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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2009 Feb 11;65(Pt 3):m265–m266. doi: 10.1107/S1600536809004176

Bis(1,3-benzothia­zol-2-amine-κN 3)silver(I) nitrate acetone solvate

Christoph E Strasser a, Leigh-Anne de Jongh a, Stephanie Cronje a,*, Helgard G Raubenheimer a
PMCID: PMC2968676  PMID: 21582055

Abstract

In the title compound, [Ag(C7H6N2S)2]NO3·C3H6O, the AgI ion is coordinated to two benzothia­zol-2-amine ligands via the thia­zole N atoms in an approximately linear arrangement. The dihedral angle between the mean planes of the two 1,3-benzothia­zole groups is 5.9 (3)°. Both amine groups on the ligands are oriented in the same direction and are engaged in N—H⋯O hydrogen bonding with the nitrate counter-anion, forming one-dimensional columns along the b-axis direction. Voids created by inefficient crystal packing are occupied by acetone solvent mol­ecules which are disordered over two sites with occupancies of 0.563 (11) and 0.437 (11).

Related literature

For general background, see: de Jongh et al. (2008); Tewari et al. (1991). For related structures, see: Ellsworth et al. (2006); Fackler et al. (1992); Fitchett & Steel (2000); Hiraoka et al. (2003); Manzoni de Oliveira et al. (2007); Murthy & Murthy (1976); Zou et al. (2004).graphic file with name e-65-0m265-scheme1.jpg

Experimental

Crystal data

  • [Ag(C7H6N2S)2]NO3·C3H6O

  • M r = 528.35

  • Monoclinic, Inline graphic

  • a = 17.096 (4) Å

  • b = 5.8166 (12) Å

  • c = 20.421 (4) Å

  • β = 102.867 (3)°

  • V = 1979.8 (7) Å3

  • Z = 4

  • Mo Kα radiation

  • μ = 1.27 mm−1

  • T = 100 (2) K

  • 0.20 × 0.08 × 0.05 mm

Data collection

  • Bruker APEX CCD area-detector diffractometer

  • Absorption correction: multi-scan (SADABS; Bruker, 2002) T min = 0.786, T max = 0.940

  • 10935 measured reflections

  • 4046 independent reflections

  • 3594 reflections with I > 2σ(I)

  • R int = 0.029

Refinement

  • R[F 2 > 2σ(F 2)] = 0.056

  • wR(F 2) = 0.133

  • S = 1.12

  • 4046 reflections

  • 259 parameters

  • 12 restraints

  • H-atom parameters constrained

  • Δρmax = 1.91 e Å−3

  • Δρmin = −1.06 e Å−3

Data collection: SMART (Bruker, 2002); cell refinement: SAINT (Bruker, 2003); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008); molecular graphics: X-SEED (Atwood & Barbour, 2003; Barbour, 2001); software used to prepare material for publication: X-SEED.

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809004176/lh2768sup1.cif

e-65-0m265-sup1.cif (23KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809004176/lh2768Isup2.hkl

e-65-0m265-Isup2.hkl (198.4KB, hkl)

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

Table 1. Selected geometric parameters (Å, °).

Ag1—N13 2.130 (4)
Ag1—N23 2.127 (4)
N13—Ag1—N23 171.84 (17)

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

D—H⋯A D—H H⋯A DA D—H⋯A
N12—H2⋯O1 0.88 1.99 2.851 (6) 165
N12—H1⋯O2ii 0.88 2.07 2.889 (6) 155
N22—H3⋯O1 0.88 2.12 2.959 (7) 158
N22—H4⋯O1iii 0.88 2.11 2.955 (6) 162

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

Acknowledgments

We thank the National Research Foundation (NRF) of South Africa for financial support.

supplementary crystallographic information

Comment

The cation in the title compound (I) (Fig. 1) is crystallographically independent and consists of two benzothiazol-2-amine ligands coordinating to an AgI ion with their thiazole imine nitrogen atoms, thus furnishing an essentially linear geometry around the metal. This is in contrast to a postulation of amino-N coordination by Tewari et al. (1991) which was based on infrared evidence. However, hydrogen bonding may have interfered in the assignment of bands. Their conclusions that nitrate is not bonded to silver and the presence of Ag···S contacts have now been verified for the structure of (I).

The nitrate counter-anion in (I) does not interact with the metal which is reflected in the close to linear N—Ag—N angle of 171.84 (17)°. Similar molecular structures wherein the AgI ion is coordinated to two thiazole imine nitrogen atoms and interacts with nitrate, have markedly bent angles of 143.2 (2) and 146.1 (2)° (Fitchett & Steel, 2000), 136.05 (17) and 130.78 (15)° (Zou et al., 2004). Perchlorate shows the same effect with an angle of 144.3 (6)° (Murthy & Murthy, 1976). Essentially linear angles of 173.5 (2), 176.1 (2) and 176.8 (2)° are, however, observed in a trinuclear silver complex (Hiraoka et al., 2003) even though trifluoromethanesulfonate or methanol additionally coordinate to the silver atoms. The Ag—N bond lengths of 2.148 (6)–2.188 (6) Å in this complex are comparable to (I) [2.130 (4) and 2.127 (4) Å], as are the appropriate bond distances in the undisturbed (i.e. the Ag centre is only coordinated by thiazole ligands and the anion does not form part of the coordination sphere) silver perchlorate complexes of bis(benzothiazol-2-ylsulfanyl)methane and 1,4-bis(benzothiazol-2-ylsulfanyl)butane reported by Zou et al. (2004) [2.136 (4) and 2.147 (4) Å in the former and 2.136 (5) Å in the latter complex].

The planes of the two 1,3-benzothiazole groups in (I) lie at an angle of 5.9 (3)° which prevents crowding between H19 and H29 that would otherwise ensue in a flat cation. A short contact between Ag1 and S11i [3.2261 (15) Å, symmetry code: (i) = x, y + 1, z] can be observed which is shorter than the sum of the van der Waals radii of the concerned atoms. Such Ag···S interactions involving thiazole rings have been observed before with distances of 3.306 Å (Ellsworth et al., 2006), 3.336 Å (Fackler Jr et al., 1992), 3.204 Å (Manzoni de Oliveira et al., 2007) and 3.543 Å (Zou et al., 2004); except for the longer distance in the last example they are comparable to (I).

The nitrate counteranion plays a crucial role in governing the crystal structure of (I). The amino groups of the cations engage in hydrogen bonds to the nitrate anion and form polar one-dimensional hydrogen bonding domains ordered around the crystallographical 21 screw axes. The apolar 1,3-benzothiazole "ends" of different columns face each other as well as the co-crystallized acetone solvent molecules (Fig. 2). The hydrogen bonding network (Fig. 1) emanates from the two amino groups of the cation which chelate O1 of the nitrate anion as well as hydrogen bonding to two other nitrates, one from the same side of the chain (via O2, related by a translation in b) and one from the other side (via O1, related by a 21 screw operation). O1 accepts three hydrogen bonds and O2 is involved in a single hydrogen bond. O3 does not exhibit hydrogen bonding which might be a cause of its larger thermal ellipsoid due to less restriction in movement.

The only possible π···π-interaction between the heteroaromatic rings is found in the 1,3-benzothiazole containing S11 and its counterpart generated by a centre of inversion [symmetry code: (v) = –x+2, –y+1, –z] with centroid–centroid distances of 3.89 Å.

The acetone solvent is highly disordered and occupies two sites in a 0.56:0.44 ratio. The carbonyl groups roughly point in opposite directions. Additional electron density peaks around the solvent as well as very high Ueq values suggest a high mobility of the acetone molecule.

Experimental

The formation of crystalline (I) occurred during the reaction of [Au(NO3)(PPh3)] (0.20 g, 0.38 mmol) with benzothiazol-2-amine (57 mg, 0.38 mmol) in acetone solution (20 ml). It could be traced to the utilization of AgNO3 and [AuCl(PPh3)] in the preceding preparation of the gold reagent.

Refinement

To obtain a satisfactory geometry, the bond lengths in both orientations of the acetone molecule were restrained to target distances (C=O 1.2 Å and C—C 1.5 Å) and the molecules themselves restrained to be flat. The occupancies for the A and B orientation refined to 0.563 (11) and 0.437 (11), respectively.

All H atoms were positioned geometrically (C—H = 0.95, 0.99 and 0.98 Å for CH, CH2 and CH3 groups, respectively; N—H = 0.92 Å) and constrained to ride on their parent atoms; Uiso(H) values were set at 1.2 times Ueq(C,N) except for methyl groups where Uiso(H) was set at 1.5 times Ueq(C).

The largest residual electron density peak of 1.91 e Å-3 is located 0.68 Å from O4A of the acetone solvent molecule, the largest hole of –1.06 e Å-3 is located 0.54 Å from O4B.

Figures

Fig. 1.

Fig. 1.

The asymmetric unit of (I), ellipsoids are drawn at the 50% probability level; the disordered acetone molecule and hydrogen atoms not involved in hydrogen bonding are omitted. A part of the symmetry-related 1,3-benzothiazole moiety that forms the Ag1···S11i contact is shown as a stick model. Symmetry codes: (i) = x, y + 1, z; (ii) = x, y–1, z; (iii) = –x+3/2, y + 1/2, –z+1/2; (iv) = –x+3/2, y–1/2, –z+1/2.

Fig. 2.

Fig. 2.

Perspective view of the crystal structure along the b axis. Only hydrogen atoms involved in hydrogen bonding (represented by dotted lines) are shown.

Crystal data

[Ag(C7H6N2S)2]NO3·C3H6O F(000) = 1064
Mr = 528.35 Dx = 1.773 Mg m3
Monoclinic, P21/n Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2yn Cell parameters from 4102 reflections
a = 17.096 (4) Å θ = 2.4–26.4°
b = 5.8166 (12) Å µ = 1.26 mm1
c = 20.421 (4) Å T = 100 K
β = 102.867 (3)° Needle, colourless
V = 1979.8 (7) Å3 0.20 × 0.08 × 0.05 mm
Z = 4

Data collection

Bruker APEX CCD area-detector diffractometer 4046 independent reflections
Radiation source: fine-focus sealed tube 3594 reflections with I > 2σ(I)
graphite Rint = 0.029
ω scans θmax = 26.4°, θmin = 1.8°
Absorption correction: multi-scan (SADABS; Bruker, 2002) h = −16→21
Tmin = 0.786, Tmax = 0.940 k = −7→7
10935 measured reflections l = −22→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)] = 0.056 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.133 H-atom parameters constrained
S = 1.12 w = 1/[σ2(Fo2) + (0.0594P)2 + 10.016P] where P = (Fo2 + 2Fc2)/3
4046 reflections (Δ/σ)max = 0.001
259 parameters Δρmax = 1.91 e Å3
12 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 > 2σ(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.The acetone molecule is disordered around two positions with the C—O vectors pointing in roughly opposite directions. The bonds were restrained to target distances (1.2 Å for C═O and 1.5 Å for C—C) and the molecules were restrained to be flat. Due to the heavy disorder, anisotropic refinement of the molecule was not possible.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2)

x y z Uiso*/Ueq Occ. (<1)
Ag1 0.98098 (2) 0.87563 (7) 0.191835 (19) 0.02109 (14)
S11 0.98002 (9) 0.2069 (2) 0.06495 (7) 0.0230 (3)
S21 0.94328 (10) 1.5059 (3) 0.32405 (7) 0.0335 (4)
O1 0.7930 (2) 0.7687 (7) 0.1790 (2) 0.0320 (9)
O2 0.8171 (3) 0.9490 (8) 0.0933 (2) 0.0407 (11)
O3 0.7210 (3) 1.0619 (9) 0.1388 (3) 0.0458 (12)
N1 0.7758 (3) 0.9271 (8) 0.1357 (2) 0.0270 (10)
N12 0.8732 (3) 0.4138 (8) 0.1233 (2) 0.0254 (10)
H2 0.8564 0.5233 0.1465 0.031*
H1 0.8424 0.2944 0.1094 0.031*
N13 0.9956 (3) 0.5987 (7) 0.1274 (2) 0.0203 (9)
N22 0.8540 (3) 1.1387 (10) 0.2764 (3) 0.0407 (14)
H3 0.8445 1.0060 0.2554 0.049*
H4 0.8165 1.2039 0.2934 0.049*
N23 0.9844 (3) 1.1572 (8) 0.2589 (2) 0.0233 (10)
C12 0.9448 (3) 0.4289 (9) 0.1092 (2) 0.0211 (11)
C14 1.0663 (3) 0.5662 (9) 0.1040 (2) 0.0211 (11)
C15 1.0682 (3) 0.3592 (9) 0.0687 (2) 0.0211 (11)
C16 1.1336 (4) 0.3037 (10) 0.0417 (3) 0.0260 (12)
H16 1.1348 0.1632 0.0182 0.031*
C17 1.1968 (4) 0.4568 (10) 0.0498 (3) 0.0291 (12)
H17 1.2419 0.4215 0.0316 0.035*
C18 1.1949 (4) 0.6625 (10) 0.0843 (3) 0.0289 (12)
H18 1.2386 0.7664 0.0891 0.035*
C19 1.1302 (3) 0.7179 (9) 0.1119 (3) 0.0234 (11)
H19 1.1297 0.8578 0.1358 0.028*
C22 0.9244 (3) 1.2400 (10) 0.2824 (3) 0.0265 (12)
C24 1.0508 (3) 1.3024 (9) 0.2740 (3) 0.0225 (11)
C25 1.0396 (4) 1.5002 (10) 0.3098 (3) 0.0271 (12)
C26 1.1004 (4) 1.6632 (11) 0.3289 (3) 0.0367 (15)
H26 1.0922 1.7971 0.3532 0.044*
C27 1.1727 (4) 1.6241 (11) 0.3114 (3) 0.0412 (16)
H27 1.2151 1.7321 0.3239 0.049*
C28 1.1841 (4) 1.4289 (11) 0.2758 (3) 0.0349 (14)
H28 1.2344 1.4051 0.2643 0.042*
C29 1.1238 (3) 1.2679 (10) 0.2568 (3) 0.0257 (12)
H29 1.1324 1.1352 0.2322 0.031*
C1B 1.3701 (7) 0.437 (2) −0.0513 (6) 0.025 (3)* 0.437 (11)
H1B1 1.3823 0.2739 −0.0424 0.037* 0.437 (11)
H1B2 1.3935 0.4888 −0.0884 0.037* 0.437 (11)
H1B3 1.3118 0.4586 −0.0634 0.037* 0.437 (11)
C2B 1.4053 (8) 0.5766 (19) 0.0114 (6) 0.048 (4)* 0.437 (11)
C3B 1.3956 (8) 0.8295 (19) 0.0124 (7) 0.031 (3)* 0.437 (11)
H3B1 1.4224 0.8892 0.0566 0.046* 0.437 (11)
H3B2 1.3384 0.8679 0.0034 0.046* 0.437 (11)
H3B3 1.4196 0.8989 −0.0222 0.046* 0.437 (11)
O4B 1.4376 (8) 0.471 (2) 0.0598 (6) 0.065 (4)* 0.437 (11)
C1A 1.3839 (5) 0.3211 (14) −0.0243 (4) 0.015 (2)* 0.563 (11)
H1A1 1.3826 0.2663 −0.0699 0.022* 0.563 (11)
H1A2 1.3316 0.2945 −0.0135 0.022* 0.563 (11)
H1A3 1.4254 0.2376 0.0078 0.022* 0.563 (11)
C2A 1.4039 (13) 0.591 (3) −0.0197 (10) 0.158 (13)* 0.563 (11)
C3A 1.3977 (5) 0.7536 (14) 0.0394 (4) 0.0124 (19)* 0.563 (11)
H3A1 1.4029 0.9136 0.0260 0.019* 0.563 (11)
H3A2 1.4408 0.7175 0.0785 0.019* 0.563 (11)
H3A3 1.3456 0.7319 0.0511 0.019* 0.563 (11)
O4A 1.437 (2) 0.641 (5) −0.0618 (14) 0.287 (19)* 0.563 (11)

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Ag1 0.0244 (2) 0.0184 (2) 0.0223 (2) −0.00038 (16) 0.00910 (15) −0.00495 (15)
S11 0.0323 (7) 0.0151 (6) 0.0244 (7) −0.0027 (5) 0.0121 (6) −0.0023 (5)
S21 0.0368 (8) 0.0349 (8) 0.0288 (8) 0.0101 (7) 0.0077 (6) −0.0126 (6)
O1 0.034 (2) 0.031 (2) 0.034 (2) 0.0076 (19) 0.0140 (18) 0.0020 (18)
O2 0.061 (3) 0.028 (2) 0.044 (3) −0.010 (2) 0.034 (2) −0.006 (2)
O3 0.034 (3) 0.044 (3) 0.058 (3) 0.012 (2) 0.009 (2) 0.000 (2)
N1 0.024 (2) 0.023 (2) 0.035 (3) −0.0036 (19) 0.008 (2) −0.004 (2)
N12 0.029 (2) 0.018 (2) 0.032 (2) −0.0029 (19) 0.013 (2) −0.0028 (19)
N13 0.027 (2) 0.015 (2) 0.020 (2) −0.0036 (18) 0.0089 (18) −0.0026 (17)
N22 0.026 (3) 0.055 (4) 0.045 (3) −0.005 (3) 0.017 (2) −0.023 (3)
N23 0.022 (2) 0.026 (2) 0.022 (2) 0.0037 (19) 0.0043 (18) −0.0069 (19)
C12 0.033 (3) 0.014 (2) 0.018 (2) 0.001 (2) 0.010 (2) 0.0057 (19)
C14 0.030 (3) 0.017 (2) 0.018 (2) 0.002 (2) 0.007 (2) 0.0011 (19)
C15 0.031 (3) 0.015 (2) 0.019 (2) −0.004 (2) 0.008 (2) 0.0008 (19)
C16 0.038 (3) 0.019 (3) 0.023 (3) 0.002 (2) 0.013 (2) 0.000 (2)
C17 0.032 (3) 0.029 (3) 0.030 (3) 0.003 (2) 0.016 (2) 0.002 (2)
C18 0.032 (3) 0.029 (3) 0.029 (3) −0.008 (2) 0.012 (2) −0.002 (2)
C19 0.029 (3) 0.020 (3) 0.021 (3) −0.003 (2) 0.006 (2) −0.005 (2)
C22 0.024 (3) 0.031 (3) 0.025 (3) 0.004 (2) 0.006 (2) −0.009 (2)
C24 0.026 (3) 0.021 (3) 0.018 (2) 0.004 (2) 0.000 (2) −0.001 (2)
C25 0.031 (3) 0.024 (3) 0.023 (3) 0.006 (2) −0.002 (2) −0.003 (2)
C26 0.049 (4) 0.024 (3) 0.031 (3) 0.002 (3) −0.004 (3) −0.003 (2)
C27 0.039 (4) 0.031 (3) 0.046 (4) −0.011 (3) −0.007 (3) 0.003 (3)
C28 0.026 (3) 0.031 (3) 0.046 (4) −0.002 (3) 0.004 (3) 0.006 (3)
C29 0.026 (3) 0.023 (3) 0.026 (3) 0.002 (2) 0.002 (2) 0.001 (2)

Geometric parameters (Å, °)

Ag1—N13 2.130 (4) C19—H19 0.9500
Ag1—N23 2.127 (4) C24—C29 1.384 (8)
Ag1—S11i 3.2261 (15) C24—C25 1.400 (7)
S11—C12 1.758 (5) C25—C26 1.397 (9)
S11—C15 1.736 (5) C26—C27 1.379 (10)
S21—C22 1.759 (6) C26—H26 0.9500
S21—C25 1.735 (6) C27—C28 1.385 (9)
O1—N1 1.264 (6) C27—H27 0.9500
O2—N1 1.240 (6) C28—C29 1.383 (8)
O3—N1 1.233 (6) C28—H28 0.9500
N12—C12 1.321 (7) C29—H29 0.9500
N12—H2 0.8800 C1B—C2B 1.522 (9)
N12—H1 0.8800 C1B—H1B1 0.9800
N13—C12 1.313 (7) C1B—H1B2 0.9800
N13—C14 1.406 (7) C1B—H1B3 0.9800
N22—C22 1.322 (8) C2B—O4B 1.189 (7)
N22—H3 0.8800 C2B—C3B 1.481 (9)
N22—H4 0.8800 C3B—H3B1 0.9800
N23—C22 1.318 (7) C3B—H3B2 0.9800
N23—C24 1.394 (7) C3B—H3B3 0.9800
C14—C19 1.387 (8) C1A—C2A 1.607 (18)
C14—C15 1.408 (7) C1A—H1A1 0.9800
C15—C16 1.390 (8) C1A—H1A2 0.9800
C16—C17 1.381 (8) C1A—H1A3 0.9800
C16—H16 0.9500 C2A—O4A 1.160 (19)
C17—C18 1.393 (8) C2A—C3A 1.553 (18)
C17—H17 0.9500 C3A—H3A1 0.9800
C18—C19 1.385 (8) C3A—H3A2 0.9800
C18—H18 0.9500 C3A—H3A3 0.9800
N13—Ag1—N23 171.84 (17) N23—C24—C25 114.4 (5)
N23—Ag1—S11i 92.96 (13) C26—C25—C24 121.6 (6)
N13—Ag1—S11i 86.30 (12) C26—C25—S21 128.0 (5)
C15—S11—C12 89.8 (3) C24—C25—S21 110.4 (4)
C25—S21—C22 88.9 (3) C27—C26—C25 118.0 (6)
O1—N1—O2 118.8 (5) C27—C26—H26 121.0
O1—N1—O3 119.3 (5) C25—C26—H26 121.0
O2—N1—O2 121.8 (5) C26—C27—C28 120.7 (6)
C12—N12—H2 120.0 C26—C27—H27 119.7
C12—N12—H1 120.0 C28—C27—H27 119.7
H2—N12—H1 120.0 C29—C28—C27 121.3 (6)
C12—N13—C14 111.6 (4) C29—C28—H28 119.4
C12—N13—Ag1 125.6 (4) C27—C28—H28 119.4
C14—N13—Ag1 122.6 (3) C28—C29—C24 119.2 (5)
C22—N22—H3 120.0 C28—C29—H29 120.4
C22—N22—H4 120.0 C24—C29—H29 120.4
H3—N22—H4 120.0 C2B—C1B—H1B1 109.5
C22—N23—C24 111.1 (5) C2B—C1B—H1B2 109.5
C22—N23—Ag1 127.2 (4) H1B1—C1B—H1B2 109.5
C24—N23—Ag1 120.9 (3) C2B—C1B—H1B3 109.5
N13—C12—N12 125.1 (5) H1B1—C1B—H1B3 109.5
N13—C12—S11 114.6 (4) H1B2—C1B—H1B3 109.5
N12—C12—S11 120.2 (4) O4B—C2B—C3B 122.3 (12)
C19—C14—N13 126.2 (5) O4B—C2B—C1B 116.5 (11)
C19—C14—C15 119.7 (5) C3B—C2B—C1B 121.1 (11)
N13—C14—C15 114.1 (5) C2B—C3B—H3B1 109.5
C16—C15—C14 121.0 (5) C2B—C3B—H3B2 109.5
C16—C15—S11 129.2 (4) H3B1—C3B—H3B2 109.5
C14—C15—S11 109.9 (4) C2B—C3B—H3B3 109.5
C17—C16—C15 118.7 (5) H3B1—C3B—H3B3 109.5
C17—C16—H16 120.7 H3B2—C3B—H3B3 109.5
C15—C16—H16 120.7 C2A—C1A—H1A1 109.5
C16—C17—C18 120.5 (5) C2A—C1A—H1A2 109.5
C16—C17—H17 119.8 H1A1—C1A—H1A2 109.5
C18—C17—H17 119.8 C2A—C1A—H1A3 109.5
C19—C18—C17 121.1 (5) H1A1—C1A—H1A3 109.5
C19—C18—H18 119.4 H1A2—C1A—H1A3 109.5
C17—C18—H18 119.4 O4A—C2A—C3A 124 (2)
C18—C19—C14 119.0 (5) O4A—C2A—C1A 109 (2)
C18—C19—H19 120.5 C3A—C2A—C1A 126.1 (16)
C14—C19—H19 120.5 C2A—C3A—H3A1 109.5
N23—C22—N22 124.8 (5) C2A—C3A—H3A2 109.5
N23—C22—S21 115.1 (4) H3A1—C3A—H3A2 109.5
N22—C22—S21 120.1 (4) C2A—C3A—H3A3 109.5
C29—C24—N23 126.3 (5) H3A1—C3A—H3A3 109.5
C29—C24—C25 119.2 (5) H3A2—C3A—H3A3 109.5
S11i—Ag1—N13—C12 −117.6 (4) C15—C14—C19—C18 0.2 (8)
S11i—Ag1—N13—C14 68.7 (4) C24—N23—C22—N22 −179.3 (6)
S11i—Ag1—N23—C22 103.0 (5) Ag1—N23—C22—N22 11.1 (9)
S11i—Ag1—N23—C24 −65.7 (4) C24—N23—C22—S21 1.0 (6)
C14—N13—C12—N12 −179.2 (5) Ag1—N23—C22—S21 −168.6 (3)
Ag1—N13—C12—N12 6.4 (7) C25—S21—C22—N23 −1.2 (5)
C14—N13—C12—S11 2.5 (6) C25—S21—C22—N22 179.1 (5)
C15—S11—C12—N13 −2.1 (4) C22—N23—C24—C29 −180.0 (5)
C15—S11—C12—N12 179.6 (5) Ag1—N23—C24—C29 −9.6 (7)
C12—N13—C14—C19 177.0 (5) C22—N23—C24—C25 −0.2 (7)
Ag1—N13—C14—C19 −8.5 (7) Ag1—N23—C24—C25 170.2 (4)
C12—N13—C14—C15 −1.7 (6) C29—C24—C25—C26 −0.2 (8)
Ag1—N13—C14—C15 172.8 (3) N23—C24—C25—C26 179.9 (5)
C19—C14—C15—C16 0.4 (8) C29—C24—C25—S21 179.1 (4)
N13—C14—C15—C16 179.2 (5) N23—C24—C25—S21 −0.7 (6)
C19—C14—C15—S11 −178.6 (4) C22—S21—C25—C26 −179.7 (6)
N13—C14—C15—S11 0.2 (6) C22—S21—C25—C24 1.0 (4)
C12—S11—C15—C16 −177.9 (5) C24—C25—C26—C27 −0.1 (9)
C12—S11—C15—C14 1.0 (4) S21—C25—C26—C27 −179.3 (5)
C14—C15—C16—C17 −0.6 (8) C25—C26—C27—C28 0.2 (9)
S11—C15—C16—C17 178.2 (4) C26—C27—C28—C29 0.0 (10)
C15—C16—C17—C18 0.1 (8) C27—C28—C29—C24 −0.3 (9)
C16—C17—C18—C19 0.5 (9) N23—C24—C29—C28 −179.8 (5)
C17—C18—C19—C14 −0.7 (9) C25—C24—C29—C28 0.5 (8)
N13—C14—C19—C18 −178.4 (5)

Symmetry codes: (i) x, y+1, z.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N12—H2···O1 0.88 1.99 2.851 (6) 165
N12—H1···O2ii 0.88 2.07 2.889 (6) 155
N22—H3···O1 0.88 2.12 2.959 (7) 158
N22—H4···O1iii 0.88 2.11 2.955 (6) 162

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

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: LH2768).

References

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Associated Data

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

Supplementary Materials

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536809004176/lh2768sup1.cif

e-65-0m265-sup1.cif (23KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536809004176/lh2768Isup2.hkl

e-65-0m265-Isup2.hkl (198.4KB, hkl)

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


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