supplementary materials


pv2240 scheme

Acta Cryst. (2009). E65, m1703    [ doi:10.1107/S1600536809050491 ]

catena-Poly[[bis[(dicyanamido)silver(I)](Ag-Ag)]-[mu]2-4,4'-bipyridine-[kappa]2N:N']

J. Zhang

Abstract top

In the title compound, [Ag2(C2N3)2(C10H8N2)]n, the Ag atoms, lying on inversion centers, are separated by 3.3226 (12) Å. Each Ag atom is connected by one bridging 4,4'-bipyridine [Ag-N = 2.177 (4)Å] and a terminal dicyanamide [Ag-N = 2.108 (4) Å]. The Ag-Ag interactions play a key role in constructing a unique neutral polymeric chain.

Comment top

The designed syntheses of metal-organic compounds have attracted great attention in recent years because of not only their intriguing structures (Eddaoudi et al., 2001; Zhang et al., 2008) but also their potential applications.(Banerjee et al., 2008; Zhang et al., 2007). The flexible and rigid bridging ligands can play different roles in constructing metal-organic frameworks. The tilte compound, (I), was constructed by employing a flexible, dicyanamide, and a rigid, 4,4'-bipyridine ligand through diffusion reactions. In this paper, the crystal structure of (I) is presented.

As illustrated in Fig. 1, 4,4'-bipyridine acts as a bridgeing ligand to connect two Ag atoms. Dicyanamide usually acts as a briding ligand to construct metal-organic compounds (Zhang et al., 2009a,b). However, in the tilte compound, it is linked to only one Ag atom. Ag—Ag bonds [3.3226 (12) Å] play a key role in constructing a unique one-dimensional neutral chain.

Related literature top

For the designed syntheses of metal-organic compounds, see: Eddaoudi et al. (2001); Zhang et al. (2008, 2009a,b). For their applications, see: Banerjee et al. (2008); Zhang et al. (2007).

Experimental top

Ag(NO3) (68.0 mg, 0.4 mmol) and NaN(CN)2 (178.2 mg, 2 mmol) were added into 3 ml dimethylformamide with thorough stirring for 5 minutes. After filtration, the colorless filtrate was carefully laid on the surface of a solution of 4,4'-bipyridine (78.0 mg, 0.5 mmol) in 8 ml i-PrOH. Colorless prismatic crystals were obtained after five days.

Refinement top

H atoms were positioned geometrically and refined with riding model, with Uiso = 1.2Ueq for pyridyl H atoms, the C—H bonds are 0.93 Å in pyridyl.

Computing details top

Data collection: CrystalClear (Rigaku, 2008); cell refinement: CrystalClear (Rigaku, 2008); data reduction: CrystalClear (Rigaku, 2008); program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: SHELXTL (Sheldrick, 2008); software used to prepare material for publication: SHELXTL (Sheldrick, 2008).

Figures top
[Figure 1] Fig. 1. The molecular structure of the title compound, with atom labels and 30% probability displacement ellipsoids; H atoms have been omitted for clarity. Symmetry code: i = -x+2, -y+1, -z+1.
catena-Poly[[bis[(dicyanamido)silver(I)](AgAg)]-µ2- 4,4'-bipyridine-κ2N:N'] top
Crystal data top
[Ag2(C2N3)2(C10H8N2)]Z = 2
Mr = 252.01F(000) = 242
Triclinic, P1Dx = 2.232 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 6.1867 (12) ÅCell parameters from 1687 reflections
b = 7.8344 (16) Åθ = 2.6–28.7°
c = 7.9649 (16) ŵ = 2.63 mm1
α = 88.83 (3)°T = 293 K
β = 84.09 (3)°Prism, colorless
γ = 77.54 (3)°0.2 × 0.16 × 0.12 mm
V = 374.95 (13) Å3
Data collection top
Rigaku Saturn724+
diffractometer
1358 independent reflections
Radiation source: fine-focus sealed tube1315 reflections with I > 2σ(I)
graphiteRint = 0.022
dtprofit.ref scansθmax = 25.5°, θmin = 2.6°
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
h = 77
Tmin = 0.407, Tmax = 0.664k = 69
2474 measured reflectionsl = 99
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.033H-atom parameters constrained
wR(F2) = 0.103 w = 1/[σ2(Fo2) + (0.0601P)2 + 0.1547P]
where P = (Fo2 + 2Fc2)/3
S = 1.24(Δ/σ)max < 0.001
1358 reflectionsΔρmax = 0.67 e Å3
110 parametersΔρmin = 0.70 e Å3
0 restraintsExtinction correction: SHELXL97 (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.055 (7)
Crystal data top
[Ag2(C2N3)2(C10H8N2)]γ = 77.54 (3)°
Mr = 252.01V = 374.95 (13) Å3
Triclinic, P1Z = 2
a = 6.1867 (12) ÅMo Kα radiation
b = 7.8344 (16) ŵ = 2.63 mm1
c = 7.9649 (16) ÅT = 293 K
α = 88.83 (3)°0.2 × 0.16 × 0.12 mm
β = 84.09 (3)°
Data collection top
Rigaku Saturn724+
diffractometer
1315 reflections with I > 2σ(I)
Absorption correction: multi-scan
(SADABS; Sheldrick, 1996)
Rint = 0.022
Tmin = 0.407, Tmax = 0.664θmax = 25.5°
2474 measured reflectionsStandard reflections: 0
1358 independent reflections
Refinement top
R[F2 > 2σ(F2)] = 0.033H-atom parameters constrained
wR(F2) = 0.103Δρmax = 0.67 e Å3
S = 1.24Δρmin = 0.70 e Å3
1358 reflectionsAbsolute structure: ?
110 parametersFlack parameter: ?
0 restraintsRogers parameter: ?
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
xyzUiso*/Ueq
Ag10.83031 (5)0.39268 (4)0.61182 (3)0.0570 (3)
N10.6869 (7)0.6445 (6)0.3950 (4)0.0626 (10)
N20.7664 (7)0.5131 (6)0.1486 (5)0.0544 (9)
N30.6751 (7)0.7081 (5)0.0944 (5)0.0518 (9)
N40.8957 (6)0.2168 (4)0.3957 (4)0.0432 (8)
C10.6855 (6)0.6651 (5)0.2524 (5)0.0428 (8)
C20.7278 (6)0.5953 (5)0.0277 (5)0.0416 (8)
C30.9785 (6)0.0426 (5)0.0830 (5)0.0367 (8)
C40.7354 (7)0.2209 (6)0.2947 (6)0.0521 (10)
H40.59330.28420.33010.063*
C50.7682 (7)0.1371 (6)0.1417 (6)0.0511 (10)
H50.64970.14340.07720.061*
C61.0962 (7)0.1231 (5)0.3420 (5)0.0447 (9)
H61.21100.11750.41000.054*
C71.1423 (6)0.0341 (5)0.1914 (5)0.0431 (8)
H71.28440.03240.16170.052*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Ag10.0661 (4)0.0685 (3)0.0347 (3)0.0119 (2)0.00158 (18)0.02256 (18)
N10.084 (3)0.067 (2)0.033 (2)0.008 (2)0.0024 (19)0.0116 (16)
N20.064 (2)0.064 (2)0.0322 (19)0.0080 (18)0.0025 (16)0.0155 (16)
N30.067 (2)0.0520 (19)0.0328 (19)0.0039 (16)0.0054 (16)0.0089 (14)
N40.0522 (19)0.0447 (17)0.0315 (17)0.0072 (14)0.0042 (14)0.0108 (13)
C10.046 (2)0.0467 (19)0.035 (2)0.0082 (15)0.0020 (16)0.0148 (15)
C20.0421 (19)0.051 (2)0.0298 (19)0.0065 (15)0.0029 (15)0.0036 (16)
C30.0445 (19)0.0327 (16)0.0321 (19)0.0068 (14)0.0026 (15)0.0023 (14)
C40.043 (2)0.060 (2)0.047 (2)0.0017 (17)0.0021 (18)0.0214 (19)
C50.043 (2)0.061 (2)0.045 (2)0.0015 (17)0.0080 (17)0.0224 (19)
C60.049 (2)0.049 (2)0.035 (2)0.0064 (16)0.0091 (17)0.0074 (16)
C70.0411 (19)0.046 (2)0.038 (2)0.0005 (15)0.0065 (16)0.0082 (15)
Geometric parameters (Å, °) top
Ag1—N2i2.108 (4)N4—C41.334 (6)
Ag1—N42.177 (4)C3—C71.387 (6)
Ag1—N12.661 (4)C3—C51.390 (6)
Ag1—Ag1ii3.3226 (12)C3—C3iv1.467 (8)
N1—C11.144 (5)C4—C51.372 (6)
N2—C21.145 (6)C4—H40.9300
N2—Ag1iii2.108 (4)C5—H50.9300
N3—C21.296 (6)C6—C71.373 (6)
N3—C11.301 (6)C6—H60.9300
N4—C61.331 (5)C7—H70.9300
N2i—Ag1—N4167.60 (15)C7—C3—C3iv122.8 (4)
N2i—Ag1—N1105.43 (14)C5—C3—C3iv121.4 (4)
N4—Ag1—N186.07 (12)N4—C4—C5123.8 (4)
N2i—Ag1—Ag1ii105.25 (12)N4—C4—H4118.1
N4—Ag1—Ag1ii84.71 (10)C5—C4—H4118.1
N1—Ag1—Ag1ii57.43 (10)C4—C5—C3120.0 (4)
C1—N1—Ag1139.3 (4)C4—C5—H5120.0
C2—N2—Ag1iii172.6 (4)C3—C5—H5120.0
C2—N3—C1123.1 (4)N4—C6—C7123.4 (4)
C6—N4—C4116.4 (4)N4—C6—H6118.3
C6—N4—Ag1123.9 (3)C7—C6—H6118.3
C4—N4—Ag1118.8 (3)C6—C7—C3120.5 (4)
N1—C1—N3173.2 (5)C6—C7—H7119.7
N2—C2—N3171.4 (4)C3—C7—H7119.7
C7—C3—C5115.8 (4)
Symmetry codes: (i) x, y, z+1; (ii) −x+2, −y+1, −z+1; (iii) x, y, z−1; (iv) −x+2, −y, −z.
Acknowledgements top

This work was supported by the Foundation of Jiangsu University (08JDG036).

references
References top

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