supplementary materials


hb2720 scheme

Acta Cryst. (2008). E64, o865    [ doi:10.1107/S1600536808010118 ]

4-(Diethylamino)salicylaldehyde phenylsulfonylhydrazone

X.-S. Tai, Y.-M. Feng and F.-Y. Kong

Abstract top

In the title compound, C17H21N3O3S, the dihedral angle between the aromatic ring planes is 84.2 (2)°. The pendant ethyl groups of the -N(C2H5)2 group are disordered over two sets of positions in a 0.84 (2):0.16 (2) ratio. The molecular conformation is stabilized by an intramolecular O-H...N hydrogen bond, and intermolecular N-H...O bonds lead to [010] chains in the crystal structure.

Comment top

As part of our ongoing studies of aroylhydrazones as potential ligands (Tai et al., 2008), we now report the synthesis and structure of the title compound, (I), (Fig. 1).

The dihedral angle between the aromatic ring planes is 84.2 (2)°. The pendant ethyl groups of the -N(C2H5)2 grouping are disordered over two sets of positions in a 0.84 (2):0.16 (2) ratio. The molecular conformation is stabilised by an intramolecular O-H···N hydrogen bond and intermolecular N-H···O bonds lead to [010] chains in the crystal (Table 1).

Related literature top

For related literature, see: Tai et al. (2008).

Experimental top

3 mmol of p-(diethylamino)salicylaldehyde (3 mmol) was added to a solution of benzenesulfonyl hydrazide (3 mmol) in 10 ml of 95% ethanol. The mixture was continuously stirred for 4 h at refluxing temperature, evaporating some ethanol, then, upon cooling, the solid product was collected by filtration and dried in vacuo (yield 67%). Colourless plates of (I) were obtained by evaporation from a methanol solution after several days.

Refinement top

The H atoms were placed geometrically (C—H = 0.93–0.96 Å, N—H = 0.86 Å, O—H = 0.82Å) and refined as riding with Uiso(H) = 1.2Ueq(C, N) or 1.5Ueq(methyl C, O).

Computing details top

Data collection: SMART (Bruker, 2000); cell refinement: SAINT (Bruker, 2000); data reduction: SAINT (Bruker, 2000); 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).

Figures top
[Figure 1] Fig. 1. The molecular structure of (I) showing 30% displacement ellipsoids for the non-hydrogen atoms. Only the major disorder component is shown and the hydrogen bond is indicated by a double-dashed line.
4-(Diethylamino)salicylaldehyde phenylsulfonylhydrazone top
Crystal data top
C17H21N3O3SDx = 1.331 Mg m3
Mr = 347.43Mo Kα radiation
λ = 0.71073 Å
Orthorhombic, PbcnCell parameters from 3546 reflections
a = 29.874 (3) Åθ = 2.7–21.4º
b = 7.5153 (12) ŵ = 0.21 mm1
c = 15.4456 (19) ÅT = 293 (2) K
V = 3467.8 (8) Å3Plate, colourless
Z = 80.43 × 0.38 × 0.04 mm
F000 = 1472
Data collection top
Bruker SMART CCD
diffractometer
3052 independent reflections
Radiation source: fine-focus sealed tube2061 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.048
T = 293(2) Kθmax = 25.0º
ω scansθmin = 2.6º
Absorption correction: multi-scan
(SADABS; Bruker, 2000)
h = 35→34
Tmin = 0.916, Tmax = 0.992k = 8→7
16321 measured reflectionsl = 18→14
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.069H-atom parameters constrained
wR(F2) = 0.175  w = 1/[σ2(Fo2) + (0.0453P)2 + 7.4306P]
where P = (Fo2 + 2Fc2)/3
S = 1.08(Δ/σ)max = 0.001
3052 reflectionsΔρmax = 0.44 e Å3
258 parametersΔρmin = 0.30 e Å3
Primary atom site location: structure-invariant direct methodsExtinction correction: none
Crystal data top
C17H21N3O3SV = 3467.8 (8) Å3
Mr = 347.43Z = 8
Orthorhombic, PbcnMo Kα
a = 29.874 (3) ŵ = 0.21 mm1
b = 7.5153 (12) ÅT = 293 (2) K
c = 15.4456 (19) Å0.43 × 0.38 × 0.04 mm
Data collection top
Bruker SMART CCD
diffractometer
3052 independent reflections
Absorption correction: multi-scan
(SADABS; Bruker, 2000)
2061 reflections with I > 2σ(I)
Tmin = 0.916, Tmax = 0.992Rint = 0.048
16321 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.069258 parameters
wR(F2) = 0.175H-atom parameters constrained
S = 1.08Δρmax = 0.44 e Å3
3052 reflectionsΔρmin = 0.30 e Å3
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*/UeqOcc. (<1)
N10.31274 (11)0.2572 (5)0.9493 (2)0.0502 (9)
H10.29490.34990.93630.060*
N20.35710 (11)0.3011 (5)0.9253 (2)0.0512 (9)
N30.54548 (13)0.6991 (6)0.8710 (3)0.0794 (14)
O10.24926 (10)0.0597 (4)0.93219 (19)0.0596 (8)
O20.32557 (10)0.0581 (4)0.9110 (2)0.0643 (9)
O30.44009 (10)0.2276 (4)0.8794 (2)0.0773 (11)
H30.41370.20600.88930.116*
S10.29375 (3)0.08000 (14)0.89918 (7)0.0481 (3)
C10.29054 (13)0.1295 (5)0.7887 (3)0.0457 (10)
C20.32787 (15)0.1092 (6)0.7367 (3)0.0602 (12)
H20.35470.06830.76010.072*
C30.32493 (18)0.1505 (7)0.6499 (3)0.0727 (14)
H3A0.34980.13630.61420.087*
C40.28604 (19)0.2114 (7)0.6164 (3)0.0700 (14)
H40.28460.23960.55780.084*
C50.24886 (19)0.2323 (7)0.6664 (3)0.0693 (14)
H50.22240.27440.64200.083*
C60.25055 (15)0.1908 (6)0.7535 (3)0.0586 (12)
H60.22530.20370.78820.070*
C70.36859 (14)0.4638 (6)0.9325 (3)0.0517 (11)
H70.34730.54760.94890.062*
C80.41362 (13)0.5202 (6)0.9160 (3)0.0545 (11)
C90.44774 (14)0.4048 (6)0.8899 (3)0.0572 (12)
C100.49056 (14)0.4634 (6)0.8754 (3)0.0630 (13)
H100.51240.38200.85880.076*
C110.50227 (15)0.6425 (6)0.8849 (3)0.0661 (13)
C120.46791 (15)0.7606 (7)0.9108 (4)0.0725 (15)
H120.47420.88090.91790.087*
C130.42560 (15)0.6996 (6)0.9256 (3)0.0670 (14)
H130.40380.78040.94270.080*
C140.5780 (8)0.571 (4)0.8341 (15)0.095 (6)0.84 (2)
H14A0.57870.46770.87150.114*0.84 (2)
H14B0.56660.53270.77840.114*0.84 (2)
C150.6231 (3)0.6286 (18)0.8217 (10)0.114 (4)0.84 (2)
H15A0.62420.71370.77540.171*0.84 (2)
H15B0.64140.52800.80740.171*0.84 (2)
H15C0.63390.68260.87400.171*0.84 (2)
C160.5597 (2)0.8789 (15)0.8999 (8)0.076 (3)0.84 (2)
H16A0.59120.87700.91470.092*0.84 (2)
H16B0.54300.91230.95130.092*0.84 (2)
C170.5517 (3)1.012 (2)0.8301 (10)0.107 (4)0.84 (2)
H17A0.56490.97120.77720.161*0.84 (2)
H17B0.56501.12390.84630.161*0.84 (2)
H17C0.52011.02810.82200.161*0.84 (2)
C14'0.585 (4)0.574 (18)0.870 (7)0.08 (2)0.16 (2)
H14C0.57480.45340.88130.098*0.16 (2)
H14D0.60630.60790.91340.098*0.16 (2)
C15'0.606 (2)0.586 (8)0.779 (5)0.11 (2)0.16 (2)
H15D0.59390.68790.74960.170*0.16 (2)
H15E0.59850.48010.74720.170*0.16 (2)
H15F0.63750.59660.78460.170*0.16 (2)
C16'0.5486 (13)0.875 (8)0.826 (4)0.082 (18)0.16 (2)
H16C0.52070.90210.79690.099*0.16 (2)
H16D0.57240.87230.78300.099*0.16 (2)
C17'0.5588 (15)1.015 (10)0.896 (4)0.089 (19)0.16 (2)
H17D0.53201.04070.92800.133*0.16 (2)
H17E0.56941.12240.86890.133*0.16 (2)
H17F0.58130.97060.93460.133*0.16 (2)
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
N10.0406 (19)0.055 (2)0.055 (2)0.0017 (16)0.0002 (16)0.0013 (18)
N20.0378 (18)0.057 (2)0.059 (2)0.0001 (16)0.0014 (16)0.0042 (18)
N30.053 (2)0.065 (3)0.120 (4)0.008 (2)0.015 (2)0.019 (3)
O10.0506 (16)0.061 (2)0.067 (2)0.0052 (15)0.0125 (15)0.0017 (16)
O20.0634 (19)0.0535 (19)0.076 (2)0.0149 (15)0.0025 (16)0.0112 (17)
O30.0547 (19)0.053 (2)0.125 (3)0.0024 (16)0.0098 (19)0.022 (2)
S10.0427 (6)0.0449 (6)0.0566 (7)0.0016 (5)0.0036 (5)0.0027 (5)
C10.044 (2)0.038 (2)0.054 (3)0.0016 (18)0.001 (2)0.0076 (19)
C20.047 (3)0.069 (3)0.065 (3)0.007 (2)0.002 (2)0.002 (3)
C30.068 (3)0.085 (4)0.065 (4)0.003 (3)0.006 (3)0.001 (3)
C40.087 (4)0.066 (3)0.057 (3)0.001 (3)0.006 (3)0.000 (3)
C50.074 (3)0.063 (3)0.071 (3)0.017 (3)0.020 (3)0.005 (3)
C60.049 (2)0.062 (3)0.065 (3)0.009 (2)0.003 (2)0.007 (2)
C70.046 (2)0.048 (3)0.061 (3)0.005 (2)0.001 (2)0.003 (2)
C80.042 (2)0.053 (3)0.069 (3)0.002 (2)0.003 (2)0.003 (2)
C90.048 (2)0.051 (3)0.073 (3)0.001 (2)0.002 (2)0.011 (2)
C100.043 (2)0.055 (3)0.090 (4)0.003 (2)0.008 (2)0.018 (3)
C110.045 (2)0.068 (3)0.085 (4)0.003 (2)0.008 (2)0.009 (3)
C120.056 (3)0.053 (3)0.109 (4)0.003 (2)0.014 (3)0.011 (3)
C130.050 (3)0.054 (3)0.098 (4)0.005 (2)0.011 (3)0.009 (3)
C140.060 (9)0.096 (8)0.129 (17)0.014 (7)0.018 (10)0.045 (13)
C150.067 (6)0.131 (9)0.145 (11)0.011 (6)0.007 (6)0.040 (7)
C160.052 (4)0.075 (7)0.101 (8)0.006 (3)0.001 (4)0.019 (5)
C170.072 (6)0.097 (10)0.152 (11)0.004 (5)0.011 (7)0.011 (9)
C14'0.06 (4)0.08 (4)0.11 (7)0.01 (3)0.00 (4)0.02 (5)
C15'0.09 (4)0.11 (4)0.13 (6)0.01 (3)0.00 (4)0.03 (4)
C16'0.06 (2)0.08 (4)0.11 (5)0.00 (2)0.01 (2)0.02 (3)
C17'0.06 (2)0.08 (4)0.13 (5)0.00 (2)0.00 (3)0.02 (4)
Geometric parameters (Å, °) top
N1—N21.415 (4)C10—C111.398 (6)
N1—S11.642 (4)C10—H100.9300
N1—H10.9000C11—C121.415 (6)
N2—C71.275 (5)C12—C131.363 (6)
N3—C111.376 (6)C12—H120.9300
N3—C141.48 (3)C13—H130.9300
N3—C161.485 (11)C14—C151.42 (3)
N3—C16'1.50 (6)C14—H14A0.9700
N3—C14'1.50 (15)C14—H14B0.9700
O1—S11.432 (3)C15—H15A0.9600
O2—S11.419 (3)C15—H15B0.9600
O3—C91.361 (5)C15—H15C0.9600
O3—H30.8200C16—C171.49 (2)
S1—C11.750 (4)C16—H16A0.9700
C1—C21.382 (6)C16—H16B0.9700
C1—C61.391 (6)C17—H17A0.9600
C2—C31.380 (7)C17—H17B0.9600
C2—H20.9300C17—H17C0.9600
C3—C41.351 (7)C14'—C15'1.53 (16)
C3—H3A0.9300C14'—H14C0.9700
C4—C51.362 (7)C14'—H14D0.9700
C4—H40.9300C15'—H15D0.9600
C5—C61.383 (6)C15'—H15E0.9600
C5—H50.9300C15'—H15F0.9600
C6—H60.9300C16'—C17'1.54 (10)
C7—C81.433 (6)C16'—H16C0.9700
C7—H70.9300C16'—H16D0.9700
C8—C91.398 (6)C17'—H17D0.9600
C8—C131.403 (6)C17'—H17E0.9600
C9—C101.371 (6)C17'—H17F0.9600
N2—N1—S1112.9 (3)C9—C10—C11121.7 (4)
N2—N1—H1108.5C9—C10—H10119.1
S1—N1—H1108.5C11—C10—H10119.1
C7—N2—N1116.9 (4)N3—C11—C10121.1 (4)
C11—N3—C14118.4 (10)N3—C11—C12122.0 (4)
C11—N3—C16120.2 (5)C10—C11—C12116.9 (4)
C14—N3—C16121.2 (10)C13—C12—C11120.6 (5)
C11—N3—C16'113.9 (16)C13—C12—H12119.7
C14—N3—C16'111 (2)C11—C12—H12119.7
C16—N3—C16'47 (2)C12—C13—C8122.8 (4)
C11—N3—C14'123 (5)C12—C13—H13118.6
C14—N3—C14'23 (4)C8—C13—H13118.6
C16—N3—C14'111 (4)C15—C14—N3118.4 (18)
C16'—N3—C14'120 (6)C15—C14—H14A107.7
C9—O3—H3109.5N3—C14—H14A107.7
O2—S1—O1119.90 (19)C15—C14—H14B107.7
O2—S1—N1107.52 (19)N3—C14—H14B107.7
O1—S1—N1103.83 (18)H14A—C14—H14B107.1
O2—S1—C1108.52 (19)N3—C16—C17110.4 (12)
O1—S1—C1108.61 (19)N3—C16—H16A109.6
N1—S1—C1107.86 (19)C17—C16—H16A109.6
C2—C1—C6120.2 (4)N3—C16—H16B109.6
C2—C1—S1119.9 (3)C17—C16—H16B109.6
C6—C1—S1119.9 (3)H16A—C16—H16B108.1
C3—C2—C1119.2 (4)N3—C14'—C15'107 (8)
C3—C2—H2120.4N3—C14'—H14C110.3
C1—C2—H2120.4C15'—C14'—H14C110.3
C4—C3—C2120.2 (5)N3—C14'—H14D110.3
C4—C3—H3A119.9C15'—C14'—H14D110.3
C2—C3—H3A119.9H14C—C14'—H14D108.5
C3—C4—C5121.6 (5)C14'—C15'—H15D109.5
C3—C4—H4119.2C14'—C15'—H15E109.5
C5—C4—H4119.2H15D—C15'—H15E109.5
C4—C5—C6119.7 (5)C14'—C15'—H15F109.5
C4—C5—H5120.1H15D—C15'—H15F109.5
C6—C5—H5120.1H15E—C15'—H15F109.5
C5—C6—C1119.1 (5)N3—C16'—C17'107 (6)
C5—C6—H6120.5N3—C16'—H16C110.4
C1—C6—H6120.5C17'—C16'—H16C110.4
N2—C7—C8121.4 (4)N3—C16'—H16D110.4
N2—C7—H7119.3C17'—C16'—H16D110.4
C8—C7—H7119.3H16C—C16'—H16D108.6
C9—C8—C13116.2 (4)C16'—C17'—H17D109.5
C9—C8—C7123.5 (4)C16'—C17'—H17E109.5
C13—C8—C7120.3 (4)H17D—C17'—H17E109.5
O3—C9—C10116.9 (4)C16'—C17'—H17F109.5
O3—C9—C8121.3 (4)H17D—C17'—H17F109.5
C10—C9—C8121.9 (4)H17E—C17'—H17F109.5
S1—N1—N2—C7153.6 (3)C16'—N3—C11—C10141 (3)
N2—N1—S1—O252.0 (3)C14'—N3—C11—C1018 (4)
N2—N1—S1—O1179.9 (3)C14—N3—C11—C12172.9 (12)
N2—N1—S1—C164.8 (3)C16—N3—C11—C1212.5 (9)
O2—S1—C1—C231.0 (4)C16'—N3—C11—C1240 (3)
O1—S1—C1—C2162.8 (3)C14'—N3—C11—C12161 (4)
N1—S1—C1—C285.2 (4)C9—C10—C11—N3179.3 (5)
O2—S1—C1—C6149.7 (3)C9—C10—C11—C120.4 (8)
O1—S1—C1—C617.8 (4)N3—C11—C12—C13178.8 (5)
N1—S1—C1—C694.1 (4)C10—C11—C12—C130.1 (8)
C6—C1—C2—C30.0 (7)C11—C12—C13—C80.2 (9)
S1—C1—C2—C3179.4 (4)C9—C8—C13—C120.1 (8)
C1—C2—C3—C40.6 (8)C7—C8—C13—C12179.9 (5)
C2—C3—C4—C50.6 (8)C11—N3—C14—C15178.5 (15)
C3—C4—C5—C60.0 (8)C16—N3—C14—C154(2)
C4—C5—C6—C10.5 (7)C16'—N3—C14—C1548 (3)
C2—C1—C6—C50.5 (7)C14'—N3—C14—C1571 (15)
S1—C1—C6—C5178.8 (4)C11—N3—C16—C1789.7 (8)
N1—N2—C7—C8175.4 (4)C14—N3—C16—C1795.8 (13)
N2—C7—C8—C91.0 (7)C16'—N3—C16—C176(2)
N2—C7—C8—C13179.0 (5)C14'—N3—C16—C17118 (5)
C13—C8—C9—O3179.3 (5)C11—N3—C14'—C15'118 (7)
C7—C8—C9—O30.8 (7)C14—N3—C14'—C15'32 (11)
C13—C8—C9—C100.6 (7)C16—N3—C14'—C15'90 (6)
C7—C8—C9—C10179.4 (5)C16'—N3—C14'—C15'39 (8)
O3—C9—C10—C11179.5 (5)C11—N3—C16'—C17'101 (3)
C8—C9—C10—C110.8 (8)C14—N3—C16'—C17'123 (2)
C14—N3—C11—C108.3 (13)C16—N3—C16'—C17'9(2)
C16—N3—C11—C10166.3 (7)C14'—N3—C16'—C17'100 (4)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
O3—H3···N20.821.922.637 (4)146
N1—H1···O1i0.902.062.944 (5)169
Symmetry codes: (i) −x+1/2, y+1/2, z.
Table 1
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
O3—H3···N20.821.922.637 (4)146
N1—H1···O1i0.902.062.944 (5)169
Symmetry codes: (i) −x+1/2, y+1/2, z.
Acknowledgements top

The authors thank the National Natural Science Foundation of China (20671073), the National Natural Science Foundation of Shandong (Y2007B60), and the Science and Technology Foundation of Weifang and Weifang University for research grants.

references
References top

Bruker (2000). SMART, SAINT and SADABS. Bruker AXS Inc., Madison, Wisconsin, USA.

Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.

Tai, X.-S., Feng, Y.-M. & Kong, F.-Y. (2008). Acta Cryst. E64, o750.