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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2013 Oct 19;69(Pt 11):m608. doi: 10.1107/S1600536813028213

catena-Poly[2-methyl­pyridinium [tungstate-di-μ-selenido-silver-di-μ-selenido] 2-methyl­pyridine monosolvate]

Lu-Jun Zhou a, Hua-Tian Shi b, Chao Xu b, Qun Chen a, Qian-Feng Zhang b,a,*
PMCID: PMC3884262  PMID: 24454038

Abstract

The title compound, {(C6H8N)[AgWSe4]·C6H7N}n, consists of anionic [WAgSe4]n chains, 2-methyl­pyridinium cations and neutral 2-methyl­pyridine mol­ecules. The Se atoms bridge the Ag and W atoms, forming a polymeric chain extending along the b-axis direction. Both the Ag and W atoms are located on a twofold rotation axis and each metal atom is coordinated by four Se atoms in distorted tetra­hedral geometry. In the crystal, the 2-methyl­pyridinium cation and 2-methyl­pyridine mol­ecule are linked via N—H⋯N hydrogen bonding. Weak C—H⋯Se inter­actions link the organic components and polymeric anions into a three-dimensional architecture.

Related literature  

For applications of compounds with [M,M′Se4] anions (M,M′ = transition metals), see: Zhang et al. (2002, 2006). For related structures, see: Huang et al. (1997); Lang et al. (1993); Müller et al. (1983); Yu et al. (1998); Dai et al. (2007); Zhang et al. (2000).graphic file with name e-69-0m608-scheme1.jpg

Experimental  

Crystal data  

  • (C6H8N)[AgWSe4]·C6H7N

  • M r = 794.82

  • Monoclinic, Inline graphic

  • a = 7.859 (2) Å

  • b = 5.9448 (15) Å

  • c = 19.830 (5) Å

  • β = 100.962 (3)°

  • V = 909.5 (4) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 15.39 mm−1

  • T = 296 K

  • 0.15 × 0.12 × 0.03 mm

Data collection  

  • Bruker APEXII CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2001) T min = 0.206, T max = 0.655

  • 5398 measured reflections

  • 2051 independent reflections

  • 1565 reflections with I > 2σ(I)

  • R int = 0.041

Refinement  

  • R[F 2 > 2σ(F 2)] = 0.034

  • wR(F 2) = 0.078

  • S = 0.97

  • 2051 reflections

  • 93 parameters

  • H-atom parameters constrained

  • Δρmax = 0.86 e Å−3

  • Δρmin = −1.06 e Å−3

Data collection: APEX2 (Bruker, 2007); cell refinement: SAINT (Bruker, 2007); data reduction: SAINT; program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; molecular graphics: SHELXTL; software used to prepare material for publication: SHELXTL.

Supplementary Material

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536813028213/xu5746sup1.cif

e-69-0m608-sup1.cif (18.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813028213/xu5746Isup2.hkl

e-69-0m608-Isup2.hkl (100.9KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Selected bond lengths (Å).

W1—Se1 2.3347 (9)
W1—Se2 2.3379 (9)
Ag1—Se1i 2.6224 (11)
Ag1—Se2 2.6210 (10)

Symmetry code: (i) Inline graphic.

Table 2. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A DA D—H⋯A
N1—H1N⋯N1ii 0.86 1.93 2.786 (12) 172
C1—H1⋯Se1 0.93 2.96 3.732 (8) 141
C4—H4⋯Se1iii 0.93 2.90 3.832 (8) 176

Symmetry codes: (ii) Inline graphic; (iii) Inline graphic.

Acknowledgments

This work was supported by the Natural Science Foundation of China (20871002) and the Program for New Century Excellent Talents in Universities of China (NCET-08–0618). QFZ is grateful to the State Key Laboratory of Coordination Chemistry at Nanjing University for assistance with the data collection.

supplementary crystallographic information

1. Comment

Tetraselenometalates [MSe4]2- (M =Mo, W) have been extensively used in the synthesis of heterselenometallic clusters with third-order nonlinear properties (Zhang et al., 2002). Of special which argentoselenometallic clusters are of good photostability and relatively stable optical limiting effects (Zhang et al., 2006). It has been found that the assembling of [MS4]2- (M =Mo, W) and Ag+ is flexible through non-bonding interactions with complementary small molecules (or cations) and the solvent, which can assemble into polymeric heterothiometallic clusters with different configurations, such as single linear, zigzag and helical and double chains (Huang et al., 1997; Lang et al., 1993; Müller et al., 1983; Yu et al., 1998). However, it has been noted that the difficulty in the synthesis of argentoselenometallic clusters is probably due to the low solubility of Ag+ species that are involved in the self-assembly with the [MSe4]2- (M =Mo, W) anion. It is thus understood that only two examples of structurally characterized argentoselenometallic clusters including one-dimensional linear {[Et4N][(µ-WSe4)Ag]}n (Dai et al., 2007) and helical {[La(Me2SO)8][(µ3-WSe4)3Ag3]}n (Zhang et al., 2000) have been appeared up to date. The one-dimensional chain structure of the title heteroselenometallic polymer {[(2-MepyH)(2-Mepy)][(µ-WSe4)Ag]}n is herein described as an addition of this family.

The title heteroselenometallic complex crystallizes in the monoclinic with P2/c space group. An analogous heterothiometallic complex, {[\>a-MepyH][MoS4Ag]}n, has been reported, which crystallizes in a monoclinic Pc space group (Lang et al., 1993). The structure determination shows that the title heteroselenometallic complex consists of [(2-MepyH)(2-Mepy)]+ (py = pyridine) cations with the N—H···N hydrogen bonds and polymeric linear chain of [(µ-WSe4)Ag]- anions, as shown in Fig. 1. The anion chain is composed of extended rhombic networks of co-planar [Ag(µ-Se2)W] units and the neighbouring rhombi in the chain are alternately almost perpendicular to each other. Both metal atoms display tetrahedron coordination in a selenium-rich environment, comparatively, the coordination geometry of the silver atoms (Se—Ag—Se: 97.67 (5)—115.91 (3)°) is more distorted than the tungsten atoms (Se—W—Se: 106.25 (3)—115.47 (5)°). The chain has a straight linear configuration with an Ag—W—Ag angle of 180°. The average W—µ-Se and Ag—µ-Se bond lengths are 2.3363 (9) and 2.6217 (10) Å, respectively. The average W···Ag distance of 2.9725 (11) Å in the title heteroselenometallic complex is comparable to those in {[Et4N][(µ-WSe4)Ag]}n (av. 3.0169 (2) Å) (Dai et al., 2007), {[La(Me2SO)8][(µ3-WSe4)3Ag3]}n (av. 3.0038 (12) Å) (Zhang, et al., 2000), and [(µ-WSe4)(AgPPh3){Ag(PPh3)2}] (av. 2.996 (1) Å) (Zhang et al., 2002). The hydrogen-bonding interactions exist between the nitrogen atom of pyridinium caion and the nitrogen atom of the pyridine molecule, forming a molecular [(2-MepyH)(2-Mepy)]+ cation with the N—H···N distance and angle of 2.786 (12) Å and 171.9 (3)°, respectively. Relatively weak interactions exist between organic cations and polymeric anions via the C—H···Se hydrogen-bonds with the C—H···Se distance and angle of 3.731 (2) Å and 141.9 (3)°, respectively, as shown in Fig. 1.

2. Experimental

A solution of AgNO3 (42.5 mg, 0.25 mmol) in MeCN (5 ml) was added dropwise to a solution of [Et4N]2[WSe4] (190 mg, 0.25 mmol) in DMF (5 ml). The mixture was stirred for 30 min at room temperature, resulting in a large amount of black precipitate. Upon addition of 2 ml 2-picoline solution, the black precipitate was re-dissolved. The resultant solution was stirred for additional 30 min at room temperature and filtered to afford a dark red filtrate. Dark-red prism crystals of the title complex were obtained after allowing the filtrate to stand at room temperature for three days. Anal. Calc. for C12H15N2Se4WAg: C, 18.13; H, 1.90; N, 3.53%. Found: C, 18.05; H, 1.87; N, 3.49%.

3. Refinement

H atoms were placed in geometrically idealized positions and refined in a riding model with N—H = 0.86, C—H = 0.93–0.97 Å, Uiso(H) = 1.5Ueq(C) for methyl H atoms and 1.2Ueq(C,N) for the others. N-bound H atom has 0.5 site occupancy in the crystal.

Figures

Fig. 1.

Fig. 1.

A perspective view of molecular structure of heteroselenometallic polymeric complex {[(2-MepyH)(2-Mepy)][(µ-WSe4)Ag]}n. The ellipsoids are drawn at the 50% probability level. Hydrogen bonds are shown in the dash lines.

Crystal data

(C6H8N)[AgWSe4]·C6H7N F(000) = 716
Mr = 794.82 Dx = 2.902 Mg m3
Monoclinic, P2/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yc Cell parameters from 1243 reflections
a = 7.859 (2) Å θ = 2.6–24.5°
b = 5.9448 (15) Å µ = 15.39 mm1
c = 19.830 (5) Å T = 296 K
β = 100.962 (3)° Prism, dark red
V = 909.5 (4) Å3 0.15 × 0.12 × 0.03 mm
Z = 2

Data collection

Bruker APEXII CCD area-detector diffractometer 2051 independent reflections
Radiation source: fine-focus sealed tube 1565 reflections with I > 2σ(I)
Graphite monochromator Rint = 0.041
phi and ω scans θmax = 27.4°, θmin = 2.6°
Absorption correction: multi-scan (SADABS; Bruker, 2001) h = −10→6
Tmin = 0.206, Tmax = 0.655 k = −7→7
5398 measured reflections l = −24→25

Refinement

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) = 0.078 H-atom parameters constrained
S = 0.97 w = 1/[σ2(Fo2) + (0.0357P)2] where P = (Fo2 + 2Fc2)/3
2051 reflections (Δ/σ)max = 0.001
93 parameters Δρmax = 0.86 e Å3
0 restraints Δρmin = −1.06 e Å3

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.
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)

x y z Uiso*/Ueq Occ. (<1)
W1 0.5000 0.30930 (6) 0.7500 0.03027 (13)
Ag1 0.5000 0.80929 (13) 0.7500 0.0524 (2)
Se1 0.24423 (10) 0.09964 (13) 0.72794 (4) 0.0417 (2)
Se2 0.50518 (11) 0.51956 (12) 0.65078 (4) 0.0434 (2)
N1 0.0998 (7) 0.3192 (10) 0.4854 (3) 0.0389 (14)
H1N 0.0423 0.4382 0.4914 0.047* 0.50
C1 0.1778 (10) 0.1984 (14) 0.5389 (4) 0.0478 (19)
H1 0.1711 0.2486 0.5828 0.057*
C2 0.2676 (11) 0.0041 (13) 0.5329 (5) 0.053 (2)
H2 0.3163 −0.0786 0.5716 0.064*
C3 0.2838 (12) −0.0653 (16) 0.4690 (5) 0.062 (2)
H3 0.3473 −0.1938 0.4635 0.075*
C4 0.2043 (11) 0.0586 (15) 0.4116 (4) 0.053 (2)
H4 0.2133 0.0114 0.3677 0.064*
C5 0.1125 (10) 0.2507 (14) 0.4203 (4) 0.0447 (19)
C6 0.0282 (12) 0.3915 (15) 0.3622 (4) 0.059 (2)
H6A 0.0500 0.3291 0.3200 0.088*
H6B 0.0741 0.5414 0.3678 0.088*
H6C −0.0945 0.3955 0.3610 0.088*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
W1 0.0371 (2) 0.0225 (2) 0.0303 (2) 0.000 0.00409 (16) 0.000
Ag1 0.0704 (6) 0.0280 (4) 0.0565 (5) 0.000 0.0061 (5) 0.000
Se1 0.0412 (4) 0.0389 (4) 0.0425 (4) −0.0057 (3) 0.0020 (3) 0.0049 (3)
Se2 0.0587 (5) 0.0342 (4) 0.0377 (4) −0.0027 (4) 0.0101 (4) 0.0051 (3)
N1 0.035 (3) 0.046 (4) 0.035 (3) −0.005 (3) 0.004 (3) −0.005 (3)
C1 0.049 (5) 0.060 (5) 0.034 (4) −0.001 (4) 0.005 (4) −0.005 (4)
C2 0.056 (5) 0.039 (5) 0.064 (5) 0.005 (4) 0.010 (5) 0.010 (4)
C3 0.053 (5) 0.053 (6) 0.089 (7) 0.004 (5) 0.032 (5) −0.007 (5)
C4 0.052 (5) 0.059 (6) 0.051 (5) −0.009 (5) 0.016 (4) −0.015 (4)
C5 0.040 (4) 0.054 (5) 0.040 (4) −0.008 (4) 0.007 (3) −0.004 (4)
C6 0.062 (6) 0.078 (6) 0.033 (4) −0.006 (5) −0.001 (4) −0.008 (4)

Geometric parameters (Å, º)

W1—Se1 2.3347 (9) N1—H1N 0.8600
W1—Se1i 2.3347 (9) C1—C2 1.371 (10)
W1—Se2i 2.3379 (9) C1—H1 0.9300
W1—Se2 2.3379 (9) C2—C3 1.361 (12)
W1—Ag1 2.9723 (11) C2—H2 0.9300
W1—Ag1ii 2.9725 (11) C3—C4 1.400 (12)
Ag1—Se1iii 2.6224 (11) C3—H3 0.9300
Ag1—Se1iv 2.6224 (11) C4—C5 1.380 (11)
Ag1—Se2 2.6210 (10) C4—H4 0.9300
Ag1—Se2i 2.6210 (10) C5—C6 1.475 (11)
Ag1—W1iv 2.9725 (11) C6—H6A 0.9600
N1—C1 1.330 (9) C6—H6B 0.9600
N1—C5 1.376 (9) C6—H6C 0.9600
Se1—W1—Se1i 115.47 (5) Se1iv—Ag1—W1iv 48.84 (2)
Se1—W1—Se2i 106.92 (3) W1—Ag1—W1iv 180.0
Se1i—W1—Se2i 106.25 (3) W1—Se1—Ag1ii 73.43 (3)
Se1—W1—Se2 106.25 (3) W1—Se2—Ag1 73.40 (3)
Se1i—W1—Se2 106.92 (3) C1—N1—C5 119.0 (6)
Se2i—W1—Se2 115.36 (4) C1—N1—H1N 120.5
Se1—W1—Ag1 122.27 (2) C5—N1—H1N 120.5
Se1i—W1—Ag1 122.27 (2) N1—C1—C2 123.5 (7)
Se2i—W1—Ag1 57.68 (2) N1—C1—H1 118.2
Se2—W1—Ag1 57.68 (2) C2—C1—H1 118.2
Se1—W1—Ag1ii 57.73 (2) C3—C2—C1 118.5 (8)
Se1i—W1—Ag1ii 57.73 (2) C3—C2—H2 120.7
Se2i—W1—Ag1ii 122.32 (2) C1—C2—H2 120.7
Se2—W1—Ag1ii 122.32 (2) C2—C3—C4 119.4 (8)
Ag1—W1—Ag1ii 180.000 (1) C2—C3—H3 120.3
Se2—Ag1—Se2i 97.84 (4) C4—C3—H3 120.3
Se2—Ag1—Se1iii 115.91 (3) C5—C4—C3 119.8 (7)
Se2i—Ag1—Se1iii 115.35 (3) C5—C4—H4 120.1
Se2—Ag1—Se1iv 115.35 (3) C3—C4—H4 120.1
Se2i—Ag1—Se1iv 115.91 (3) N1—C5—C4 119.7 (7)
Se1iii—Ag1—Se1iv 97.67 (5) N1—C5—C6 117.6 (7)
Se2—Ag1—W1 48.92 (2) C4—C5—C6 122.7 (7)
Se2i—Ag1—W1 48.92 (2) C5—C6—H6A 109.5
Se1iii—Ag1—W1 131.16 (2) C5—C6—H6B 109.5
Se1iv—Ag1—W1 131.16 (2) H6A—C6—H6B 109.5
Se2—Ag1—W1iv 131.08 (2) C5—C6—H6C 109.5
Se2i—Ag1—W1iv 131.08 (2) H6A—C6—H6C 109.5
Se1iii—Ag1—W1iv 48.84 (2) H6B—C6—H6C 109.5

Symmetry codes: (i) −x+1, y, −z+3/2; (ii) x, y−1, z; (iii) −x+1, y+1, −z+3/2; (iv) x, y+1, z.

Hydrogen-bond geometry (Å, º)

D—H···A D—H H···A D···A D—H···A
N1—H1N···N1v 0.86 1.93 2.786 (12) 172
C1—H1···Se1 0.93 2.96 3.732 (8) 141
C4—H4···Se1vi 0.93 2.90 3.832 (8) 176

Symmetry codes: (v) −x, −y+1, −z+1; (vi) x, −y, z−1/2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: XU5746).

References

  1. Bruker (2001). SADABS Bruker AXS Inc., Madison, Wisconsin, USA.
  2. Bruker (2007). APEX2 and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
  3. Dai, J.-X., Zhang, Q.-F., Song, Y., Wong, W.-Y., Rothenberger, A. & Leung, W.-H. (2007). Polyhedron, 26, 3182–3188.
  4. Huang, Q., Wu, X.-T. & Lu, J.-X. (1997). Chem. Commun. pp. 703–704.
  5. Lang, J.-P., Li, J.-G., Bao, S.-A. & Xin, X.-Q. (1993). Polyhedron, 12, 801–806.
  6. Müller, A., Jaegermann, W. & Hellmann, W. (1983). J. Mol. Struct. 100, 559–570.
  7. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  8. Yu, H., Zhang, W.-J., Wu, X.-T., Sheng, T.-L., Wang, Q.-M. & Lin, P. (1998). Angew. Chem. Int. Ed. 37, 2520–2522. [DOI] [PubMed]
  9. Zhang, Q.-F., Ding, J., Yu, Z., Song, Y., Rothenberger, A., Fenske, D. & Leung, W.-H. (2006). Inorg. Chem. 45, 8638–8647. [DOI] [PubMed]
  10. Zhang, Q.-F., Leung, W.-H. & Xin, X.-Q. (2002). Coord. Chem. Rev. 224, 35–49.
  11. Zhang, Q.-F., Leung, W.-H., Xin, X.-Q. & Fun, H.-F. (2000). Inorg. Chem. 39, 417–426. [DOI] [PubMed]

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablock(s) I, global. DOI: 10.1107/S1600536813028213/xu5746sup1.cif

e-69-0m608-sup1.cif (18.4KB, cif)

Structure factors: contains datablock(s) I. DOI: 10.1107/S1600536813028213/xu5746Isup2.hkl

e-69-0m608-Isup2.hkl (100.9KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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