organic compounds\(\def\hfill{\hskip 5em}\def\hfil{\hskip 3em}\def\eqno#1{\hfil {#1}}\)

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(E)-Benzyl 2-{4-[eth­yl(2-hy­dr­oxy­eth­yl)amino]­benzyl­­idene}hydrazinecarbodi­thio­ate

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aDepartment of Chemistry, Anhui University, Hefei, Anhui 230039, People's Republic of China
*Correspondence e-mail: 1295913906@qq.com

Edited by W. T. A. Harrison, University of Aberdeen, Scotland (Received 8 June 2021; accepted 31 August 2021; online 3 September 2021)

In the title compound, C19H23N3OS2, the dihedral angle between the aromatic rings is 86.80 (8)° and the tertiary amine grouping is almost planar (bond-angle sum at the N atom = 360.0°). In the crystal, pairwise N—H⋯O hydrogen bonds link the mol­ecules into inversion dimers, and O—H⋯S hydrogen bonds link the dimers into [101] chains.

3D view (loading...)
[Scheme 3D1]
Chemical scheme
[Scheme 1]

Structure description

The title compound, C19H23N3OS2, is a DπA type Schiff base with an aniline derivative as the electron-donating (D) group and a hydrazino­thioic acid benzyl ester as the electron-withdrawing (A) group. Schiff base ligands based on benzyl hydrazino­thio­ate are an important class of compounds that have attracted widespread inter­est (Zhao et al., 2008[Zhao, Q., Li, L., Li, F. Y., Yu, M. X., Liu, Z. P., Yi, T. & Huang, C. H. (2008). Chem. Commun. pp. 685-687.]).

The crystal structure has triclinic (P[\overline{1}]) symmetry. The dihedral angle between the C3–C8 and C10–C15 benzene rings is 86.80 (8)° and the C1—N1—N2—C9 torsion angle is −170.6 (2)° (Fig. 1[link]). This twisted conformation may effectively inhibit fluorescence quenching in the crystal by reducing ππ stacking between mol­ecules. The S1/S2/N1/N2/C1 grouping is close to planar (r.m.s. deviation = 0.026 Å) and the geometry at N3 is almost planar (bond-angle sum = 360.0°) and C17 and C19 point from C13/C16/C18/N3 in opposite directions [deviations = −1.411 (2) and 1.334 (2) Å, respectively].

[Figure 1]
Figure 1
The mol­ecular structure of the title compound showing 50% displacement ellipsoids.

In the extended structure, pairwise N—H⋯O hydrogen bonds (Table 1[link]) generate inversion dimers featuring R22(22) loops, and O—H⋯S hydrogen bonds link the dimers into [101] chains (Fig. 2[link]).

Table 1
Hydrogen-bond geometry (Å, °)

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1A⋯O1i 0.88 2.06 2.933 (3) 175
O1—H1⋯S1ii 0.84 2.36 3.1749 (19) 163
Symmetry codes: (i) [-x+1, -y, -z+1]; (ii) [x-1, y, z-1].
[Figure 2]
Figure 2
The inter­molecular hydrogen bond diagram of compound. Symmetry codes: (i) −x + 1, −y, −z + 1; (ii) x + 1, y, z + 1

Synthesis and crystallization

In a 100 ml round-bottomed flask, 3.40 g (0.17 mol) of benzyl­hydrazine carbon di­sulfide and 3.00 g (0.17 mol) of 4-(eth­yl(2-hy­droxy­eth­yl) amino) benzaldehyde were dissolved in 50 ml of ethanol and stirred at room temperature for 15 minutes and then transferred to an oil bath for reflux at 353 K for 3 h. After the reaction was cooled to room temperature, a yellow solid 5.10 g (yield 84%) was precipitated out and recovered by filtration. Colourless blocks were recrystallized from ethanol solution.

Refinement

Crystal data, data collection and structure refinement details are summarized in Table 2[link].

Table 2
Experimental details

Crystal data
Chemical formula C19H23N3OS2
Mr 373.52
Crystal system, space group Triclinic, P[\overline{1}]
Temperature (K) 120
a, b, c (Å) 9.1794 (18), 9.4642 (19), 11.665 (2)
α, β, γ (°) 101.78 (3), 107.81 (3), 93.57 (3)
V3) 936.1 (4)
Z 2
Radiation type Mo Kα
μ (mm−1) 0.30
Crystal size (mm) 0.12 × 0.11 × 0.1
 
Data collection
Diffractometer Stoe X-AREA CCD
Absorption correction Multi-scan (X-RED32; Stoe, 2018[Stoe (2018). X-AREA and X-RED32. Stoe & Cie, Darmstadt, Germany.])
Tmin, Tmax 0.342, 0.808
No. of measured, independent and observed [I > 2σ(I)] reflections 8565, 3419, 2508
Rint 0.038
(sin θ/λ)max−1) 0.609
 
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.039, 0.097, 0.92
No. of reflections 3419
No. of parameters 228
H-atom treatment H-atom parameters constrained
Δρmax, Δρmin (e Å−3) 0.43, −0.25
Computer programs: X-AREA (Stoe, 2018[Stoe (2018). X-AREA and X-RED32. Stoe & Cie, Darmstadt, Germany.]), SHELXT2018/2 (Sheldrick, 2015a[Sheldrick, G. M. (2015a). Acta Cryst. A71, 3-8.]), SHELXL2018/3 (Sheldrick, 2015b[Sheldrick, G. M. (2015b). Acta Cryst. C71, 3-8.]) and OLEX2 (Dolomanov et al., 2009[Dolomanov, O. V., Bourhis, L. J., Gildea, R. J., Howard, J. A. K. & Puschmann, H. (2009). J. Appl. Cryst. 42, 339-341.]).

Structural data


Computing details top

Data collection: X-AREA Pilatus3_SV (Stoe, 2018); cell refinement: X-AREA Recipe (Stoe, 2018); data reduction: X-AREA Integrate (Stoe, 2018) X-AREA LANA (Stoe, 2018); program(s) used to solve structure: SHELXT2018/2 (Sheldrick, 2015a); program(s) used to refine structure: SHELXL2018/3 (Sheldrick, 2015b); molecular graphics: OLEX2 (Dolomanov et al., 2009); software used to prepare material for publication: OLEX2 (Dolomanov et al., 2009).

(E)-Benzyl 2-{4-[ethyl(2-hydroxyethyl)amino]benzylidene}hydrazinecarbodithioate top
Crystal data top
C19H23N3OS2Z = 2
Mr = 373.52F(000) = 396
Triclinic, P1Dx = 1.325 Mg m3
a = 9.1794 (18) ÅMo Kα radiation, λ = 0.71073 Å
b = 9.4642 (19) ÅCell parameters from 8567 reflections
c = 11.665 (2) Åθ = 69.8–4.3°
α = 101.78 (3)°µ = 0.30 mm1
β = 107.81 (3)°T = 120 K
γ = 93.57 (3)°Block, colourless
V = 936.1 (4) Å30.12 × 0.11 × 0.1 mm
Data collection top
Stoe X-Area CCD
diffractometer
2508 reflections with I > 2σ(I)
φ and ω scansRint = 0.038
Absorption correction: multi-scan
(X-Red32; Stoe, 2018)
θmax = 25.6°, θmin = 1.9°
Tmin = 0.342, Tmax = 0.808h = 1110
8565 measured reflectionsk = 410
3419 independent reflectionsl = 1413
Refinement top
Refinement on F2Primary atom site location: dual
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.039H-atom parameters constrained
wR(F2) = 0.097 w = 1/[σ2(Fo2) + (0.0568P)2]
where P = (Fo2 + 2Fc2)/3
S = 0.92(Δ/σ)max = 0.001
3419 reflectionsΔρmax = 0.43 e Å3
228 parametersΔρmin = 0.25 e Å3
0 restraints
Special details top

Geometry. All esds (except the esd in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell esds are taken into account individually in the estimation of esds in distances, angles and torsion angles; correlations between esds in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell esds is used for estimating esds involving l.s. planes.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
S11.15987 (6)0.04410 (6)0.90983 (5)0.02333 (15)
S21.05575 (6)0.31931 (6)0.83421 (5)0.02330 (15)
O10.22245 (18)0.21535 (18)0.18795 (14)0.0262 (4)
H10.2233360.1816750.1157670.039*
N10.8765 (2)0.0761 (2)0.79056 (16)0.0233 (4)
H1A0.8507890.0135760.7943320.028*
N20.7650 (2)0.1512 (2)0.73042 (16)0.0228 (4)
N30.1089 (2)0.2823 (2)0.39125 (16)0.0224 (4)
C11.0235 (2)0.1382 (2)0.84322 (19)0.0223 (5)
C21.2647 (3)0.3598 (3)0.9062 (2)0.0290 (5)
H2A1.2941230.3552900.9942450.035*
H2B1.3157570.2872560.8635820.035*
C31.3150 (2)0.5093 (3)0.8965 (2)0.0238 (5)
C41.3139 (3)0.6313 (3)0.9856 (2)0.0273 (5)
H41.2769950.6203161.0514070.033*
C51.3663 (3)0.7686 (3)0.9790 (2)0.0308 (6)
H51.3657200.8512171.0406720.037*
C61.4193 (3)0.7867 (3)0.8836 (2)0.0320 (6)
H61.4552930.8812180.8795350.038*
C71.4196 (3)0.6659 (3)0.7939 (2)0.0335 (6)
H71.4558630.6777090.7280000.040*
C81.3675 (3)0.5285 (3)0.7997 (2)0.0298 (5)
H81.3673710.4463180.7373040.036*
C90.6253 (2)0.0890 (2)0.6989 (2)0.0228 (5)
H90.6069100.0015680.7233930.027*
C100.4956 (2)0.1479 (2)0.6275 (2)0.0220 (5)
C110.5133 (3)0.2530 (2)0.5624 (2)0.0231 (5)
H110.6144000.2938220.5710930.028*
C120.3883 (2)0.2988 (2)0.4861 (2)0.0231 (5)
H120.4050890.3692350.4423120.028*
C130.2348 (2)0.2430 (2)0.47130 (19)0.0208 (5)
C140.2178 (3)0.1427 (2)0.5421 (2)0.0240 (5)
H140.1172630.1070960.5391120.029*
C150.3445 (3)0.0952 (3)0.6157 (2)0.0255 (5)
H150.3288340.0247290.6597590.031*
C160.1209 (3)0.3845 (2)0.3153 (2)0.0243 (5)
H16A0.2214830.4476820.3544560.029*
H16B0.0385550.4476870.3131280.029*
C170.1074 (3)0.3110 (2)0.1842 (2)0.0243 (5)
H17A0.0034080.2550980.1408830.029*
H17B0.1226810.3850340.1384670.029*
C180.0480 (2)0.2184 (3)0.3739 (2)0.0244 (5)
H18A0.0472290.1148060.3775210.029*
H18B0.1160340.2216950.2905400.029*
C190.1142 (3)0.2960 (3)0.4705 (2)0.0324 (6)
H19A0.2161510.2449270.4575630.049*
H19B0.1238430.3963990.4625460.049*
H19C0.0451870.2967060.5534570.049*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
S10.0216 (3)0.0248 (3)0.0193 (3)0.0069 (2)0.0006 (2)0.0039 (2)
S20.0180 (3)0.0264 (3)0.0225 (3)0.0036 (2)0.0004 (2)0.0086 (2)
O10.0268 (9)0.0339 (9)0.0189 (8)0.0075 (7)0.0093 (7)0.0048 (7)
N10.0204 (10)0.0239 (10)0.0225 (10)0.0028 (7)0.0021 (8)0.0063 (8)
N20.0201 (10)0.0292 (10)0.0175 (9)0.0060 (8)0.0026 (8)0.0064 (8)
N30.0176 (9)0.0329 (11)0.0173 (9)0.0039 (7)0.0045 (7)0.0086 (8)
C10.0237 (12)0.0291 (13)0.0131 (11)0.0043 (9)0.0048 (9)0.0041 (9)
C20.0198 (12)0.0321 (13)0.0284 (13)0.0033 (9)0.0017 (10)0.0077 (10)
C30.0151 (11)0.0304 (13)0.0225 (12)0.0031 (9)0.0002 (9)0.0075 (9)
C40.0231 (12)0.0371 (14)0.0230 (12)0.0088 (10)0.0066 (10)0.0097 (10)
C50.0267 (13)0.0301 (14)0.0300 (14)0.0075 (10)0.0017 (11)0.0049 (10)
C60.0188 (12)0.0337 (14)0.0402 (15)0.0008 (10)0.0007 (11)0.0184 (12)
C70.0213 (12)0.0544 (17)0.0271 (13)0.0045 (11)0.0068 (10)0.0164 (12)
C80.0231 (12)0.0393 (14)0.0227 (12)0.0041 (10)0.0040 (10)0.0035 (10)
C90.0226 (12)0.0241 (12)0.0200 (11)0.0021 (9)0.0055 (9)0.0041 (9)
C100.0195 (11)0.0252 (12)0.0182 (11)0.0031 (9)0.0037 (9)0.0024 (9)
C110.0178 (11)0.0318 (13)0.0195 (11)0.0010 (9)0.0079 (9)0.0031 (9)
C120.0225 (12)0.0287 (13)0.0200 (12)0.0030 (9)0.0088 (9)0.0072 (9)
C130.0205 (11)0.0255 (12)0.0137 (11)0.0026 (8)0.0041 (9)0.0011 (9)
C140.0165 (11)0.0297 (13)0.0235 (12)0.0007 (9)0.0036 (9)0.0074 (9)
C150.0224 (12)0.0294 (13)0.0228 (12)0.0009 (9)0.0036 (10)0.0090 (10)
C160.0260 (12)0.0251 (12)0.0207 (12)0.0065 (9)0.0049 (10)0.0060 (9)
C170.0240 (12)0.0287 (13)0.0203 (12)0.0056 (9)0.0055 (9)0.0081 (9)
C180.0170 (11)0.0332 (13)0.0194 (11)0.0029 (9)0.0027 (9)0.0031 (9)
C190.0261 (13)0.0457 (16)0.0237 (13)0.0038 (11)0.0104 (10)0.0013 (11)
Geometric parameters (Å, º) top
S1—C11.670 (2)C8—H80.9500
S2—C11.751 (2)C9—H90.9500
S2—C21.823 (2)C9—C101.445 (3)
O1—H10.8400C10—C111.398 (3)
O1—C171.429 (3)C10—C151.400 (3)
N1—H1A0.8800C11—H110.9500
N1—N21.379 (3)C11—C121.375 (3)
N1—C11.338 (3)C12—H120.9500
N2—C91.286 (3)C12—C131.420 (3)
N3—C131.371 (3)C13—C141.411 (3)
N3—C161.459 (3)C14—H140.9500
N3—C181.464 (3)C14—C151.380 (3)
C2—H2A0.9900C15—H150.9500
C2—H2B0.9900C16—H16A0.9900
C2—C31.498 (3)C16—H16B0.9900
C3—C41.390 (3)C16—C171.509 (3)
C3—C81.395 (3)C17—H17A0.9900
C4—H40.9500C17—H17B0.9900
C4—C51.382 (3)C18—H18A0.9900
C5—H50.9500C18—H18B0.9900
C5—C61.379 (3)C18—C191.521 (3)
C6—H60.9500C19—H19A0.9800
C6—C71.384 (4)C19—H19B0.9800
C7—H70.9500C19—H19C0.9800
C7—C81.379 (4)
C1—S2—C2101.28 (11)C15—C10—C9120.5 (2)
C17—O1—H1109.5C10—C11—H11119.1
N2—N1—H1A119.7C12—C11—C10121.8 (2)
C1—N1—H1A119.7C12—C11—H11119.1
C1—N1—N2120.63 (18)C11—C12—H12119.3
C9—N2—N1114.97 (19)C11—C12—C13121.4 (2)
C13—N3—C16123.26 (18)C13—C12—H12119.3
C13—N3—C18121.00 (18)N3—C13—C12122.15 (19)
C16—N3—C18115.70 (18)N3—C13—C14121.34 (19)
S1—C1—S2124.96 (13)C14—C13—C12116.5 (2)
N1—C1—S1120.51 (17)C13—C14—H14119.4
N1—C1—S2114.53 (17)C15—C14—C13121.2 (2)
S2—C2—H2A110.0C15—C14—H14119.4
S2—C2—H2B110.0C10—C15—H15119.0
H2A—C2—H2B108.4C14—C15—C10121.9 (2)
C3—C2—S2108.51 (16)C14—C15—H15119.0
C3—C2—H2A110.0N3—C16—H16A108.9
C3—C2—H2B110.0N3—C16—H16B108.9
C4—C3—C2120.6 (2)N3—C16—C17113.41 (19)
C4—C3—C8118.8 (2)H16A—C16—H16B107.7
C8—C3—C2120.6 (2)C17—C16—H16A108.9
C3—C4—H4119.8C17—C16—H16B108.9
C5—C4—C3120.4 (2)O1—C17—C16108.64 (18)
C5—C4—H4119.8O1—C17—H17A110.0
C4—C5—H5119.7O1—C17—H17B110.0
C6—C5—C4120.6 (2)C16—C17—H17A110.0
C6—C5—H5119.7C16—C17—H17B110.0
C5—C6—H6120.3H17A—C17—H17B108.3
C5—C6—C7119.4 (2)N3—C18—H18A109.0
C7—C6—H6120.3N3—C18—H18B109.0
C6—C7—H7119.8N3—C18—C19113.08 (19)
C8—C7—C6120.4 (2)H18A—C18—H18B107.8
C8—C7—H7119.8C19—C18—H18A109.0
C3—C8—H8119.8C19—C18—H18B109.0
C7—C8—C3120.4 (2)C18—C19—H19A109.5
C7—C8—H8119.8C18—C19—H19B109.5
N2—C9—H9119.0C18—C19—H19C109.5
N2—C9—C10122.0 (2)H19A—C19—H19B109.5
C10—C9—H9119.0H19A—C19—H19C109.5
C11—C10—C9122.4 (2)H19B—C19—H19C109.5
C11—C10—C15117.1 (2)
S2—C2—C3—C486.2 (2)C6—C7—C8—C30.5 (4)
S2—C2—C3—C895.4 (2)C8—C3—C4—C51.0 (3)
N1—N2—C9—C10175.48 (19)C9—C10—C11—C12174.2 (2)
N2—N1—C1—S1176.94 (15)C9—C10—C15—C14176.0 (2)
N2—N1—C1—S22.7 (3)C10—C11—C12—C131.0 (3)
N2—C9—C10—C1116.2 (3)C11—C10—C15—C140.8 (3)
N2—C9—C10—C15167.2 (2)C11—C12—C13—N3176.9 (2)
N3—C13—C14—C15175.2 (2)C11—C12—C13—C142.2 (3)
N3—C16—C17—O156.2 (2)C12—C13—C14—C153.9 (3)
C1—S2—C2—C3175.21 (17)C13—N3—C16—C1798.0 (2)
C1—N1—N2—C9170.6 (2)C13—N3—C18—C1984.7 (3)
C2—S2—C1—S12.66 (17)C13—C14—C15—C102.4 (4)
C2—S2—C1—N1176.95 (17)C15—C10—C11—C122.6 (3)
C2—C3—C4—C5177.4 (2)C16—N3—C13—C120.4 (3)
C2—C3—C8—C7177.4 (2)C16—N3—C13—C14179.4 (2)
C3—C4—C5—C60.5 (3)C16—N3—C18—C1997.4 (2)
C4—C3—C8—C71.1 (3)C18—N3—C13—C12177.3 (2)
C4—C5—C6—C70.1 (4)C18—N3—C13—C141.7 (3)
C5—C6—C7—C80.1 (3)C18—N3—C16—C1779.8 (2)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1A···O1i0.882.062.933 (3)175
O1—H1···S1ii0.842.363.1749 (19)163
Symmetry codes: (i) x+1, y, z+1; (ii) x1, y, z1.
 

Funding information

Funding for this research was provided by: National Natural Science Foundation of China (award No. 21871003; award No. 51672002).

References

First citationDolomanov, O. V., Bourhis, L. J., Gildea, R. J., Howard, J. A. K. & Puschmann, H. (2009). J. Appl. Cryst. 42, 339–341.  Web of Science CrossRef CAS IUCr Journals Google Scholar
First citationSheldrick, G. M. (2015a). Acta Cryst. A71, 3–8.  Web of Science CrossRef IUCr Journals Google Scholar
First citationSheldrick, G. M. (2015b). Acta Cryst. C71, 3–8.  Web of Science CrossRef IUCr Journals Google Scholar
First citationStoe (2018). X-AREA and X-RED32. Stoe & Cie, Darmstadt, Germany.  Google Scholar
First citationZhao, Q., Li, L., Li, F. Y., Yu, M. X., Liu, Z. P., Yi, T. & Huang, C. H. (2008). Chem. Commun. pp. 685–687.  Web of Science CSD CrossRef Google Scholar

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