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The title compound, C14H11FN2O2, crystallizes with two mol­ecules in the asymmetric unit. Both mol­ecules are roughly planar and adopts a trans configuration with respect to the C=N double bond. In the crystal structure, inter­molecular O—H...O and N—H...O hydrogen bonds result in the formation of sheets parallel to the ac plane.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536805040420/dn6282sup1.cif
Contains datablocks global, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536805040420/dn6282Isup2.hkl
Contains datablock I

CCDC reference: 296556

Key indicators

  • Single-crystal X-ray study
  • T = 298 K
  • Mean [sigma](C-C) = 0.004 Å
  • R factor = 0.054
  • wR factor = 0.148
  • Data-to-parameter ratio = 12.6

checkCIF/PLATON results

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Alert level C PLAT026_ALERT_3_C Ratio Observed / Unique Reflections too Low .... 49 Perc. PLAT066_ALERT_1_C Predicted and Reported Transmissions Identical . ? PLAT242_ALERT_2_C Check Low Ueq as Compared to Neighbors for C12
0 ALERT level A = In general: serious problem 0 ALERT level B = Potentially serious problem 3 ALERT level C = Check and explain 0 ALERT level G = General alerts; check 1 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 1 ALERT type 3 Indicator that the structure quality may be low 0 ALERT type 4 Improvement, methodology, query or suggestion

Comment top

Schiff base compounds have been of great interest for many years. These compounds play an important role in the development of coordination chemistry related to catalysis and enzymatic reactions (Brunner et al., 1983), magnetism and molecular architectures (Miller et al., 2000). The deprotonated hydroxyl group of the salicylhydrazone will sometimes cause the N atom of the hydrazone to become more electron-rich as a result of conjugation effects, and the N atom can thus coordinate more strongly (Bansse et al., 1998). As an extension of work on the structural characterization of salicylhydrazone Schiff base compounds (Ma et al., 2005), we report here the crystal structure of (I), a new salicylhydrazone with 4-fluorobenzaldehyde.

In the title compound, (I), which crystallizes with two molecules in the asymmetric unit (Fig. 1), C—N bonds in the hydrazone units are rather short (Table 1) owing to conjugation effects (Ma et al., 2005). All other bond lengths are within normal ranges (Allen, 2002). The dihedral angles between the two benzene rings are 7.3 (2) ° and 18.7 (1) ° in the two molecules.

The occurrence of O—H···O hydrogen bonds results in the formation of infinite chains which are linked by N—H···O hydrogen bonds, forming sheets parallel to the ac plane (Table 2 and Fig. 2).

Experimental top

The reagents were commercial products and were used without further purification. 4-Fluorobenzaldehyde (0.2 mmol, 28 mg) and 2-hydroxybenzohydrazide (0.2 mmol, 30.4 mg) were dissolved in methanol (10 ml). The mixture was stirred at room temperature for about 10 min to give a clear yellow solution. The solution was set aside for 8 d to allow slow evaporation of the solvent. Large colourless block-shaped crystals separated; these were collected and washed three times with water.

Refinement top

All the H atoms were placed in geometrically idealized positions (

N—H 0.86, O—H 0.82 and C—H 0.93 Å) and treated as riding on their parent atoms withUiso(H) = 1.2Ueq(C,O,N).

Computing details top

Data collection: SMART (Bruker, 2002); cell refinement: SAINT (Bruker, 2002); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEPIII(Burnett & Johnson, 1996), ORTEP-3 for Windows (Farrugia, 1997) and CAMERON (Watkin et al., 1993); software used to prepare material for publication: SHELXL97.

Figures top
[Figure 1] Fig. 1. The structure of (I), showing 30% probability displacement ellipsoids and the atom-numbering scheme. The O—H···O hydrogen contact is represented by dashed line.
[Figure 2] Fig. 2. The crystal packing of (I), showing the formation of sheets. O—H···O and N—H···O hydrogen bonds are represented by dashed lines. H atoms not involved in hydrogen bonding have been omitted for clarity.
4-Fluorobenzaldehyde salicylhydrazone top
Crystal data top
C14H11FN2O2F(000) = 1072
Mr = 258.25Dx = 1.383 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ynCell parameters from 3063 reflections
a = 4.9532 (4) Åθ = 4.7–41.4°
b = 47.867 (4) ŵ = 0.10 mm1
c = 10.7392 (9) ÅT = 298 K
β = 102.953 (2)°Prism, colourless
V = 2481.4 (4) Å30.35 × 0.18 × 0.12 mm
Z = 8
Data collection top
Bruker SMART APEX area-detector
diffractometer
4358 independent reflections
Radiation source: fine-focus sealed tube2137 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.078
ϕ and ω scansθmax = 25.0°, θmin = 1.7°
Absorption correction: multi-scan
(SADABS; Bruker, 2002)
h = 55
Tmin = 0.964, Tmax = 0.988k = 5656
23870 measured reflectionsl = 1212
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)] = 0.054Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.148H-atom parameters constrained
S = 0.87 w = 1/[σ2(Fo2) + (0.086P)2]
where P = (Fo2 + 2Fc2)/3
4358 reflections(Δ/σ)max < 0.001
345 parametersΔρmax = 0.23 e Å3
0 restraintsΔρmin = 0.22 e Å3
Crystal data top
C14H11FN2O2V = 2481.4 (4) Å3
Mr = 258.25Z = 8
Monoclinic, P21/nMo Kα radiation
a = 4.9532 (4) ŵ = 0.10 mm1
b = 47.867 (4) ÅT = 298 K
c = 10.7392 (9) Å0.35 × 0.18 × 0.12 mm
β = 102.953 (2)°
Data collection top
Bruker SMART APEX area-detector
diffractometer
4358 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2002)
2137 reflections with I > 2σ(I)
Tmin = 0.964, Tmax = 0.988Rint = 0.078
23870 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0540 restraints
wR(F2) = 0.148H-atom parameters constrained
S = 0.87Δρmax = 0.23 e Å3
4358 reflectionsΔρmin = 0.22 e Å3
345 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
F10.6257 (6)0.26229 (4)0.7221 (2)0.1301 (9)
F20.3108 (4)0.00028 (4)0.19112 (19)0.0936 (7)
O10.5721 (4)0.11916 (4)0.48385 (17)0.0565 (5)
H10.67690.12020.43480.085*
O20.2614 (4)0.10829 (4)0.80849 (17)0.0652 (6)
O30.9649 (4)0.13193 (4)0.04409 (17)0.0578 (6)
H31.04210.12800.10180.087*
O40.9312 (4)0.13221 (4)0.34209 (16)0.0571 (5)
N10.2285 (5)0.13388 (5)0.6296 (2)0.0535 (6)
H1A0.26950.13570.55630.064*
N20.0700 (5)0.15371 (5)0.6713 (2)0.0522 (6)
N30.7514 (5)0.11446 (4)0.1462 (2)0.0487 (6)
H3A0.74740.11500.06570.058*
N40.5807 (5)0.09600 (4)0.1911 (2)0.0471 (6)
C10.4945 (5)0.09089 (5)0.6551 (2)0.0440 (7)
C20.6209 (5)0.09505 (6)0.5511 (2)0.0442 (7)
C30.7911 (6)0.07461 (6)0.5199 (3)0.0553 (8)
H3B0.87890.07770.45310.066*
C40.8323 (6)0.04992 (7)0.5859 (3)0.0624 (9)
H40.94780.03640.56370.075*
C50.7031 (7)0.04498 (6)0.6856 (3)0.0648 (9)
H50.72700.02810.72930.078*
C60.5394 (6)0.06549 (6)0.7184 (3)0.0562 (8)
H60.45470.06230.78610.067*
C70.3197 (5)0.11167 (6)0.7026 (3)0.0471 (7)
C80.0106 (6)0.17390 (6)0.5964 (3)0.0580 (8)
H80.03770.17430.51760.070*
C90.1765 (6)0.19658 (6)0.6295 (3)0.0550 (8)
C100.2270 (8)0.22005 (7)0.5530 (3)0.0793 (10)
H100.15710.22080.47960.095*
C110.3791 (9)0.24251 (7)0.5822 (4)0.0926 (12)
H110.41160.25830.53030.111*
C120.4793 (8)0.24048 (7)0.6911 (4)0.0851 (11)
C130.4365 (8)0.21777 (8)0.7673 (4)0.0851 (11)
H130.50910.21710.83990.102*
C140.2851 (7)0.19566 (6)0.7375 (3)0.0665 (9)
H140.25560.18000.79010.080*
C151.1052 (5)0.14987 (5)0.1685 (2)0.0429 (7)
C161.1297 (6)0.14964 (5)0.0406 (2)0.0462 (7)
C171.3156 (6)0.16702 (6)0.0006 (3)0.0551 (8)
H171.33180.16640.08400.066*
C181.4765 (6)0.18518 (6)0.0840 (3)0.0629 (9)
H181.60110.19680.05610.075*
C191.4533 (7)0.18615 (6)0.2101 (3)0.0672 (9)
H191.56010.19860.26720.081*
C201.2722 (6)0.16866 (6)0.2495 (3)0.0575 (8)
H201.25980.16930.33460.069*
C210.9230 (6)0.13160 (5)0.2254 (3)0.0460 (7)
C220.4147 (6)0.08257 (6)0.1039 (3)0.0490 (7)
H220.41590.08640.01910.059*
C230.2236 (6)0.06160 (5)0.1308 (3)0.0457 (7)
C240.0353 (6)0.04995 (6)0.0293 (3)0.0611 (8)
H240.03270.05600.05330.073*
C250.1479 (7)0.02965 (7)0.0480 (3)0.0679 (9)
H250.27590.02210.02060.082*
C260.1370 (7)0.02085 (6)0.1702 (3)0.0617 (8)
C270.0456 (7)0.03181 (6)0.2732 (3)0.0663 (9)
H270.04750.02560.35540.080*
C280.2269 (7)0.05228 (6)0.2532 (3)0.0593 (8)
H280.35250.05990.32240.071*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
F10.156 (2)0.0998 (16)0.146 (2)0.0663 (16)0.0584 (18)0.0092 (14)
F20.0897 (15)0.0772 (12)0.1212 (18)0.0317 (11)0.0388 (13)0.0007 (11)
O10.0657 (14)0.0655 (12)0.0473 (12)0.0061 (11)0.0317 (10)0.0092 (10)
O20.0869 (15)0.0802 (14)0.0377 (11)0.0165 (12)0.0333 (11)0.0089 (10)
O30.0662 (13)0.0778 (14)0.0370 (11)0.0146 (11)0.0275 (10)0.0108 (10)
O40.0658 (13)0.0781 (14)0.0319 (11)0.0136 (10)0.0207 (9)0.0006 (9)
N10.0694 (17)0.0592 (15)0.0382 (13)0.0120 (13)0.0256 (12)0.0039 (12)
N20.0597 (16)0.0573 (15)0.0418 (14)0.0087 (13)0.0160 (12)0.0019 (12)
N30.0590 (15)0.0543 (14)0.0371 (13)0.0086 (13)0.0198 (12)0.0005 (11)
N40.0521 (14)0.0500 (14)0.0429 (14)0.0042 (12)0.0184 (12)0.0027 (11)
C10.0477 (16)0.0533 (17)0.0328 (14)0.0022 (14)0.0130 (13)0.0003 (13)
C20.0453 (17)0.0534 (17)0.0342 (15)0.0009 (14)0.0095 (13)0.0000 (13)
C30.0581 (19)0.071 (2)0.0408 (17)0.0088 (17)0.0202 (14)0.0006 (15)
C40.066 (2)0.068 (2)0.054 (2)0.0182 (17)0.0173 (17)0.0019 (16)
C50.084 (2)0.063 (2)0.0497 (19)0.0135 (18)0.0218 (17)0.0106 (15)
C60.065 (2)0.066 (2)0.0425 (17)0.0064 (17)0.0215 (15)0.0059 (15)
C70.0489 (17)0.0596 (18)0.0355 (16)0.0032 (15)0.0154 (14)0.0002 (14)
C80.074 (2)0.063 (2)0.0416 (17)0.0090 (18)0.0217 (16)0.0000 (15)
C90.064 (2)0.0549 (19)0.0457 (18)0.0072 (16)0.0117 (15)0.0005 (15)
C100.108 (3)0.074 (2)0.058 (2)0.020 (2)0.024 (2)0.0079 (18)
C110.127 (3)0.065 (2)0.085 (3)0.027 (2)0.023 (3)0.020 (2)
C120.101 (3)0.065 (2)0.093 (3)0.031 (2)0.031 (2)0.002 (2)
C130.106 (3)0.084 (3)0.078 (3)0.030 (2)0.048 (2)0.009 (2)
C140.077 (2)0.067 (2)0.062 (2)0.0204 (18)0.0311 (18)0.0084 (17)
C150.0482 (16)0.0491 (16)0.0353 (15)0.0021 (14)0.0176 (13)0.0006 (13)
C160.0476 (17)0.0529 (17)0.0394 (16)0.0004 (14)0.0128 (14)0.0021 (14)
C170.063 (2)0.0665 (19)0.0403 (17)0.0057 (17)0.0219 (15)0.0069 (15)
C180.066 (2)0.065 (2)0.063 (2)0.0183 (17)0.0244 (18)0.0059 (17)
C190.081 (2)0.075 (2)0.0477 (19)0.0281 (19)0.0184 (17)0.0067 (16)
C200.073 (2)0.0629 (19)0.0418 (17)0.0141 (17)0.0241 (15)0.0048 (15)
C210.0498 (17)0.0515 (17)0.0400 (17)0.0028 (14)0.0170 (14)0.0004 (14)
C220.0545 (18)0.0556 (18)0.0396 (16)0.0014 (15)0.0162 (14)0.0004 (14)
C230.0512 (18)0.0454 (16)0.0426 (16)0.0017 (14)0.0148 (14)0.0035 (13)
C240.061 (2)0.072 (2)0.0492 (19)0.0114 (18)0.0112 (16)0.0049 (16)
C250.065 (2)0.075 (2)0.060 (2)0.0102 (18)0.0054 (17)0.0065 (17)
C260.058 (2)0.0504 (19)0.081 (3)0.0139 (16)0.0248 (18)0.0088 (17)
C270.083 (2)0.061 (2)0.064 (2)0.0103 (19)0.035 (2)0.0035 (17)
C280.071 (2)0.0609 (19)0.0462 (18)0.0104 (17)0.0137 (15)0.0011 (15)
Geometric parameters (Å, º) top
F1—C121.355 (4)C10—C111.389 (4)
F2—C261.359 (3)C10—H100.9300
O1—C21.354 (3)C11—C121.372 (5)
O1—H10.8200C11—H110.9300
O2—C71.245 (3)C12—C131.348 (4)
O3—C161.371 (3)C13—C141.376 (4)
O3—H30.8200C13—H130.9300
O4—C211.245 (3)C14—H140.9300
N1—C71.338 (3)C15—C201.388 (4)
N1—N21.370 (3)C15—C161.406 (3)
N1—H1A0.8600C15—C211.483 (3)
N2—C81.263 (3)C16—C171.379 (4)
N3—C211.340 (3)C17—C181.369 (4)
N3—N41.383 (3)C17—H170.9300
N3—H3A0.8600C18—C191.386 (4)
N4—C221.273 (3)C18—H180.9300
C1—C61.386 (3)C19—C201.362 (4)
C1—C21.411 (3)C19—H190.9300
C1—C71.483 (4)C20—H200.9300
C2—C31.381 (3)C22—C231.452 (4)
C3—C41.370 (4)C22—H220.9300
C3—H3B0.9300C23—C241.384 (4)
C4—C51.385 (4)C23—C281.385 (4)
C4—H40.9300C24—C251.375 (4)
C5—C61.369 (4)C24—H240.9300
C5—H50.9300C25—C261.367 (4)
C6—H60.9300C25—H250.9300
C8—C91.453 (4)C26—C271.367 (4)
C8—H80.9300C27—C281.378 (4)
C9—C101.381 (4)C27—H270.9300
C9—C141.384 (4)C28—H280.9300
C2—O1—H1109.5C12—C13—H13120.0
C16—O3—H3109.5C14—C13—H13120.0
C7—N1—N2120.1 (2)C13—C14—C9120.3 (3)
C7—N1—H1A119.9C13—C14—H14119.8
N2—N1—H1A119.9C9—C14—H14119.8
C8—N2—N1116.4 (2)C20—C15—C16116.6 (2)
C21—N3—N4121.4 (2)C20—C15—C21117.1 (2)
C21—N3—H3A119.3C16—C15—C21126.3 (2)
N4—N3—H3A119.3O3—C16—C17120.4 (2)
C22—N4—N3114.3 (2)O3—C16—C15119.0 (2)
C6—C1—C2117.5 (2)C17—C16—C15120.7 (3)
C6—C1—C7117.5 (2)C18—C17—C16120.7 (3)
C2—C1—C7125.1 (2)C18—C17—H17119.6
O1—C2—C3121.3 (2)C16—C17—H17119.6
O1—C2—C1119.0 (2)C17—C18—C19119.8 (3)
C3—C2—C1119.7 (2)C17—C18—H18120.1
C4—C3—C2120.9 (3)C19—C18—H18120.1
C4—C3—H3B119.5C20—C19—C18119.2 (3)
C2—C3—H3B119.5C20—C19—H19120.4
C3—C4—C5120.4 (3)C18—C19—H19120.4
C3—C4—H4119.8C19—C20—C15123.0 (3)
C5—C4—H4119.8C19—C20—H20118.5
C6—C5—C4118.6 (3)C15—C20—H20118.5
C6—C5—H5120.7O4—C21—N3121.8 (2)
C4—C5—H5120.7O4—C21—C15121.0 (2)
C5—C6—C1122.8 (3)N3—C21—C15117.2 (2)
C5—C6—H6118.6N4—C22—C23123.0 (3)
C1—C6—H6118.6N4—C22—H22118.5
O2—C7—N1121.4 (2)C23—C22—H22118.5
O2—C7—C1120.0 (3)C24—C23—C28118.7 (3)
N1—C7—C1118.6 (2)C24—C23—C22118.4 (3)
N2—C8—C9122.1 (3)C28—C23—C22122.8 (3)
N2—C8—H8119.0C25—C24—C23121.3 (3)
C9—C8—H8119.0C25—C24—H24119.3
C10—C9—C14118.2 (3)C23—C24—H24119.3
C10—C9—C8119.9 (3)C26—C25—C24118.2 (3)
C14—C9—C8121.9 (3)C26—C25—H25120.9
C9—C10—C11122.0 (3)C24—C25—H25120.9
C9—C10—H10119.0F2—C26—C27118.2 (3)
C11—C10—H10119.0F2—C26—C25119.4 (3)
C12—C11—C10117.1 (3)C27—C26—C25122.3 (3)
C12—C11—H11121.4C26—C27—C28118.8 (3)
C10—C11—H11121.4C26—C27—H27120.6
C13—C12—F1119.5 (4)C28—C27—H27120.6
C13—C12—C11122.4 (3)C27—C28—C23120.5 (3)
F1—C12—C11118.1 (3)C27—C28—H28119.7
C12—C13—C14119.9 (3)C23—C28—H28119.7
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1···O40.821.862.662 (2)165
O3—H3···O2i0.821.862.643 (2)159
N1—H1A···O10.862.002.653 (3)132
N1—H1A···O4ii0.862.533.109 (3)126
N3—H3A···O30.861.942.638 (3)137
Symmetry codes: (i) x+1, y, z1; (ii) x1, y, z.

Experimental details

Crystal data
Chemical formulaC14H11FN2O2
Mr258.25
Crystal system, space groupMonoclinic, P21/n
Temperature (K)298
a, b, c (Å)4.9532 (4), 47.867 (4), 10.7392 (9)
β (°) 102.953 (2)
V3)2481.4 (4)
Z8
Radiation typeMo Kα
µ (mm1)0.10
Crystal size (mm)0.35 × 0.18 × 0.12
Data collection
DiffractometerBruker SMART APEX area-detector
diffractometer
Absorption correctionMulti-scan
(SADABS; Bruker, 2002)
Tmin, Tmax0.964, 0.988
No. of measured, independent and
observed [I > 2σ(I)] reflections
23870, 4358, 2137
Rint0.078
(sin θ/λ)max1)0.595
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.054, 0.148, 0.87
No. of reflections4358
No. of parameters345
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)0.23, 0.22

Computer programs: SMART (Bruker, 2002), SAINT (Bruker, 2002), SAINT, SHELXS97 (Sheldrick, 1997), SHELXL97 (Sheldrick, 1997), ORTEPIII(Burnett & Johnson, 1996), ORTEP-3 for Windows (Farrugia, 1997) and CAMERON (Watkin et al., 1993), SHELXL97.

Selected bond lengths (Å) top
N1—C71.338 (3)N3—C211.340 (3)
N1—N21.370 (3)N3—N41.383 (3)
N2—C81.263 (3)N4—C221.273 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
O1—H1···O40.821.862.662 (2)165
O3—H3···O2i0.821.862.643 (2)159
N1—H1A···O10.862.002.653 (3)132
N1—H1A···O4ii0.862.533.109 (3)126
N3—H3A···O30.861.942.638 (3)137
Symmetry codes: (i) x+1, y, z1; (ii) x1, y, z.
 

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