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The title compound, C10H8BrNS, is used as a precursor to diarylethene derivatives. The dihedral angle between the thiophene and pyridine rings is 4.9 (1)°, and there is evidence for conjugation throughout the molecule. The structure is stabilized by π–π stacking interactions down the c axis.
Supporting information
CCDC reference: 274625
Key indicators
- Single-crystal X-ray study
- T = 295 K
- Mean
(C-C) = 0.007 Å
- R factor = 0.049
- wR factor = 0.098
- Data-to-parameter ratio = 14.9
checkCIF/PLATON results
No syntax errors found
Alert level C
PLAT341_ALERT_3_C Low Bond Precision on C-C bonds (x 1000) Ang ... 7
0 ALERT level A = In general: serious problem
0 ALERT level B = Potentially serious problem
1 ALERT level C = Check and explain
0 ALERT level G = General alerts; check
0 ALERT type 1 CIF construction/syntax error, inconsistent or missing data
0 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
Data collection: XSCANS (Bruker, 1997); cell refinement: XSCANS; data reduction: XSCANS; program(s) used to solve structure: SHELXTL (Bruker, 1997); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.
4-(4-bromo-5-methylthiophen-2-yl)pyridine
top
Crystal data top
C10H8BrNS | F(000) = 1008 |
Mr = 254.14 | Dx = 1.665 Mg m−3 |
Orthorhombic, Pbca | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -P 2ac 2ab | Cell parameters from 47 reflections |
a = 12.726 (4) Å | θ = 5.1–12.5° |
b = 11.629 (4) Å | µ = 4.21 mm−1 |
c = 13.705 (5) Å | T = 295 K |
V = 2028.3 (11) Å3 | Prism, yellow |
Z = 8 | 0.4 × 0.4 × 0.3 mm |
Data collection top
Bruker P4 diffractometer | 1028 reflections with I > 2σ(I) |
Radiation source: fine-focus sealed tube | Rint = 0.049 |
Graphite monochromator | θmax = 25.0°, θmin = 2.8° |
ω scans | h = −1→15 |
Absorption correction: multi-scan (North et al., 1968) | k = −1→13 |
Tmin = 0.217, Tmax = 0.283 | l = −16→1 |
2321 measured reflections | 3 standard reflections every 97 reflections |
1776 independent reflections | intensity decay: none |
Refinement top
Refinement on F2 | Primary atom site location: structure-invariant direct methods |
Least-squares matrix: full | Secondary atom site location: difference Fourier map |
R[F2 > 2σ(F2)] = 0.049 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.098 | H-atom parameters constrained |
S = 1.04 | w = 1/[σ2(Fo2) + (0.001P)2 + 3.5P] where P = (Fo2 + 2Fc2)/3 |
1776 reflections | (Δ/σ)max < 0.001 |
119 parameters | Δρmax = 0.26 e Å−3 |
0 restraints | Δρmin = −0.30 e Å−3 |
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 | x | y | z | Uiso*/Ueq | |
Br1 | 0.58285 (6) | 0.09948 (5) | 0.58074 (6) | 0.0932 (3) | |
S1 | 0.63015 (11) | 0.46445 (12) | 0.63320 (12) | 0.0639 (4) | |
N1 | 0.2656 (4) | 0.6984 (4) | 0.6460 (4) | 0.0766 (14) | |
C1 | 0.4972 (4) | 0.4335 (4) | 0.6283 (4) | 0.0549 (13) | |
C2 | 0.4827 (4) | 0.3181 (4) | 0.6130 (4) | 0.0587 (15) | |
H2A | 0.4172 | 0.2828 | 0.6088 | 0.070* | |
C3 | 0.5792 (4) | 0.2595 (4) | 0.6044 (4) | 0.0608 (14) | |
C4 | 0.6657 (4) | 0.3231 (4) | 0.6139 (4) | 0.0593 (15) | |
C5 | 0.7819 (4) | 0.2910 (5) | 0.6119 (5) | 0.0739 (18) | |
H5A | 0.8206 | 0.3497 | 0.5783 | 0.111* | |
H5B | 0.7906 | 0.2190 | 0.5787 | 0.111* | |
H5C | 0.8076 | 0.2842 | 0.6775 | 0.111* | |
C6 | 0.4189 (4) | 0.5242 (4) | 0.6365 (4) | 0.0539 (13) | |
C7 | 0.3132 (4) | 0.4983 (4) | 0.6342 (4) | 0.0660 (15) | |
H7A | 0.2904 | 0.4226 | 0.6292 | 0.079* | |
C8 | 0.2414 (5) | 0.5886 (5) | 0.6395 (5) | 0.0769 (17) | |
H8A | 0.1704 | 0.5696 | 0.6384 | 0.092* | |
C9 | 0.3682 (5) | 0.7210 (5) | 0.6495 (5) | 0.0752 (18) | |
H9A | 0.3887 | 0.7974 | 0.6557 | 0.090* | |
C10 | 0.4462 (4) | 0.6388 (4) | 0.6447 (4) | 0.0658 (16) | |
H10A | 0.5165 | 0.6604 | 0.6469 | 0.079* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
Br1 | 0.0957 (5) | 0.0556 (3) | 0.1283 (6) | 0.0089 (4) | 0.0006 (5) | −0.0164 (4) |
S1 | 0.0511 (7) | 0.0553 (8) | 0.0853 (11) | −0.0011 (7) | −0.0027 (8) | −0.0011 (8) |
N1 | 0.077 (4) | 0.069 (3) | 0.084 (4) | 0.018 (3) | 0.009 (3) | 0.005 (3) |
C1 | 0.049 (3) | 0.050 (3) | 0.066 (4) | 0.002 (2) | −0.001 (3) | 0.000 (3) |
C2 | 0.052 (3) | 0.059 (3) | 0.065 (4) | −0.005 (3) | 0.001 (3) | −0.004 (3) |
C3 | 0.063 (3) | 0.048 (3) | 0.071 (4) | 0.001 (3) | 0.001 (3) | −0.008 (3) |
C4 | 0.063 (3) | 0.050 (3) | 0.064 (4) | 0.007 (3) | 0.001 (3) | 0.005 (3) |
C5 | 0.058 (3) | 0.067 (4) | 0.097 (5) | 0.023 (3) | −0.001 (3) | 0.004 (3) |
C6 | 0.052 (3) | 0.056 (3) | 0.054 (3) | 0.003 (3) | −0.006 (3) | 0.000 (3) |
C7 | 0.059 (3) | 0.049 (3) | 0.090 (4) | 0.004 (3) | 0.004 (3) | 0.003 (3) |
C8 | 0.054 (3) | 0.080 (4) | 0.096 (5) | 0.006 (3) | 0.009 (3) | 0.009 (4) |
C9 | 0.081 (4) | 0.052 (3) | 0.092 (5) | 0.011 (3) | 0.002 (4) | −0.002 (3) |
C10 | 0.055 (3) | 0.060 (3) | 0.082 (4) | −0.003 (3) | 0.001 (3) | −0.004 (3) |
Geometric parameters (Å, º) top
Br1—C3 | 1.889 (5) | C5—H5A | 0.9600 |
S1—C4 | 1.726 (5) | C5—H5B | 0.9600 |
S1—C1 | 1.731 (5) | C5—H5C | 0.9600 |
N1—C8 | 1.317 (7) | C6—C7 | 1.379 (6) |
N1—C9 | 1.333 (7) | C6—C10 | 1.382 (7) |
C1—C2 | 1.371 (7) | C7—C8 | 1.393 (7) |
C1—C6 | 1.456 (6) | C7—H7A | 0.9300 |
C2—C3 | 1.410 (7) | C8—H8A | 0.9300 |
C2—H2A | 0.9300 | C9—C10 | 1.379 (7) |
C3—C4 | 1.332 (7) | C9—H9A | 0.9300 |
C4—C5 | 1.526 (7) | C10—H10A | 0.9300 |
| | | |
C4—S1—C1 | 93.0 (2) | H5A—C5—H5C | 109.5 |
C8—N1—C9 | 115.0 (5) | H5B—C5—H5C | 109.5 |
C2—C1—C6 | 128.9 (5) | C7—C6—C10 | 117.3 (5) |
C2—C1—S1 | 110.0 (4) | C7—C6—C1 | 120.5 (5) |
C6—C1—S1 | 121.0 (4) | C10—C6—C1 | 122.2 (5) |
C1—C2—C3 | 111.6 (5) | C6—C7—C8 | 118.3 (5) |
C1—C2—H2A | 124.2 | C6—C7—H7A | 120.9 |
C3—C2—H2A | 124.2 | C8—C7—H7A | 120.9 |
C4—C3—C2 | 116.3 (5) | N1—C8—C7 | 125.5 (5) |
C4—C3—Br1 | 122.9 (4) | N1—C8—H8A | 117.2 |
C2—C3—Br1 | 120.8 (4) | C7—C8—H8A | 117.2 |
C3—C4—C5 | 131.6 (5) | N1—C9—C10 | 124.5 (5) |
C3—C4—S1 | 109.1 (4) | N1—C9—H9A | 117.8 |
C5—C4—S1 | 119.3 (4) | C10—C9—H9A | 117.8 |
C4—C5—H5A | 109.5 | C9—C10—C6 | 119.4 (5) |
C4—C5—H5B | 109.5 | C9—C10—H10A | 120.3 |
H5A—C5—H5B | 109.5 | C6—C10—H10A | 120.3 |
C4—C5—H5C | 109.5 | | |

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