organic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

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ISSN: 2056-9890
Volume 65| Part 5| May 2009| Page o1115

N-Benzyl-2-propynamide

aDepartment of Pharmacy, Medical College of Xiamen University, Xiamen 361005, People's Republic of China, bDepartment of Chemistry and the Key Laboratory for Chemical Biology of Fujian Province, College of Chemistry and Chemical Engineering, Xiamen University, Xiamen 361005, People's Republic of China, and cThe Third Institute of Oceanography, State Oceanic Administration of China, Xiamen 361005, People's Republic of China
*Correspondence e-mail: daxiong@xmu.edu.cn

(Received 8 March 2009; accepted 19 April 2009; online 25 April 2009)

Pale-yellow crystals of the title compound, C10H9NO, have been obtained by the reaction of benzyl­amine and methyl propiolate. Weak inter­molecular hydrogen bonding is observed between acetyl­enic H and carbonyl O atoms. The crystal packing is stabilized by these C—H⋯O and by N—H⋯O inter­molecular hydrogen-bonding inter­actions.

Related literature

The title compound was synthesized using a similar synthetic method to that described by Williamson et al. (1994[Williamson, B. L., Tykwinski, R. R. & Stang, P. J. (1994). J. Am. Chem. Soc. 116, 93-98.]). For the synthesis of triazole derivatives, see: Katritzky & Singh (2002[Katritzky, A. R. & Singh, K. (2002). J. Org. Chem. 67, 9077-9079.]). For the structure of the methyl analogue of the title compound, see: Leiserowitz & Tuval (1978[Leiserowitz, L. & Tuval, M. (1978). Acta Cryst. B34, 1230-1247.]). For the program ROTAX, used to investigate possible pseudo-merohedral twinning, see: Parsons & Gould (2003[ Parsons, S. & Gould, B. (2003). ROTAX. University of Edinburgh, Scotland.]).

[Scheme 1]

Experimental

Crystal data
  • C10H9NO

  • Mr = 159.18

  • Monoclinic, P 21 /c

  • a = 9.495 (2) Å

  • b = 10.703 (2) Å

  • c = 8.9120 (19) Å

  • β = 101.637 (3)°

  • V = 887.1 (3) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 0.08 mm−1

  • T = 173 K

  • 0.57 × 0.30 × 0.30 mm

Data collection
  • Bruker SMART APEX area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2001[Bruker (2001). SAINT, SMART and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.]) Tmin = 0.848, Tmax = 1.000 (expected range = 0.828–0.977)

  • 5825 measured reflections

  • 1550 independent reflections

  • 1510 reflections with I > 2σ(I)

  • Rint = 0.030

Refinement
  • R[F2 > 2σ(F2)] = 0.070

  • wR(F2) = 0.221

  • S = 1.26

  • 1550 reflections

  • 113 parameters

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.45 e Å−3

  • Δρmin = −0.23 e Å−3

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1A⋯O1i 0.88 1.99 2.839 (3) 163
C1—H1⋯O1ii 0.93 (4) 2.17 (4) 3.105 (4) 176 (3)
Symmetry codes: (i) [x, -y+{\script{1\over 2}}, z+{\script{1\over 2}}]; (ii) [-x+2, y-{\script{1\over 2}}, -z+{\script{1\over 2}}].

Data collection: SMART (Bruker, 2001[Bruker (2001). SAINT, SMART and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.]); cell refinement: SAINT (Bruker, 2001[Bruker (2001). SAINT, SMART and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.]); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008[Sheldrick, G. M. (2008). Acta Cryst. A64, 112-122.]); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997[Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565.]); software used to prepare material for publication: SHELXL97.

Supporting information


Comment top

The title compound is a terminal alkyne, which is an intermediate in the synthesis of triazole derivatives (Katritzky et al., 2002).

The molecular structure of the title compound is shown in Fig. 1. The bond lengths and bond angles in the compound are comparable to those in the structure of the methyl analogue (Leiserowitz et al., 1978). The atoms C1, C2, C3, O1, N1 and C4 of the title compound are nearly in a plane, and the r.m.s. deviation of these atoms from their mean plane is 0.007 Å. The dihedral angle between the plane of C5 and the phenyl ring and the mean plane of C1 to C4 and N1 is 76.8 (2)°. Hydrogen bonding plays a significant role in stabilizing the crystal structure; see Table 1 for geometric parameters and symmetry operations. The most prominent link occurs between the acylamide O and the N atoms, to form chains along the b axis. Weak intermolecular hydrogen bonding is observed between the alkyne H and the carbonyl O atoms (table 1). Molecules are connected into a double chain by C—H···O and N—H···O intermolecular hydrogen-bonding interactions (Figure 2).

Related literature top

The title compound was synthesized using a similar synthetic method to that described by Williamson et al. (1994). For the synthesis of triazole derivatives, see: Katritzky et al. (2002). For the structure of the methyl analogue of the title compound, see: Leiserowitz et al. (1978). For the program ROTAX, used to investigate possible pseudo-merohedral twinning, see: Parsons & Gould (2003).

Experimental top

The title compound was synthesized using a similar synthetic method as for the preparation of 1-(pyrrolidin-1-yl)prop-2-yn-1-one (Williamson et al., 1994). To a solution of benzyl amine (1.07 g, 10 mmol) in methanol (4 ml) was slowly added methyl propiolate (0.84 g, 10 mmol) at 195 K with stirring. After addition of the propiolate, the stirring was continued for 10 h and then the mixture warmed to 248 K for 5 h. The reaction was quenched with a saturated NH4Cl solution (12 ml) and extracted with ethyl acetate. The organic layer was washed with brine, dried over anhydrous MgSO4, concentrated under vacuum and the crude product was purified by column chromatography (petroleum ether: ethyl acetate, 2:1) to give the title compound as a pale yellow solid in 72% yield. Single crystals of the title compound were grown in a petroleum ether/ethyl acetate solution (v/v = 5:1) by slow evaporation.

Refinement top

All non-hydrogen atoms were refined anisotropically. The acetylenic H atom was located from a difference Fourier map and both the position and isotropic thermal parameter were freely refined. The remaining H atoms were placed in ideal positions and refined via a riding model with N-H distances of 0.88, C-Hmethyelene = 0.99 and C-Haromatic = 0.95 Å and Uiso = 1.2 Ueq(C,N). Torsion angles were refined to fit the electron density. The metric parameters suggest the possibility of pseudo-merohedral twinning by a two fold rotation around either the a or the c axis. Application of the respective twin law of (-1 0 - 0.43, 0 1 0, 0 0 1), obtained using the program Rotax (Parsons & Gould, 2003)) however indicated that the crystal at hand was not twinned.

Computing details top

Data collection: SMART (Bruker, 2001); cell refinement: SAINT (Bruker, 2001); data reduction: SAINT (Bruker, 2001); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: SHELXL97 (Sheldrick, 2008.

Figures top
[Figure 1] Fig. 1. The molecular structure of the compound with 50% probability displacement ellipsoids (arbitrary spheres for H atoms).
[Figure 2] Fig. 2. Part of the packing of the title compound. Intermolecular hydrogen bonds are represented by dashed lines.
N-benzyl-2-propynamide top
Crystal data top
C10H9NOF(000) = 336
Mr = 159.18Dx = 1.192 Mg m3
Monoclinic, P21/cMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybcCell parameters from 4373 reflections
a = 9.495 (2) Åθ = 2.2–28.3°
b = 10.703 (2) ŵ = 0.08 mm1
c = 8.9120 (19) ÅT = 173 K
β = 101.637 (3)°Chunk, pale yellow
V = 887.1 (3) Å30.57 × 0.30 × 0.30 mm
Z = 4
Data collection top
Bruker APEX area-detector
diffractometer
1550 independent reflections
Radiation source: fine-focus sealed tube1510 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.030
ϕ and ω scansθmax = 25.0°, θmin = 2.9°
Absorption correction: multi-scan
(SADABS; Bruker, 2001)
h = 1111
Tmin = 0.848, Tmax = 1.000k = 1212
5825 measured reflectionsl = 1010
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.070Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.221H atoms treated by a mixture of independent and constrained refinement
S = 1.26 w = 1/[σ2(Fo2) + (0.0874P)2 + 1.0844P]
where P = (Fo2 + 2Fc2)/3
1550 reflections(Δ/σ)max < 0.001
113 parametersΔρmax = 0.45 e Å3
0 restraintsΔρmin = 0.23 e Å3
Crystal data top
C10H9NOV = 887.1 (3) Å3
Mr = 159.18Z = 4
Monoclinic, P21/cMo Kα radiation
a = 9.495 (2) ŵ = 0.08 mm1
b = 10.703 (2) ÅT = 173 K
c = 8.9120 (19) Å0.57 × 0.30 × 0.30 mm
β = 101.637 (3)°
Data collection top
Bruker APEX area-detector
diffractometer
1550 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2001)
1510 reflections with I > 2σ(I)
Tmin = 0.848, Tmax = 1.000Rint = 0.030
5825 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0700 restraints
wR(F2) = 0.221H atoms treated by a mixture of independent and constrained refinement
S = 1.26Δρmax = 0.45 e Å3
1550 reflectionsΔρmin = 0.23 e Å3
113 parameters
Special details top

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) top
xyzUiso*/Ueq
O10.8163 (2)0.3454 (2)0.1877 (2)0.0356 (6)
N10.7947 (3)0.3179 (2)0.4330 (3)0.0323 (7)
H1A0.82030.27280.51660.039*
C11.0048 (4)0.0859 (3)0.3289 (4)0.0401 (8)
C20.9317 (3)0.1756 (3)0.3242 (3)0.0317 (7)
C30.8422 (3)0.2867 (3)0.3095 (3)0.0290 (7)
C40.7008 (4)0.4254 (3)0.4350 (4)0.0365 (8)
H4A0.73890.49710.38550.044*
H4B0.70150.44870.54270.044*
C50.5485 (3)0.4009 (3)0.3545 (3)0.0323 (7)
C60.4870 (4)0.4688 (3)0.2258 (4)0.0413 (8)
H6A0.54180.53090.18730.050*
C70.3471 (4)0.4469 (4)0.1532 (4)0.0483 (9)
H7A0.30580.49430.06530.058*
C80.2665 (4)0.3569 (4)0.2069 (4)0.0466 (9)
H8A0.17020.34150.15590.056*
C90.3268 (4)0.2895 (3)0.3353 (4)0.0464 (9)
H9A0.27150.22770.37360.056*
C100.4673 (4)0.3113 (3)0.4089 (4)0.0411 (8)
H10A0.50810.26430.49740.049*
H11.061 (4)0.014 (4)0.328 (4)0.050 (11)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.0461 (13)0.0335 (12)0.0286 (12)0.0005 (10)0.0112 (9)0.0028 (9)
N10.0378 (14)0.0352 (14)0.0246 (13)0.0058 (11)0.0076 (10)0.0010 (10)
C10.0344 (17)0.0376 (19)0.049 (2)0.0016 (16)0.0091 (14)0.0036 (15)
C20.0313 (16)0.0355 (17)0.0297 (16)0.0050 (13)0.0091 (12)0.0018 (12)
C30.0285 (15)0.0301 (15)0.0275 (15)0.0076 (12)0.0038 (11)0.0021 (12)
C40.0432 (18)0.0323 (16)0.0342 (17)0.0031 (14)0.0086 (13)0.0064 (13)
C50.0406 (17)0.0284 (15)0.0292 (15)0.0061 (13)0.0104 (12)0.0050 (12)
C60.050 (2)0.0380 (18)0.0368 (18)0.0070 (15)0.0116 (15)0.0024 (14)
C70.051 (2)0.054 (2)0.0379 (19)0.0174 (18)0.0061 (16)0.0028 (16)
C80.0387 (18)0.053 (2)0.046 (2)0.0078 (16)0.0040 (15)0.0089 (16)
C90.043 (2)0.0391 (19)0.057 (2)0.0032 (15)0.0112 (16)0.0014 (16)
C100.0459 (19)0.0358 (17)0.0412 (18)0.0040 (14)0.0080 (15)0.0049 (14)
Geometric parameters (Å, º) top
O1—C31.235 (4)C5—C61.384 (5)
N1—C31.314 (4)C6—C71.376 (5)
N1—C41.458 (4)C6—H6A0.9500
N1—H1A0.8800C7—C81.374 (6)
C1—C21.180 (5)C7—H7A0.9500
C1—H10.93 (4)C8—C91.376 (5)
C2—C31.453 (4)C8—H8A0.9500
C4—C51.502 (5)C9—C101.383 (5)
C4—H4A0.9900C9—H9A0.9500
C4—H4B0.9900C10—H10A0.9500
C5—C101.378 (5)
C3—N1—C4121.7 (3)C6—C5—C4120.6 (3)
C3—N1—H1A119.2C7—C6—C5120.4 (3)
C4—N1—H1A119.2C7—C6—H6A119.8
C2—C1—H1178 (2)C5—C6—H6A119.8
C1—C2—C3176.9 (3)C8—C7—C6120.6 (3)
O1—C3—N1124.5 (3)C8—C7—H7A119.7
O1—C3—C2120.3 (3)C6—C7—H7A119.7
N1—C3—C2115.2 (3)C7—C8—C9119.3 (3)
N1—C4—C5112.8 (2)C7—C8—H8A120.4
N1—C4—H4A109.0C9—C8—H8A120.4
C5—C4—H4A109.0C8—C9—C10120.4 (3)
N1—C4—H4B109.0C8—C9—H9A119.8
C5—C4—H4B109.0C10—C9—H9A119.8
H4A—C4—H4B107.8C5—C10—C9120.4 (3)
C10—C5—C6119.0 (3)C5—C10—H10A119.8
C10—C5—C4120.4 (3)C9—C10—H10A119.8
C4—N1—C3—O12.1 (5)C5—C6—C7—C80.3 (5)
C4—N1—C3—C2178.4 (3)C6—C7—C8—C90.6 (5)
C3—N1—C4—C576.0 (4)C7—C8—C9—C100.5 (5)
N1—C4—C5—C1063.6 (4)C6—C5—C10—C90.3 (5)
N1—C4—C5—C6117.3 (3)C4—C5—C10—C9179.4 (3)
C10—C5—C6—C70.2 (5)C8—C9—C10—C50.0 (5)
C4—C5—C6—C7179.3 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1A···O1i0.881.992.839 (3)163
C1—H1···O1ii0.93 (4)2.17 (4)3.105 (4)176 (3)
Symmetry codes: (i) x, y+1/2, z+1/2; (ii) x+2, y1/2, z+1/2.

Experimental details

Crystal data
Chemical formulaC10H9NO
Mr159.18
Crystal system, space groupMonoclinic, P21/c
Temperature (K)173
a, b, c (Å)9.495 (2), 10.703 (2), 8.9120 (19)
β (°) 101.637 (3)
V3)887.1 (3)
Z4
Radiation typeMo Kα
µ (mm1)0.08
Crystal size (mm)0.57 × 0.30 × 0.30
Data collection
DiffractometerBruker APEX area-detector
diffractometer
Absorption correctionMulti-scan
(SADABS; Bruker, 2001)
Tmin, Tmax0.848, 1.000
No. of measured, independent and
observed [I > 2σ(I)] reflections
5825, 1550, 1510
Rint0.030
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.070, 0.221, 1.26
No. of reflections1550
No. of parameters113
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.45, 0.23

Computer programs: SMART (Bruker, 2001), SAINT (Bruker, 2001), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), ORTEP-3 for Windows (Farrugia, 1997), SHELXL97 (Sheldrick, 2008.

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1A···O1i0.881.992.839 (3)162.6
C1—H1···O1ii0.93 (4)2.17 (4)3.105 (4)176 (3)
Symmetry codes: (i) x, y+1/2, z+1/2; (ii) x+2, y1/2, z+1/2.
 

Acknowledgements

The authors thank the National Science Foundation of China (grant No. 40706043) and the Science Foundation of Xiamen University (grant No. Z03120) for supporting this work. We also thank Mr Z.-B. Wei for technical assistance.

References

First citationBruker (2001). SAINT, SMART and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.  Google Scholar
First citationFarrugia, L. J. (1997). J. Appl. Cryst. 30, 565.  CrossRef IUCr Journals Google Scholar
First citationKatritzky, A. R. & Singh, K. (2002). J. Org. Chem. 67, 9077–9079.  Web of Science CrossRef PubMed CAS Google Scholar
First citationLeiserowitz, L. & Tuval, M. (1978). Acta Cryst. B34, 1230–1247.  CSD CrossRef CAS IUCr Journals Web of Science Google Scholar
First citation Parsons, S. & Gould, B. (2003). ROTAX. University of Edinburgh, Scotland.  Google Scholar
First citationSheldrick, G. M. (2008). Acta Cryst. A64, 112–122.  Web of Science CrossRef CAS IUCr Journals Google Scholar
First citationWilliamson, B. L., Tykwinski, R. R. & Stang, P. J. (1994). J. Am. Chem. Soc. 116, 93–98.  CrossRef CAS Web of Science Google Scholar

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Journal logoCRYSTALLOGRAPHIC
COMMUNICATIONS
ISSN: 2056-9890
Volume 65| Part 5| May 2009| Page o1115
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