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ISSN: 2056-9890

N-{4-[(E)-(4-Methyl­phen­yl)imino­meth­yl]phen­yl}acetamide

aDepartment of Physics, University of Sargodha, Sargodha, Pakistan, and bDepartment of Chemistry, Govt. M. D. College, Toba Tek Singh, Punjab, Pakistan
*Correspondence e-mail: dmntahir_uos@yahoo.com

(Received 12 January 2011; accepted 12 January 2011; online 22 January 2011)

There are two symmetry-independent mol­ecules in the asymmetric unit of the title compound, C16H16N2O, that differ in conformation. The dihedral angles between the benzene rings in the two mol­ecules are 44.35 (19) and 48.14 (17)°, but the rings twist in opposite directions. The acetamide groups make nearly equal dihedral angles of 25.4 (3) and 25.7 (3)° with the parent benzene rings. An S(6) ring motif is formed in each mol­ecule by intra­molecular C—H⋯O close contacts. In the crystal, strong N—H⋯O hydrogen bonds between acetamide groups generate a C(4) chain motif arranging the mol­ecules into two symmetry-independent polymeric structures extending along [010].

Related literature

For related structures, see: Karlsen et al. (1988[Karlsen, J., Mostad, A., Romming, C. & Tonnesen, H. H. (1988). Acta Chem. Scand. Ser. A, 42, 27-31.]); Tahir et al. (2010[Tahir, M. N., Shad, H. A., Khan, M. N. & Tariq, R. H. (2010). Acta Cryst. E66, o3293.]). For graph-set notation, see: Bernstein et al. (1995[Bernstein, J., Davis, R. E., Shimoni, L. & Chang, N.-L. (1995). Angew. Chem. Int. Ed. Engl. 34, 1555-1573.]).

[Scheme 1]

Experimental

Crystal data
  • C16H16N2O

  • Mr = 252.31

  • Triclinic, P 1

  • a = 7.1044 (8) Å

  • b = 9.7393 (10) Å

  • c = 10.9236 (12) Å

  • α = 109.731 (5)°

  • β = 91.799 (6)°

  • γ = 100.679 (6)°

  • V = 695.51 (13) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.08 mm−1

  • T = 296 K

  • 0.26 × 0.16 × 0.12 mm

Data collection
  • Bruker Kappa APEXII CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2005[Bruker (2005). SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.]) Tmin = 0.980, Tmax = 0.990

  • 10024 measured reflections

  • 2453 independent reflections

  • 1460 reflections with I > 2σ(I)

  • Rint = 0.059

Refinement
  • R[F2 > 2σ(F2)] = 0.044

  • wR(F2) = 0.112

  • S = 0.97

  • 2453 reflections

  • 339 parameters

  • 3 restraints

  • H-atom parameters constrained

  • Δρmax = 0.16 e Å−3

  • Δρmin = −0.15 e Å−3

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
N2—H2A⋯O2i 0.86 2.00 2.854 (5) 172
N4—H4⋯O1ii 0.86 2.06 2.911 (4) 173
C13—H13⋯O1 0.93 2.40 2.922 (6) 116
C29—H29⋯O2 0.93 2.35 2.864 (6) 114
Symmetry codes: (i) x+2, y, z-1; (ii) x-2, y-1, z+1.

Data collection: APEX2 (Bruker, 2009[Bruker (2009). APEX2 and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA.]); cell refinement: SAINT (Bruker, 2009[Bruker (2009). APEX2 and SAINT. 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.]) and PLATON (Spek, 2009[Spek, A. L. (2009). Acta Cryst. D65, 148-155.]); software used to prepare material for publication: WinGX (Farrugia, 1999[Farrugia, L. J. (1999). J. Appl. Cryst. 32, 837-838.]) and PLATON.

Supporting information


Comment top

The title compound (I, Fig. 1) is being reported as a part of our ongoing project related to the synthesis of various Schiff bases of 4-methylaniline. In this regard recently we have reported the synthesis and crystal structure of N-[(E)-1,3-benzodioxol-5-ylmethylidene]-4-methylaniline (Tahir et al., 2010).

The crystal structure of thiacetazone i.e., N-{4-[-(2-carbamothioylhydrazinylidene)methyl]phenyl}acetamide (Karlsen et al., 1988) has been published which contains the common moiety of N-(4-formylphenyl)acetamide as in (I).

The title compound consists of two molecules in the crystallographic asymmetric unit which differ from each other geometrically. In one molecule, the 4-methylaniline group A (C1—C7/N1), groups B (C8—C14) and C (N2/C15/C16/O1) of N-(4-formylphenyl)acetamide are planar with r. m. s deviation of 0.0062, 0.0169 and 0.0005 Å, respectively. The dihedral angle between A/B, A/C and B/C is 48.11 (15)°, 25.13 (25)° and 25.88 (27)°, respectively. In second molecule, the 4-methylaniline group D (C17—C23/N3), groups E (C24—C30) and F (N4/C31/C32/O2) of N-(4-formylphenyl)acetamide are planar with r. m. s deviation of 0.0292, 0.0146 and 0.0027 Å, respectively. The dihedral angle between D/E, D/F and E/F is 44.36 (17)°, 69.79 (17)° and 25.43 (23)°, respectively. In each molecule there exist S(6) ring motif (Bernstein et al., 1995) due to intramolecular H-bonding of C—H···O type (Table 1, Fig. 1). The molecules are stabilized in the form of one dimensional polymeric chains extending along the crystallographic b-axis due to intermolecular hydrogen bonds of N—H···O type (Table 1, Fig. 2). These C(4) chains (Bernstein et al., 1995) are formed via interaction of the amide groups. There does not exist any kind of strong π-interaction.

Related literature top

For related structures, see: Karlsen et al. (1988); Tahir et al. (2010). For graph-set notation, see: Bernstein et al. (1995).

Experimental top

Equimolar quantities of 4-methylaniline and N-(4-formylphenyl)acetamide were refluxed in methanol along with a few drops of acetic acid as catalyst for 30 min resulting in colorless solution. The solution was kept at room temperature. After six days colourless needles of the title compound were isolated.

Refinement top

In the absence of anomalous scattering all Friedal pairs were merged. All H atoms were positioned geometrically (N–H = 0.86, C–H = 0.93–0.96 Å) and were included in the refinement in the riding model approximation, with Uiso(H) = xUeq(C, N), where x = 1.5 for methyl H-atoms and x = 1.2 for all other H-atoms.

Computing details top

Data collection: APEX2 (Bruker, 2009); cell refinement: SAINT (Bruker, 2009); data reduction: SAINT (Bruker, 2009); 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) and PLATON (Spek, 2009); software used to prepare material for publication: WinGX (Farrugia, 1999) and PLATON (Spek, 2009).

Figures top
[Figure 1] Fig. 1. Molecular structure of the title compound with the atom numbering scheme. The displacement ellipsoids are drawn at the 50% probability level. H atoms are shown by small circles of arbitrary radii. The dotted line represent the intramolecular hydrogen bond.
[Figure 2] Fig. 2. The crystal packing (PLATON; Spek, 2009) showing two symmetry independent one dimensional polymeric chains along the b-axis.
N-{4-[(E)-(4-Methylphenyl)iminomethyl]phenyl}acetamide top
Crystal data top
C16H16N2OZ = 2
Mr = 252.31F(000) = 268
Triclinic, P1Dx = 1.205 Mg m3
Hall symbol: P 1Mo Kα radiation, λ = 0.71073 Å
a = 7.1044 (8) ÅCell parameters from 1460 reflections
b = 9.7393 (10) Åθ = 2.0–25.1°
c = 10.9236 (12) ŵ = 0.08 mm1
α = 109.731 (5)°T = 296 K
β = 91.799 (6)°Needle, colorless
γ = 100.679 (6)°0.26 × 0.16 × 0.12 mm
V = 695.51 (13) Å3
Data collection top
Bruker Kappa APEXII CCD
diffractometer
2453 independent reflections
Radiation source: fine-focus sealed tube1460 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.059
Detector resolution: 8.20 pixels mm-1θmax = 25.1°, θmin = 2.0°
ω scansh = 88
Absorption correction: multi-scan
(SADABS; Bruker, 2005)
k = 1011
Tmin = 0.980, Tmax = 0.990l = 1313
10024 measured reflections
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)] = 0.044Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.112H-atom parameters constrained
S = 0.97 w = 1/[σ2(Fo2) + (0.052P)2]
where P = (Fo2 + 2Fc2)/3
2453 reflections(Δ/σ)max < 0.001
339 parametersΔρmax = 0.16 e Å3
3 restraintsΔρmin = 0.15 e Å3
Crystal data top
C16H16N2Oγ = 100.679 (6)°
Mr = 252.31V = 695.51 (13) Å3
Triclinic, P1Z = 2
a = 7.1044 (8) ÅMo Kα radiation
b = 9.7393 (10) ŵ = 0.08 mm1
c = 10.9236 (12) ÅT = 296 K
α = 109.731 (5)°0.26 × 0.16 × 0.12 mm
β = 91.799 (6)°
Data collection top
Bruker Kappa APEXII CCD
diffractometer
2453 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2005)
1460 reflections with I > 2σ(I)
Tmin = 0.980, Tmax = 0.990Rint = 0.059
10024 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0443 restraints
wR(F2) = 0.112H-atom parameters constrained
S = 0.97Δρmax = 0.16 e Å3
2453 reflectionsΔρmin = 0.15 e Å3
339 parameters
Special details top

Geometry. Bond distances, angles etc. have been calculated using the rounded fractional coordinates. All su's are estimated from the variances of the (full) variance-covariance matrix. The cell e.s.d.'s are taken into account in the estimation of distances, angles and torsion angles

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
O11.4696 (5)1.0625 (3)0.3349 (3)0.0708 (16)
N10.7543 (5)0.8296 (4)0.1036 (4)0.0574 (17)
N21.4290 (5)0.8628 (4)0.2684 (4)0.0507 (14)
C10.5901 (7)0.8407 (5)0.1748 (5)0.0533 (17)
C20.4818 (7)0.7111 (5)0.1826 (5)0.0581 (19)
C30.3211 (7)0.7168 (5)0.2509 (5)0.0609 (19)
C40.2630 (7)0.8479 (5)0.3122 (5)0.057 (2)
C50.3734 (7)0.9758 (5)0.3047 (5)0.066 (2)
C60.5329 (7)0.9738 (5)0.2353 (5)0.063 (2)
C70.0872 (8)0.8530 (7)0.3878 (6)0.082 (3)
C80.7950 (7)0.9097 (5)0.0340 (5)0.0546 (17)
C90.9643 (7)0.9052 (5)0.0396 (4)0.0488 (17)
C101.1009 (7)0.8263 (5)0.0238 (5)0.0560 (17)
C111.2543 (7)0.8186 (5)0.0978 (4)0.0527 (17)
C121.2758 (6)0.8876 (5)0.1894 (4)0.0461 (17)
C131.1414 (6)0.9688 (5)0.2060 (4)0.0525 (17)
C140.9869 (7)0.9764 (5)0.1296 (5)0.0568 (17)
C151.5113 (6)0.9450 (5)0.3384 (4)0.0530 (17)
C161.6605 (5)0.8800 (3)0.4230 (4)0.0656 (19)
O20.4539 (3)0.5959 (2)0.7256 (3)0.0861 (18)
N30.2922 (3)0.3139 (2)0.2969 (3)0.0618 (17)
N40.3891 (3)0.3652 (2)0.6710 (3)0.0590 (17)
C170.4543 (7)0.3342 (5)0.2265 (5)0.055 (2)
C180.4305 (7)0.2583 (5)0.0940 (5)0.0638 (19)
C190.5805 (8)0.2744 (5)0.0169 (5)0.0649 (19)
C200.7579 (8)0.3651 (6)0.0740 (6)0.061 (2)
C210.7813 (7)0.4324 (6)0.2065 (6)0.073 (2)
C220.6329 (7)0.4202 (5)0.2829 (5)0.0637 (17)
C230.9201 (8)0.3872 (7)0.0095 (7)0.093 (3)
C240.2638 (7)0.4188 (5)0.3945 (5)0.060 (2)
C250.0999 (7)0.4058 (5)0.4693 (5)0.0534 (17)
C260.0233 (8)0.2677 (5)0.4452 (5)0.067 (2)
C270.1822 (8)0.2570 (5)0.5138 (5)0.063 (2)
C280.2240 (7)0.3849 (5)0.6071 (5)0.0509 (19)
C290.1015 (7)0.5213 (5)0.6306 (5)0.0594 (19)
C300.0582 (7)0.5293 (5)0.5624 (5)0.0601 (19)
C310.4956 (7)0.4670 (5)0.7260 (5)0.0609 (19)
C320.6685 (8)0.4123 (6)0.7853 (6)0.082 (3)
H20.516950.620270.142070.0694*
H2A1.475580.786140.272360.0609*
H30.249790.628680.255480.0730*
H50.339781.066630.347700.0789*
H60.601811.061900.229250.0763*
H7A0.019680.858510.334890.1221*
H7B0.113960.939110.466380.1221*
H7C0.056090.764520.409790.1221*
H80.714850.973570.029340.0652*
H101.088830.778360.037010.0673*
H111.345420.765740.085750.0631*
H131.154081.016980.266620.0630*
H140.896941.031030.139760.0682*
H16A1.615240.852730.513490.0982*
H16B1.682040.793270.406260.0982*
H16C1.778900.952950.402970.0982*
H40.427050.278220.675710.0708*
H180.313040.195510.055030.0760*
H190.561280.224040.073000.0775*
H210.901680.488600.246760.0868*
H220.653340.470210.372810.0761*
H23A0.954010.490520.000530.1393*
H23B0.878560.327850.099430.1393*
H23C1.030170.357320.018780.1393*
H240.352000.509290.420330.0709*
H260.001870.182640.382720.0806*
H270.262230.164370.498090.0755*
H290.126600.607110.691990.0708*
H300.140460.621370.579950.0723*
H32A0.758070.476780.793490.1221*
H32B0.628960.412330.870190.1221*
H32C0.728960.312780.730230.1221*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
O10.085 (3)0.051 (2)0.086 (3)0.0129 (18)0.032 (2)0.0348 (19)
N10.051 (3)0.062 (3)0.063 (3)0.010 (2)0.015 (2)0.027 (2)
N20.052 (2)0.044 (2)0.061 (3)0.0141 (18)0.013 (2)0.022 (2)
C10.051 (3)0.060 (3)0.057 (3)0.016 (2)0.012 (3)0.028 (3)
C20.060 (3)0.058 (3)0.064 (4)0.016 (2)0.010 (3)0.029 (3)
C30.061 (3)0.058 (3)0.075 (4)0.011 (2)0.013 (3)0.038 (3)
C40.051 (3)0.071 (4)0.057 (4)0.018 (3)0.007 (3)0.030 (3)
C50.071 (4)0.058 (3)0.072 (4)0.020 (3)0.019 (3)0.022 (3)
C60.066 (4)0.052 (3)0.073 (4)0.006 (3)0.021 (3)0.025 (3)
C70.071 (4)0.104 (5)0.083 (4)0.023 (3)0.024 (4)0.046 (4)
C80.051 (3)0.057 (3)0.056 (3)0.011 (2)0.008 (3)0.020 (3)
C90.047 (3)0.051 (3)0.051 (3)0.010 (2)0.008 (3)0.021 (2)
C100.064 (3)0.058 (3)0.053 (3)0.014 (3)0.014 (3)0.027 (3)
C110.057 (3)0.055 (3)0.052 (3)0.014 (2)0.005 (3)0.025 (3)
C120.044 (3)0.049 (3)0.046 (3)0.008 (2)0.008 (3)0.018 (2)
C130.053 (3)0.052 (3)0.057 (3)0.010 (2)0.008 (3)0.025 (2)
C140.053 (3)0.062 (3)0.062 (3)0.014 (2)0.006 (3)0.029 (3)
C150.055 (3)0.047 (3)0.050 (3)0.001 (2)0.006 (3)0.013 (2)
C160.061 (3)0.069 (3)0.073 (4)0.014 (3)0.024 (3)0.031 (3)
O20.081 (3)0.060 (2)0.133 (4)0.0285 (18)0.030 (2)0.045 (2)
N30.066 (3)0.056 (3)0.064 (3)0.011 (2)0.014 (3)0.022 (2)
N40.064 (3)0.050 (3)0.075 (3)0.021 (2)0.023 (3)0.031 (2)
C170.061 (4)0.045 (3)0.060 (4)0.010 (2)0.011 (3)0.020 (3)
C180.061 (3)0.056 (3)0.065 (4)0.007 (2)0.006 (3)0.012 (3)
C190.075 (4)0.060 (3)0.054 (3)0.015 (3)0.009 (3)0.012 (3)
C200.063 (4)0.063 (3)0.064 (4)0.015 (3)0.015 (3)0.028 (3)
C210.050 (3)0.080 (4)0.082 (5)0.005 (3)0.005 (3)0.025 (3)
C220.061 (3)0.071 (3)0.057 (3)0.011 (3)0.002 (3)0.022 (3)
C230.071 (4)0.098 (4)0.104 (5)0.014 (3)0.031 (4)0.029 (4)
C240.068 (4)0.046 (3)0.059 (4)0.000 (2)0.003 (3)0.018 (3)
C250.053 (3)0.052 (3)0.057 (3)0.006 (2)0.006 (3)0.024 (3)
C260.084 (4)0.047 (3)0.070 (4)0.015 (3)0.026 (4)0.018 (3)
C270.079 (4)0.040 (3)0.072 (4)0.008 (3)0.021 (3)0.023 (3)
C280.055 (3)0.043 (3)0.057 (4)0.007 (2)0.006 (3)0.022 (3)
C290.065 (3)0.050 (3)0.063 (4)0.013 (2)0.006 (3)0.019 (3)
C300.063 (3)0.047 (3)0.066 (4)0.004 (2)0.009 (3)0.018 (3)
C310.062 (3)0.060 (3)0.070 (4)0.019 (3)0.009 (3)0.031 (3)
C320.078 (4)0.090 (4)0.104 (5)0.034 (3)0.034 (4)0.058 (4)
Geometric parameters (Å, º) top
O1—C151.223 (6)C11—H110.9300
O2—C311.237 (6)C13—H130.9300
N1—C11.423 (6)C14—H140.9300
N1—C81.265 (7)C16—H16C0.9600
N2—C121.415 (6)C16—H16A0.9600
N2—C151.355 (6)C16—H16B0.9600
N2—H2A0.8600C17—C221.378 (7)
N3—C241.255 (6)C17—C181.373 (7)
N3—C171.425 (6)C18—C191.398 (7)
N4—C281.399 (6)C19—C201.387 (8)
N4—C311.349 (6)C20—C211.362 (9)
N4—H40.8600C20—C231.521 (9)
C1—C21.382 (7)C21—C221.378 (8)
C1—C61.384 (7)C24—C251.454 (7)
C2—C31.383 (7)C25—C301.376 (7)
C3—C41.373 (7)C25—C261.398 (7)
C4—C51.373 (7)C26—C271.382 (8)
C4—C71.518 (8)C27—C281.406 (7)
C5—C61.383 (7)C28—C291.384 (7)
C8—C91.467 (7)C29—C301.381 (7)
C9—C101.385 (7)C31—C321.501 (8)
C9—C141.379 (7)C18—H180.9300
C10—C111.375 (7)C19—H190.9300
C11—C121.379 (7)C21—H210.9300
C12—C131.391 (7)C22—H220.9300
C13—C141.397 (7)C23—H23A0.9600
C15—C161.514 (6)C23—H23B0.9600
C2—H20.9300C23—H23C0.9600
C3—H30.9300C24—H240.9300
C5—H50.9300C26—H260.9300
C6—H60.9300C27—H270.9300
C7—H7C0.9600C29—H290.9300
C7—H7A0.9600C30—H300.9300
C7—H7B0.9600C32—H32A0.9600
C8—H80.9300C32—H32B0.9600
C10—H100.9300C32—H32C0.9600
C1—N1—C8119.8 (4)H16A—C16—H16B109.00
C12—N2—C15128.0 (4)C15—C16—H16A109.00
C15—N2—H2A116.00C15—C16—H16C109.00
C12—N2—H2A116.00C15—C16—H16B110.00
C17—N3—C24120.6 (4)N3—C17—C22124.5 (4)
C28—N4—C31127.5 (3)N3—C17—C18117.0 (4)
C31—N4—H4116.00C18—C17—C22118.4 (5)
C28—N4—H4116.00C17—C18—C19120.9 (5)
N1—C1—C6123.5 (5)C18—C19—C20120.2 (5)
N1—C1—C2117.9 (4)C19—C20—C21117.8 (5)
C2—C1—C6118.6 (5)C19—C20—C23120.6 (5)
C1—C2—C3119.8 (5)C21—C20—C23121.6 (5)
C2—C3—C4122.4 (5)C20—C21—C22122.3 (5)
C3—C4—C7121.9 (5)C17—C22—C21120.2 (5)
C5—C4—C7121.0 (5)N3—C24—C25123.2 (4)
C3—C4—C5117.1 (5)C24—C25—C30121.1 (5)
C4—C5—C6122.1 (5)C26—C25—C30118.3 (5)
C1—C6—C5120.0 (5)C24—C25—C26120.6 (5)
N1—C8—C9122.2 (5)C25—C26—C27120.3 (5)
C10—C9—C14118.6 (5)C26—C27—C28120.6 (5)
C8—C9—C10121.2 (4)N4—C28—C27117.1 (4)
C8—C9—C14120.1 (5)C27—C28—C29118.9 (5)
C9—C10—C11120.2 (5)N4—C28—C29124.0 (4)
C10—C11—C12121.4 (5)C28—C29—C30119.7 (5)
N2—C12—C11117.2 (4)C25—C30—C29122.3 (5)
C11—C12—C13119.4 (4)N4—C31—C32115.5 (4)
N2—C12—C13123.3 (4)O2—C31—N4121.9 (4)
C12—C13—C14118.6 (4)O2—C31—C32122.7 (5)
C9—C14—C13121.8 (5)C17—C18—H18120.00
N2—C15—C16114.8 (4)C19—C18—H18120.00
O1—C15—C16121.9 (4)C18—C19—H19120.00
O1—C15—N2123.4 (4)C20—C19—H19120.00
C1—C2—H2120.00C20—C21—H21119.00
C3—C2—H2120.00C22—C21—H21119.00
C2—C3—H3119.00C17—C22—H22120.00
C4—C3—H3119.00C21—C22—H22120.00
C6—C5—H5119.00C20—C23—H23A109.00
C4—C5—H5119.00C20—C23—H23B109.00
C1—C6—H6120.00C20—C23—H23C109.00
C5—C6—H6120.00H23A—C23—H23B109.00
H7A—C7—H7C109.00H23A—C23—H23C109.00
H7B—C7—H7C110.00H23B—C23—H23C109.00
C4—C7—H7A109.00N3—C24—H24118.00
C4—C7—H7B109.00C25—C24—H24118.00
C4—C7—H7C109.00C25—C26—H26120.00
H7A—C7—H7B109.00C27—C26—H26120.00
N1—C8—H8119.00C26—C27—H27120.00
C9—C8—H8119.00C28—C27—H27120.00
C11—C10—H10120.00C28—C29—H29120.00
C9—C10—H10120.00C30—C29—H29120.00
C10—C11—H11119.00C25—C30—H30119.00
C12—C11—H11119.00C29—C30—H30119.00
C14—C13—H13121.00C31—C32—H32A109.00
C12—C13—H13121.00C31—C32—H32B109.00
C9—C14—H14119.00C31—C32—H32C109.00
C13—C14—H14119.00H32A—C32—H32B109.00
H16A—C16—H16C109.00H32A—C32—H32C109.00
H16B—C16—H16C109.00H32B—C32—H32C109.00
C8—N1—C1—C2141.7 (5)C10—C9—C14—C131.0 (7)
C8—N1—C1—C637.7 (7)C9—C10—C11—C120.4 (7)
C1—N1—C8—C9178.8 (4)C10—C11—C12—N2174.8 (4)
C15—N2—C12—C11160.9 (4)C10—C11—C12—C131.1 (7)
C15—N2—C12—C1323.5 (7)N2—C12—C13—C14174.9 (4)
C12—N2—C15—O15.3 (7)C11—C12—C13—C140.7 (7)
C12—N2—C15—C16174.5 (4)C12—C13—C14—C90.4 (7)
C24—N3—C17—C18146.3 (5)N3—C17—C18—C19178.5 (4)
C24—N3—C17—C2235.9 (7)C22—C17—C18—C193.6 (8)
C17—N3—C24—C25179.1 (4)N3—C17—C22—C21179.7 (5)
C31—N4—C28—C27154.6 (5)C18—C17—C22—C211.9 (8)
C31—N4—C28—C2925.5 (7)C17—C18—C19—C201.5 (8)
C28—N4—C31—O20.4 (7)C18—C19—C20—C212.2 (8)
C28—N4—C31—C32178.7 (4)C18—C19—C20—C23178.1 (5)
N1—C1—C2—C3180.0 (5)C19—C20—C21—C224.0 (9)
C6—C1—C2—C30.6 (8)C23—C20—C21—C22176.4 (6)
N1—C1—C6—C5178.9 (5)C20—C21—C22—C171.9 (9)
C2—C1—C6—C51.7 (8)N3—C24—C25—C268.0 (8)
C1—C2—C3—C40.2 (8)N3—C24—C25—C30169.8 (5)
C2—C3—C4—C50.9 (8)C24—C25—C26—C27178.0 (5)
C2—C3—C4—C7179.5 (5)C30—C25—C26—C270.0 (8)
C3—C4—C5—C62.0 (8)C24—C25—C30—C29176.9 (5)
C7—C4—C5—C6179.3 (5)C26—C25—C30—C291.0 (8)
C4—C5—C6—C12.5 (8)C25—C26—C27—C281.1 (8)
N1—C8—C9—C108.0 (8)C26—C27—C28—N4179.0 (5)
N1—C8—C9—C14169.9 (5)C26—C27—C28—C291.1 (8)
C8—C9—C14—C13176.9 (5)N4—C28—C29—C30180.0 (4)
C8—C9—C10—C11177.3 (5)C27—C28—C29—C300.1 (8)
C14—C9—C10—C110.7 (7)C28—C29—C30—C250.9 (8)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H2A···O2i0.862.002.854 (5)172
N4—H4···O1ii0.862.062.911 (4)173
C13—H13···O10.932.402.922 (6)116
C29—H29···O20.932.352.864 (6)114
Symmetry codes: (i) x+2, y, z1; (ii) x2, y1, z+1.

Experimental details

Crystal data
Chemical formulaC16H16N2O
Mr252.31
Crystal system, space groupTriclinic, P1
Temperature (K)296
a, b, c (Å)7.1044 (8), 9.7393 (10), 10.9236 (12)
α, β, γ (°)109.731 (5), 91.799 (6), 100.679 (6)
V3)695.51 (13)
Z2
Radiation typeMo Kα
µ (mm1)0.08
Crystal size (mm)0.26 × 0.16 × 0.12
Data collection
DiffractometerBruker Kappa APEXII CCD
diffractometer
Absorption correctionMulti-scan
(SADABS; Bruker, 2005)
Tmin, Tmax0.980, 0.990
No. of measured, independent and
observed [I > 2σ(I)] reflections
10024, 2453, 1460
Rint0.059
(sin θ/λ)max1)0.596
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.044, 0.112, 0.97
No. of reflections2453
No. of parameters339
No. of restraints3
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.16, 0.15

Computer programs: APEX2 (Bruker, 2009), SAINT (Bruker, 2009), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), ORTEP-3 for Windows (Farrugia, 1997) and PLATON (Spek, 2009), WinGX (Farrugia, 1999) and PLATON (Spek, 2009).

Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N2—H2A···O2i0.862.002.854 (5)172
N4—H4···O1ii0.862.062.911 (4)173
C13—H13···O10.932.402.922 (6)116
C29—H29···O20.932.352.864 (6)114
Symmetry codes: (i) x+2, y, z1; (ii) x2, y1, z+1.
 

Acknowledgements

The authors acknowledge the provision of funds for the purchase of the diffractometer and encouragement by Dr Muhammad Akram Chaudhary, Vice Chancellor, University of Sargodha, Pakistan. The authors also acknowledge the technical support provided by Bana Inter­national, Karachi, Pakistan.

References

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First citationTahir, M. N., Shad, H. A., Khan, M. N. & Tariq, R. H. (2010). Acta Cryst. E66, o3293.  Web of Science CSD CrossRef IUCr Journals Google Scholar

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