organic compounds
1,2,4,5-Tetrafluoro-3,6-diiodobenzene–4-(pyridin-4-ylsulfanyl)pyridine (1/1)
aDepartment of Chemistry, The University of Texas at San Antonio, One UTSA Circle, San Antonio, Texas 78249-0698, USA, and bDepartment of Chemistry, University of Malaya, 50603 Kuala Lumpur, Malaysia
*Correspondence e-mail: edward.tiekink@gmail.com
The 10H8N2S·C6F4I2, comprises a half-molecule of 1,2,4,5-tetrafluoro-3,6-diiodobenzene, and half a 4-(pyridin-4-ylsulfanyl)pyridine molecule. The former is completed by crystallographic inversion symmetry, the latter by twofold symmetry, with the S atom lying on the rotation axis. The almost planar 1,2,4,5-tetrafluoro-3,6-diiodobenzene molecule (r.m.s. deviation of all 12 atoms = 0.016 Å) and twisted 4-(pyridin-4-ylsulfanyl)pyridine molecule [dihedral angle between pyridyl rings = 54.88 (13)°] are connected by N⋯I interactions [2.838 (4) Å], generating a supramolecular chain with a step-ladder topology. These chains are connected in the crystal by C—H⋯F and C—H⋯π(pyridyl) interactions.
of the title 1:1 adduct, CRelated literature
For related studies on et al. (2008); Arman et al. (2010). For background to halogen bonding, see: Metrangolo et al. (2008); Pennington et al. (2008). For the of 4-(pyridin-4-yldisulfanyl)pyridine, see: Aragoni et al. (2007).
formation, see: BrokerExperimental
Crystal data
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Refinement
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Data collection: CrystalClear (Molecular Structure Corporation & Rigaku, 2005); cell CrystalClear; data reduction: CrystalClear; 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).
Supporting information
10.1107/S1600536810038316/hb5647sup1.cif
contains datablocks global, I. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536810038316/hb5647Isup2.hkl
Initially 1,2,4,5-tetrafluoro-3,6-diiodobenzene (Aldrich, 0.04 mmol) and 4-(pyridin-4-yldisulfanyl)pyridine (Aldrich, 0.04 mmol) were dissolved in a THF/acetone (1/1) mixture and after evaporation of the solvent, the powder was then dissolved in ethanol. Again, crystals did not form so the powder was dissolved in a CHCl3/acetone (1/1) mixture. Slow evaporation of this solution deposited yellow blocks of (I) which, after crystallographic characterization, was proven to contain 4-(pyridin-4-ylsulfanyl)pyridine, indicating that ═N; 2924 (s) C—H.
of 4-(pyridin-4-yldisulfanyl)pyridine had occurred (Aragoni et al., 2007). M. pt:. 423–427 K. IR assignment (cm-1): 757 (m, sh); 807 (s, sh); 939 (s, sh); 1065 (s, sh); 1208 (m, sh) (C—F); 1408 (m, sh), 1456 (s, sh) C—C (aromatic); 1570 (s, sh) CC-bound H-atoms were placed in calculated positions (C–H 0.95 Å) and were included in the
in the riding model approximation with Uiso(H) set to 1.2Ueq(C). The maximum and minimum residual electron density peaks of 1.34 and 0.63 e Å-3, respectively, were located 1.06 Å and 0.88 Å from the S1 and I1 atoms, respectively.Data collection: CrystalClear (Molecular Structure Corporation & Rigaku, 2005); cell
CrystalClear (Molecular Structure Corporation & Rigaku, 2005); data reduction: CrystalClear (Molecular Structure Corporation & Rigaku, 2005); 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).C10H8N2S·C6F4I2 | F(000) = 1104 |
Mr = 590.10 | Dx = 2.219 Mg m−3 |
Monoclinic, C2/c | Mo Kα radiation, λ = 0.71073 Å |
Hall symbol: -C 2yc | Cell parameters from 3043 reflections |
a = 13.804 (5) Å | θ = 3.0–40.2° |
b = 5.829 (2) Å | µ = 3.72 mm−1 |
c = 22.164 (8) Å | T = 98 K |
β = 97.989 (7)° | Block, yellow |
V = 1766.1 (11) Å3 | 0.30 × 0.20 × 0.05 mm |
Z = 4 |
Rigaku AFC12K/SATURN724 diffractometer | 1823 independent reflections |
Radiation source: fine-focus sealed tube | 1733 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.027 |
ω scans | θmax = 26.5°, θmin = 3.0° |
Absorption correction: multi-scan (ABSCOR; Higashi, 1995) | h = −17→14 |
Tmin = 0.757, Tmax = 1.000 | k = −5→7 |
5209 measured reflections | l = −27→26 |
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)] = 0.034 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.073 | H-atom parameters constrained |
S = 1.07 | w = 1/[σ2(Fo2) + (0.0202P)2 + 21.2619P] where P = (Fo2 + 2Fc2)/3 |
1823 reflections | (Δ/σ)max = 0.001 |
114 parameters | Δρmax = 1.34 e Å−3 |
0 restraints | Δρmin = −0.63 e Å−3 |
C10H8N2S·C6F4I2 | V = 1766.1 (11) Å3 |
Mr = 590.10 | Z = 4 |
Monoclinic, C2/c | Mo Kα radiation |
a = 13.804 (5) Å | µ = 3.72 mm−1 |
b = 5.829 (2) Å | T = 98 K |
c = 22.164 (8) Å | 0.30 × 0.20 × 0.05 mm |
β = 97.989 (7)° |
Rigaku AFC12K/SATURN724 diffractometer | 1823 independent reflections |
Absorption correction: multi-scan (ABSCOR; Higashi, 1995) | 1733 reflections with I > 2σ(I) |
Tmin = 0.757, Tmax = 1.000 | Rint = 0.027 |
5209 measured reflections |
R[F2 > 2σ(F2)] = 0.034 | 0 restraints |
wR(F2) = 0.073 | H-atom parameters constrained |
S = 1.07 | w = 1/[σ2(Fo2) + (0.0202P)2 + 21.2619P] where P = (Fo2 + 2Fc2)/3 |
1823 reflections | Δρmax = 1.34 e Å−3 |
114 parameters | Δρmin = −0.63 e Å−3 |
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. |
x | y | z | Uiso*/Ueq | ||
I1 | 0.33988 (2) | 0.75767 (5) | 0.089898 (12) | 0.02060 (11) | |
F1 | 0.4107 (2) | 0.9003 (5) | −0.03751 (12) | 0.0253 (6) | |
F2 | 0.5292 (2) | 0.6993 (5) | −0.10663 (12) | 0.0257 (6) | |
C1 | 0.4356 (3) | 0.6036 (8) | 0.0360 (2) | 0.0186 (9) | |
C2 | 0.4540 (3) | 0.6999 (7) | −0.0181 (2) | 0.0180 (9) | |
C3 | 0.5168 (3) | 0.5980 (8) | −0.0534 (2) | 0.0205 (9) | |
S1 | 0.0000 | 0.4266 (3) | 0.2500 | 0.0201 (3) | |
N1 | 0.2103 (3) | −0.0202 (7) | 0.15987 (18) | 0.0248 (9) | |
C4 | 0.1787 (3) | 0.1842 (9) | 0.1379 (2) | 0.0239 (10) | |
H4 | 0.2032 | 0.2404 | 0.1028 | 0.029* | |
C5 | 0.1121 (3) | 0.3192 (8) | 0.1635 (2) | 0.0215 (9) | |
H5 | 0.0905 | 0.4616 | 0.1455 | 0.026* | |
C6 | 0.0779 (3) | 0.2417 (8) | 0.2158 (2) | 0.0191 (9) | |
C7 | 0.1112 (3) | 0.0326 (8) | 0.2401 (2) | 0.0193 (9) | |
H7 | 0.0900 | −0.0242 | 0.2763 | 0.023* | |
C8 | 0.1762 (3) | −0.0926 (8) | 0.2104 (2) | 0.0203 (9) | |
H8 | 0.1977 | −0.2373 | 0.2268 | 0.024* |
U11 | U22 | U33 | U12 | U13 | U23 | |
I1 | 0.01922 (17) | 0.02358 (17) | 0.01968 (17) | 0.00034 (12) | 0.00505 (11) | −0.00148 (11) |
F1 | 0.0271 (15) | 0.0212 (14) | 0.0285 (15) | 0.0061 (12) | 0.0072 (12) | 0.0045 (11) |
F2 | 0.0288 (16) | 0.0283 (14) | 0.0218 (14) | 0.0026 (12) | 0.0099 (11) | 0.0084 (11) |
C1 | 0.013 (2) | 0.023 (2) | 0.020 (2) | −0.0024 (17) | 0.0021 (16) | −0.0062 (17) |
C2 | 0.015 (2) | 0.017 (2) | 0.021 (2) | −0.0005 (17) | −0.0009 (16) | 0.0016 (16) |
C3 | 0.021 (2) | 0.023 (2) | 0.018 (2) | −0.0036 (19) | 0.0029 (17) | 0.0006 (17) |
S1 | 0.0203 (8) | 0.0166 (7) | 0.0245 (8) | 0.000 | 0.0068 (6) | 0.000 |
N1 | 0.020 (2) | 0.026 (2) | 0.028 (2) | 0.0012 (17) | 0.0057 (16) | −0.0018 (17) |
C4 | 0.017 (2) | 0.031 (3) | 0.023 (2) | −0.0047 (19) | 0.0040 (18) | 0.0002 (19) |
C5 | 0.022 (2) | 0.020 (2) | 0.022 (2) | −0.0007 (18) | 0.0005 (18) | 0.0007 (17) |
C6 | 0.015 (2) | 0.020 (2) | 0.023 (2) | −0.0012 (17) | 0.0041 (17) | −0.0043 (17) |
C7 | 0.014 (2) | 0.019 (2) | 0.024 (2) | −0.0025 (17) | 0.0003 (17) | −0.0017 (17) |
C8 | 0.016 (2) | 0.018 (2) | 0.026 (2) | −0.0010 (17) | −0.0013 (17) | −0.0009 (17) |
I1—C1 | 2.101 (4) | N1—C4 | 1.337 (6) |
F1—C2 | 1.355 (5) | C4—C5 | 1.389 (7) |
F2—C3 | 1.352 (5) | C4—H4 | 0.9500 |
C1—C2 | 1.379 (6) | C5—C6 | 1.387 (6) |
C1—C3i | 1.375 (6) | C5—H5 | 0.9500 |
C2—C3 | 1.381 (6) | C6—C7 | 1.385 (6) |
C3—C1i | 1.375 (6) | C7—C8 | 1.392 (6) |
S1—C6ii | 1.766 (4) | C7—H7 | 0.9500 |
S1—C6 | 1.766 (4) | C8—H8 | 0.9500 |
N1—C8 | 1.342 (6) | ||
C2—C1—C3i | 116.9 (4) | C5—C4—H4 | 118.0 |
C2—C1—I1 | 121.8 (3) | C6—C5—C4 | 118.5 (4) |
C3i—C1—I1 | 121.3 (3) | C6—C5—H5 | 120.7 |
C1—C2—F1 | 120.0 (4) | C4—C5—H5 | 120.7 |
C1—C2—C3 | 121.6 (4) | C7—C6—C5 | 118.6 (4) |
F1—C2—C3 | 118.4 (4) | C7—C6—S1 | 124.0 (4) |
F2—C3—C1i | 120.3 (4) | C5—C6—S1 | 117.3 (3) |
F2—C3—C2 | 118.2 (4) | C6—C7—C8 | 118.6 (4) |
C1i—C3—C2 | 121.5 (4) | C6—C7—H7 | 120.7 |
C6ii—S1—C6 | 104.8 (3) | C8—C7—H7 | 120.7 |
C8—N1—C4 | 116.7 (4) | N1—C8—C7 | 123.7 (4) |
N1—C4—C5 | 123.9 (4) | N1—C8—H8 | 118.2 |
N1—C4—H4 | 118.0 | C7—C8—H8 | 118.2 |
C3i—C1—C2—F1 | −179.1 (4) | N1—C4—C5—C6 | 1.7 (7) |
I1—C1—C2—F1 | 0.6 (6) | C4—C5—C6—C7 | −0.3 (7) |
C3i—C1—C2—C3 | 0.4 (7) | C4—C5—C6—S1 | 175.7 (4) |
I1—C1—C2—C3 | −179.9 (3) | C6ii—S1—C6—C7 | −34.9 (3) |
C1—C2—C3—F2 | 178.2 (4) | C6ii—S1—C6—C5 | 149.3 (4) |
F1—C2—C3—F2 | −2.3 (6) | C5—C6—C7—C8 | −1.1 (6) |
C1—C2—C3—C1i | −0.4 (8) | S1—C6—C7—C8 | −176.8 (3) |
F1—C2—C3—C1i | 179.0 (4) | C4—N1—C8—C7 | 0.0 (7) |
C8—N1—C4—C5 | −1.5 (7) | C6—C7—C8—N1 | 1.3 (7) |
Symmetry codes: (i) −x+1, −y+1, −z; (ii) −x, y, −z+1/2. |
Cg1 is the centroid of the N1,C4–C8 ring. |
D—H···A | D—H | H···A | D···A | D—H···A |
C5—H5···F1iii | 0.95 | 2.52 | 3.213 (5) | 130 |
C8—H8···Cg1iv | 0.95 | 2.82 | 3.557 (5) | 135 |
Symmetry codes: (iii) −x+1/2, −y+3/2, −z; (iv) −x+1/2, y−1/2, −z+1/2. |
Experimental details
Crystal data | |
Chemical formula | C10H8N2S·C6F4I2 |
Mr | 590.10 |
Crystal system, space group | Monoclinic, C2/c |
Temperature (K) | 98 |
a, b, c (Å) | 13.804 (5), 5.829 (2), 22.164 (8) |
β (°) | 97.989 (7) |
V (Å3) | 1766.1 (11) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 3.72 |
Crystal size (mm) | 0.30 × 0.20 × 0.05 |
Data collection | |
Diffractometer | Rigaku AFC12K/SATURN724 diffractometer |
Absorption correction | Multi-scan (ABSCOR; Higashi, 1995) |
Tmin, Tmax | 0.757, 1.000 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 5209, 1823, 1733 |
Rint | 0.027 |
(sin θ/λ)max (Å−1) | 0.628 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.034, 0.073, 1.07 |
No. of reflections | 1823 |
No. of parameters | 114 |
H-atom treatment | H-atom parameters constrained |
w = 1/[σ2(Fo2) + (0.0202P)2 + 21.2619P] where P = (Fo2 + 2Fc2)/3 | |
Δρmax, Δρmin (e Å−3) | 1.34, −0.63 |
Computer programs: CrystalClear (Molecular Structure Corporation & Rigaku, 2005), SHELXS97 (Sheldrick, 2008), SHELXL97 (Sheldrick, 2008), ORTEP-3 (Farrugia, 1997) and DIAMOND (Brandenburg, 2006), publCIF (Westrip, 2010).
Cg1 is the centroid of the N1,C4–C8 ring. |
D—H···A | D—H | H···A | D···A | D—H···A |
C5—H5···F1i | 0.95 | 2.52 | 3.213 (5) | 130 |
C8—H8···Cg1ii | 0.95 | 2.82 | 3.557 (5) | 135 |
Symmetry codes: (i) −x+1/2, −y+3/2, −z; (ii) −x+1/2, y−1/2, −z+1/2. |
References
Aragoni, M. C., Arca, M., Crespo, M., Devillanova, F. A., Hursthouse, M. B., Huth, S. L., Isaia, F., Lippolis, V. & Verani, G. (2007). CrystEngComm, 9, 873–878. Web of Science CSD CrossRef CAS Google Scholar
Arman, H. D., Kaulgud, T. & Tiekink, E. R. T. (2010). Acta Cryst. E66, o2356. Web of Science CSD CrossRef IUCr Journals Google Scholar
Brandenburg, K. (2006). DIAMOND. Crystal Impact GbR, Bonn, Germany. Google Scholar
Broker, G. A., Bettens, R. P. A. & Tiekink, E. R. T. (2008). CrystEngComm, 10, 879–887. Web of Science CSD CrossRef CAS Google Scholar
Farrugia, L. J. (1997). J. Appl. Cryst. 30, 565. CrossRef IUCr Journals Google Scholar
Higashi, T. (1995). ABSCOR. Rigaku Corporation, Tokyo, Japan. Google Scholar
Metrangolo, P., Resnati, G., Pilati, T. & Biella, S. (2008). Struct. Bond. 126, 105–136. Web of Science CrossRef CAS Google Scholar
Molecular Structure Corporation & Rigaku (2005). CrystalClear. MSC, The Woodlands, Texas, USA, and Rigaku Corporation, Tokyo, Japan. Google Scholar
Pennington, W. T., Hanks, T. W. & Arman, H. D. (2008). Struct. Bond. 126, 65–104. Web of Science CrossRef CAS Google Scholar
Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. Web of Science CrossRef CAS IUCr Journals Google Scholar
Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925. Web of Science CrossRef CAS IUCr Journals Google Scholar
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As a continuation of studies into the phenomenon of co-crystallization (Broker et al., 2008; Arman et al., 2010), including investigations of halogen bonding (Pennington et al., 2008), the co-crystallization of 1,2,4,5-tetrafluoro-3,6-diiodobenzene and 4-(pyridin-4-yldisulfanyl)pyridine was investigated. This lead to the isolation of the title 1/1 co-crystal, (I), in which desulfurization of 4-(pyridin-4-yldisulfanyl)pyridine has occurred, a process that has literature precedents (Aragoni et al., 2007).
The asymmetric unit in (I) comprises half a molecule of 1,2,4,5-tetrafluoro-3,6-diiodobenzene as this is situated about a centre of inversion, Fig. 1, and half a molecule of 4-(pyridin-4-ylsulfanyl)pyridine, Fig. 2, with the S atom lying on a 2-fold axis. The C6F4I2 molecule is planar with the r.m.s. deviation of all 12 atoms being 0.016 Å. The pyridyl rings in 4-(pyridin-4-ylsulfanyl)pyridine are twisted and form a dihedral angle of 54.88 (13) °.
The components of the co-crystal are connected via N···I interactions [2.838 (4) Å] to form a supramolecular chain with a step-ladder topology and with a base vector 2 0 1, Fig. 3. The chains are consolidated in the crystal packing by C—H···F and C—H···π(pyridyl) interactions, Table 1 and Fig. 4. The N···I interactions observed in (I) represents a further example of N···I—C halogen bonding (Metrangolo et al., 2008).