metal-organic compounds
Poly[(μ4-5-bromopyridine-3-sulfonato)silver(I)]
aCollege of Chemistry and Chemical Engineering, Gannan Normal University, Ganzhou 341000, People's Republic of China
*Correspondence e-mail: yblu@fjirsm.ac.cn
The silver(I) complex, [Ag(C5H3BrNO3S)]n, was obtained by reaction of AgNO3 and 5-bromopyridine-3-sulfonic acid. The AgI ion is coordinated by an O3N donor set in a slightly distorted tetrahedral geometry. The AgI ions are linked by μ4-5-bromopyridine-3-sulfonate ligands, forming a layer parallel to (100). The layers are further connected via C—H⋯Br hydrogen-bonding interactions into a three-dimensional supramolecular network. The Ag⋯Ag separation is 3.0159 (6) Å, indicating the presence of argentophilic interactions.
Related literature
For background information on pyridinesulfonato ligands, see: Chandler et al. (2002); Makinen et al. (2001); May & Shimizu (2005). For similar C—H⋯Br hydrogen bonding, see: Lu et al. (2011).
Experimental
Crystal data
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Refinement
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Data collection: SMART (Bruker, 2001); cell SAINT (Bruker, 2001); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008b); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008b); molecular graphics: SHELXTL (Sheldrick, 2008b); software used to prepare material for publication: SHELXTL.
Supporting information
10.1107/S1600536811055206/zj2045sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536811055206/zj2045Isup2.hkl
AgNO3 (85 mg, 0.5 mmol) and bromopyridinesulfonato ligands (103 mg, 0.5 mmol) were dissolved in 20 ml water, stirring for 2 h. The resulting solution was filtrated and allowed to evaporate slowly at room temperature. Colorless block crystals appeared after 1 week. Yield based on Ag: 15%.
H atoms were placed in calculated positions with C—H = 0.93 Å (aromatic), and refined in riding mode with Uiso(H) = 1.2Ueq(C). The abnormal reflections (-7 1 2), (-4 2 3), (8 0 0), (1 1 6) (-4 0 2), (-2 06) and (-5 1 3) have been omitted during the
The "delu 0.005 C1 N1 Ag1 O1" has been employed during the to modify the small difference of anisotropic displacement parameters along chemical bonds.Data collection: SMART (Bruker, 2001); cell
SAINT (Bruker, 2001); data reduction: SAINT (Bruker, 2001); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008b); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008b); molecular graphics: SHELXTL (Sheldrick, 2008b); software used to prepare material for publication: SHELXTL (Sheldrick, 2008b).[Ag(C5H3BrNO3S)] | F(000) = 1296 |
Mr = 344.92 | Dx = 2.990 Mg m−3 |
Monoclinic, C2/c | Melting point: not measured K |
a = 20.103 (3) Å | Mo Kα radiation, λ = 0.71073 Å |
b = 5.0634 (9) Å | θ = 2.2–25° |
c = 16.036 (3) Å | µ = 8.08 mm−1 |
β = 110.142 (2)° | T = 296 K |
V = 1532.5 (5) Å3 | Blcok, colorless |
Z = 8 | 0.20 × 0.18 × 0.16 mm |
Bruker SMART CCD area-detector diffractometer | 1310 independent reflections |
Radiation source: fine-focus sealed tube | 1204 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.022 |
phi and ω scans | θmax = 25.0°, θmin = 2.2° |
Absorption correction: multi-scan (SADABS; Sheldrick, 2008a) | h = −23→23 |
Tmin = 0.512, Tmax = 0.746 | k = −6→6 |
4188 measured reflections | l = −19→19 |
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)] = 0.038 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.152 | H-atom parameters constrained |
S = 1.01 | w = 1/[σ2(Fo2) + (0.132P)2] where P = (Fo2 + 2Fc2)/3 |
1310 reflections | (Δ/σ)max = 0.009 |
109 parameters | Δρmax = 0.88 e Å−3 |
2 restraints | Δρmin = −1.72 e Å−3 |
0 constraints |
[Ag(C5H3BrNO3S)] | V = 1532.5 (5) Å3 |
Mr = 344.92 | Z = 8 |
Monoclinic, C2/c | Mo Kα radiation |
a = 20.103 (3) Å | µ = 8.08 mm−1 |
b = 5.0634 (9) Å | T = 296 K |
c = 16.036 (3) Å | 0.20 × 0.18 × 0.16 mm |
β = 110.142 (2)° |
Bruker SMART CCD area-detector diffractometer | 1310 independent reflections |
Absorption correction: multi-scan (SADABS; Sheldrick, 2008a) | 1204 reflections with I > 2σ(I) |
Tmin = 0.512, Tmax = 0.746 | Rint = 0.022 |
4188 measured reflections |
R[F2 > 2σ(F2)] = 0.038 | 2 restraints |
wR(F2) = 0.152 | H-atom parameters constrained |
S = 1.01 | Δρmax = 0.88 e Å−3 |
1310 reflections | Δρmin = −1.72 e Å−3 |
109 parameters |
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. |
x | y | z | Uiso*/Ueq | ||
Ag1 | 0.325354 (14) | 0.79247 (6) | 0.004298 (16) | 0.03990 (8) | |
Br1 | 0.505370 (16) | 0.92599 (7) | 0.38247 (2) | 0.03684 (10) | |
S1 | 0.31936 (4) | 0.26125 (15) | 0.13294 (5) | 0.0237 (2) | |
N1 | 0.36109 (14) | 0.3610 (6) | 0.39356 (17) | 0.0280 (7) | |
O1 | 0.36615 (13) | 0.3588 (6) | 0.08721 (15) | 0.0417 (6) | |
O2 | 0.25004 (15) | 0.3786 (6) | 0.10181 (17) | 0.0468 (8) | |
O3 | 0.31813 (13) | −0.0272 (5) | 0.13609 (16) | 0.0365 (7) | |
C1 | 0.33643 (16) | 0.2719 (7) | 0.3129 (2) | 0.0252 (8) | |
H1A | 0.3026 | 0.1385 | 0.2993 | 0.030* | |
C2 | 0.35925 (15) | 0.3708 (6) | 0.24497 (18) | 0.0201 (7) | |
C3 | 0.40983 (15) | 0.5648 (7) | 0.26565 (19) | 0.0237 (8) | |
H3A | 0.4265 | 0.6324 | 0.2226 | 0.028* | |
C4 | 0.43547 (15) | 0.6575 (7) | 0.3514 (2) | 0.0269 (8) | |
C5 | 0.41094 (16) | 0.5505 (7) | 0.4151 (2) | 0.0285 (9) | |
H5A | 0.4292 | 0.6107 | 0.4733 | 0.034* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Ag1 | 0.05584 (14) | 0.04198 (16) | 0.02679 (13) | 0.01450 (12) | 0.02051 (11) | 0.00050 (10) |
Br1 | 0.03597 (16) | 0.0366 (2) | 0.03715 (17) | −0.00643 (15) | 0.01160 (13) | −0.00657 (15) |
S1 | 0.0333 (3) | 0.0199 (4) | 0.0160 (3) | 0.0027 (3) | 0.0060 (3) | −0.0009 (3) |
N1 | 0.0360 (12) | 0.0253 (13) | 0.0241 (11) | −0.0001 (12) | 0.0120 (9) | −0.0010 (11) |
O1 | 0.0639 (13) | 0.0433 (10) | 0.0244 (9) | −0.0083 (12) | 0.0236 (9) | 0.0060 (9) |
O2 | 0.0498 (13) | 0.0449 (14) | 0.0294 (12) | 0.0224 (13) | −0.0071 (11) | −0.0057 (12) |
O3 | 0.0608 (13) | 0.0185 (11) | 0.0306 (10) | −0.0012 (11) | 0.0164 (10) | −0.0084 (9) |
C1 | 0.0207 (11) | 0.0258 (16) | 0.0285 (14) | −0.0027 (12) | 0.0075 (11) | 0.0065 (12) |
C2 | 0.0308 (12) | 0.0156 (13) | 0.0149 (11) | 0.0024 (12) | 0.0091 (10) | 0.0012 (11) |
C3 | 0.0241 (11) | 0.0291 (17) | 0.0216 (12) | 0.0056 (12) | 0.0126 (10) | 0.0014 (12) |
C4 | 0.0160 (11) | 0.0322 (17) | 0.0297 (15) | 0.0008 (14) | 0.0044 (11) | 0.0033 (14) |
C5 | 0.0294 (13) | 0.0385 (19) | 0.0159 (13) | 0.0021 (15) | 0.0056 (11) | 0.0012 (13) |
Ag1—N1i | 2.270 (3) | N1—C5 | 1.344 (4) |
Ag1—O3ii | 2.352 (3) | N1—Ag1iv | 2.270 (3) |
Ag1—O2iii | 2.488 (3) | O2—Ag1iii | 2.488 (3) |
Ag1—O1 | 2.552 (3) | O3—Ag1v | 2.352 (3) |
Ag1—Ag1iii | 3.0159 (8) | C1—C2 | 1.411 (5) |
Br1—C4 | 1.894 (3) | C1—H1A | 0.9300 |
S1—O2 | 1.437 (3) | C2—C3 | 1.370 (4) |
S1—O3 | 1.462 (3) | C3—C4 | 1.374 (4) |
S1—O1 | 1.463 (3) | C3—H3A | 0.9300 |
S1—C2 | 1.785 (3) | C4—C5 | 1.388 (5) |
N1—C1 | 1.297 (4) | C5—H5A | 0.9300 |
N1i—Ag1—O3ii | 165.92 (9) | S1—O1—Ag1 | 113.87 (15) |
N1i—Ag1—O2iii | 88.66 (10) | S1—O2—Ag1iii | 143.5 (2) |
O3ii—Ag1—O2iii | 98.22 (9) | S1—O3—Ag1v | 110.48 (15) |
N1i—Ag1—O1 | 88.93 (10) | N1—C1—C2 | 122.2 (3) |
O3ii—Ag1—O1 | 88.52 (8) | N1—C1—H1A | 118.9 |
O2iii—Ag1—O1 | 160.60 (9) | C2—C1—H1A | 118.9 |
N1i—Ag1—Ag1iii | 119.93 (7) | C3—C2—C1 | 118.6 (3) |
O3ii—Ag1—Ag1iii | 74.01 (6) | C3—C2—S1 | 120.3 (2) |
O2iii—Ag1—Ag1iii | 72.45 (7) | C1—C2—S1 | 120.9 (2) |
O1—Ag1—Ag1iii | 92.22 (6) | C2—C3—C4 | 118.6 (3) |
O2—S1—O3 | 113.53 (16) | C2—C3—H3A | 120.7 |
O2—S1—O1 | 113.59 (17) | C4—C3—H3A | 120.7 |
O3—S1—O1 | 112.07 (17) | C3—C4—C5 | 119.8 (3) |
O2—S1—C2 | 105.49 (15) | C3—C4—Br1 | 119.8 (3) |
O3—S1—C2 | 106.43 (14) | C5—C4—Br1 | 120.4 (2) |
O1—S1—C2 | 104.83 (15) | N1—C5—C4 | 120.8 (3) |
C1—N1—C5 | 120.0 (3) | N1—C5—H5A | 119.6 |
C1—N1—Ag1iv | 123.1 (2) | C4—C5—H5A | 119.6 |
C5—N1—Ag1iv | 116.9 (2) |
Symmetry codes: (i) x, −y+1, z−1/2; (ii) x, y+1, z; (iii) −x+1/2, −y+3/2, −z; (iv) x, −y+1, z+1/2; (v) x, y−1, z. |
D—H···A | D—H | H···A | D···A | D—H···A |
C3—H3A···Br1vi | 0.93 | 2.92 | 3.832 (3) | 168 |
Symmetry code: (vi) −x+1, y, −z+1/2. |
Experimental details
Crystal data | |
Chemical formula | [Ag(C5H3BrNO3S)] |
Mr | 344.92 |
Crystal system, space group | Monoclinic, C2/c |
Temperature (K) | 296 |
a, b, c (Å) | 20.103 (3), 5.0634 (9), 16.036 (3) |
β (°) | 110.142 (2) |
V (Å3) | 1532.5 (5) |
Z | 8 |
Radiation type | Mo Kα |
µ (mm−1) | 8.08 |
Crystal size (mm) | 0.20 × 0.18 × 0.16 |
Data collection | |
Diffractometer | Bruker SMART CCD area-detector diffractometer |
Absorption correction | Multi-scan (SADABS; Sheldrick, 2008a) |
Tmin, Tmax | 0.512, 0.746 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 4188, 1310, 1204 |
Rint | 0.022 |
(sin θ/λ)max (Å−1) | 0.595 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.038, 0.152, 1.01 |
No. of reflections | 1310 |
No. of parameters | 109 |
No. of restraints | 2 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.88, −1.72 |
Computer programs: SMART (Bruker, 2001), SAINT (Bruker, 2001), SHELXS97 (Sheldrick, 2008b), SHELXL97 (Sheldrick, 2008b), SHELXTL (Sheldrick, 2008b).
D—H···A | D—H | H···A | D···A | D—H···A |
C3—H3A···Br1i | 0.93 | 2.92 | 3.832 (3) | 167.5 |
Symmetry code: (i) −x+1, y, −z+1/2. |
Acknowledgements
We acknowledge financial support from the NSF of Jiangxi Provincial Education Department (Nos. GJJ10717 and 2009ZDG02800) and the Key Laboratory of Jiangxi University for Function of Materials Chemistry.
References
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As bridging ligands, sulfonate ligands and their derivatives have drawn much attention owing to their diverse coordination modes, forming numerous coordination complexes. In this paper, we report the new title compound 1, which displays a two-dimensional layer structure.
X-ray diffraction analyses reveal that the title compound crystallizes in the C2/c group space. In the asymmetrical unit of 1 (Fig. 1), there is one crystallographically independent Ag+ ion and one 5-Bromopyridine-3-sulfonato ligand. The Ag1 atom is in a distorted tetrahedral coordination environment and coordinated by one O1 atom, one O2 atom, one O3 atom and N1 atom from four different 5-Bromopyridine-3-sulfonato ligands. As shown in Figure 2, the Ag1 ions are linked by three oxygen atoms from sulfonate groups to form 1-D chain. Interestingly, the Ag···Ag separation in the [Ag1]2 dimers is 3.0159 (6) Å, which is much shorter than the sum of van der Waals radii for silver (3.4 Å), suggesting significant silver-silver interactions. These chains are further connected through N1 atoms from µ4-5-Bromopyridine-3-sulfonato ligands to generate a two-dimensional layer. The layers are connected via C3—H3A···Br1 hydrogen bonding interactions (Lu et al., 2011) into a three-dimensional supramolecular architecture (Fig. 3 and Table 1).