H15B0.39680.25800.06760.074*
C161.0073 (2)0.8027 (3)0.1157 (5)0.0921 (11)
H16A1.05690.76490.13740.138*
H16B0.99680.84700.21840.138*
H16C1.01010.84860.01130.138*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0424 (10)0.0407 (11)0.0617 (13)0.0019 (9)0.0007 (9)0.0026 (9)
N20.0432 (11)0.0418 (11)0.0585 (13)0.0002 (9)0.0026 (9)0.0039 (9)
N40.0368 (10)0.0412 (11)0.0581 (13)0.0021 (8)0.0039 (9)0.0023 (9)
O10.0554 (10)0.0464 (10)0.0678 (12)0.0062 (8)0.0189 (9)0.0037 (8)
O20.0477 (10)0.0882 (14)0.0579 (12)0.0226 (9)0.0101 (8)0.0129 (10)
N30.0373 (10)0.0382 (11)0.0796 (15)0.0020 (8)0.0072 (10)0.0020 (10)
C10.0409 (12)0.0430 (13)0.0461 (13)0.0018 (10)0.0015 (10)0.0002 (10)
C20.0438 (12)0.0405 (13)0.0428 (13)0.0027 (10)0.0001 (10)0.0001 (10)
C30.0560 (15)0.0425 (14)0.0654 (17)0.0017 (11)0.0071 (12)0.0009 (12)
C40.0697 (18)0.0407 (14)0.082 (2)0.0094 (13)0.0100 (15)0.0012 (14)
C50.0509 (15)0.0536 (16)0.090 (2)0.0143 (12)0.0097 (14)0.0021 (15)
C60.0426 (13)0.0525 (16)0.0771 (19)0.0020 (11)0.0053 (12)0.0019 (13)
C70.0385 (12)0.0428 (13)0.0603 (15)0.0017 (10)0.0020 (11)0.0070 (11)
C80.0420 (13)0.0508 (15)0.0726 (18)0.0000 (11)0.0029 (12)0.0010 (13)
C90.0587 (16)0.0510 (16)0.0737 (18)0.0109 (12)0.0113 (14)0.0017 (13)
C100.0525 (15)0.0679 (18)0.0669 (18)0.0196 (13)0.0083 (13)0.0146 (15)
C110.0412 (14)0.078 (2)0.084 (2)0.0023 (13)0.0095 (13)0.0153 (17)
C120.0469 (14)0.0481 (14)0.086 (2)0.0037 (12)0.0122 (13)0.0078 (14)
C130.0422 (12)0.0436 (13)0.0398 (12)0.0002 (10)0.0004 (10)0.0004 (10)
C140.0487 (14)0.0481 (14)0.0508 (15)0.0031 (11)0.0051 (11)0.0011 (11)
C150.0456 (14)0.0737 (19)0.0643 (18)0.0056 (13)0.0097 (12)0.0006 (15)
C160.073 (2)0.103 (3)0.100 (3)0.043 (2)0.0043 (18)0.016 (2)
Geometric parameters (Å, °) top
N1—N21.264 (3)C6—H6A0.9300
N1—C11.417 (3)C7—C81.375 (4)
N2—N31.319 (3)C7—C121.381 (3)
N4—C131.329 (3)C8—C91.383 (3)
N4—C141.447 (3)C8—H8A0.9300
N4—H4A0.8600C9—C101.381 (4)
O1—C131.238 (3)C9—H9A0.9300
O2—C151.420 (3)C10—C111.363 (4)
O2—H2B0.8200C10—C161.513 (4)
N3—C71.395 (3)C11—C121.382 (4)
N3—H3A0.8600C11—H11A0.9300
C1—C61.393 (3)C12—H12A0.9300
C1—C21.404 (3)C14—C151.486 (4)
C2—C31.400 (3)C14—H14A0.9700
C2—C131.503 (3)C14—H14B0.9700
C3—C41.368 (3)C15—H15A0.9700
C3—H3B0.9300C15—H15B0.9700
C4—C51.376 (4)C16—H16A0.9600
C4—H4B0.9300C16—H16B0.9600
C5—C61.367 (4)C16—H16C0.9600
C5—H5A0.9300
N2—N1—C1114.01 (19)C10—C9—C8121.2 (3)
N1—N2—N3111.82 (19)C10—C9—H9A119.4
C13—N4—C14122.64 (19)C8—C9—H9A119.4
C13—N4—H4A118.7C11—C10—C9117.4 (2)
C14—N4—H4A118.7C11—C10—C16121.5 (3)
C15—O2—H2B109.5C9—C10—C16121.0 (3)
N2—N3—C7121.21 (19)C10—C11—C12122.6 (3)
N2—N3—H3A119.4C10—C11—H11A118.7
C7—N3—H3A119.4C12—C11—H11A118.7
C6—C1—C2119.0 (2)C7—C12—C11119.3 (3)
C6—C1—N1123.2 (2)C7—C12—H12A120.3
C2—C1—N1117.79 (19)C11—C12—H12A120.3
C3—C2—C1118.0 (2)O1—C13—N4121.8 (2)
C3—C2—C13115.7 (2)O1—C13—C2118.9 (2)
C1—C2—C13126.3 (2)N4—C13—C2119.3 (2)
C4—C3—C2121.7 (2)N4—C14—C15114.9 (2)
C4—C3—H3B119.1N4—C14—H14A108.5
C2—C3—H3B119.1C15—C14—H14A108.5
C3—C4—C5119.9 (3)N4—C14—H14B108.5
C3—C4—H4B120.1C15—C14—H14B108.5
C5—C4—H4B120.1H14A—C14—H14B107.5
C6—C5—C4119.8 (2)O2—C15—C14114.5 (2)
C6—C5—H5A120.1O2—C15—H15A108.6
C4—C5—H5A120.1C14—C15—H15A108.6
C5—C6—C1121.5 (2)O2—C15—H15B108.6
C5—C6—H6A119.3C14—C15—H15B108.6
C1—C6—H6A119.3H15A—C15—H15B107.6
C8—C7—C12119.1 (2)C10—C16—H16A109.5
C8—C7—N3118.6 (2)C10—C16—H16B109.5
C12—C7—N3122.3 (2)H16A—C16—H16B109.5
C7—C8—C9120.3 (2)C10—C16—H16C109.5
C7—C8—H8A119.8H16A—C16—H16C109.5
C9—C8—H8A119.8H16B—C16—H16C109.5
C1—N1—N2—N3178.6 (2)N3—C7—C8—C9179.6 (2)
N1—N2—N3—C7177.7 (2)C7—C8—C9—C100.9 (4)
N2—N1—C1—C63.2 (3)C8—C9—C10—C110.6 (4)
N2—N1—C1—C2176.6 (2)C8—C9—C10—C16178.0 (3)
C6—C1—C2—C32.7 (3)C9—C10—C11—C121.2 (4)
N1—C1—C2—C3177.6 (2)C16—C10—C11—C12177.4 (3)
C6—C1—C2—C13174.8 (2)C8—C7—C12—C111.3 (4)
N1—C1—C2—C135.0 (3)N3—C7—C12—C11179.8 (2)
C1—C2—C3—C42.1 (4)C10—C11—C12—C70.2 (5)
C13—C2—C3—C4175.6 (2)C14—N4—C13—O16.1 (4)
C2—C3—C4—C50.5 (4)C14—N4—C13—C2173.9 (2)
C3—C4—C5—C62.5 (5)C3—C2—C13—O111.0 (3)
C4—C5—C6—C12.0 (5)C1—C2—C13—O1166.5 (2)
C2—C1—C6—C50.7 (4)C3—C2—C13—N4169.0 (2)
N1—C1—C6—C5179.5 (3)C1—C2—C13—N413.5 (3)
N2—N3—C7—C8169.7 (2)C13—N4—C14—C1576.5 (3)
N2—N3—C7—C128.8 (4)N4—C14—C15—O271.8 (3)
C12—C7—C8—C91.9 (4)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
N4—H4A···N10.862.052.696 (3)132
O2—H2B···O1i0.821.922.729 (2)169
N3—H3A···O2ii0.862.002.851 (2)170
Symmetry codes: (i) x, −y+1/2, z+1/2; (ii) −x+1, −y+1, −z.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
N4—H4A···N10.862.052.696 (3)132
O2—H2B···O1i0.821.922.729 (2)169
N3—H3A···O2ii0.862.002.851 (2)170
Symmetry codes: (i) x, −y+1/2, z+1/2; (ii) −x+1, −y+1, −z.
Acknowledgements top

We gratefully acknowledge support for this project by Consejo Nacional de Ciencia y Tecnología (CONACyT grant 60467), Consejo del Sistema Nacional de EducaciónTecnológica (COSNET grant 486–02-P) and a graduate scholarship from CONACyT for F. Rocha-Alonzo. The authors are indebted to Adrián Ochoa Terán and Ignacio Rivero Espejel for their support in this work. We acknowledge Universidad Autónoma de Nuevo-León (Monterrey, México) for diffractometer time.

references
References top

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