metal-organic compounds
Figure 3
A perspective view of the three-dimensional supramolecular framework
of (I), showing intersheet hydrogen bonds and Agꢁ ꢁ ꢁO, Agꢁ ꢁ ꢁN and ꢀ–ꢀ
interactions as dashed lines. (In the electronic version of the paper, these
dashed lines are green, blue, purple and red, respectively.)
[symmetry code: (v) x ꢀ 1, y, z]. The intersheet distance is ca
˚
3.3 A, which is comparable with those of graphite and Ag6-
(benzene-1,3,5-tricarboxylic acid)2(2-aminopyrazine)6 (Sun,
Luo, Xu et al. 2009), and is a result of the fact that there are no
axial ligands perpendicular to the two-dimensional sheets.
The shortest centroid–centroid distance between parallel
Figure 2
˚
benzene rings of the anbz ligands is 3.8523 (9) A, with a large
A perspective view of the two-dimensional supramolecular sheet of (I),
incorporating intra- and intermolecular N—Hꢁ ꢁ ꢁO hydrogen bonds
(dashed lines).
˚
slippage of 2.065 A, which suggests the existence of weak
offset face-to-face ꢀ–ꢀ stacking interactions. These combine
with the inter-sheet ammine–nitro N—Hꢁ ꢁ ꢁO [mean Nꢁ ꢁ ꢁO
˚
distance = 3.131 (2) A] hydrogen bonds and Agꢁ ꢁ ꢁOnitro and
ion (Ag1) adopts a linear coordination environment, coordi-
nated by two symmetry-related ammonia molecules to form
the [Ag(NH3)2]+ cation. The Ag1—N3 bond length is
Agꢁ ꢁ ꢁNamino interactions to stabilize the resultant three-
dimensional supramolecular framework (Fig. 3).
˚
2.1193 (16) A, which is comparable with the corresponding
values observed in another silver(I)–ammonia complex (You
& Zhu, 2004). The other AgI ion (Ag2) is located in a rare
four-coordination planar environment (only ꢂ2% of all
reported silver complexes possess this stereochemistry (Young
& Hanton, 2008), which is completed by two chelating inver-
sion-related anbz ligands. This geometry is not a perfect
square-planar arrangement, but is distorted due to the acute
bite angle [53.02 (4)ꢃ] and differing Ag—O bond lengths
(Table 1), both of which are imposed by the asymmetrically
chelated ring.
Experimental
All reagents and solvents were obtained commercially and used
without further purification. A mixture of Ag2O (116 mg, 0.5 mmol)
and H2anbz (182 mg, 1 mmol) was stirred in a methanol–H2O mixed
solvent (10 ml, 1:1 v/v). An aqueous NH3 solution (25%, 0.5 ml) was
then added dropwise to the mixture to give a clear solution under
ultrasonic treatment. The resulting solution was allowed to evaporate
slowly in the dark at room temperature for several days to give
colourless crystals of (I), which were washed with a small volume of
cold ethanol and diethyl ether (yield 61%, based on Ag2O). Analysis
calculated for C14H16Ag2N6O8: C 27.47, H 2.63, N 13.73%; found:
C 27.51, H 2.59, N 13.64%.
There are abundant weak interactions around Ag1 and
i
˚
Ag2. Ag1ꢁ ꢁ ꢁO2 and Ag1ꢁ ꢁ ꢁN1 [3.1195 (15) and 3.1885 (16) A,
respectively; symmetry code: (i) x + 1, y, z ꢀ 1] are slightly
Crystal data
shorter than the sums of the van der Waals radii of Ag and O
[Ag(NH3)2][Ag(C7H5N2O4)2]
Mr = 612.07
Triclinic, P1
ꢃ = 62.077 (8)ꢃ
3
˚
˚
(3.24 A) and Ag and N (3.27 A) (Bondi, 1964). The
Ag2ꢁ ꢁ ꢁO2ii interaction [symmetry code: (ii) ꢀx + 2, ꢀy + 1,
ꢀz + 1] is along the axial direction above and below the AgO4
plane. A possible reason for the four-coordinate planar
geometry may be the steric shielding of axial sites by the nitro
groups (Reger et al., 2004).
˚
V = 456.86 (6) A
Z = 1
˚
˚
a = 7.1361 (5) A
Mo Kꢁ radiation
ꢄ = 2.20 mmꢀ1
T = 173 K
0.10 ꢄ 0.10 ꢄ 0.08 mm
b = 7.4070 (6) A
˚
c = 9.9686 (6) A
ꢁ = 87.064 (6)ꢃ
ꢂ = 79.170 (6)ꢃ
The anionic and cationic parts of (I) interact with each other
to form a one-dimensional zigzag chain through weak
Agꢁ ꢁ ꢁOnitro interactions, alternating with interionic N3—
H3Bꢁ ꢁ ꢁO1 hydrogen bonds (Table 2) to give a C22(6) chain-like
motif (Bernstein et al., 1995). Additionally, intra-anion N1—
H1Cꢁ ꢁ ꢁO4 hydrogen bonds, showing an S(6) motif, consoli-
date the one-dimensional chains, which are further linked into
a slightly undulating two-dimensional supramolecular sheet
(Fig. 2) via intermolecular N1—H1Bꢁ ꢁ ꢁO3v hydrogen bonds
Data collection
Oxford Xcalibur diffractometer
with a Sapphire3 Gemini Ultra
detector
Absorption correction: multi-scan
[CrysAlis Pro (Oxford
Diffraction, 2009); empirical
(using intensity measurements)
absorption correction using
spherical harmonics, imple-
mented in SCALE3 ABSPACK
scaling algorithm]
Tmin = 0.810, Tmax = 0.843
3721 measured reflections
1800 independent reflections
1627 reflections with I > 2ꢅ(I)
Rint = 0.014
ꢅ
Acta Cryst. (2010). C66, m174–m176
Sun et al.
[Ag(NH3)2][Ag(C7H5N2O4)2] m175