supplementary materials


Acta Cryst. (2007). E63, m2548    [ doi:10.1107/S1600536807044431 ]

Bis(cyanido-[kappa]C)(ethane-1,2-diamine-[kappa]2N,N')silver(II)

S. Ahmad, M. Monim-ul-Mehboob, M. Hanif, M. Altaf and H. Stoeckli-Evans

Abstract top

The title compound, [Ag(CN)2(C2H8N2)], was obtained from the reaction of ethane-1,2-diamine (en) with K[Ag(CN)2]. The compound crystallizes as an inversion twin, the ratio of the twin components being 0.72 (4):0.28 (4). The AgII atom is in a slightly disorted square-planar environment. The chelate ring has an envelope conformation. The AgII-N(en) bond lengths are 2.071 (2) and 2.078 (2) Å. In the crystal structure, symmetry-related molecules are linked by N-H...N hydrogen bonds to form a three-dimensional network.

Comment top

The molecular stucture of the title compound is shown in Fig. 1. The compound crystallized in the chiral space group P212121 as an inversion twin; the refined BASF value is 0.28 (4).

The AgII atom has an almost perfect square planar environement (Table 1). The five-membered chelate ring has an envelope conformation with atom C1 at the flap.

The AgII—N(en) bond distances of 2.071 (2) and 2.078 (2) Å are significantly shorter than the same distances observed in some silver(II) 1,4,8,11-tetramethyl-1,4,8,11-tetraazacyclotetradecane macrocyclic complexes; 2.185 (5) to 2.195 (6) Å (Wang et al., 2002) and 2.194 (3) to 2.196 (3) Å (Po et al., 1991). In the corresponding silver(I) complex, [Ag(CN)en)], prepared solvothermally, the AgI—N(en) distances are 2.283 (6) and 2.355 (6) Å (Pretsch & Hartl, 2005).

In the crystal structure symmetry related molecules are linked by N—H···N(CN) hydrogen bonds to form a three-dimensional network (Fig. 2).

Related literature top

For related literature, see: Pretsch & Hartl (2005); Wang et al. (2002); Po et al. (1991).

Experimental top

The title compound was prepared by the addition of ethane-1,2-diamine in methanol to an equimolar amount of K[Ag(CN)2] in water. The solution was stirred for 15 min then filtered and allowed to evaporate slowly in air. Colourless crystals appeared along with some black deposits on the walls of the vessel, which suggested disproportionation of silver(I) to give silver(II) and silver(0).

Refinement top

The H-atoms were included in calculated positions and treated as riding atoms: N—H = 0.92 Å and C—H = 0.99 Å, with Uiso(H) = 1.2Ueq(N or C).

Computing details top

Data collection: X-AREA (Stoe & Cie, 2005); cell refinement: X-AREA (Stoe & Cie, 2005); data reduction: X-RED32 (Stoe & Cie, 2005); program(s) used to solve structure: SHELXS97 (Sheldrick, 1997); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: PLATON (Spek, 2003); software used to prepare material for publication: SHELXL97 (Sheldrick, 1997).

Figures top
[Figure 1] Fig. 1. The molecular sturcture showing the atomic numbering scheme and displacement parameters drawn at the 50% probabilty level.
[Figure 2] Fig. 2. The crystal packing viewed along the c axis. Intermolecular N—H···N hydrogen bonds are shown as dotted lines.
Bis(cyanido-κC)(ethane-1,2-diamine-κ2N,N')silver(II) top
Crystal data top
[Ag(CN)2(C2H8N2)]F000 = 428
Mr = 220.01Dx = 2.050 Mg m3
Orthorhombic, P212121Mo Kα radiation
λ = 0.71073 Å
Hall symbol: P 2ac 2abCell parameters from 6960 reflections
a = 6.9140 (8) Åθ = 1.8–28.7º
b = 9.3481 (11) ŵ = 2.74 mm1
c = 11.0289 (11) ÅT = 173 (2) K
V = 712.83 (14) Å3Needle, colourless
Z = 40.50 × 0.20 × 0.10 mm
Data collection top
Stoe IPDS II
diffractometer
1913 independent reflections
Radiation source: fine-focus sealed tube1889 reflections with I > 2σ(I)
Monochromator: graphiteRint = 0.022
T = 173(2) Kθmax = 29.1º
φ and ω scansθmin = 2.9º
Absorption correction: multi-scan
(MULABS in PLATON; Spek, 2003)
h = 9→9
Tmin = 0.539, Tmax = 0.760k = 12→12
6842 measured reflectionsl = 14→15
Refinement top
Refinement on F2H-atom parameters constrained
Least-squares matrix: full  w = 1/[σ2(Fo2) + (0.0247P)2 + 0.4752P]
where P = (Fo2 + 2Fc2)/3
R[F2 > 2σ(F2)] = 0.016(Δ/σ)max = 0.001
wR(F2) = 0.042Δρmax = 0.46 e Å3
S = 1.08Δρmin = 0.51 e Å3
1913 reflectionsExtinction correction: SHELXL 97 (Sheldrick, 1997), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
84 parametersExtinction coefficient: 0.0269 (10)
Primary atom site location: structure-invariant direct methodsAbsolute structure: Flack (1983), with 784 Friedel pairs (99.7%)
Secondary atom site location: difference Fourier mapFlack parameter: 0.28 (4)
Hydrogen site location: inferred from neighbouring sites
Crystal data top
[Ag(CN)2(C2H8N2)]V = 712.83 (14) Å3
Mr = 220.01Z = 4
Orthorhombic, P212121Mo Kα
a = 6.9140 (8) ŵ = 2.74 mm1
b = 9.3481 (11) ÅT = 173 (2) K
c = 11.0289 (11) Å0.50 × 0.20 × 0.10 mm
Data collection top
Stoe IPDS II
diffractometer
1913 independent reflections
Absorption correction: multi-scan
(MULABS in PLATON; Spek, 2003)
1889 reflections with I > 2σ(I)
Tmin = 0.539, Tmax = 0.760Rint = 0.022
6842 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.016H-atom parameters constrained
wR(F2) = 0.042Δρmax = 0.46 e Å3
S = 1.08Δρmin = 0.51 e Å3
1913 reflectionsAbsolute structure: Flack (1983), with 784 Friedel pairs (99.7%)
84 parametersFlack parameter: 0.28 (4)
Special details top

Geometry. Bond distances, angles etc. have been calculated using the rounded fractional coordinates. All su's are estimated from the variances of the (full) variance-covariance matrix. The cell e.s.d.'s are taken into account in the estimation of distances, angles and torsion angles

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
Ag10.31636 (2)0.86283 (2)0.26335 (1)0.0170 (1)
N10.1329 (3)0.7590 (2)0.3838 (2)0.0200 (6)
N20.1723 (3)0.7398 (2)0.13599 (18)0.0198 (5)
N30.5059 (3)1.0508 (2)0.4625 (2)0.0265 (6)
N40.5486 (4)1.0323 (3)0.0698 (2)0.0269 (6)
C10.0334 (4)0.7046 (3)0.3122 (2)0.0247 (6)
C20.0448 (4)0.6364 (3)0.1993 (2)0.0268 (6)
C30.4387 (4)0.9800 (2)0.3892 (2)0.0196 (6)
C40.4706 (4)0.9651 (3)0.1414 (2)0.0204 (6)
H1NA0.196500.684500.421000.0240*
H1A0.121300.784400.290800.0300*
H1B0.107100.633600.360100.0300*
H1NB0.090800.821500.442500.0240*
H2A0.119100.549400.220700.0320*
H2B0.063100.608000.145500.0320*
H2NA0.099700.797700.086300.0240*
H2NB0.260300.691300.088800.0240*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Ag10.0170 (1)0.0154 (1)0.0187 (1)0.0005 (1)0.0004 (1)0.0002 (1)
N10.0218 (10)0.0187 (9)0.0195 (10)0.0020 (7)0.0021 (7)0.0031 (8)
N20.0204 (9)0.0184 (9)0.0207 (9)0.0039 (9)0.0009 (9)0.0017 (7)
N30.0250 (11)0.0283 (11)0.0261 (11)0.0039 (8)0.0002 (8)0.0037 (9)
N40.0252 (10)0.0304 (11)0.0252 (11)0.0051 (10)0.0005 (9)0.0003 (9)
C10.0223 (10)0.0255 (11)0.0264 (12)0.0071 (9)0.0016 (9)0.0010 (10)
C20.0318 (11)0.0209 (9)0.0278 (11)0.0119 (11)0.0012 (10)0.0019 (11)
C30.0182 (10)0.0195 (10)0.0210 (11)0.0009 (9)0.0016 (9)0.0028 (9)
C40.0173 (10)0.0228 (10)0.0212 (11)0.0023 (9)0.0005 (9)0.0006 (9)
Geometric parameters (Å, °) top
Ag1—N12.078 (2)N1—H1NB0.9200
Ag1—N22.071 (2)N2—H2NA0.9200
Ag1—C31.960 (2)N2—H2NB0.9200
Ag1—C41.965 (3)C1—C21.500 (3)
N1—C11.485 (3)C1—H1A0.9900
N2—C21.483 (3)C1—H1B0.9900
N3—C31.143 (3)C2—H2A0.9900
N4—C41.144 (4)C2—H2B0.9900
N1—H1NA0.9200
N1—Ag1—N283.14 (8)C2—N2—H2NA110.00
N1—Ag1—C394.12 (9)C2—N2—H2NB110.00
N1—Ag1—C4175.20 (10)N1—C1—C2107.9 (2)
N2—Ag1—C3176.69 (10)N2—C2—C1109.2 (2)
N2—Ag1—C493.84 (9)Ag1—C3—N3178.2 (2)
C3—Ag1—C488.78 (10)Ag1—C4—N4174.6 (3)
Ag1—N1—C1107.03 (15)N1—C1—H1A110.00
Ag1—N2—C2109.18 (14)N1—C1—H1B110.00
C1—N1—H1NB110.00C2—C1—H1A110.00
H1NA—N1—H1NB109.00C2—C1—H1B110.00
Ag1—N1—H1NB110.00H1A—C1—H1B108.00
C1—N1—H1NA110.00N2—C2—H2A110.00
Ag1—N1—H1NA110.00N2—C2—H2B110.00
Ag1—N2—H2NA110.00C1—C2—H2A110.00
Ag1—N2—H2NB110.00C1—C2—H2B110.00
H2NA—N2—H2NB108.00H2A—C2—H2B108.00
N2—Ag1—N1—C120.61 (15)Ag1—N1—C1—C245.1 (2)
C3—Ag1—N1—C1157.53 (16)Ag1—N2—C2—C134.7 (2)
N1—Ag1—N2—C27.65 (16)N1—C1—C2—N253.5 (3)
C4—Ag1—N2—C2176.10 (17)
Hydrogen-bond geometry (Å, °) top
D—H···AD—HH···AD···AD—H···A
N1—H1NA···N4i0.922.273.099 (3)150
N1—H1NB···N4ii0.922.183.097 (3)172
N2—H2NA···N3iii0.922.103.002 (3)167
N2—H2NB···N3i0.922.163.042 (3)161
Symmetry codes: (i) −x+1, y−1/2, −z+1/2; (ii) −x+1/2, −y+2, z+1/2; (iii) −x+1/2, −y+2, z−1/2.
Table 1
Selected geometric parameters (Å, °)
top
Ag1—N12.078 (2)Ag1—C31.960 (2)
Ag1—N22.071 (2)Ag1—C41.965 (3)
N1—Ag1—N283.14 (8)N2—Ag1—C493.84 (9)
N1—Ag1—C394.12 (9)C3—Ag1—C488.78 (10)
N1—Ag1—C4175.20 (10)Ag1—N1—C1107.03 (15)
N2—Ag1—C3176.69 (10)Ag1—N2—C2109.18 (14)
Table 2
Hydrogen-bond geometry (Å, °)
top
D—H···AD—HH···AD···AD—H···A
N1—H1NA···N4i0.922.273.099 (3)150
N1—H1NB···N4ii0.922.183.097 (3)172
N2—H2NA···N3iii0.922.103.002 (3)167
N2—H2NB···N3i0.922.163.042 (3)161
Symmetry codes: (i) −x+1, y−1/2, −z+1/2; (ii) −x+1/2, −y+2, z+1/2; (iii) −x+1/2, −y+2, z−1/2.
Acknowledgements top

Financial support from the Pakistan Council for Science and Technology, Islamabad, is gratefully acknowledged.

references
References top

Flack, H. D. (1983). Acta Cryst. A39, 876–881.

Po, H. N., Brinkman, E. & Doedens, R. J. (1991). Acta Cryst. C47, 2310–2312.

Pretsch, T. & Hartl, H. (2005). Inorg. Chim. Acta, 358, 1179–1185.

Sheldrick, G. M. (1997). SHELXS97 and SHELXL97. University of Göttingen, Germany.

Spek, A. L. (2003). J. Appl. Cryst. 36, 7–13.

Stoe & Cie. (2005). X-AREA (Version 1.26) and X-RED32 (Version 1.26). Stoe & Cie, Darmstadt, Germany.

Wang, Q.-M., Kay Lee, H. & Mak, T. C. W. (2002). New J. Chem. 26, 513–515.