metal-organic compounds
of 8-iodoquinolinium tetrachloridoaurate(III)
aDepartment of Chemistry, University of South Dakota, 414 E. Clark St., Vermillion, SD 57069, USA
*Correspondence e-mail: jhoefelm@usd.edu
The structure of the title salt, (C9H7IN)[AuCl4], is comprised of planar 8-iodoquinolinium cations (r.m.s. deviation = 0.05 Å) and square-planar tetrachloridoaurate(III) anions. The contains one 8-iodoquinolinium cation and two halfs of [AuCl4]− anions, in each case with the central AuIII atom located on an inversion center. Intermolecular halogen–halogen contacts were found between centrosymmetric pairs of I [3.6178 (4) Å] and Cl atoms [3.1484 (11), 3.3762 (13), and 3.4935 (12) Å]. Intermolecular N—H⋯Cl and C—H⋯Cl hydrogen bonding is also found in the structure. These interactions lead to the formation of a three-dimensional network. Additionally, there is an intramolecular N—H⋯I hydrogen bond between the aromatic iminium and iodine. There are no aurophilic interactions or short contacts between I and Au atoms, and there are no notable π-stacking interactions between the aromatic cations.
Keywords: crystal structure; 8-iodoquinolinium cation; tetrachloridoaurate anion; salt structure.
CCDC reference: 1438910
1. Related literature
There are only two reported structures containing the 8-iodoquinolinium cation, viz. 8-iodoquinolinium chloride dihydrate (Son & Hoefelmeyer, 2008a) and 8-iodoquinolinium triiodide tetrahydrofuran solvate (Son & Hoefelmeyer, 2008b). Recently, the zwitterionic 8-iodoquinoline N-oxide was also reported (Hwang et al., 2014).
2. Experimental
2.1. Crystal data
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2.3. Refinement
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Data collection: APEX2 (Bruker, 2009); cell SAINT (Bruker, 2009); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2015); molecular graphics: Mercury (Macrea et al., 2006); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).
Supporting information
CCDC reference: 1438910
https://doi.org/10.1107/S2056989015022574/wm5236sup1.cif
contains datablocks I, New_Global_Publ_Block. DOI:Structure factors: contains datablock I. DOI: https://doi.org/10.1107/S2056989015022574/wm5236Isup2.hkl
Supporting information file. DOI: https://doi.org/10.1107/S2056989015022574/wm5236Isup3.rtf
In a 4 ml vial, HAuCl4·3H2O (0.12 g, 0.33 mmol), 8-iodoquinoline (0.10 g, 0.39 mmol) and acetonitrile (2 ml) were combined and sonicated for 30 minutes. The 4 ml vial was placed in a 20 ml vial with 5 ml diethylether. Diffusion of the ether vapor into the solution within the smaller vial gave yellow-green crystals, mostly with a cuboid-like form.
C-bound H atoms were placed in ideal positions and refined as riding atoms (C—H = 0.93 Å; Uiso(H) = 1.2Ueq(H)). The H atom bound to the N atom was located from a difference map and refined freely. The highest remaining electron density peak was located 0.20 Å from H6. A
of 0.62 was calculated using the ratio of Tmin (0.4593) to Tmax (0.7452) taken from the absorption correction output file, whereas experimental Tmin (0.174) and Tmax (0.573) give a of 0.30.There are only two reported structures containing the 8-iodoquinolinium cation, viz. 8-iodoquinolinium chloride dihydrate (Son & Hoefelmeyer, 2008a) and 8-iodoquinolinium triiodide tetrahydrofuran solvate (Son & Hoefelmeyer, 2008b). Recently, the zwitterionic 8-iodoquinoline N-oxide was also reported (Hwang et al., 2014).
In a 4 ml vial, HAuCl4·3H2O (0.12 g, 0.33 mmol), 8-iodoquinoline (0.10 g, 0.39 mmol) and acetonitrile (2 ml) were combined and sonicated for 30 minutes. The 4 ml vial was placed in a 20 ml vial with 5 ml diethylether. Diffusion of the ether vapor into the solution within the smaller vial gave yellow-green crystals, mostly with a cuboid-like form.
detailsC-bound H atoms were placed in ideal positions and refined as riding atoms (C—H = 0.93 Å; Uiso(H) = 1.2Ueq(H)). The H atom bound to the N atom was located from a difference map and refined freely. The highest remaining electron density peak was located 0.20 Å from H6. A
of 0.62 was calculated using the ratio of Tmin (0.4593) to Tmax (0.7452) taken from the absorption correction output file, whereas experimental Tmin (0.174) and Tmax (0.573) give a of 0.30.Data collection: APEX2 (Bruker, 2009); cell
SAINT (Bruker, 2009); data reduction: SAINT (Bruker, 2009); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL2014 (Sheldrick, 2015); molecular graphics: Mercury (Macrea et al., 2006); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).Fig. 1. The expanded asymmetric unit of the crystal shown with intermolecular halogen···halogen contacts and hydrogen bonds as dashed lines. [Symmetry codes: (i) 1 - x, 2 - y, 2 - z; (ii) 2 - x, -y, 1 - z; (iii) 1 - x, -1 - y, 1 - z; (iv) -x, -y - 1, -z; (v) x + 1, y + 1, z + 1; (vi) x + 1, y + 1, z; (vii) -x + 2, -y, -z + 1.] | |
Fig. 2. The centrosymmetric unit cell of the title compound. Displacement ellipsoids are drawn at the 50% probability level. | |
Fig. 3. Examination of the nearest distances (Å) between iodine and Au—Cl bond centroids. These distances are beyond the sum of the van der Waals radii of the atoms. |
(C9H7IN)[AuCl4] | Z = 2 |
Mr = 594.82 | F(000) = 536 |
Triclinic, P1 | Dx = 2.920 Mg m−3 |
a = 7.6299 (5) Å | Mo Kα radiation, λ = 0.71073 Å |
b = 7.8609 (5) Å | Cell parameters from 5508 reflections |
c = 11.7125 (7) Å | θ = 2.6–25.6° |
α = 80.160 (1)° | µ = 13.92 mm−1 |
β = 78.143 (1)° | T = 100 K |
γ = 85.178 (1)° | Plate, light green |
V = 676.52 (7) Å3 | 0.16 × 0.11 × 0.04 mm |
Bruker APEXII CCD diffractometer | 2407 reflections with I > 2σ(I) |
φ and ω scans | Rint = 0.024 |
Absorption correction: multi-scan (SADABS; Bruker, 2009) | θmax = 25.4°, θmin = 1.8° |
Tmin = 0.174, Tmax = 0.573 | h = −9→9 |
6855 measured reflections | k = −9→9 |
2482 independent reflections | l = −14→14 |
Refinement on F2 | 0 restraints |
Least-squares matrix: full | Hydrogen site location: mixed |
R[F2 > 2σ(F2)] = 0.016 | H atoms treated by a mixture of independent and constrained refinement |
wR(F2) = 0.040 | w = 1/[σ2(Fo2) + (0.019P)2 + 0.5573P] where P = (Fo2 + 2Fc2)/3 |
S = 1.04 | (Δ/σ)max = 0.001 |
2482 reflections | Δρmax = 1.19 e Å−3 |
152 parameters | Δρmin = −0.94 e Å−3 |
(C9H7IN)[AuCl4] | γ = 85.178 (1)° |
Mr = 594.82 | V = 676.52 (7) Å3 |
Triclinic, P1 | Z = 2 |
a = 7.6299 (5) Å | Mo Kα radiation |
b = 7.8609 (5) Å | µ = 13.92 mm−1 |
c = 11.7125 (7) Å | T = 100 K |
α = 80.160 (1)° | 0.16 × 0.11 × 0.04 mm |
β = 78.143 (1)° |
Bruker APEXII CCD diffractometer | 2482 independent reflections |
Absorption correction: multi-scan (SADABS; Bruker, 2009) | 2407 reflections with I > 2σ(I) |
Tmin = 0.174, Tmax = 0.573 | Rint = 0.024 |
6855 measured reflections |
R[F2 > 2σ(F2)] = 0.016 | 0 restraints |
wR(F2) = 0.040 | H atoms treated by a mixture of independent and constrained refinement |
S = 1.04 | Δρmax = 1.19 e Å−3 |
2482 reflections | Δρmin = −0.94 e Å−3 |
152 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
I1 | 0.54637 (3) | 0.86196 (3) | 0.88748 (2) | 0.01671 (7) | |
Au2 | 0.0000 | 0.0000 | 0.0000 | 0.01009 (6) | |
Au1 | 0.5000 | 0.0000 | 0.5000 | 0.00870 (6) | |
Cl3 | 0.07524 (11) | 0.00792 (10) | −0.20000 (7) | 0.01714 (17) | |
Cl2 | 0.20893 (10) | 0.01686 (10) | 0.47699 (7) | 0.01590 (17) | |
Cl4 | 0.00376 (12) | −0.29552 (11) | 0.02554 (8) | 0.01672 (18) | |
C8 | 0.5841 (5) | 0.6220 (4) | 0.8290 (3) | 0.0137 (7) | |
C7 | 0.4426 (5) | 0.5185 (5) | 0.8453 (3) | 0.0167 (8) | |
H7 | 0.3321 | 0.5507 | 0.8887 | 0.020* | |
C6 | 0.4621 (5) | 0.3624 (5) | 0.7968 (3) | 0.0201 (8) | |
H6 | 0.3655 | 0.2923 | 0.8092 | 0.024* | |
C5 | 0.6244 (5) | 0.3160 (5) | 0.7317 (3) | 0.0173 (8) | |
H5 | 0.6359 | 0.2155 | 0.6982 | 0.021* | |
C10 | 0.7737 (5) | 0.4170 (4) | 0.7144 (3) | 0.0136 (7) | |
C4 | 0.9432 (5) | 0.3733 (5) | 0.6493 (3) | 0.0163 (7) | |
H4 | 0.9589 | 0.2741 | 0.6142 | 0.020* | |
N1 | 0.9009 (4) | 0.6662 (4) | 0.7494 (3) | 0.0146 (6) | |
C9 | 0.7541 (5) | 0.5716 (5) | 0.7656 (3) | 0.0134 (7) | |
Cl1 | 0.49806 (11) | −0.29443 (10) | 0.53814 (8) | 0.01473 (17) | |
C3 | 1.0864 (5) | 0.4757 (5) | 0.6369 (3) | 0.0172 (8) | |
H3 | 1.1983 | 0.4458 | 0.5942 | 0.021* | |
C2 | 1.0612 (5) | 0.6228 (5) | 0.6887 (3) | 0.0166 (8) | |
H2 | 1.1569 | 0.6925 | 0.6812 | 0.020* | |
H99 | 0.890 (6) | 0.755 (6) | 0.776 (4) | 0.026 (12)* |
U11 | U22 | U33 | U12 | U13 | U23 | |
I1 | 0.01797 (12) | 0.01529 (12) | 0.01717 (12) | 0.00269 (9) | −0.00223 (9) | −0.00651 (9) |
Au2 | 0.01106 (10) | 0.00938 (10) | 0.01044 (10) | −0.00048 (7) | −0.00355 (7) | −0.00150 (7) |
Au1 | 0.00681 (9) | 0.01063 (10) | 0.00881 (10) | 0.00010 (7) | −0.00208 (7) | −0.00155 (7) |
Cl3 | 0.0245 (4) | 0.0160 (4) | 0.0109 (4) | −0.0024 (3) | −0.0030 (3) | −0.0017 (3) |
Cl2 | 0.0086 (4) | 0.0191 (4) | 0.0211 (4) | 0.0000 (3) | −0.0055 (3) | −0.0036 (3) |
Cl4 | 0.0233 (4) | 0.0104 (4) | 0.0166 (4) | −0.0010 (3) | −0.0040 (4) | −0.0020 (3) |
C8 | 0.0163 (17) | 0.0134 (17) | 0.0117 (17) | 0.0026 (14) | −0.0041 (14) | −0.0028 (13) |
C7 | 0.0180 (18) | 0.0184 (18) | 0.0124 (17) | −0.0002 (14) | −0.0022 (14) | −0.0001 (14) |
C6 | 0.025 (2) | 0.0210 (19) | 0.0133 (18) | 0.0035 (16) | −0.0067 (15) | 0.0009 (15) |
C5 | 0.027 (2) | 0.0131 (17) | 0.0139 (18) | −0.0024 (15) | −0.0092 (15) | −0.0016 (14) |
C10 | 0.0198 (18) | 0.0127 (17) | 0.0077 (16) | 0.0013 (14) | −0.0048 (14) | 0.0014 (13) |
C4 | 0.0235 (19) | 0.0133 (17) | 0.0130 (17) | 0.0058 (14) | −0.0080 (15) | −0.0021 (14) |
N1 | 0.0164 (15) | 0.0125 (15) | 0.0153 (15) | 0.0006 (12) | −0.0041 (12) | −0.0024 (12) |
C9 | 0.0177 (17) | 0.0125 (17) | 0.0098 (16) | 0.0008 (13) | −0.0067 (14) | 0.0027 (13) |
Cl1 | 0.0150 (4) | 0.0115 (4) | 0.0176 (4) | −0.0005 (3) | −0.0037 (3) | −0.0014 (3) |
C3 | 0.0138 (17) | 0.0234 (19) | 0.0117 (17) | 0.0055 (15) | −0.0005 (14) | −0.0007 (14) |
C2 | 0.0159 (18) | 0.0173 (18) | 0.0159 (18) | −0.0029 (14) | −0.0053 (14) | 0.0026 (14) |
I1—C8 | 2.093 (3) | C6—H6 | 0.9300 |
Au2—Cl3 | 2.2857 (8) | C5—C10 | 1.404 (5) |
Au2—Cl3i | 2.2857 (8) | C5—H5 | 0.9300 |
Au2—Cl4i | 2.2894 (8) | C10—C4 | 1.407 (5) |
Au2—Cl4 | 2.2895 (8) | C10—C9 | 1.429 (5) |
Au1—Cl1ii | 2.2817 (8) | C4—C3 | 1.381 (5) |
Au1—Cl1 | 2.2817 (8) | C4—H4 | 0.9300 |
Au1—Cl2ii | 2.2818 (8) | N1—C2 | 1.331 (5) |
Au1—Cl2 | 2.2818 (8) | N1—C9 | 1.360 (5) |
C8—C7 | 1.369 (5) | N1—H99 | 0.80 (4) |
C8—C9 | 1.418 (5) | C3—C2 | 1.377 (5) |
C7—C6 | 1.422 (5) | C3—H3 | 0.9300 |
C7—H7 | 0.9300 | C2—H2 | 0.9300 |
C6—C5 | 1.371 (5) | ||
Cl3—Au2—Cl3i | 180.0 | C6—C5—C10 | 121.4 (3) |
Cl3—Au2—Cl4i | 90.15 (3) | C6—C5—H5 | 119.3 |
Cl3i—Au2—Cl4i | 89.85 (3) | C10—C5—H5 | 119.3 |
Cl3—Au2—Cl4 | 89.85 (3) | C5—C10—C4 | 123.3 (3) |
Cl3i—Au2—Cl4 | 90.15 (3) | C5—C10—C9 | 118.8 (3) |
Cl4i—Au2—Cl4 | 180.0 | C4—C10—C9 | 117.9 (4) |
Cl1ii—Au1—Cl1 | 180.0 | C3—C4—C10 | 120.9 (3) |
Cl1ii—Au1—Cl2ii | 90.54 (3) | C3—C4—H4 | 119.6 |
Cl1—Au1—Cl2ii | 89.46 (3) | C10—C4—H4 | 119.6 |
Cl1ii—Au1—Cl2 | 89.46 (3) | C2—N1—C9 | 123.7 (3) |
Cl1—Au1—Cl2 | 90.54 (3) | C2—N1—H99 | 118 (3) |
Cl2ii—Au1—Cl2 | 180.0 | C9—N1—H99 | 118 (3) |
C7—C8—C9 | 119.9 (3) | N1—C9—C8 | 122.7 (3) |
C7—C8—I1 | 120.2 (3) | N1—C9—C10 | 117.9 (3) |
C9—C8—I1 | 119.8 (3) | C8—C9—C10 | 119.4 (3) |
C8—C7—C6 | 121.0 (3) | C2—C3—C4 | 119.0 (3) |
C8—C7—H7 | 119.5 | C2—C3—H3 | 120.5 |
C6—C7—H7 | 119.5 | C4—C3—H3 | 120.5 |
C5—C6—C7 | 119.5 (4) | N1—C2—C3 | 120.6 (3) |
C5—C6—H6 | 120.3 | N1—C2—H2 | 119.7 |
C7—C6—H6 | 120.3 | C3—C2—H2 | 119.7 |
Symmetry codes: (i) −x, −y, −z; (ii) −x+1, −y, −z+1. |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H99···Cl3iii | 0.80 (5) | 2.62 (5) | 3.287 (3) | 142 (4) |
N1—H99···I1 | 0.80 (5) | 2.81 (5) | 3.264 (3) | 118 (4) |
C2—H2···Cl1iv | 0.93 | 2.79 | 3.493 (4) | 133 |
C3—H3···Cl1v | 0.93 | 2.81 | 3.722 (4) | 168 |
Symmetry codes: (iii) x+1, y+1, z+1; (iv) x+1, y+1, z; (v) −x+2, −y, −z+1. |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H99···Cl3i | 0.80 (5) | 2.62 (5) | 3.287 (3) | 142 (4) |
N1—H99···I1 | 0.80 (5) | 2.81 (5) | 3.264 (3) | 118 (4) |
C2—H2···Cl1ii | 0.93 | 2.79 | 3.493 (4) | 133 |
C3—H3···Cl1iii | 0.93 | 2.81 | 3.722 (4) | 168 |
Symmetry codes: (i) x+1, y+1, z+1; (ii) x+1, y+1, z; (iii) −x+2, −y, −z+1. |
Acknowledgements
Purchase of the X-ray diffractometer was made possible by funding from the National Science Foundation (grant No. EPS-0554609).
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