organic compounds
Experimental
Acta Crystallographica Section E
Structure Reports
Online
Crystal data
ISSN 1600-5368
2,5-Bis{[( )-(S)-1-(4-bromophenyl)ethyl]iminomethyl}thiophene
Angel Mendoza,a* Sylvain Bernès,b Guadalupe
Hernández-Téllez,c Oscar Portillo-Morenoc and René
Gutiérrezc
a
Centro de Quı́mica, Instituto de Ciencias, Benemérita Universidad Autónoma de
Puebla, 72570 Puebla, Puebla, Mexico, bDEP, Facultad de Ciencias Quı́micas,
UANL, Guerrero y Progreso S/N, Col. Treviño 64570 Monterrey, NL, Mexico, and
c
Laboratorio de Sı́ntesis de Complejos, Facultad de Ciencias Quı́micas, Benemérita
Universidad Autónoma de Puebla, PO Box 1067, 72001 Puebla, Puebla, Mexico
Correspondence e-mail: angel.mendoza@correo.buap.mx
Received 7 February 2014; accepted 18 February 2014
C22H20Br2N2S
Mr = 504.27
Monoclinic, C2
a = 24.5329 (15) Å
b = 5.9762 (5) Å
c = 7.5944 (5) Å
= 98.536 (6)
V = 1101.11 (14) Å3
Z=2
Mo K radiation
= 3.79 mm 1
T = 298 K
0.52 0.15 0.06 mm
Data collection
Agilent Xcalibur (Atlas, Gemini)
diffractometer
Absorption correction: numerical
(CrysAlis PRO; Agilent, 2013)
Tmin = 0.400, Tmax = 0.815
6101 measured reflections
2107 independent reflections
1630 reflections with I > 2(I)
Rint = 0.035
Refinement
R[F 2 > 2(F 2)] = 0.036
wR(F 2) = 0.072
S = 1.03
2107 reflections
124 parameters
1 restraint
H-atom parameters constrained
max = 0.20 e Å 3
min = 0.35 e Å 3
Absolute structure: Flack (1983),
914 Friedel pairs
Absolute structure parameter:
0.011 (8)
Key indicators: single-crystal X-ray study; T = 298 K; mean (C–C) = 0.007 Å;
R factor = 0.036; wR factor = 0.072; data-to-parameter ratio = 17.0.
The title compound, C22H20Br2N2S, was synthesized under
solvent-free conditions. The molecule shows crystallographic
C2 symmetry, with the S atom of the central thiophene ring
lying on a twofold rotation axis. Furthermore, as a consequence of the (S,S) stereochemistry, the molecule has a
twisted conformation. The dihedral angle between the thiophene and benzene rings is 72.7 (2) and that between the two
benzene rings is 55.9 (2) . In the crystal, molecules are
arranged in a chevron-like pattern, without any significant
intermolecular interactions.
Related literature
For the solvent-free organic synthesis, see: Tanaka & Toda
(2000). For the structure of a chiral bis-aldimine compound,
see: Espinosa Leija et al. (2009). For structures of thiophenes
substituted in positions 2 and 5 by imine functionalities, see:
Bernès et al. (2013); Kudyakova et al. (2012).
Acta Cryst. (2014). E70, o345
Data collection: CrysAlis PRO (Agilent, 2013); cell refinement:
CrysAlis PRO; data reduction: CrysAlis RED (Agilent, 2013);
program(s) used to solve structure: SHELXS2013 (Sheldrick, 2008);
program(s) used to refine structure: SHELXL2013 (Sheldrick, 2008);
molecular graphics: ORTEP-3 for Windows (Farrugia, 2012); software used to prepare material for publication: WinGX (Farrugia,
2012).
Support from VIEP-UAP (GUPJ-NAT12-G-2013) is
acknowledged.
Supporting information for this paper is available from the IUCr
electronic archives (Reference: IS5340).
References
Agilent (2013). CrysAlis PRO and CrysAlis RED. Agilent Technologies Inc.,
Santa Clara, CA, USA.
Bernès, S., Hernández-Téllez, G., Sharma, M., Portillo-Moreno, O. &
Gutiérrez, R. (2013). Acta Cryst. E69, o1428.
Espinosa Leija, A., Hernández, G., Cruz, S., Bernès, S. & Gutiérrez, R. (2009).
Acta Cryst. E65, o1316.
Farrugia, L. J. (2012). J. Appl. Cryst. 45, 849–854.
Flack, H. D. (1983). Acta Cryst. A39, 876–881.
Kudyakova, Y. S., Burgart, Y. V., Slepukhin, P. A. & Saloutin, V. I. (2012).
Mendeleev Commun. 22, 284–286.
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122.
Tanaka, K. & Toda, F. (2000). Chem. Rev. 100, 1025–1074.
doi:10.1107/S1600536814003651
Mendoza et al.
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Acta Cryst. (2014). E70, o345
[doi:10.1107/S1600536814003651]
2,5-Bis{[(−)-(S)-1-(4-bromophenyl)ethyl]iminomethyl}thiophene
Angel Mendoza, Sylvain Bernès, Guadalupe Hernández-Téllez, Oscar Portillo-Moreno and René
Gutiérrez
S1. Comment
In continuation of our work focused on chiral bisimines (Espinosa Leija et al., 2009; Bernès et al., 2013), we have now
synthesized the title compound under the solvent-free approach because of the cleaner, safer, and easier aspects to
perform in the synthetic work. So, solvent-free conditions are becoming more popular and it is often claimed that the best
solvent is no solvent. (Tanaka & Toda, 2000).
The bis-aldimine compound shows an E configuration over every imine bond (Fig. 1). The molecule is an (S,S)
diastereoisomer as expected by synthetic procedure. The asymmetric unit contains a half-molecule. The S atom of the
molecule is located on a twofold rotation axis of the space group C2. and as a consequence the Br-aldimines groups are
placed opposite to the central thiophene ring. Only some previous reports of 2,5-thiophene compounds with achiral or
chiral substituents have showed C2 crystallographic symmetry like title compound (Kudyakova et al., 2012, space group
C2/c; Bernès et al., 2013, space group P22121). The crystal packing does not feature any particular interactions (intra or
intermolecular) and the supramolecular arrangement in the solid state shows a chevron-like pattern viewed along the b
axis (Fig. 2).
S2. Experimental
Under solvent-free conditions, a mixture of 2,5-thiophenedicarboxaldehyde (100 mg, 0.71 mmol) and (S)-(–)-1-(4bromophenyl)ethylamine (285 mg, 1.42 mmol) in a 1:2 molar ratio were mixed at room temperature, giving a white solid.
The crude was recrystallized from CH2Cl2, affording colorless crystals of the title compound.
Yield 96%; m.p. 147–149 °C. Spectroscopic data: [a]D25 = +59.6 (c 1, CHCl3). IR (KBr): 1623 cm-1 (C=N). 1H NMR
(400 MHz, CDCl3/TMS): δ = 1.51, 1.53 (d, 6H, CHCH3,), 4.44, 4.45, 4.47, 4.49(q, 2H, CH), 7.29–7.45 (m, 10 H, Ar),
8.36 (s, 2 H, HC=N). 13C NMR (100 MHz, CDCl3/TMS) δ = 25.1 (CCH3), 68.7 (CHCH3), 120.6 (Ar), 128.3 (Ar), 130.1
(Ar), 131.4 (Ar), 144.0 (Ar), 145.1 (Ar), 152. 7 (HC=N). MS—EI: m/z= 504 (M+).
S3. Refinement
The absolute configuration was determined using the anomalous dispersion of the Br atom, and was that expected from
the synthesis, carried-out with an enantiomerically pure amine. All H atoms were placed in calculated positions, with C—
H bond lengths fixed to 0.96 Å for the methyl group and 0.93 Å for aromatic CH groups. Isotropic displacement
parameters were calculated as Uiso(H) = 1.5Ueq(carrier atom) for the methyl group and Uiso(H) = 1.2Ueq(carrier atom)
otherwise.
Acta Cryst. (2014). E70, o345
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Figure 1
The molecular structure of title compound, with atom labels and 30% probability displacement ellipsoids for non-H
atoms.
Figure 2
A packing diagram of the title compound, viewed along the b axis.
2,5-Bis{[(–)-(S)-1-(4-bromophenyl)ethyl]iminomethyl}thiophene
Crystal data
C22H20Br2N2S
Mr = 504.27
Monoclinic, C2
Hall symbol: C 2y
a = 24.5329 (15) Å
b = 5.9762 (5) Å
c = 7.5944 (5) Å
β = 98.536 (6)°
V = 1101.11 (14) Å3
Z=2
F(000) = 504
Dx = 1.521 Mg m−3
Melting point: 420 K
Mo Kα radiation, λ = 0.71073 Å
Cell parameters from 1609 reflections
θ = 4.4–25.2°
µ = 3.79 mm−1
T = 298 K
Prism, colourless
0.52 × 0.15 × 0.06 mm
Data collection
Agilent Xcalibur (Atlas, Gemini)
diffractometer
Radiation source: Enhance (Mo) X-ray Source
Graphite monochromator
Detector resolution: 10.5564 pixels mm-1
ω scans
Absorption correction: numerical
(CrysAlis PRO; Agilent, 2013)
Tmin = 0.400, Tmax = 0.815
Acta Cryst. (2014). E70, o345
6101 measured reflections
2107 independent reflections
1630 reflections with I > 2σ(I)
Rint = 0.035
θmax = 26.1°, θmin = 3.0°
h = −30→30
k = −7→7
l = −9→9
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Refinement
Refinement on F2
Least-squares matrix: full
R[F2 > 2σ(F2)] = 0.036
wR(F2) = 0.072
S = 1.03
2107 reflections
124 parameters
1 restraint
0 constraints
Hydrogen site location: inferred from
neighbouring sites
H-atom parameters constrained
w = 1/[σ2(Fo2) + (0.0288P)2 + 0.0296P]
where P = (Fo2 + 2Fc2)/3
(Δ/σ)max < 0.001
Δρmax = 0.20 e Å−3
Δρmin = −0.35 e Å−3
Absolute structure: Flack (1983), 914 Friedel
pairs
Absolute structure parameter: 0.011 (8)
Special details
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.
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)
Br1
S1
C9
C11
H11A
H11B
H11C
C4
C1
C6
H6
N1
C5
H5
C2
H2
C3
H3
C7
H7
C8
H8
C10
H10
x
y
z
Uiso*/Ueq
0.15628 (2)
0.5
0.47486 (16)
0.4216 (2)
0.4194
0.4595
0.4013
0.2306 (2)
0.33894 (18)
0.3243 (2)
0.3514
0.43094 (15)
0.2703 (2)
0.2613
0.2971 (2)
0.3056
0.2431 (2)
0.2157
0.3974 (2)
0.398
0.44434 (18)
0.4339
0.4853 (2)
0.4743
0.49000 (18)
0.2196 (2)
0.0181 (7)
0.4840 (10)
0.6248
0.4499
0.4929
0.4327 (11)
0.3489 (7)
0.5418 (9)
0.6457
0.2748 (6)
0.5823 (9)
0.711
0.1997 (9)
0.0688
0.2389 (11)
0.135
0.3024 (8)
0.1616
0.0769 (7)
−0.038
−0.1907 (8)
−0.3205
0.61658 (7)
0.5
0.6292 (5)
1.0744 (5)
1.0129
1.1175
1.173
0.7169 (6)
0.8651 (5)
0.7670 (6)
0.7513
0.8052 (5)
0.6921 (7)
0.6253
0.8837 (6)
0.9482
0.8092 (7)
0.8218
0.9485 (5)
1.0149
0.7709 (6)
0.8414
0.5728 (7)
0.625
0.1112 (4)
0.0472 (4)
0.0427 (10)
0.0657 (13)
0.099*
0.099*
0.099*
0.0639 (15)
0.0441 (11)
0.0569 (13)
0.068*
0.0452 (9)
0.0674 (16)
0.081*
0.0603 (13)
0.072*
0.0690 (14)
0.083*
0.0501 (12)
0.06*
0.0469 (12)
0.056*
0.0540 (13)
0.065*
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Atomic displacement parameters (Å2)
Br1
S1
C9
C11
C4
C1
C6
N1
C5
C2
C3
C7
C8
C10
U11
U22
U33
U12
U13
U23
0.0529 (4)
0.0553 (11)
0.043 (2)
0.058 (3)
0.044 (3)
0.044 (3)
0.052 (3)
0.042 (2)
0.063 (4)
0.064 (4)
0.051 (3)
0.051 (3)
0.039 (3)
0.057 (3)
0.2036 (8)
0.0347 (8)
0.038 (2)
0.085 (3)
0.106 (5)
0.053 (3)
0.062 (3)
0.052 (2)
0.084 (4)
0.067 (3)
0.094 (4)
0.060 (3)
0.051 (3)
0.035 (2)
0.0729 (4)
0.0547 (10)
0.047 (2)
0.053 (2)
0.042 (2)
0.037 (2)
0.056 (3)
0.0439 (19)
0.053 (3)
0.053 (3)
0.065 (3)
0.043 (2)
0.051 (3)
0.073 (3)
0.0279 (5)
0
0.001 (2)
0.009 (3)
0.005 (3)
0.001 (2)
−0.002 (3)
0.0014 (17)
0.010 (3)
−0.002 (3)
−0.019 (3)
0.006 (2)
0.000 (2)
−0.001 (2)
−0.0044 (3)
0.0179 (8)
0.0052 (18)
0.005 (2)
0.006 (2)
0.012 (2)
0.007 (2)
0.0134 (17)
0.003 (3)
0.017 (2)
0.017 (3)
0.017 (2)
0.008 (2)
0.017 (3)
−0.0229 (5)
0
0.005 (2)
−0.003 (3)
−0.009 (3)
0.002 (2)
0.016 (3)
0.0053 (16)
0.014 (3)
0.011 (3)
−0.005 (3)
0.011 (2)
0.013 (2)
0.005 (2)
Geometric parameters (Å, º)
Br1—C4
S1—C9i
S1—C9
C9—C8
C9—C10
C11—H11A
C11—H11B
C11—H11C
C11—C7
C4—C5
C4—C3
C1—C6
C1—C2
1.899 (5)
1.724 (4)
1.724 (4)
1.442 (6)
1.356 (6)
0.96
0.96
0.96
1.509 (7)
1.356 (7)
1.365 (7)
1.391 (6)
1.383 (7)
C1—C7
C6—H6
C6—C5
N1—C7
N1—C8
C5—H5
C2—H2
C2—C3
C3—H3
C7—H7
C8—H8
C10—C10i
C10—H10
1.505 (6)
0.93
1.383 (7)
1.468 (5)
1.265 (5)
0.93
0.93
1.382 (7)
0.93
0.98
0.93
1.405 (10)
0.93
C9—S1—C9i
C8—C9—S1
C10—C9—S1
C10—C9—C8
H11A—C11—H11B
H11A—C11—H11C
H11B—C11—H11C
C7—C11—H11A
C7—C11—H11B
C7—C11—H11C
C5—C4—Br1
C5—C4—C3
C3—C4—Br1
C6—C1—C7
91.4 (3)
121.6 (3)
111.2 (3)
127.1 (4)
109.5
109.5
109.5
109.5
109.5
109.5
119.5 (4)
121.3 (5)
119.2 (4)
122.2 (4)
C4—C5—H5
C6—C5—H5
C1—C2—H2
C3—C2—C1
C3—C2—H2
C4—C3—C2
C4—C3—H3
C2—C3—H3
C11—C7—H7
C1—C7—C11
C1—C7—H7
N1—C7—C11
N1—C7—C1
N1—C7—H7
120.3
120.3
119
122.0 (5)
119
118.9 (5)
120.6
120.6
108.5
113.2 (4)
108.5
109.9 (4)
108.2 (3)
108.5
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C2—C1—C6
C2—C1—C7
C1—C6—H6
C5—C6—C1
C5—C6—H6
C8—N1—C7
C4—C5—C6
116.9 (4)
120.9 (4)
119.3
121.3 (5)
119.3
116.7 (3)
119.5 (5)
C9—C8—H8
N1—C8—C9
N1—C8—H8
C9—C10—C10i
C9—C10—H10
C10i—C10—H10
117.9
124.1 (4)
117.9
113.1 (3)
123.5
123.5
Br1—C4—C5—C6
Br1—C4—C3—C2
S1—C9—C8—N1
S1—C9—C10—C10i
C9i—S1—C9—C8
C9i—S1—C9—C10
C1—C6—C5—C4
C1—C2—C3—C4
C6—C1—C2—C3
C6—C1—C7—C11
C6—C1—C7—N1
C5—C4—C3—C2
179.2 (4)
−179.2 (4)
4.2 (6)
1.2 (7)
−177.3 (4)
−0.4 (3)
1.0 (7)
−1.0 (7)
−0.2 (7)
57.3 (5)
−64.8 (5)
2.3 (7)
C2—C1—C6—C5
C2—C1—C7—C11
C2—C1—C7—N1
C3—C4—C5—C6
C7—C1—C6—C5
C7—C1—C2—C3
C7—N1—C8—C9
C8—C9—C10—C10i
C8—N1—C7—C11
C8—N1—C7—C1
C10—C9—C8—N1
0.2 (7)
−122.6 (5)
115.3 (4)
−2.3 (8)
−179.6 (4)
179.7 (4)
176.9 (4)
177.9 (5)
131.9 (4)
−104.0 (4)
−172.2 (5)
Symmetry code: (i) −x+1, y, −z+1.
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