Literature DB >> 21589065

N,N'-Bis[(E)-(3-methyl-2-thienyl)methyl-idene]ethane-1,2-diamine.

R Prasath, P Bhavana, Seik Weng Ng, Edward R T Tiekink.   

Abstract

Two independent half-mol-ecules, each being completed by inversion symmetry, comprise the asymmetric unit of the title compound, C(14)H(16)N(2)S(2). The major difference between the mol-ecules is found in the central C-C bond [the C-N-C-C torsion angles are 114.66 (18) and 128.94 (18)° in the two mol-ecules]. The thio-phene and imine groups are almost co-planar in each case [S-C-C-N torsion angles = -6.9 (2) and -3.6 (2)°]. In the crystal, the mol-ecules aggregate into supra-molecular chains via C-H⋯π inter-actions.

Entities:  

Year:  2010        PMID: 21589065      PMCID: PMC3009173          DOI: 10.1107/S1600536810041632

Source DB:  PubMed          Journal:  Acta Crystallogr Sect E Struct Rep Online        ISSN: 1600-5368


Related literature

For background to 2-substituted thio­phenes, see: Campaigne (1984 ▶); Kleemann et al. (2006 ▶). For related structures, see: Wang et al. (2007 ▶); Wardell et al. (2010 ▶).

Experimental

Crystal data

C14H16N2S2 M = 276.41 Triclinic, a = 8.7610 (6) Å b = 8.9502 (6) Å c = 8.9853 (6) Å α = 92.760 (1)° β = 91.653 (1)° γ = 106.066 (1)° V = 675.61 (8) Å3 Z = 2 Mo Kα radiation μ = 0.38 mm−1 T = 100 K 0.30 × 0.30 × 0.10 mm

Data collection

Bruker SMART APEX diffractometer Absorption correction: multi-scan (SADABS; Sheldrick, 1996 ▶) T min = 0.797, T max = 0.862 6435 measured reflections 3089 independent reflections 2822 reflections with I > 2σ(I) R int = 0.019

Refinement

R[F 2 > 2σ(F 2)] = 0.031 wR(F 2) = 0.100 S = 1.10 3089 reflections 165 parameters H-atom parameters constrained Δρmax = 0.45 e Å−3 Δρmin = −0.27 e Å−3 Data collection: APEX2 (Bruker, 2008 ▶); cell refinement: SAINT (Bruker, 2008 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: ORTEP-3 (Farrugia, 1997 ▶) and DIAMOND (Brandenburg, 2006 ▶); software used to prepare material for publication: publCIF (Westrip, 2010 ▶). Crystal structure: contains datablocks general, I. DOI: 10.1107/S1600536810041632/pk2279sup1.cif Structure factors: contains datablocks I. DOI: 10.1107/S1600536810041632/pk2279Isup2.hkl Additional supplementary materials: crystallographic information; 3D view; checkCIF report
C14H16N2S2Z = 2
Mr = 276.41F(000) = 292
Triclinic, P1Dx = 1.359 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 8.7610 (6) ÅCell parameters from 4410 reflections
b = 8.9502 (6) Åθ = 4.3–28.3°
c = 8.9853 (6) ŵ = 0.38 mm1
α = 92.760 (1)°T = 100 K
β = 91.653 (1)°Prism, colourless
γ = 106.066 (1)°0.30 × 0.30 × 0.10 mm
V = 675.61 (8) Å3
Bruker SMART APEX diffractometer3089 independent reflections
Radiation source: fine-focus sealed tube2822 reflections with I > 2σ(I)
graphiteRint = 0.019
ω scansθmax = 27.5°, θmin = 2.3°
Absorption correction: multi-scan (SADABS; Sheldrick, 1996)h = −11→11
Tmin = 0.797, Tmax = 0.862k = −11→10
6435 measured reflectionsl = −11→11
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.031Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.100H-atom parameters constrained
S = 1.10w = 1/[σ2(Fo2) + (0.0508P)2 + 0.4238P] where P = (Fo2 + 2Fc2)/3
3089 reflections(Δ/σ)max < 0.001
165 parametersΔρmax = 0.45 e Å3
0 restraintsΔρmin = −0.27 e Å3
Geometry. All s.u.'s (except the s.u. in the dihedral angle between two l.s. planes) are estimated using the full covariance matrix. The cell s.u.'s are taken into account individually in the estimation of s.u.'s in distances, angles and torsion angles; correlations between s.u.'s in cell parameters are only used when they are defined by crystal symmetry. An approximate (isotropic) treatment of cell s.u.'s is used for estimating s.u.'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 > 2σ(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.
xyzUiso*/Ueq
S10.47805 (4)0.72178 (4)0.45069 (4)0.01583 (12)
N10.48699 (16)0.93243 (16)0.19349 (14)0.0171 (3)
C10.47949 (19)1.03494 (19)0.07326 (17)0.0170 (3)
H1A0.55541.13870.09680.020*
H1B0.37121.04830.06370.020*
C20.59455 (18)0.98652 (18)0.29593 (17)0.0151 (3)
H20.66411.08810.28900.018*
C30.61453 (18)0.89825 (18)0.42300 (17)0.0147 (3)
C40.73245 (18)0.93799 (18)0.53428 (17)0.0157 (3)
C50.7128 (2)0.82044 (19)0.63988 (17)0.0174 (3)
H50.78440.82640.72280.021*
C60.5808 (2)0.69924 (19)0.60906 (17)0.0180 (3)
H60.54930.61200.66860.022*
C70.8608 (2)1.0898 (2)0.5493 (2)0.0223 (3)
H7A0.82131.16820.60350.033*
H7B0.89131.12470.45000.033*
H7C0.95351.07560.60430.033*
S20.08033 (5)0.56857 (5)0.69562 (4)0.01757 (12)
N20.01928 (16)0.80946 (15)0.92178 (15)0.0166 (3)
C8−0.0229 (2)0.91842 (18)1.02823 (18)0.0179 (3)
H8A0.03280.91891.12570.021*
H8B−0.13880.88461.04270.021*
C90.09982 (18)0.72358 (18)0.97335 (17)0.0151 (3)
H90.13200.73691.07610.018*
C100.14457 (18)0.60595 (17)0.88127 (17)0.0138 (3)
C110.23606 (18)0.51136 (18)0.92386 (17)0.0147 (3)
C120.25375 (19)0.40900 (18)0.80306 (18)0.0177 (3)
H120.31340.33560.81160.021*
C130.1767 (2)0.42700 (19)0.67441 (19)0.0196 (3)
H130.17640.36800.58360.023*
C140.30760 (19)0.5131 (2)1.07776 (18)0.0191 (3)
H14A0.36630.62001.11080.029*
H14B0.38030.44731.07660.029*
H14C0.22290.47311.14640.029*
U11U22U33U12U13U23
S10.0184 (2)0.01340 (19)0.0147 (2)0.00282 (14)0.00089 (14)0.00138 (14)
N10.0216 (7)0.0169 (6)0.0123 (6)0.0044 (5)0.0017 (5)0.0028 (5)
C10.0196 (7)0.0176 (7)0.0136 (7)0.0046 (6)0.0003 (6)0.0034 (6)
C20.0176 (7)0.0133 (7)0.0152 (7)0.0054 (6)0.0039 (6)0.0008 (5)
C30.0172 (7)0.0130 (7)0.0142 (7)0.0045 (6)0.0029 (6)0.0009 (5)
C40.0185 (7)0.0146 (7)0.0149 (7)0.0061 (6)0.0014 (6)0.0001 (6)
C50.0229 (8)0.0178 (7)0.0133 (7)0.0090 (6)−0.0003 (6)0.0006 (6)
C60.0250 (8)0.0171 (7)0.0140 (7)0.0087 (6)0.0034 (6)0.0031 (6)
C70.0213 (8)0.0178 (8)0.0256 (8)0.0024 (6)−0.0047 (6)0.0022 (6)
S20.0210 (2)0.0169 (2)0.0142 (2)0.00442 (15)−0.00034 (14)0.00084 (14)
N20.0193 (6)0.0113 (6)0.0188 (6)0.0040 (5)−0.0001 (5)−0.0004 (5)
C80.0230 (8)0.0132 (8)0.0187 (7)0.0068 (6)0.0021 (6)0.0007 (6)
C90.0148 (7)0.0129 (7)0.0159 (7)0.0010 (5)0.0007 (5)0.0015 (6)
C100.0148 (7)0.0115 (7)0.0144 (7)0.0022 (5)0.0018 (5)0.0012 (5)
C110.0134 (7)0.0138 (7)0.0160 (7)0.0017 (5)0.0032 (5)0.0024 (6)
C120.0163 (7)0.0141 (7)0.0225 (8)0.0034 (6)0.0059 (6)0.0011 (6)
C130.0214 (8)0.0158 (7)0.0199 (8)0.0026 (6)0.0061 (6)−0.0026 (6)
C140.0171 (7)0.0228 (8)0.0186 (8)0.0069 (6)−0.0005 (6)0.0034 (6)
S1—C61.7119 (16)S2—C131.7125 (17)
S1—C31.7309 (16)S2—C101.7318 (16)
N1—C21.274 (2)N2—C91.272 (2)
N1—C11.4621 (19)N2—C81.460 (2)
C1—C1i1.525 (3)C8—C8ii1.520 (3)
C1—H1A0.9900C8—H8A0.9900
C1—H1B0.9900C8—H8B0.9900
C2—C31.453 (2)C9—C101.453 (2)
C2—H20.9500C9—H90.9500
C3—C41.377 (2)C10—C111.377 (2)
C4—C51.429 (2)C11—C121.426 (2)
C4—C71.502 (2)C11—C141.499 (2)
C5—C61.360 (2)C12—C131.361 (2)
C5—H50.9500C12—H120.9500
C6—H60.9500C13—H130.9500
C7—H7A0.9800C14—H14A0.9800
C7—H7B0.9800C14—H14B0.9800
C7—H7C0.9800C14—H14C0.9800
C6—S1—C391.47 (8)C13—S2—C1091.55 (8)
C2—N1—C1116.35 (13)C9—N2—C8116.78 (14)
N1—C1—C1i109.83 (16)N2—C8—C8ii110.34 (17)
N1—C1—H1A109.7N2—C8—H8A109.6
C1i—C1—H1A109.7C8ii—C8—H8A109.6
N1—C1—H1B109.7N2—C8—H8B109.6
C1i—C1—H1B109.7C8ii—C8—H8B109.6
H1A—C1—H1B108.2H8A—C8—H8B108.1
N1—C2—C3122.28 (14)N2—C9—C10122.61 (14)
N1—C2—H2118.9N2—C9—H9118.7
C3—C2—H2118.9C10—C9—H9118.7
C4—C3—C2127.93 (14)C11—C10—C9127.42 (14)
C4—C3—S1111.67 (12)C11—C10—S2111.68 (12)
C2—C3—S1120.39 (12)C9—C10—S2120.89 (11)
C3—C4—C5111.63 (14)C10—C11—C12111.52 (14)
C3—C4—C7124.67 (14)C10—C11—C14124.84 (14)
C5—C4—C7123.60 (14)C12—C11—C14123.64 (14)
C6—C5—C4112.87 (14)C13—C12—C11113.24 (14)
C6—C5—H5123.6C13—C12—H12123.4
C4—C5—H5123.6C11—C12—H12123.4
C5—C6—S1112.33 (12)C12—C13—S2112.00 (12)
C5—C6—H6123.8C12—C13—H13124.0
S1—C6—H6123.8S2—C13—H13124.0
C4—C7—H7A109.5C11—C14—H14A109.5
C4—C7—H7B109.5C11—C14—H14B109.5
H7A—C7—H7B109.5H14A—C14—H14B109.5
C4—C7—H7C109.5C11—C14—H14C109.5
H7A—C7—H7C109.5H14A—C14—H14C109.5
H7B—C7—H7C109.5H14B—C14—H14C109.5
C2—N1—C1—C1i114.66 (18)C9—N2—C8—C8ii128.94 (18)
C1—N1—C2—C3179.26 (14)C8—N2—C9—C10177.52 (14)
N1—C2—C3—C4174.57 (16)N2—C9—C10—C11177.29 (16)
N1—C2—C3—S1−6.9 (2)N2—C9—C10—S2−3.6 (2)
C6—S1—C3—C4−1.13 (13)C13—S2—C10—C11−0.31 (12)
C6—S1—C3—C2−179.90 (13)C13—S2—C10—C9−179.53 (13)
C2—C3—C4—C5−179.55 (15)C9—C10—C11—C12179.52 (15)
S1—C3—C4—C51.80 (17)S2—C10—C11—C120.36 (17)
C2—C3—C4—C73.9 (3)C9—C10—C11—C140.1 (3)
S1—C3—C4—C7−174.74 (13)S2—C10—C11—C14−179.05 (12)
C3—C4—C5—C6−1.7 (2)C10—C11—C12—C13−0.2 (2)
C7—C4—C5—C6174.86 (15)C14—C11—C12—C13179.18 (14)
C4—C5—C6—S10.86 (18)C11—C12—C13—S20.01 (18)
C3—S1—C6—C50.14 (13)C10—S2—C13—C120.17 (13)
Cg1 is the centroid of the S1,C3–C6 ring.
D—H···AD—HH···AD···AD—H···A
C13—H13···Cg1iii0.952.893.6179 (19)134
Table 1

Hydrogen-bond geometry (Å, °)

Cg1 is the centroid of the S1,C3–C6 ring.

D—H⋯AD—HH⋯ADAD—H⋯A
C13—H13⋯Cg1i0.952.893.6179 (19)134

Symmetry code: (i) .

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