Literature DB >> 21582899

N-Phenyl-formamide.

B Thimme Gowda, Sabine Foro, Hartmut Fuess.   

Abstract

There are two independent mol-ecules in the asymmetric unit of the title compound, C(7)H(7)NO. The conformation of the N-H bond in the structure is syn to the C=O bond in one of the mol-ecules and anti in the other. In the crystal, mol-ecules are packed into chains diagonally in the ac plane via N-H⋯O hydrogen bonds.

Entities:  

Year:  2009        PMID: 21582899      PMCID: PMC2969504          DOI: 10.1107/S1600536809022776

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


Related literature

For related structures, see: Gowda et al. (2006 ▶); Brown (1966 ▶). For our study of the effect of ring and side chain substitutions on the crystal structures of aromatic amides, see: Gowda et al. (2000 ▶, 2007 ▶, 2009 ▶).

Experimental

Crystal data

C7H7NO M = 121.14 Monoclinic, a = 30.923 (3) Å b = 6.1737 (6) Å c = 14.814 (1) Å β = 113.14 (1)° V = 2600.6 (4) Å3 Z = 16 Mo Kα radiation μ = 0.08 mm−1 T = 298 K 0.48 × 0.44 × 0.40 mm

Data collection

Oxford Diffraction Xcalibur diffractometer with a Sapphire CCD detector Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009 ▶) T min = 0.966, T max = 0.969 8394 measured reflections 2383 independent reflections 1679 reflections with I > 2σ(I) R int = 0.016

Refinement

R[F 2 > 2σ(F 2)] = 0.037 wR(F 2) = 0.115 S = 1.12 2383 reflections 170 parameters H atoms treated by a mixture of independent and constrained refinement Δρmax = 0.11 e Å−3 Δρmin = −0.10 e Å−3 Data collection: CrysAlis CCD (Oxford Diffraction, 2009 ▶); cell refinement: CrysAlis RED (Oxford Diffraction, 2009 ▶); data reduction: CrysAlis RED; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: PLATON (Spek, 2009 ▶); software used to prepare material for publication: SHELXL97. Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809022776/rk2151sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536809022776/rk2151Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C7H7NOF(000) = 1024
Mr = 121.14Dx = 1.238 Mg m3
Monoclinic, C2/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -C 2ycCell parameters from 2475 reflections
a = 30.923 (3) Åθ = 2.7–28.2°
b = 6.1737 (6) ŵ = 0.08 mm1
c = 14.814 (1) ÅT = 298 K
β = 113.14 (1)°Needle, colourless
V = 2600.6 (4) Å30.48 × 0.44 × 0.40 mm
Z = 16
Oxford Diffraction Xcalibur diffractometer with a Sapphire CCD detector2383 independent reflections
Radiation source: Fine–focus sealed tube1679 reflections with I > 2σ(I)
GraphiteRint = 0.016
ω and φ scansθmax = 25.4°, θmin = 2.8°
Absorption correction: multi-scan (CrysAlis RED; Oxford Diffraction, 2009)h = −37→36
Tmin = 0.966, Tmax = 0.969k = −7→7
8394 measured reflectionsl = −17→17
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.037H atoms treated by a mixture of independent and constrained refinement
wR(F2) = 0.115w = 1/[σ2(Fo2) + (0.0651P)2] where P = (Fo2 + 2Fc2)/3
S = 1.12(Δ/σ)max < 0.001
2383 reflectionsΔρmax = 0.11 e Å3
170 parametersΔρmin = −0.10 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: 0.0028 (7)
Experimental. Absorption correction: CrysAlis RED (Oxford Diffraction, 2009); empirical absorption correction using spherical harmonics, implemented in SCALE3 ABSPACK scaling algorithm.
Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(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
O10.09999 (4)0.21410 (18)0.62537 (8)0.0921 (4)
N10.04841 (4)0.34831 (19)0.47961 (9)0.0694 (4)
H1N0.0202 (6)0.322 (2)0.4332 (11)0.083*
C10.07229 (4)0.5289 (2)0.46365 (9)0.0561 (3)
C20.04734 (5)0.6657 (3)0.38753 (10)0.0727 (4)
H20.01590.63670.34910.087*
C30.06857 (6)0.8441 (3)0.36825 (12)0.0893 (5)
H30.05150.93510.31640.107*
C40.11462 (6)0.8895 (3)0.42461 (12)0.0890 (5)
H40.12891.01190.41190.107*
C50.13948 (6)0.7535 (3)0.49972 (12)0.0828 (5)
H50.17090.78340.53780.099*
C60.11890 (5)0.5734 (2)0.51989 (11)0.0687 (4)
H60.13630.48180.57120.082*
C70.06296 (6)0.2094 (2)0.55435 (12)0.0792 (5)
H70.04260.09660.55180.095*
O20.04140 (4)0.2563 (2)0.16582 (9)0.0996 (4)
N20.11861 (4)0.1904 (2)0.22825 (8)0.0628 (3)
H2N0.1131 (5)0.067 (3)0.1994 (10)0.075*
C80.16640 (5)0.2389 (2)0.28235 (9)0.0565 (3)
C90.18179 (6)0.4299 (3)0.33258 (13)0.0862 (5)
H90.16030.53690.33090.103*
C100.22921 (7)0.4618 (3)0.38543 (14)0.1024 (6)
H100.23940.59010.42020.123*
C110.26131 (6)0.3093 (3)0.38760 (14)0.0963 (6)
H110.29320.33240.42350.116*
C120.24605 (6)0.1230 (3)0.33668 (13)0.0919 (5)
H120.26780.01840.33710.110*
C130.19895 (5)0.0867 (2)0.28451 (11)0.0750 (4)
H130.1891−0.04250.25030.090*
C140.08175 (6)0.3109 (3)0.21441 (12)0.0771 (4)
H140.08670.44710.24360.093*
U11U22U33U12U13U23
O10.0813 (8)0.0791 (7)0.0881 (8)−0.0120 (6)0.0032 (6)0.0215 (5)
N10.0527 (7)0.0658 (8)0.0743 (8)−0.0096 (6)0.0082 (6)0.0067 (6)
C10.0522 (8)0.0564 (8)0.0570 (7)−0.0001 (6)0.0186 (6)−0.0032 (6)
C20.0644 (9)0.0780 (10)0.0644 (9)−0.0023 (7)0.0131 (7)0.0049 (7)
C30.1006 (14)0.0823 (11)0.0750 (10)−0.0058 (10)0.0236 (9)0.0207 (9)
C40.0993 (14)0.0849 (12)0.0826 (11)−0.0263 (10)0.0355 (10)0.0063 (9)
C50.0682 (10)0.0902 (12)0.0847 (11)−0.0210 (9)0.0242 (8)0.0026 (9)
C60.0555 (8)0.0699 (9)0.0742 (9)−0.0033 (7)0.0184 (7)0.0063 (7)
C70.0714 (10)0.0648 (9)0.0897 (11)−0.0116 (8)0.0189 (9)0.0098 (8)
O20.0556 (7)0.1164 (10)0.1092 (9)0.0152 (6)0.0132 (6)0.0123 (7)
N20.0567 (7)0.0615 (7)0.0645 (7)0.0048 (6)0.0175 (6)−0.0040 (5)
C80.0557 (8)0.0602 (8)0.0522 (7)−0.0013 (6)0.0197 (6)0.0026 (6)
C90.0790 (12)0.0746 (10)0.1005 (12)−0.0037 (8)0.0303 (9)−0.0202 (9)
C100.0939 (14)0.0939 (13)0.1047 (13)−0.0311 (11)0.0233 (11)−0.0271 (10)
C110.0647 (11)0.1055 (15)0.0999 (13)−0.0158 (11)0.0122 (9)0.0068 (11)
C120.0601 (10)0.0924 (12)0.1119 (13)0.0070 (9)0.0218 (9)0.0067 (10)
C130.0618 (9)0.0680 (9)0.0873 (10)0.0029 (7)0.0209 (8)−0.0064 (7)
C140.0667 (11)0.0739 (10)0.0865 (11)0.0132 (8)0.0256 (9)0.0104 (8)
O1—C71.2132 (17)O2—C141.2178 (18)
N1—C71.3314 (19)N2—C141.3082 (19)
N1—C11.4076 (17)N2—C81.4089 (17)
N1—H1N0.888 (16)N2—H2N0.857 (16)
C1—C21.3771 (19)C8—C131.3684 (19)
C1—C61.3797 (18)C8—C91.375 (2)
C2—C31.369 (2)C9—C101.378 (2)
C2—H20.9300C9—H90.9300
C3—C41.367 (2)C10—C111.359 (3)
C3—H30.9300C10—H100.9300
C4—C51.365 (2)C11—C121.354 (3)
C4—H40.9300C11—H110.9300
C5—C61.371 (2)C12—C131.373 (2)
C5—H50.9300C12—H120.9300
C6—H60.9300C13—H130.9300
C7—H70.9300C14—H140.9300
C7—N1—C1128.45 (13)C14—N2—C8128.51 (14)
C7—N1—H1N115.8 (10)C14—N2—H2N115.9 (10)
C1—N1—H1N115.7 (10)C8—N2—H2N115.6 (10)
C2—C1—C6119.24 (13)C13—C8—C9118.76 (14)
C2—C1—N1117.46 (12)C13—C8—N2117.69 (12)
C6—C1—N1123.29 (12)C9—C8—N2123.55 (13)
C3—C2—C1120.27 (14)C8—C9—C10119.64 (16)
C3—C2—H2119.9C8—C9—H9120.2
C1—C2—H2119.9C10—C9—H9120.2
C4—C3—C2120.51 (15)C11—C10—C9121.22 (17)
C4—C3—H3119.7C11—C10—H10119.4
C2—C3—H3119.7C9—C10—H10119.4
C5—C4—C3119.30 (15)C12—C11—C10118.93 (17)
C5—C4—H4120.4C12—C11—H11120.5
C3—C4—H4120.4C10—C11—H11120.5
C4—C5—C6121.06 (15)C11—C12—C13120.85 (17)
C4—C5—H5119.5C11—C12—H12119.6
C6—C5—H5119.5C13—C12—H12119.6
C5—C6—C1119.62 (14)C8—C13—C12120.59 (15)
C5—C6—H6120.2C8—C13—H13119.7
C1—C6—H6120.2C12—C13—H13119.7
O1—C7—N1126.94 (14)O2—C14—N2124.22 (16)
O1—C7—H7116.5O2—C14—H14117.9
N1—C7—H7116.5N2—C14—H14117.9
C7—N1—C1—C2−171.26 (15)C14—N2—C8—C13−178.73 (14)
C7—N1—C1—C69.0 (2)C14—N2—C8—C91.3 (2)
C6—C1—C2—C3−0.2 (2)C13—C8—C9—C10−1.4 (2)
N1—C1—C2—C3180.00 (14)N2—C8—C9—C10178.58 (15)
C1—C2—C3—C4−0.5 (3)C8—C9—C10—C111.1 (3)
C2—C3—C4—C50.8 (3)C9—C10—C11—C120.0 (3)
C3—C4—C5—C6−0.5 (3)C10—C11—C12—C13−0.8 (3)
C4—C5—C6—C1−0.2 (2)C9—C8—C13—C120.7 (2)
C2—C1—C6—C50.5 (2)N2—C8—C13—C12−179.34 (13)
N1—C1—C6—C5−179.70 (14)C11—C12—C13—C80.4 (3)
C1—N1—C7—O11.5 (3)C8—N2—C14—O2179.62 (13)
D—H···AD—HH···AD···AD—H···A
N1—H1N···O2i0.888 (16)1.936 (16)2.8239 (17)178.1 (14)
N2—H2N···O1ii0.857 (16)2.007 (16)2.8637 (17)177.0 (14)
Table 1

Hydrogen-bond geometry (Å, °)

D—H⋯AD—HH⋯ADAD—H⋯A
N1—H1N⋯O2i0.888 (16)1.936 (16)2.8239 (17)178.1 (14)
N2—H2N⋯O1ii0.857 (16)2.007 (16)2.8637 (17)177.0 (14)

Symmetry codes: (i) ; (ii) .

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