Related literature
For background to Schiff bases, see: Cimerman et al. (1997
).
Experimental
Crystal data
C9H10N2O2 Mr = 178.19 Orthorhombic, P b c a a = 12.278 (3) Å b = 7.8035 (16) Å c = 19.466 (4) Å V = 1865.1 (7) Å3 Z = 8 Mo Kα radiation μ = 0.09 mm−1 T = 293 K 0.25 × 0.21 × 0.19 mm
|
Data collection
Bruker SMART CCD area-detector diffractometer Absorption correction: none 16349 measured reflections 2132 independent reflections 1693 reflections with I > 2σ(I) Rint = 0.048
|
D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A | N1—H1A⋯O2i | 0.86 | 2.04 | 2.8986 (15) | 179 | Symmetry code: (i) . | |
Data collection: SMART (Bruker, 1997
); cell refinement: SAINT (Bruker, 1997
); data reduction: SAINT; 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
A mixture of benzaldehyde (0.1 mol), and methyl carbazate (0.1 mol) was stirred in refluxing ethanol (20 mL) for 4 h to afford the title compound (0.089 mol, yield 89%). Colourless blocks of (I) were obtained by recrystallization from ethanol at room temperature.
H atoms were fixed geometrically and allowed to ride on their attached atoms, with C—H = 0.97 Å, and with Uiso = 1.2–1.5Ueq.
Structure description
top For background to Schiff bases, see: Cimerman et al. (1997).
Data collection: SMART (Bruker, 1997); cell refinement: SAINT (Bruker, 1997); data reduction: SAINT (Bruker, 1997); 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).
Methyl 3-benzylidenecarbazate
top Crystal data top C9H10N2O2 | F(000) = 752 |
Mr = 178.19 | Dx = 1.269 Mg m−3 |
Orthorhombic, Pbca | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ac 2ab | Cell parameters from 1984 reflections |
a = 12.278 (3) Å | θ = 3.5–27.5° |
b = 7.8035 (16) Å | µ = 0.09 mm−1 |
c = 19.466 (4) Å | T = 293 K |
V = 1865.1 (7) Å3 | Block, colourless |
Z = 8 | 0.25 × 0.21 × 0.19 mm |
Data collection top Bruker SMART CCD area-detector diffractometer | 1693 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.048 |
Graphite monochromator | θmax = 27.5°, θmin = 3.3° |
φ and ω scans | h = −15→15 |
16349 measured reflections | k = −10→8 |
2132 independent reflections | l = −25→25 |
Refinement top 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)] = 0.040 | H-atom parameters constrained |
wR(F2) = 0.147 | w = 1/[σ2(Fo2) + (0.1P)2] where P = (Fo2 + 2Fc2)/3 |
S = 1.08 | (Δ/σ)max = 0.001 |
2132 reflections | Δρmax = 0.23 e Å−3 |
119 parameters | Δρmin = −0.18 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: 0.011 (3) |
Crystal data top C9H10N2O2 | V = 1865.1 (7) Å3 |
Mr = 178.19 | Z = 8 |
Orthorhombic, Pbca | Mo Kα radiation |
a = 12.278 (3) Å | µ = 0.09 mm−1 |
b = 7.8035 (16) Å | T = 293 K |
c = 19.466 (4) Å | 0.25 × 0.21 × 0.19 mm |
Data collection top Bruker SMART CCD area-detector diffractometer | 1693 reflections with I > 2σ(I) |
16349 measured reflections | Rint = 0.048 |
2132 independent reflections | |
Refinement top R[F2 > 2σ(F2)] = 0.040 | 0 restraints |
wR(F2) = 0.147 | H-atom parameters constrained |
S = 1.08 | Δρmax = 0.23 e Å−3 |
2132 reflections | Δρmin = −0.18 e Å−3 |
119 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 | x | y | z | Uiso*/Ueq | |
O2 | 0.87392 (7) | 0.13497 (11) | 0.52542 (4) | 0.0522 (3) | |
N2 | 0.72993 (8) | 0.24691 (12) | 0.62265 (4) | 0.0434 (3) | |
O1 | 0.85158 (9) | 0.38853 (12) | 0.47171 (5) | 0.0613 (3) | |
C3 | 0.65739 (9) | 0.31376 (15) | 0.66062 (6) | 0.0443 (3) | |
H3A | 0.6184 | 0.4077 | 0.6445 | 0.053* | |
N1 | 0.74972 (9) | 0.33172 (13) | 0.56166 (5) | 0.0505 (3) | |
H1A | 0.7125 | 0.4207 | 0.5504 | 0.061* | |
C4 | 0.63373 (10) | 0.24621 (14) | 0.72925 (5) | 0.0418 (3) | |
C2 | 0.82860 (10) | 0.27174 (15) | 0.52044 (5) | 0.0434 (3) | |
C9 | 0.70485 (10) | 0.13562 (16) | 0.76285 (6) | 0.0508 (3) | |
H9A | 0.7678 | 0.0986 | 0.7408 | 0.061* | |
C7 | 0.58904 (13) | 0.13493 (19) | 0.86228 (7) | 0.0599 (4) | |
H7A | 0.5747 | 0.0988 | 0.9069 | 0.072* | |
C5 | 0.54021 (11) | 0.29976 (18) | 0.76341 (6) | 0.0532 (3) | |
H5A | 0.4922 | 0.3747 | 0.7419 | 0.064* | |
C8 | 0.68246 (13) | 0.08046 (19) | 0.82877 (6) | 0.0596 (4) | |
H8A | 0.7304 | 0.0063 | 0.8508 | 0.072* | |
C6 | 0.51809 (12) | 0.24207 (18) | 0.82934 (7) | 0.0607 (4) | |
H6A | 0.4545 | 0.2765 | 0.8513 | 0.073* | |
C1 | 0.93760 (15) | 0.3429 (2) | 0.42527 (8) | 0.0764 (5) | |
H1B | 0.9484 | 0.4338 | 0.3928 | 0.115* | |
H1C | 0.9184 | 0.2397 | 0.4013 | 0.115* | |
H1D | 1.0036 | 0.3246 | 0.4507 | 0.115* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
O2 | 0.0572 (6) | 0.0453 (5) | 0.0541 (5) | 0.0041 (4) | 0.0082 (4) | 0.0034 (3) |
N2 | 0.0465 (6) | 0.0427 (6) | 0.0410 (5) | 0.0010 (4) | 0.0018 (4) | 0.0047 (4) |
O1 | 0.0771 (7) | 0.0523 (6) | 0.0546 (5) | 0.0022 (5) | 0.0182 (4) | 0.0139 (4) |
C3 | 0.0451 (6) | 0.0414 (6) | 0.0464 (6) | 0.0032 (5) | −0.0009 (4) | 0.0013 (5) |
N1 | 0.0609 (6) | 0.0439 (6) | 0.0467 (6) | 0.0103 (4) | 0.0078 (4) | 0.0111 (4) |
C4 | 0.0426 (6) | 0.0396 (6) | 0.0431 (6) | −0.0032 (4) | 0.0012 (4) | −0.0018 (5) |
C2 | 0.0485 (7) | 0.0411 (6) | 0.0406 (6) | −0.0053 (5) | −0.0008 (4) | 0.0020 (4) |
C9 | 0.0478 (7) | 0.0529 (7) | 0.0517 (7) | 0.0042 (5) | 0.0020 (5) | 0.0018 (5) |
C7 | 0.0777 (9) | 0.0568 (8) | 0.0452 (7) | −0.0139 (7) | 0.0074 (6) | −0.0002 (5) |
C5 | 0.0488 (7) | 0.0525 (7) | 0.0584 (7) | 0.0036 (5) | 0.0066 (5) | 0.0004 (5) |
C8 | 0.0678 (9) | 0.0585 (8) | 0.0526 (7) | −0.0012 (6) | −0.0053 (6) | 0.0085 (5) |
C6 | 0.0614 (8) | 0.0595 (8) | 0.0613 (8) | −0.0038 (6) | 0.0204 (6) | −0.0057 (6) |
C1 | 0.0882 (11) | 0.0756 (10) | 0.0652 (9) | −0.0041 (8) | 0.0305 (8) | 0.0085 (8) |
Geometric parameters (Å, º) top O2—C2 | 1.2075 (15) | C9—H9A | 0.9300 |
N2—C3 | 1.2694 (15) | C7—C6 | 1.367 (2) |
N2—N1 | 1.3808 (13) | C7—C8 | 1.386 (2) |
O1—C2 | 1.3453 (14) | C7—H7A | 0.9300 |
O1—C1 | 1.4351 (18) | C5—C6 | 1.3868 (17) |
C3—C4 | 1.4653 (16) | C5—H5A | 0.9300 |
C3—H3A | 0.9300 | C8—H8A | 0.9300 |
N1—C2 | 1.3420 (16) | C6—H6A | 0.9300 |
N1—H1A | 0.8600 | C1—H1B | 0.9600 |
C4—C9 | 1.3911 (18) | C1—H1C | 0.9600 |
C4—C5 | 1.3912 (17) | C1—H1D | 0.9600 |
C9—C8 | 1.3811 (18) | | |
| | | |
C3—N2—N1 | 115.28 (10) | C6—C7—H7A | 120.2 |
C2—O1—C1 | 115.48 (11) | C8—C7—H7A | 120.2 |
N2—C3—C4 | 121.47 (11) | C6—C5—C4 | 120.43 (13) |
N2—C3—H3A | 119.3 | C6—C5—H5A | 119.8 |
C4—C3—H3A | 119.3 | C4—C5—H5A | 119.8 |
C2—N1—N2 | 118.29 (10) | C9—C8—C7 | 120.42 (13) |
C2—N1—H1A | 120.9 | C9—C8—H8A | 119.8 |
N2—N1—H1A | 120.9 | C7—C8—H8A | 119.8 |
C9—C4—C5 | 118.66 (11) | C7—C6—C5 | 120.52 (13) |
C9—C4—C3 | 121.84 (11) | C7—C6—H6A | 119.7 |
C5—C4—C3 | 119.43 (11) | C5—C6—H6A | 119.7 |
O2—C2—N1 | 126.35 (10) | O1—C1—H1B | 109.5 |
O2—C2—O1 | 123.97 (11) | O1—C1—H1C | 109.5 |
N1—C2—O1 | 109.67 (10) | H1B—C1—H1C | 109.5 |
C8—C9—C4 | 120.35 (12) | O1—C1—H1D | 109.5 |
C8—C9—H9A | 119.8 | H1B—C1—H1D | 109.5 |
C4—C9—H9A | 119.8 | H1C—C1—H1D | 109.5 |
C6—C7—C8 | 119.60 (12) | | |
Hydrogen-bond geometry (Å, º) top D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1A···O2i | 0.86 | 2.04 | 2.8986 (15) | 179 |
Symmetry code: (i) −x+3/2, y+1/2, z. |
Experimental details
Crystal data |
Chemical formula | C9H10N2O2 |
Mr | 178.19 |
Crystal system, space group | Orthorhombic, Pbca |
Temperature (K) | 293 |
a, b, c (Å) | 12.278 (3), 7.8035 (16), 19.466 (4) |
V (Å3) | 1865.1 (7) |
Z | 8 |
Radiation type | Mo Kα |
µ (mm−1) | 0.09 |
Crystal size (mm) | 0.25 × 0.21 × 0.19 |
|
Data collection |
Diffractometer | Bruker SMART CCD area-detector |
Absorption correction | – |
No. of measured, independent and observed [I > 2σ(I)] reflections | 16349, 2132, 1693 |
Rint | 0.048 |
(sin θ/λ)max (Å−1) | 0.649 |
|
Refinement |
R[F2 > 2σ(F2)], wR(F2), S | 0.040, 0.147, 1.08 |
No. of reflections | 2132 |
No. of parameters | 119 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.23, −0.18 |
Hydrogen-bond geometry (Å, º) top D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1A···O2i | 0.86 | 2.04 | 2.8986 (15) | 179 |
Symmetry code: (i) −x+3/2, y+1/2, z. |
Acknowledgements
The authors thank the Science Foundation of Weifang University (No. 2009Z24).
References
Bruker (1997). SMART and SAINT. Bruker AXS Inc., Madison, Wisconsin, USA. Google Scholar
Cimerman, Z., Galic, N. & Bosner, B. (1997). Anal. Chim. Acta, 343, 145–153. CrossRef CAS Web of Science Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
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