Related literature
For a related structure, see: Li & Jian (2008
).
Experimental
Crystal data
C10H11ClN2O Mr = 210.66 Monoclinic, P 21 /c a = 15.944 (3) Å b = 5.0061 (10) Å c = 13.950 (3) Å β = 109.45 (3)° V = 1049.9 (4) Å3 Z = 4 Mo Kα radiation μ = 0.33 mm−1 T = 293 K 0.25 × 0.20 × 0.20 mm
|
Data collection
Bruker SMART CCD diffractometer 9225 measured reflections 2368 independent reflections 1840 reflections with I > 2σ(I) Rint = 0.028
|
D—H⋯A | D—H | H⋯A | D⋯A | D—H⋯A | N2—H2A⋯O1i | 0.93 (2) | 2.02 (2) | 2.9384 (18) | 170.3 (18) | Symmetry code: (i) -x+1, -y-1, -z. | |
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 4-fluorobenzophenone (0.02 mol) and acethydrazide (0.02 mol) was stirred in refluxing ethanol(30 ml) for 2 h to afford the title compound (yield 82%). Yellow bars of (I) were obtained by recrystallization from acetic ether at room temperature.
All H atoms were fixed geometrically and allowed to ride on their attached atoms, with C—H and N—H distances in the range 0.93–0.97Å and 0.86 Å, and with Uiso(H) = 1.2Ueq of the parent atoms.
Structure description
top For a related structure, see: Li & Jian (2008).
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).
N'-[1-(4-Chlorophenyl)ethylidene]acetohydrazide
top Crystal data top C10H11ClN2O | F(000) = 440 |
Mr = 210.66 | Dx = 1.333 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ybc | Cell parameters from 2368 reflections |
a = 15.944 (3) Å | θ = 3.1–27.5° |
b = 5.0061 (10) Å | µ = 0.33 mm−1 |
c = 13.950 (3) Å | T = 293 K |
β = 109.45 (3)° | Bar, yellow |
V = 1049.9 (4) Å3 | 0.25 × 0.20 × 0.20 mm |
Z = 4 | |
Data collection top Bruker SMART CCD diffractometer | 1840 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.028 |
Graphite monochromator | θmax = 27.5°, θmin = 3.1° |
phi and ω scans | h = −20→20 |
9225 measured reflections | k = −6→6 |
2368 independent reflections | l = −18→18 |
Refinement top Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.046 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.164 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.22 | w = 1/[σ2(Fo2) + (0.1P)2] where P = (Fo2 + 2Fc2)/3 |
2368 reflections | (Δ/σ)max < 0.001 |
143 parameters | Δρmax = 0.29 e Å−3 |
0 restraints | Δρmin = −0.22 e Å−3 |
Crystal data top C10H11ClN2O | V = 1049.9 (4) Å3 |
Mr = 210.66 | Z = 4 |
Monoclinic, P21/c | Mo Kα radiation |
a = 15.944 (3) Å | µ = 0.33 mm−1 |
b = 5.0061 (10) Å | T = 293 K |
c = 13.950 (3) Å | 0.25 × 0.20 × 0.20 mm |
β = 109.45 (3)° | |
Data collection top Bruker SMART CCD diffractometer | 1840 reflections with I > 2σ(I) |
9225 measured reflections | Rint = 0.028 |
2368 independent reflections | |
Refinement top R[F2 > 2σ(F2)] = 0.046 | 0 restraints |
wR(F2) = 0.164 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.22 | Δρmax = 0.29 e Å−3 |
2368 reflections | Δρmin = −0.22 e Å−3 |
143 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 | |
Cl1 | 0.05552 (4) | 0.51605 (12) | 0.20233 (5) | 0.0784 (3) | |
O1 | 0.58233 (7) | −0.3084 (2) | 0.08042 (9) | 0.0515 (3) | |
N2 | 0.43948 (8) | −0.2513 (3) | 0.06514 (10) | 0.0437 (3) | |
N1 | 0.37755 (9) | −0.1121 (3) | 0.09450 (10) | 0.0450 (3) | |
C4 | 0.29443 (11) | −0.1619 (3) | 0.04835 (12) | 0.0449 (4) | |
C5 | 0.23285 (11) | −0.0057 (3) | 0.08658 (12) | 0.0449 (4) | |
C2 | 0.52624 (10) | −0.1844 (3) | 0.10492 (11) | 0.0409 (3) | |
C8 | 0.12309 (12) | 0.3099 (3) | 0.15743 (15) | 0.0544 (4) | |
C7 | 0.20770 (13) | 0.2495 (4) | 0.22141 (14) | 0.0598 (5) | |
H7A | 0.2280 | 0.3142 | 0.2877 | 0.072* | |
C6 | 0.26121 (11) | 0.0927 (4) | 0.18559 (13) | 0.0544 (4) | |
H6A | 0.3181 | 0.0507 | 0.2287 | 0.065* | |
C10 | 0.14651 (12) | 0.0543 (4) | 0.02497 (14) | 0.0572 (5) | |
H10A | 0.1251 | −0.0132 | −0.0408 | 0.069* | |
C1 | 0.55118 (11) | 0.0442 (3) | 0.17832 (14) | 0.0517 (4) | |
H1B | 0.6144 | 0.0700 | 0.2004 | 0.078* | |
H1C | 0.5332 | 0.0054 | 0.2360 | 0.078* | |
H1D | 0.5219 | 0.2036 | 0.1456 | 0.078* | |
C9 | 0.09182 (12) | 0.2137 (4) | 0.06054 (15) | 0.0620 (5) | |
H9A | 0.0344 | 0.2544 | 0.0186 | 0.074* | |
C3 | 0.25881 (16) | −0.3524 (5) | −0.0385 (2) | 0.0663 (6) | |
H2A | 0.4257 (13) | −0.391 (4) | 0.0186 (17) | 0.062 (5)* | |
H3A | 0.197 (2) | −0.372 (5) | −0.064 (2) | 0.106 (9)* | |
H3B | 0.279 (3) | −0.503 (7) | −0.022 (3) | 0.155 (16)* | |
H3C | 0.278 (2) | −0.321 (6) | −0.094 (2) | 0.115 (10)* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
Cl1 | 0.0715 (4) | 0.0887 (5) | 0.0850 (5) | 0.0221 (3) | 0.0396 (3) | 0.0014 (3) |
O1 | 0.0511 (6) | 0.0533 (6) | 0.0489 (7) | 0.0016 (5) | 0.0151 (5) | −0.0108 (5) |
N2 | 0.0479 (7) | 0.0422 (7) | 0.0401 (7) | 0.0027 (6) | 0.0134 (5) | −0.0058 (5) |
N1 | 0.0475 (7) | 0.0469 (7) | 0.0399 (7) | 0.0038 (6) | 0.0137 (5) | −0.0018 (5) |
C4 | 0.0495 (8) | 0.0424 (8) | 0.0417 (8) | −0.0018 (6) | 0.0138 (6) | 0.0016 (6) |
C5 | 0.0462 (9) | 0.0451 (8) | 0.0414 (9) | −0.0024 (6) | 0.0119 (7) | 0.0029 (6) |
C2 | 0.0510 (8) | 0.0378 (7) | 0.0325 (7) | 0.0033 (6) | 0.0122 (6) | 0.0004 (5) |
C8 | 0.0520 (9) | 0.0554 (9) | 0.0615 (11) | 0.0043 (7) | 0.0267 (8) | 0.0037 (8) |
C7 | 0.0601 (10) | 0.0706 (11) | 0.0469 (10) | 0.0085 (9) | 0.0154 (8) | −0.0030 (8) |
C6 | 0.0501 (9) | 0.0641 (10) | 0.0442 (9) | 0.0074 (8) | 0.0092 (7) | −0.0016 (7) |
C10 | 0.0466 (9) | 0.0701 (11) | 0.0496 (10) | −0.0019 (8) | 0.0089 (7) | −0.0065 (8) |
C1 | 0.0571 (10) | 0.0488 (9) | 0.0491 (10) | −0.0064 (7) | 0.0175 (7) | −0.0115 (7) |
C9 | 0.0429 (8) | 0.0705 (11) | 0.0663 (12) | 0.0032 (8) | 0.0097 (8) | 0.0008 (9) |
C3 | 0.0595 (12) | 0.0661 (13) | 0.0687 (14) | −0.0060 (10) | 0.0154 (10) | −0.0225 (10) |
Geometric parameters (Å, º) top Cl1—C8 | 1.7512 (17) | C7—C6 | 1.370 (2) |
O1—C2 | 1.2269 (18) | C7—H7A | 0.9300 |
N2—C2 | 1.350 (2) | C6—H6A | 0.9300 |
N2—N1 | 1.3773 (17) | C10—C9 | 1.390 (3) |
N2—H2A | 0.93 (2) | C10—H10A | 0.9300 |
N1—C4 | 1.290 (2) | C1—H1B | 0.9600 |
C4—C5 | 1.486 (2) | C1—H1C | 0.9600 |
C4—C3 | 1.497 (2) | C1—H1D | 0.9600 |
C5—C10 | 1.391 (2) | C9—H9A | 0.9300 |
C5—C6 | 1.392 (2) | C3—H3A | 0.93 (3) |
C2—C1 | 1.498 (2) | C3—H3B | 0.83 (4) |
C8—C9 | 1.363 (3) | C3—H3C | 0.94 (3) |
C8—C7 | 1.381 (3) | | |
| | | |
C2—N2—N1 | 119.36 (13) | C7—C6—H6A | 119.1 |
C2—N2—H2A | 116.5 (12) | C5—C6—H6A | 119.1 |
N1—N2—H2A | 124.2 (12) | C9—C10—C5 | 120.84 (17) |
C4—N1—N2 | 118.22 (13) | C9—C10—H10A | 119.6 |
N1—C4—C5 | 114.25 (13) | C5—C10—H10A | 119.6 |
N1—C4—C3 | 125.23 (16) | C2—C1—H1B | 109.5 |
C5—C4—C3 | 120.50 (15) | C2—C1—H1C | 109.5 |
C10—C5—C6 | 117.66 (16) | H1B—C1—H1C | 109.5 |
C10—C5—C4 | 121.86 (15) | C2—C1—H1D | 109.5 |
C6—C5—C4 | 120.46 (14) | H1B—C1—H1D | 109.5 |
O1—C2—N2 | 120.14 (14) | H1C—C1—H1D | 109.5 |
O1—C2—C1 | 121.64 (14) | C8—C9—C10 | 119.41 (16) |
N2—C2—C1 | 118.22 (14) | C8—C9—H9A | 120.3 |
C9—C8—C7 | 121.30 (16) | C10—C9—H9A | 120.3 |
C9—C8—Cl1 | 119.82 (14) | C4—C3—H3A | 116.6 (17) |
C7—C8—Cl1 | 118.88 (15) | C4—C3—H3B | 110 (3) |
C6—C7—C8 | 118.87 (17) | H3A—C3—H3B | 106 (3) |
C6—C7—H7A | 120.6 | C4—C3—H3C | 115.3 (18) |
C8—C7—H7A | 120.6 | H3A—C3—H3C | 107 (2) |
C7—C6—C5 | 121.89 (16) | H3B—C3—H3C | 101 (3) |
Hydrogen-bond geometry (Å, º) top D—H···A | D—H | H···A | D···A | D—H···A |
N2—H2A···O1i | 0.93 (2) | 2.02 (2) | 2.9384 (18) | 170.3 (18) |
Symmetry code: (i) −x+1, −y−1, −z. |
Experimental details
Crystal data |
Chemical formula | C10H11ClN2O |
Mr | 210.66 |
Crystal system, space group | Monoclinic, P21/c |
Temperature (K) | 293 |
a, b, c (Å) | 15.944 (3), 5.0061 (10), 13.950 (3) |
β (°) | 109.45 (3) |
V (Å3) | 1049.9 (4) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.33 |
Crystal size (mm) | 0.25 × 0.20 × 0.20 |
|
Data collection |
Diffractometer | Bruker SMART CCD |
Absorption correction | – |
No. of measured, independent and observed [I > 2σ(I)] reflections | 9225, 2368, 1840 |
Rint | 0.028 |
(sin θ/λ)max (Å−1) | 0.649 |
|
Refinement |
R[F2 > 2σ(F2)], wR(F2), S | 0.046, 0.164, 1.22 |
No. of reflections | 2368 |
No. of parameters | 143 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.29, −0.22 |
Hydrogen-bond geometry (Å, º) top D—H···A | D—H | H···A | D···A | D—H···A |
N2—H2A···O1i | 0.93 (2) | 2.02 (2) | 2.9384 (18) | 170.3 (18) |
Symmetry code: (i) −x+1, −y−1, −z. |
Acknowledgements
The authors would like to thank the National Natural Science Foundation of Shandong Province (Y2008B29) and Yuandu Scholar of Weifang City.
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