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The title compound, C13H15ClN2O4, adopts a keto–hydrazo tautomeric form stabilized by intra­molecular N—H...O hydrogen bonds. The phenyl­hydrazone fragment is planar within ±0.028 (2) Å. The dihedral angle between the phenyl­hydrazone and oxobutanoate planes is 8.15 (9)°. Symmetry-related mol­ecules are linked via C—H...O hydrogen bonds to form chains along [101].

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536805030163/ci6657sup1.cif
Contains datablocks I, gokhan3

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536805030163/ci6657Isup2.hkl
Contains datablock I

CCDC reference: 287532

Key indicators

  • Single-crystal X-ray study
  • T = 296 K
  • Mean [sigma](C-C) = 0.004 Å
  • R factor = 0.040
  • wR factor = 0.117
  • Data-to-parameter ratio = 14.7

checkCIF/PLATON results

No syntax errors found



Alert level C PLAT250_ALERT_2_C Large U3/U1 Ratio for Average U(i,j) Tensor .... 2.12
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 1 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data 1 ALERT type 2 Indicator that the structure model may be wrong or deficient 0 ALERT type 3 Indicator that the structure quality may be low 0 ALERT type 4 Improvement, methodology, query or suggestion

Comment top

Various hydrazone compounds possess strong bactericidal, herbicidal, insecticidal and fungicidal properties (Sahni et al., 1977). Some phenylhydrazone derivatives have been shown to be potentially DNA-damaging and are mutagenic agents (Okabe et al., 1993). In addition, hydrazones have analytical applications (Heit & Ryan, 1966; Jensen & Pflaum, 1967; Dey et al., 1985). Hydrazones have interesting ligational properties as a result of the presence of several potential coordination sites (Dutta & Hossain, 1985), and both transition and non-transition metal complexes of these ligands have been synthesized previously (Dey et al., 1992).

As part of our ongoing research on phenylhydrazonodiones, the title compound, (I), has been synthesized and its crystal structure is reported here. Previously we reported the structure of ethyl 4-chloro- 3-oxo-2-(phenylhydrazono)butyrate (Alpaslan et al., 2005a), (E)-ethyl 4-chloro-3-[2-(2-fluorophenyl)hydrazono]butanoate (Alpaslan et al., 2005b), ethyl 4-chloro-2-[(2-nitrophenyl) hydrazono]-3-oxobutyrate (Odabaşoǧlu et al., 2005a) and ethyl 4-chloro-2-[(4-nitrophenyl)hydrazono]-3-oxobutyrate (Odabaşoǧlu et al., 2005b).

Our investigations show that, in the solid state, the molecular structure of (I) adopts the keto–hydrazo tautomeric form with intramolecular hydrogen bonds (Fig. 1). The phenylhydrazone fragment is planar within ±0.028 (2) Å, and atoms O4 and C7 deviate from that plane by 0.014 (3) and −0.165 (4) Å, respectively. The oxobutanoate fragment (O1–O3/C8–C13) is planar (r.m.s deviation 0.020 Å). The dihedral angle between the phenylhydrazone and O1–O3/C8–C13 planes is 8.15 (9)°.

It is remarkable that the Z isomer of the methoxyphenylhydrazone derivative was formed preferentially over the E isomer since the latter would almost certainly feature an N—H···OC intramolecular hydrogen bond. In (I), the imine group adopts a Z configuration, with bond lengths C1—N1 = 1.408 (2) Å, C8—N2 = 1.311 (2) Å and N1—N2 = 1.300 (2) Å. These data show that there is significant elongation of the N1—N2 bond and contraction of the C1—C2 bond in comparsion with azo compounds. For example, the NN and C—N bonds in azobenzene are 1.255 (2) Å and 1.432 (2) Å, respectively (Patai, 1975), while the CN double bonds in imine compounds are in the range 1.270 (5)–1.303 (3) Å (Ersanlı, Odabaşoǧlu, et al., 2004; Baughman et al., 2004; Ersanlı, Albayrak et al., 2004; Odabaşoǧlu et al., 2005; Şahin et al., 2005; Butcher et al., 2005). There is a moderately strong intramolecular N1—H1···O1 hydrogen bond, which is a common feature of similar systems {N—H···O = 1.99 (2) Å in ethyl 4-chloro-3-oxo-2-(phenlyhydrazono)butyrate (Alpaslan et al., 2005a); N—H···O = 1.96 (2) Å in (E)-ethyl 4-chloro-3-[2-(2-fluorophenly) hydrazono]butanoate (Alpaslan et al., 2005b)}. The carbonyl groups point in opposite sides of the C9—C11 chain and their bond distances of 1.203 (2) and 1.215 (2) Å are shorter than those observed in similar compounds (Chen et al., 2004; Odabaşoǧlu et al., 2003) but within the normal range for carbonyl compounds (Loudon, 2002).

In the crystal structure, C5—H5···O3i intermolecular hydrogen bonds link the molecules into a chain along [101] (Fig. 2); symmetry code (i) is given in Table 2.

Experimental top

A mixture of o-methoxyaniline (10 mmol), water (50 ml) and concentrated hydrochloric acid (30 mmol) was heated with stirring until a clear solution was obtained. This solution was cooled to 273–278 K and a solution of sodium nitrite (14 mmol) in water was added dropwise while the temperature was maintained below 278 K. The resulting mixture was stirred for 30 min in an ice bath. The pH was raised to 8–9 by adding dilute NaOH solution. Ethyl 4-chloroacetoacetate (10 mmol) solution in ethanol was gradually added to a cooled solution of the o-methoxybenzenediazonium chloride, prepared as described above. The resulting mixture was stirred at 273–278 K for 60 min in an ice bath and the pH was lowered to 5 with dilute HCl. The product was recrystallized from glacial acetic acid to obtain well shaped crystals of (I) (yield 86%, m.p. 423–424 K).

Refinement top

The H atom bonded to N1 was refined freely. All other H atoms were placed in calculated positions and constrained to ride on their parent atoms, with C—H = 0.93–0.97 Å and Uiso(H) = 1.2 Ueq(C) [1.5Ueq(methyl C)].

Computing details top

Data collection: X-AREA (Stoe & Cie, 2002); cell refinement: X-AREA; data reduction: X-RED32 (Stoe & Cie, 2002); program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).

Figures top
[Figure 1] Fig. 1. A view of (I), with the atomic numbering scheme and 50% probability displacement ellipsoids. Intramolecular hydrogen bonds are drawn as dashed lines.
[Figure 2] Fig. 2. Part of the crystal packing of (I). Hydrogen bonds are drawn as dashed lines.
(Z)-ethyl 4-chloro-2-(2-(2-methoxyphenyl)hydrazono)-3-oxobutanoate top
Crystal data top
C13H15ClN2O4Z = 2
Mr = 298.72F(000) = 312
Triclinic, P1Dx = 1.409 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71069 Å
a = 8.605 (5) ÅCell parameters from 8830 reflections
b = 8.981 (5) Åθ = 2.4–27.2°
c = 9.974 (5) ŵ = 0.29 mm1
α = 107.615 (5)°T = 296 K
β = 103.543 (5)°Prism, yellow
γ = 94.952 (5)°0.49 × 0.36 × 0.14 mm
V = 703.9 (7) Å3
Data collection top
STOE IPDS-II
diffractometer
2741 independent reflections
Radiation source: fine-focus sealed tube1906 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.027
Detector resolution: 6.67 pixels mm-1θmax = 26.0°, θmin = 2.4°
w scansh = 1010
Absorption correction: integration
(X-RED32; Stoe & Cie, 2002)
k = 1111
Tmin = 0.885, Tmax = 0.964l = 1212
10993 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)] = 0.040Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.117H atoms treated by a mixture of independent and constrained refinement
S = 1.03 w = 1/[σ2(Fo2) + (0.0645P)2 + 0.0281P]
where P = (Fo2 + 2Fc2)/3
2741 reflections(Δ/σ)max = 0.001
187 parametersΔρmax = 0.15 e Å3
0 restraintsΔρmin = 0.18 e Å3
Crystal data top
C13H15ClN2O4γ = 94.952 (5)°
Mr = 298.72V = 703.9 (7) Å3
Triclinic, P1Z = 2
a = 8.605 (5) ÅMo Kα radiation
b = 8.981 (5) ŵ = 0.29 mm1
c = 9.974 (5) ÅT = 296 K
α = 107.615 (5)°0.49 × 0.36 × 0.14 mm
β = 103.543 (5)°
Data collection top
STOE IPDS-II
diffractometer
2741 independent reflections
Absorption correction: integration
(X-RED32; Stoe & Cie, 2002)
1906 reflections with I > 2σ(I)
Tmin = 0.885, Tmax = 0.964Rint = 0.027
10993 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0400 restraints
wR(F2) = 0.117H atoms treated by a mixture of independent and constrained refinement
S = 1.03Δρmax = 0.15 e Å3
2741 reflectionsΔρmin = 0.18 e Å3
187 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
C10.1950 (2)0.5853 (2)0.4889 (2)0.0594 (5)
C20.1743 (3)0.7305 (3)0.5723 (2)0.0744 (6)
H20.24040.77820.66730.089*
C30.0556 (3)0.8064 (3)0.5156 (3)0.0921 (7)
H30.04050.90430.57250.110*
C40.0399 (3)0.7356 (4)0.3742 (4)0.0964 (9)
H40.12040.78610.33610.116*
C50.0184 (3)0.5927 (4)0.2894 (3)0.0833 (7)
H50.08280.54740.19350.100*
C60.0993 (2)0.5143 (3)0.3454 (2)0.0655 (5)
C70.0222 (3)0.2850 (4)0.1324 (2)0.0999 (8)
H7A0.08670.27280.14080.120*
H7B0.05070.18240.09530.120*
H7C0.02930.34260.06650.120*
C80.4985 (2)0.4883 (2)0.74401 (18)0.0521 (4)
C90.5891 (2)0.5861 (2)0.89488 (19)0.0554 (4)
C100.5456 (3)0.7501 (2)0.9452 (2)0.0768 (6)
H10A0.43910.74080.96180.092*
H10B0.54000.79610.86820.092*
C110.5138 (2)0.3230 (2)0.67202 (19)0.0568 (4)
C120.6319 (3)0.1000 (2)0.6823 (2)0.0728 (6)
H12A0.66340.09020.59310.087*
H12B0.52890.03080.65720.087*
C130.7580 (3)0.0549 (3)0.7864 (3)0.0876 (7)
H13A0.85880.12530.81190.105*
H13B0.77190.05190.74130.105*
H13C0.72430.06230.87310.105*
N10.30838 (19)0.5002 (2)0.54512 (17)0.0570 (4)
N20.39947 (17)0.56386 (17)0.67872 (15)0.0536 (4)
O10.43650 (18)0.24860 (17)0.54691 (14)0.0750 (4)
O20.61716 (17)0.26297 (15)0.75319 (13)0.0645 (4)
O30.68687 (18)0.54210 (16)0.97574 (14)0.0745 (4)
O40.13042 (18)0.3696 (2)0.27202 (15)0.0792 (4)
Cl10.68642 (8)0.87846 (7)1.10700 (6)0.0881 (2)
H10.307 (3)0.412 (3)0.499 (3)0.074 (7)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.0548 (10)0.0677 (12)0.0561 (10)0.0082 (9)0.0013 (8)0.0322 (9)
C20.0797 (14)0.0692 (13)0.0743 (13)0.0188 (11)0.0049 (11)0.0345 (11)
C30.0944 (17)0.0855 (17)0.1098 (19)0.0348 (14)0.0165 (15)0.0550 (16)
C40.0746 (15)0.113 (2)0.120 (2)0.0290 (15)0.0056 (15)0.077 (2)
C50.0612 (12)0.117 (2)0.0773 (14)0.0083 (13)0.0049 (11)0.0605 (16)
C60.0543 (11)0.0858 (15)0.0559 (11)0.0069 (10)0.0002 (9)0.0357 (11)
C70.0833 (16)0.132 (2)0.0541 (12)0.0032 (15)0.0121 (11)0.0154 (13)
C80.0550 (10)0.0515 (10)0.0448 (8)0.0088 (8)0.0018 (7)0.0180 (7)
C90.0594 (10)0.0522 (10)0.0473 (9)0.0079 (8)0.0005 (8)0.0176 (8)
C100.0890 (15)0.0580 (11)0.0575 (11)0.0137 (10)0.0155 (10)0.0089 (9)
C110.0562 (10)0.0590 (11)0.0493 (9)0.0110 (9)0.0043 (8)0.0172 (8)
C120.0932 (15)0.0572 (11)0.0577 (11)0.0294 (11)0.0055 (10)0.0116 (9)
C130.1139 (19)0.0707 (14)0.0689 (14)0.0370 (14)0.0027 (13)0.0210 (11)
N10.0586 (9)0.0589 (10)0.0445 (8)0.0112 (8)0.0041 (7)0.0178 (7)
N20.0542 (8)0.0565 (8)0.0437 (7)0.0071 (7)0.0008 (6)0.0190 (6)
O10.0829 (9)0.0651 (8)0.0530 (8)0.0236 (7)0.0093 (7)0.0038 (6)
O20.0781 (9)0.0546 (7)0.0503 (7)0.0203 (6)0.0010 (6)0.0140 (6)
O30.0829 (9)0.0653 (8)0.0560 (7)0.0185 (7)0.0161 (7)0.0177 (6)
O40.0683 (9)0.1021 (12)0.0498 (7)0.0104 (8)0.0073 (6)0.0196 (8)
Cl10.1087 (5)0.0644 (3)0.0593 (3)0.0090 (3)0.0121 (3)0.0034 (2)
Geometric parameters (Å, º) top
C1—C21.370 (3)C8—C91.475 (2)
C1—C61.392 (3)C9—O31.203 (2)
C1—N11.408 (2)C9—C101.516 (3)
C2—C31.382 (3)C10—Cl11.766 (2)
C2—H20.93C10—H10A0.97
C3—C41.376 (4)C10—H10B0.97
C3—H30.93C11—O11.215 (2)
C4—C51.362 (4)C11—O21.321 (2)
C4—H40.93C12—O21.451 (2)
C5—C61.389 (3)C12—C131.491 (3)
C5—H50.93C12—H12A0.97
C6—O41.368 (3)C12—H12B0.97
C7—O41.419 (3)C13—H13A0.96
C7—H7A0.96C13—H13B0.96
C7—H7B0.96C13—H13C0.96
C7—H7C0.96N1—N21.300 (2)
C8—N21.311 (2)N1—H10.79 (2)
C8—C111.473 (3)
C2—C1—C6120.45 (19)C8—C9—C10114.38 (15)
C2—C1—N1121.94 (18)C9—C10—Cl1112.93 (14)
C6—C1—N1117.6 (2)C9—C10—H10A109.0
C1—C2—C3120.2 (2)Cl1—C10—H10A109.0
C1—C2—H2119.9C9—C10—H10B109.0
C3—C2—H2119.9Cl1—C10—H10B109.0
C4—C3—C2119.4 (3)H10A—C10—H10B107.8
C4—C3—H3120.3O1—C11—O2123.04 (18)
C2—C3—H3120.3O1—C11—C8121.8 (2)
C5—C4—C3120.9 (2)O2—C11—C8115.15 (15)
C5—C4—H4119.5O2—C12—C13107.74 (17)
C3—C4—H4119.5O2—C12—H12A110.2
C4—C5—C6120.3 (2)C13—C12—H12A110.2
C4—C5—H5119.8O2—C12—H12B110.2
C6—C5—H5119.8C13—C12—H12B110.2
O4—C6—C5125.7 (2)H12A—C12—H12B108.5
O4—C6—C1115.59 (18)C12—C13—H13A109.5
C5—C6—C1118.7 (2)C12—C13—H13B109.5
O4—C7—H7A109.5H13A—C13—H13B109.5
O4—C7—H7B109.5C12—C13—H13C109.5
H7A—C7—H7B109.5H13A—C13—H13C109.5
O4—C7—H7C109.5H13B—C13—H13C109.5
H7A—C7—H7C109.5N2—N1—C1118.9 (2)
H7B—C7—H7C109.5N2—N1—H1121.6 (18)
N2—C8—C11122.51 (15)C1—N1—H1119.1 (18)
N2—C8—C9112.68 (16)N1—N2—C8122.97 (16)
C11—C8—C9124.8 (2)C11—O2—C12115.11 (15)
O3—C9—C8124.6 (2)C6—O4—C7117.03 (19)
O3—C9—C10121.01 (16)
C6—C1—C2—C31.4 (3)C8—C9—C10—Cl1166.16 (14)
N1—C1—C2—C3176.44 (19)N2—C8—C11—O11.0 (3)
C1—C2—C3—C40.8 (4)C9—C8—C11—O1179.55 (18)
C2—C3—C4—C50.5 (4)N2—C8—C11—O2179.07 (16)
C3—C4—C5—C61.1 (4)C9—C8—C11—O20.4 (3)
C4—C5—C6—O4178.8 (2)C2—C1—N1—N22.2 (3)
C4—C5—C6—C10.5 (3)C6—C1—N1—N2179.89 (16)
C2—C1—C6—O4179.86 (18)C1—N1—N2—C8174.2 (2)
N1—C1—C6—O42.2 (2)C11—C8—N2—N10.8 (3)
C2—C1—C6—C50.8 (3)C9—C8—N2—N1179.69 (16)
N1—C1—C6—C5177.21 (18)O1—C11—O2—C120.2 (3)
N2—C8—C9—O3179.88 (17)C8—C11—O2—C12179.9 (2)
C11—C8—C9—O30.6 (3)C13—C12—O2—C11177.42 (18)
N2—C8—C9—C102.1 (2)C5—C6—O4—C77.0 (3)
C11—C8—C9—C10177.41 (18)C1—C6—O4—C7172.30 (19)
O3—C9—C10—Cl115.7 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C5—H5···O3i0.932.563.413 (3)153
N1—H1···O10.79 (2)2.02 (2)2.602 (2)131 (2)
N1—H1···O40.79 (2)2.31 (2)2.635 (2)106 (2)
Symmetry code: (i) x1, y, z1.

Experimental details

Crystal data
Chemical formulaC13H15ClN2O4
Mr298.72
Crystal system, space groupTriclinic, P1
Temperature (K)296
a, b, c (Å)8.605 (5), 8.981 (5), 9.974 (5)
α, β, γ (°)107.615 (5), 103.543 (5), 94.952 (5)
V3)703.9 (7)
Z2
Radiation typeMo Kα
µ (mm1)0.29
Crystal size (mm)0.49 × 0.36 × 0.14
Data collection
DiffractometerSTOE IPDS-II
diffractometer
Absorption correctionIntegration
(X-RED32; Stoe & Cie, 2002)
Tmin, Tmax0.885, 0.964
No. of measured, independent and
observed [I > 2σ(I)] reflections
10993, 2741, 1906
Rint0.027
(sin θ/λ)max1)0.617
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.040, 0.117, 1.03
No. of reflections2741
No. of parameters187
H-atom treatmentH atoms treated by a mixture of independent and constrained refinement
Δρmax, Δρmin (e Å3)0.15, 0.18

Computer programs: X-AREA (Stoe & Cie, 2002), X-AREA, X-RED32 (Stoe & Cie, 2002), SHELXS97 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997), ORTEP-3 for Windows (Farrugia, 1997), WinGX (Farrugia, 1999).

Selected geometric parameters (Å, º) top
C6—O41.368 (3)C11—O11.215 (2)
C7—O41.419 (3)C11—O21.321 (2)
C9—O31.203 (2)C12—O21.451 (2)
N2—C8—C9112.68 (16)O1—C11—O2123.04 (18)
C11—C8—C9124.8 (2)O2—C11—C8115.15 (15)
O3—C9—C8124.6 (2)N2—N1—C1118.9 (2)
C8—C9—C10114.38 (15)N1—N2—C8122.97 (16)
N1—C1—C6—O42.2 (2)C1—N1—N2—C8174.2 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
C5—H5···O3i0.932.563.413 (3)153
N1—H1···O10.79 (2)2.02 (2)2.602 (2)131 (2)
N1—H1···O40.79 (2)2.31 (2)2.635 (2)106 (2)
Symmetry code: (i) x1, y, z1.
 

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