organic compounds
1-Chloro-1-[(Z)-2-phenylhydrazin-1-ylidene]propan-2-one
aDepartment of Pharmaceutical Chemistry, College of Pharmacy, King Saud University, PO Box 2457, Riyadh 11451, Saudi Arabia, and bX-ray Crystallography Unit, School of Physics, Universiti Sains Malaysia, 11800 USM, Penang, Malaysia
*Correspondence e-mail: hkfun@usm.my
The title compound, C9H9ClN2O, is close to planar (r.m.s. deviation for the non-H atoms = 0.0446 Å); it exists in a cis conformation with respect to the C=N double bond. In the crystal, the ketone O atom accepts both N—H⋯O and C—H⋯O hydrogen bonds, which leads to [010] infinite chains incorporating R21(6) loops. The also features a C—H⋯π interaction.
Related literature
For synthetic applications of hydrazonoyl chlorides, see: Abdel-Aziz & Mekawey (2009). For graph-set descriptors of hydrogen-bond motifs, see: Bernstein et al. (1995). For related structures. see: Asiri et al. (2011a,b). For a historical perspective on the synthesis, see: Dieckmann & Platz (1905). For the stability of the temperature controller used in the data collection, see: Cosier & Glazer (1986).
Experimental
Crystal data
|
Refinement
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Data collection: APEX2 (Bruker, 2009); cell SAINT (Bruker, 2009); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL and PLATON (Spek, 2009).
Supporting information
https://doi.org/10.1107/S1600536812028759/hb6870sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S1600536812028759/hb6870Isup2.hkl
Supporting information file. DOI: https://doi.org/10.1107/S1600536812028759/hb6870Isup3.cml
The title compound was prepared by the coupling reaction of 3-chloro-2,4-pentanedione and the diazonium salt of aniline at 0–5 °C (Dieckmann & Platz, 1905). Yellow blocks were recrystallised from ethanol solution.
The atom H1N1 was located in a difference fourier map and refined freely [N1—H1N1 = 1.00 (3) Å]. The remaining H atoms were positioned geometrically [C—H = 0.95 and 0.98 Å] and refined using a riding model with Uiso(H) = 1.2 or 1.5Ueq(C). A rotating group model was applied to the methyl group. Five outliers, (102), (213), (113), (315) and (011) were omitted in the final refinement.
As part of our ongoing studies of the synthetic chemistry of hydrazonoyl chlorides (Abdel-Aziz & Mekawey, 2009), the title compound was prepared and its
is now reported.The ═N2 double bond. Bond lengths and angles are comparable to those in related structures (Asiri et al., 2011a,b).
of the title compound is shown in Fig. 1. All of the non-H atoms lie nearly on a plane with r.m.s. deviation of 0.0446 Å. The molecule exists in cis configuration with respect to the C7In the crystal (Fig. 2), molecules are linked by N1—H1N1···O1 and C1—H1A···O1 hydrogen bonds (Table 1), generating R21(6) loops (Bernstein et al., 1995) and forming infinite wave-like chains along [010]. The packing also features a C—H···π interaction (Table 1), involving Cg1, which is the centroid of C1–C6 ring.
For synthetic applications of hydrazonoyl chlorides, see: Abdel-Aziz & Mekawey (2009). For graph-set descriptors of hydrogen-bond motifs, see: Bernstein et al. (1995). For related structures. see: Asiri et al. (2011a,b). For a historical perspective on the synthesis, see: Dieckmann & Platz (1905). For the stability of the temperature controller used in the data collection, see: Cosier & Glazer (1986).
Data collection: APEX2 (Bruker, 2009); cell
SAINT (Bruker, 2009); data reduction: SAINT (Bruker, 2009); program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008) and PLATON (Spek, 2009).C9H9ClN2O | F(000) = 408 |
Mr = 196.63 | Dx = 1.384 Mg m−3 |
Monoclinic, P21/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ybc | Cell parameters from 3613 reflections |
a = 7.2681 (14) Å | θ = 2.5–30.0° |
b = 12.361 (2) Å | µ = 0.36 mm−1 |
c = 10.704 (2) Å | T = 100 K |
β = 101.158 (3)° | Block, yellow |
V = 943.5 (3) Å3 | 0.37 × 0.21 × 0.10 mm |
Z = 4 |
Bruker APEX DUO CCD diffractometer | 2722 independent reflections |
Radiation source: fine-focus sealed tube | 2225 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.030 |
φ and ω scans | θmax = 30.0°, θmin = 2.9° |
Absorption correction: multi-scan (SADABS; Bruker, 2009) | h = −10→10 |
Tmin = 0.877, Tmax = 0.963 | k = −17→14 |
8906 measured reflections | l = −15→13 |
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)] = 0.049 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.148 | w = 1/[σ2(Fo2) + (0.0802P)2 + 0.7657P] where P = (Fo2 + 2Fc2)/3 |
S = 1.06 | (Δ/σ)max < 0.001 |
2722 reflections | Δρmax = 0.86 e Å−3 |
124 parameters | Δρmin = −0.37 e Å−3 |
0 restraints | Extinction correction: SHELXTL (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.008 (3) |
C9H9ClN2O | V = 943.5 (3) Å3 |
Mr = 196.63 | Z = 4 |
Monoclinic, P21/c | Mo Kα radiation |
a = 7.2681 (14) Å | µ = 0.36 mm−1 |
b = 12.361 (2) Å | T = 100 K |
c = 10.704 (2) Å | 0.37 × 0.21 × 0.10 mm |
β = 101.158 (3)° |
Bruker APEX DUO CCD diffractometer | 2722 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2009) | 2225 reflections with I > 2σ(I) |
Tmin = 0.877, Tmax = 0.963 | Rint = 0.030 |
8906 measured reflections |
R[F2 > 2σ(F2)] = 0.049 | 0 restraints |
wR(F2) = 0.148 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.06 | Δρmax = 0.86 e Å−3 |
2722 reflections | Δρmin = −0.37 e Å−3 |
124 parameters |
Experimental. The crystal was placed in the cold stream of an Oxford Cryosystems Cobra open-flow nitrogen cryostat (Cosier & Glazer, 1986) operating at 100.0 (1) K. |
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 | ||
Cl1 | −0.00357 (7) | 0.01567 (4) | 0.18248 (4) | 0.02310 (16) | |
O1 | 0.0096 (2) | 0.24567 (12) | 0.25220 (13) | 0.0275 (3) | |
N1 | 0.1947 (2) | −0.08946 (14) | 0.41978 (16) | 0.0235 (4) | |
N2 | 0.1820 (2) | 0.01726 (13) | 0.42826 (16) | 0.0220 (3) | |
C1 | 0.2872 (3) | −0.26204 (17) | 0.51547 (19) | 0.0230 (4) | |
H1A | 0.2243 | −0.2962 | 0.4397 | 0.028* | |
C2 | 0.3780 (3) | −0.32397 (18) | 0.6175 (2) | 0.0265 (4) | |
H2A | 0.3769 | −0.4006 | 0.6112 | 0.032* | |
C3 | 0.4705 (3) | −0.27448 (19) | 0.72882 (19) | 0.0278 (4) | |
H3A | 0.5321 | −0.3169 | 0.7985 | 0.033* | |
C4 | 0.4715 (3) | −0.16205 (19) | 0.7370 (2) | 0.0277 (4) | |
H4A | 0.5349 | −0.1281 | 0.8128 | 0.033* | |
C5 | 0.3816 (3) | −0.09862 (18) | 0.63614 (19) | 0.0250 (4) | |
H5A | 0.3831 | −0.0220 | 0.6428 | 0.030* | |
C6 | 0.2890 (3) | −0.14930 (17) | 0.52499 (18) | 0.0216 (4) | |
C7 | 0.0985 (3) | 0.07370 (17) | 0.33405 (18) | 0.0225 (4) | |
C8 | 0.0876 (3) | 0.19245 (16) | 0.34351 (18) | 0.0221 (4) | |
C9 | 0.1800 (3) | 0.24284 (17) | 0.46791 (19) | 0.0256 (4) | |
H9A | 0.1471 | 0.3197 | 0.4678 | 0.038* | |
H9B | 0.3164 | 0.2353 | 0.4787 | 0.038* | |
H9C | 0.1367 | 0.2063 | 0.5382 | 0.038* | |
H1N1 | 0.129 (4) | −0.130 (2) | 0.344 (3) | 0.032 (7)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cl1 | 0.0330 (3) | 0.0140 (2) | 0.0192 (2) | 0.00383 (16) | −0.00273 (17) | −0.00116 (15) |
O1 | 0.0323 (8) | 0.0238 (7) | 0.0241 (7) | 0.0020 (6) | −0.0001 (6) | 0.0020 (6) |
N1 | 0.0275 (8) | 0.0211 (8) | 0.0202 (8) | 0.0017 (6) | 0.0006 (6) | 0.0010 (6) |
N2 | 0.0214 (7) | 0.0211 (8) | 0.0235 (8) | 0.0000 (6) | 0.0040 (6) | 0.0013 (6) |
C1 | 0.0220 (9) | 0.0246 (10) | 0.0210 (8) | −0.0009 (7) | 0.0010 (7) | 0.0004 (7) |
C2 | 0.0271 (9) | 0.0252 (10) | 0.0268 (10) | 0.0011 (8) | 0.0041 (8) | 0.0040 (8) |
C3 | 0.0270 (10) | 0.0324 (11) | 0.0222 (9) | 0.0008 (8) | 0.0000 (7) | 0.0064 (8) |
C4 | 0.0280 (10) | 0.0326 (11) | 0.0206 (9) | −0.0028 (8) | −0.0005 (7) | 0.0000 (8) |
C5 | 0.0274 (9) | 0.0234 (10) | 0.0234 (9) | −0.0017 (7) | 0.0027 (7) | 0.0002 (7) |
C6 | 0.0207 (8) | 0.0234 (9) | 0.0208 (9) | 0.0004 (7) | 0.0040 (7) | 0.0035 (7) |
C7 | 0.0237 (9) | 0.0233 (10) | 0.0196 (8) | 0.0003 (7) | 0.0019 (7) | −0.0002 (7) |
C8 | 0.0211 (8) | 0.0240 (10) | 0.0212 (9) | 0.0000 (7) | 0.0039 (7) | 0.0005 (7) |
C9 | 0.0283 (10) | 0.0240 (10) | 0.0227 (9) | −0.0004 (7) | 0.0002 (7) | −0.0018 (7) |
Cl1—C7 | 1.798 (2) | C3—C4 | 1.392 (3) |
O1—C8 | 1.223 (2) | C3—H3A | 0.9500 |
N1—N2 | 1.327 (2) | C4—C5 | 1.391 (3) |
N1—C6 | 1.409 (2) | C4—H4A | 0.9500 |
N1—H1N1 | 1.00 (3) | C5—C6 | 1.397 (3) |
N2—C7 | 1.279 (3) | C5—H5A | 0.9500 |
C1—C2 | 1.392 (3) | C7—C8 | 1.475 (3) |
C1—C6 | 1.397 (3) | C8—C9 | 1.505 (3) |
C1—H1A | 0.9500 | C9—H9A | 0.9800 |
C2—C3 | 1.391 (3) | C9—H9B | 0.9800 |
C2—H2A | 0.9500 | C9—H9C | 0.9800 |
N2—N1—C6 | 119.79 (17) | C4—C5—H5A | 120.5 |
N2—N1—H1N1 | 121.9 (15) | C6—C5—H5A | 120.5 |
C6—N1—H1N1 | 118.0 (15) | C5—C6—C1 | 120.37 (18) |
C7—N2—N1 | 121.15 (18) | C5—C6—N1 | 121.67 (18) |
C2—C1—C6 | 119.68 (19) | C1—C6—N1 | 117.96 (18) |
C2—C1—H1A | 120.2 | N2—C7—C8 | 120.84 (18) |
C6—C1—H1A | 120.2 | N2—C7—Cl1 | 122.96 (16) |
C3—C2—C1 | 120.5 (2) | C8—C7—Cl1 | 116.16 (14) |
C3—C2—H2A | 119.8 | O1—C8—C7 | 120.24 (18) |
C1—C2—H2A | 119.8 | O1—C8—C9 | 122.88 (19) |
C2—C3—C4 | 119.25 (19) | C7—C8—C9 | 116.87 (17) |
C2—C3—H3A | 120.4 | C8—C9—H9A | 109.5 |
C4—C3—H3A | 120.4 | C8—C9—H9B | 109.5 |
C5—C4—C3 | 121.2 (2) | H9A—C9—H9B | 109.5 |
C5—C4—H4A | 119.4 | C8—C9—H9C | 109.5 |
C3—C4—H4A | 119.4 | H9A—C9—H9C | 109.5 |
C4—C5—C6 | 119.0 (2) | H9B—C9—H9C | 109.5 |
C6—N1—N2—C7 | 179.46 (17) | N2—N1—C6—C5 | −4.6 (3) |
C6—C1—C2—C3 | 0.0 (3) | N2—N1—C6—C1 | 175.28 (17) |
C1—C2—C3—C4 | −0.1 (3) | N1—N2—C7—C8 | −178.98 (17) |
C2—C3—C4—C5 | 0.2 (3) | N1—N2—C7—Cl1 | −1.3 (3) |
C3—C4—C5—C6 | −0.1 (3) | N2—C7—C8—O1 | 179.02 (17) |
C4—C5—C6—C1 | −0.1 (3) | Cl1—C7—C8—O1 | 1.2 (2) |
C4—C5—C6—N1 | 179.75 (18) | N2—C7—C8—C9 | 0.5 (3) |
C2—C1—C6—C5 | 0.1 (3) | Cl1—C7—C8—C9 | −177.33 (13) |
C2—C1—C6—N1 | −179.73 (17) |
Cg1 is the centroid of the C1–C6 ring. |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1N1···O1i | 0.99 (3) | 2.01 (3) | 2.948 (2) | 157 (2) |
C1—H1A···O1i | 0.95 | 2.45 | 3.237 (3) | 140 |
C9—H9B···Cg1ii | 0.98 | 2.68 | 3.560 (2) | 149 |
Symmetry codes: (i) −x, y−1/2, −z+1/2; (ii) −x+1, −y, −z+1. |
Experimental details
Crystal data | |
Chemical formula | C9H9ClN2O |
Mr | 196.63 |
Crystal system, space group | Monoclinic, P21/c |
Temperature (K) | 100 |
a, b, c (Å) | 7.2681 (14), 12.361 (2), 10.704 (2) |
β (°) | 101.158 (3) |
V (Å3) | 943.5 (3) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 0.36 |
Crystal size (mm) | 0.37 × 0.21 × 0.10 |
Data collection | |
Diffractometer | Bruker APEX DUO CCD |
Absorption correction | Multi-scan (SADABS; Bruker, 2009) |
Tmin, Tmax | 0.877, 0.963 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 8906, 2722, 2225 |
Rint | 0.030 |
(sin θ/λ)max (Å−1) | 0.703 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.049, 0.148, 1.06 |
No. of reflections | 2722 |
No. of parameters | 124 |
H-atom treatment | H atoms treated by a mixture of independent and constrained refinement |
Δρmax, Δρmin (e Å−3) | 0.86, −0.37 |
Computer programs: APEX2 (Bruker, 2009), SAINT (Bruker, 2009), SHELXTL (Sheldrick, 2008) and PLATON (Spek, 2009).
Cg1 is the centroid of the C1–C6 ring. |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1N1···O1i | 0.99 (3) | 2.01 (3) | 2.948 (2) | 157 (2) |
C1—H1A···O1i | 0.95 | 2.45 | 3.237 (3) | 140 |
C9—H9B···Cg1ii | 0.98 | 2.68 | 3.560 (2) | 149 |
Symmetry codes: (i) −x, y−1/2, −z+1/2; (ii) −x+1, −y, −z+1. |
Footnotes
‡Thomson Reuters ResearcherID: A-3561-2009.
Acknowledgements
HKF and TSC thank Universiti Sains Malaysia (USM) for the Research University Grant (1001/PFIZIK/811160). TSC also thanks the Malaysian Government and USM for the award of a research fellowship. The authors thank the Deanship of Scientific Research and the Research Center, College of Pharmacy, King Saud University.
References
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This is an open-access article distributed under the terms of the Creative Commons Attribution (CC-BY) Licence, which permits unrestricted use, distribution, and reproduction in any medium, provided the original authors and source are cited.
As part of our ongoing studies of the synthetic chemistry of hydrazonoyl chlorides (Abdel-Aziz & Mekawey, 2009), the title compound was prepared and its crystal structure is now reported.
The asymmetric unit of the title compound is shown in Fig. 1. All of the non-H atoms lie nearly on a plane with r.m.s. deviation of 0.0446 Å. The molecule exists in cis configuration with respect to the C7═N2 double bond. Bond lengths and angles are comparable to those in related structures (Asiri et al., 2011a,b).
In the crystal (Fig. 2), molecules are linked by N1—H1N1···O1 and C1—H1A···O1 hydrogen bonds (Table 1), generating R21(6) loops (Bernstein et al., 1995) and forming infinite wave-like chains along [010]. The packing also features a C—H···π interaction (Table 1), involving Cg1, which is the centroid of C1–C6 ring.