organic compounds
2-Cyano-2-methylpropanamide
aCollege of Chemical and Biological Engineering, Yancheng Institute of Technology, Yinbing Road No. 9 Yancheng, Yancheng 224051, People's Republic of China, and bDepartment of Chemical Engineering, Yancheng College of Textile Technology, People's Republic of China
*Correspondence e-mail: xujiaying-1984@163.com
In the 5H8N2O, molecules are linked via pairs of N—H⋯O hydrogen bonds, forming inversion dimers. These dimers are linked via pairs of N—H⋯H hydrogen bonds into zigzag chains propagating along [101].
of the title compound, CRelated literature
For the synthesis of the title compound, see: Zhang et al. (2011). For standard bond-length data, see: Allen et al. (1987).
Experimental
Crystal data
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Refinement
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Data collection: CAD-4 Software (Enraf–Nonius, 1985); cell CAD-4 Software; data reduction: XCAD4 (Harms & Wocadlo, 1995); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL.
Supporting information
10.1107/S1600536812013360/su2395sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536812013360/su2395Isup2.hkl
Supporting information file. DOI: 10.1107/S1600536812013360/su2395Isup3.cml
The title compound was prepared by the literature procedure (Zhang et al., 2011). To a solution of methyl 2-cyano-2-methylpropanoate (5 g, 39.3 mmol) in methanol (20 ml), ammonia was added slowly at room temperature. After being stirred for 18 h at the room tempreature, a yellow solid was obtained. It was dissolved in ethanol and colourless block-like crystals of the title compound, suitable for X-ray
were obtained by slow evaporation of the solvent over 7 days.The NH2 H atoms were located in a difference
and refined freely. The methyl H atoms were positioned geometrically and constrained to ride on their parent atoms: C—H = 0.96 Å with Uiso(H) = 1.5Ueq(C).The title compound has attracted considerable attention in drug research because of its outstanding biological activity. In recent years it has been used as an imtermediate in the synthesis of the high blood pressure rennin inhibitor, Aliskiren (Zhang et al., 2011).
The molecular structure of the title compound is shown in Fig. 1. The bond lengths (Allen et al., 1987) and angles are within normal ranges.
In the crystal, molecules are connected via pairs of N—H···O hydrogen bonds to form inversion dimers (Table 1 and Fig. 2). These dimers are connected via pairs of N—H···N hydrogen bonds resulting in the formation of zigzag chains (Table 1 and Fig. 2), propagating along direction [101].
For the synthesis of the title compound, see: Zhang et al. (2011). For standard bond-length data, see: Allen et al. (1987).
Data collection: CAD-4 Software (Enraf–Nonius, 1985); cell
CAD-4 Software (Enraf–Nonius, 1985); data reduction: XCAD4 (Harms & Wocadlo, 1995); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).C5H8N2O | Z = 2 |
Mr = 112.13 | F(000) = 120 |
Triclinic, P1 | Dx = 1.193 Mg m−3 |
Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
a = 5.8916 (12) Å | Cell parameters from 1603 reflections |
b = 6.4349 (14) Å | θ = 2.3–30.1° |
c = 9.1263 (19) Å | µ = 0.09 mm−1 |
α = 95.659 (4)° | T = 293 K |
β = 102.379 (4)° | Block, colourless |
γ = 109.859 (4)° | 0.20 × 0.18 × 0.15 mm |
V = 312.27 (11) Å3 |
Enraf–Nonius CAD-4 diffractometer | 1000 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.021 |
Graphite monochromator | θmax = 25.0°, θmin = 2.3° |
ω/2θ scans | h = −6→6 |
Absorption correction: ψ scan (North et al., 1968) | k = −6→7 |
Tmin = 0.983, Tmax = 0.987 | l = −10→7 |
1699 measured reflections | 3 standard reflections every 200 reflections |
1077 independent reflections | intensity decay: 1% |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.050 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.143 | w = 1/[σ2(Fo2) + (0.1061P)2 + 0.0265P] where P = (Fo2 + 2Fc2)/3 |
S = 1.05 | (Δ/σ)max < 0.001 |
1077 reflections | Δρmax = 0.26 e Å−3 |
84 parameters | Δρmin = −0.26 e Å−3 |
0 restraints | Extinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 2.05 (18) |
C5H8N2O | γ = 109.859 (4)° |
Mr = 112.13 | V = 312.27 (11) Å3 |
Triclinic, P1 | Z = 2 |
a = 5.8916 (12) Å | Mo Kα radiation |
b = 6.4349 (14) Å | µ = 0.09 mm−1 |
c = 9.1263 (19) Å | T = 293 K |
α = 95.659 (4)° | 0.20 × 0.18 × 0.15 mm |
β = 102.379 (4)° |
Enraf–Nonius CAD-4 diffractometer | 1000 reflections with I > 2σ(I) |
Absorption correction: ψ scan (North et al., 1968) | Rint = 0.021 |
Tmin = 0.983, Tmax = 0.987 | 3 standard reflections every 200 reflections |
1699 measured reflections | intensity decay: 1% |
1077 independent reflections |
R[F2 > 2σ(F2)] = 0.050 | 0 restraints |
wR(F2) = 0.143 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.05 | Δρmax = 0.26 e Å−3 |
1077 reflections | Δρmin = −0.26 e Å−3 |
84 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
O1 | 0.29396 (18) | 0.69885 (17) | 0.01288 (11) | 0.0555 (4) | |
N1 | 0.2126 (2) | 0.51350 (19) | 0.20281 (15) | 0.0495 (5) | |
N2 | 0.7598 (2) | 0.6725 (2) | 0.48798 (16) | 0.0644 (5) | |
C1 | 0.6955 (2) | 0.7399 (2) | 0.38232 (15) | 0.0448 (5) | |
C2 | 0.6156 (2) | 0.83173 (18) | 0.24687 (13) | 0.0364 (4) | |
C3 | 0.8132 (2) | 0.8719 (2) | 0.15614 (16) | 0.0479 (5) | |
H3A | 0.9726 | 0.9721 | 0.2208 | 0.072* | |
H3B | 0.7658 | 0.9376 | 0.0703 | 0.072* | |
H3C | 0.8246 | 0.7312 | 0.1206 | 0.072* | |
C4 | 0.5862 (3) | 1.0547 (2) | 0.29886 (16) | 0.0494 (5) | |
H4A | 0.4580 | 1.0266 | 0.3521 | 0.074* | |
H4B | 0.5407 | 1.1176 | 0.2112 | 0.074* | |
H4C | 0.7418 | 1.1586 | 0.3656 | 0.074* | |
C5 | 0.3573 (2) | 0.66995 (19) | 0.14359 (14) | 0.0381 (4) | |
H1A | 0.059 (4) | 0.429 (3) | 0.138 (2) | 0.069 (5)* | |
H1B | 0.254 (4) | 0.491 (3) | 0.296 (2) | 0.064 (5)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
O1 | 0.0468 (7) | 0.0567 (7) | 0.0374 (6) | −0.0025 (5) | −0.0094 (4) | 0.0185 (5) |
N1 | 0.0391 (7) | 0.0511 (8) | 0.0394 (7) | 0.0004 (5) | −0.0051 (5) | 0.0174 (5) |
N2 | 0.0506 (8) | 0.0740 (9) | 0.0501 (8) | 0.0094 (6) | −0.0086 (6) | 0.0274 (7) |
C1 | 0.0344 (7) | 0.0472 (7) | 0.0392 (8) | 0.0058 (5) | −0.0033 (5) | 0.0101 (6) |
C2 | 0.0332 (7) | 0.0376 (7) | 0.0308 (7) | 0.0087 (5) | −0.0002 (5) | 0.0073 (5) |
C3 | 0.0390 (7) | 0.0570 (8) | 0.0438 (8) | 0.0150 (6) | 0.0075 (6) | 0.0102 (6) |
C4 | 0.0487 (8) | 0.0470 (8) | 0.0447 (8) | 0.0170 (6) | 0.0013 (6) | 0.0001 (6) |
C5 | 0.0360 (7) | 0.0366 (7) | 0.0328 (7) | 0.0086 (5) | −0.0018 (5) | 0.0087 (5) |
O1—C5 | 1.2234 (16) | C2—C5 | 1.5504 (15) |
N1—C5 | 1.3243 (17) | C3—H3A | 0.9600 |
N1—H1A | 0.92 (2) | C3—H3B | 0.9600 |
N1—H1B | 0.88 (2) | C3—H3C | 0.9600 |
N2—C1 | 1.1395 (18) | C4—H4A | 0.9600 |
C1—C2 | 1.4774 (17) | C4—H4B | 0.9600 |
C2—C3 | 1.5356 (18) | C4—H4C | 0.9600 |
C2—C4 | 1.5438 (18) | ||
C5—N1—H1A | 114.6 (12) | C2—C3—H3C | 109.5 |
C5—N1—H1B | 124.9 (12) | H3A—C3—H3C | 109.5 |
H1A—N1—H1B | 120.5 (18) | H3B—C3—H3C | 109.5 |
N2—C1—C2 | 178.86 (14) | C2—C4—H4A | 109.5 |
C1—C2—C3 | 109.07 (10) | C2—C4—H4B | 109.5 |
C1—C2—C4 | 109.37 (10) | H4A—C4—H4B | 109.5 |
C3—C2—C4 | 110.22 (10) | C2—C4—H4C | 109.5 |
C1—C2—C5 | 111.37 (9) | H4A—C4—H4C | 109.5 |
C3—C2—C5 | 109.91 (10) | H4B—C4—H4C | 109.5 |
C4—C2—C5 | 106.88 (10) | O1—C5—N1 | 123.35 (11) |
C2—C3—H3A | 109.5 | O1—C5—C2 | 118.09 (10) |
C2—C3—H3B | 109.5 | N1—C5—C2 | 118.50 (10) |
H3A—C3—H3B | 109.5 | ||
N2—C1—C2—C3 | 78 (8) | C4—C2—C5—O1 | 76.58 (15) |
N2—C1—C2—C4 | −42 (8) | C1—C2—C5—N1 | 18.55 (16) |
N2—C1—C2—C5 | −160 (8) | C3—C2—C5—N1 | 139.54 (12) |
C1—C2—C5—O1 | −164.02 (12) | C4—C2—C5—N1 | −100.85 (14) |
C3—C2—C5—O1 | −43.03 (15) |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1A···O1i | 0.92 (2) | 2.07 (2) | 2.9714 (18) | 168.2 (18) |
N1—H1B···N2ii | 0.874 (18) | 2.328 (18) | 3.166 (2) | 160.8 (19) |
Symmetry codes: (i) −x, −y+1, −z; (ii) −x+1, −y+1, −z+1. |
Experimental details
Crystal data | |
Chemical formula | C5H8N2O |
Mr | 112.13 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 293 |
a, b, c (Å) | 5.8916 (12), 6.4349 (14), 9.1263 (19) |
α, β, γ (°) | 95.659 (4), 102.379 (4), 109.859 (4) |
V (Å3) | 312.27 (11) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 0.09 |
Crystal size (mm) | 0.20 × 0.18 × 0.15 |
Data collection | |
Diffractometer | Enraf–Nonius CAD-4 |
Absorption correction | ψ scan (North et al., 1968) |
Tmin, Tmax | 0.983, 0.987 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 1699, 1077, 1000 |
Rint | 0.021 |
(sin θ/λ)max (Å−1) | 0.594 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.050, 0.143, 1.05 |
No. of reflections | 1077 |
No. of parameters | 84 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.26, −0.26 |
Computer programs: CAD-4 Software (Enraf–Nonius, 1985), XCAD4 (Harms & Wocadlo, 1995), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), SHELXTL (Sheldrick, 2008).
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1A···O1i | 0.92 (2) | 2.07 (2) | 2.9714 (18) | 168.2 (18) |
N1—H1B···N2ii | 0.874 (18) | 2.328 (18) | 3.166 (2) | 160.8 (19) |
Symmetry codes: (i) −x, −y+1, −z; (ii) −x+1, −y+1, −z+1. |
Acknowledgements
The authors thank the Center of Testing and Analysis, Nanjing University, for the data collection. They also thank the Foundation of Yancheng Institute of Technology (XKR2010055) and the National Natural Science Foundation of China (No. 31000142) for financial support.
References
Allen, F. H., Kennard, O., Watson, D. G., Brammer, L., Orpen, A. G. & Taylor, R. (1987). J. Chem. Soc. Perkin Trans. 2, pp. S1–19. CSD CrossRef Web of Science Google Scholar
Enraf–Nonius (1985). CAD-4 Software. Enraf–Nonius, Delft, The Netherlands. Google Scholar
Harms, K. & Wocadlo, S. (1995). XCAD4. University of Marburg, Germany. Google Scholar
North, A. C. T., Phillips, D. C. & Mathews, F. S. (1968). Acta Cryst. A24, 351–359. CrossRef IUCr Journals Web of Science Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
Zhang, W. L., Wang, P. & Gan, L. X. (2011). Patent Pub. No. WO/2011/091677; Int. Appl. No. PCT/CN2010/078549. Google Scholar
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The title compound has attracted considerable attention in drug research because of its outstanding biological activity. In recent years it has been used as an imtermediate in the synthesis of the high blood pressure rennin inhibitor, Aliskiren (Zhang et al., 2011).
The molecular structure of the title compound is shown in Fig. 1. The bond lengths (Allen et al., 1987) and angles are within normal ranges.
In the crystal, molecules are connected via pairs of N—H···O hydrogen bonds to form inversion dimers (Table 1 and Fig. 2). These dimers are connected via pairs of N—H···N hydrogen bonds resulting in the formation of zigzag chains (Table 1 and Fig. 2), propagating along direction [101].