Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536802007614/br6048sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S1600536802007614/br6048Isup2.hkl |
Key indicators
- Single-crystal X-ray study
- T = 173 K
- Mean (S-O) = 0.005 Å
- R factor = 0.058
- wR factor = 0.179
- Data-to-parameter ratio = 26.6
checkCIF results
No syntax errors found ADDSYM reports no extra symmetry
Alert Level A:
DIFF_019 Alert A _diffrn_standards_number is missing Number of standards used in measurement. DIFF_020 Alert A _diffrn_standards_interval_count and _diffrn_standards_interval_time are missing. Number of measurements between standards or time (min) between standards.
Alert Level B:
ABSTM_02 Alert B The ratio of expected to reported Tmax/Tmin(RR') is < 0.75 Tmin and Tmax reported: 0.266 0.495 Tmin' and Tmax expected: 0.428 0.441 RR' = 0.552 Please check that your absorption correction is appropriate.
Alert Level C:
PLAT_420 Alert C D-H Without Acceptor N(4) - H(4B) ? General Notes
ABSTM_02 When printed, the submitted absorption T values will be replaced by the scaled T values. Since the ratio of scaled T's is identical to the ratio of reported T values, the scaling does not imply a change to the absorption corrections used in the study. Ratio of Tmax expected/reported 0.891 Tmax scaled 0.441 Tmin scaled 0.237 REFLT_03 From the CIF: _diffrn_reflns_theta_max 29.58 From the CIF: _reflns_number_total 2019 Count of symmetry unique reflns 1134 Completeness (_total/calc) 178.04% TEST3: Check Friedels for noncentro structure Estimate of Friedel pairs measured 885 Fraction of Friedel pairs measured 0.780 Are heavy atom types Z>Si present yes Please check that the estimate of the number of Friedel pairs is correct. If it is not, please give the correct count in the _publ_section_exptl_refinement section of the submitted CIF.
2 Alert Level A = Potentially serious problem
1 Alert Level B = Potential problem
1 Alert Level C = Please check
Crystals of the title compound were found in solutions during studies of waste photolaboratory solutions.
Data collection: X-AREA (Stoe & Cie, 2001); cell refinement: X-AREA; data reduction: X-AREA; program(s) used to solve structure: SHELXS97 (Sheldrick, 1990); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: XP in SHELXTL-Plus (Sheldrick, 1991).
(NH4)9Br[Ag(S2O3)4] | Dx = 2.016 Mg m−3 |
Mr = 878.55 | Mo Kα radiation, λ = 0.71073 Å |
Tetragonal, I42d | Cell parameters from 72726 reflections |
Hall symbol: I -4 2bw | θ = 2.8–29.7° |
a = 13.2634 (7) Å | µ = 4.09 mm−1 |
c = 16.4524 (11) Å | T = 173 K |
V = 2894.3 (3) Å3 | Block, colourless |
Z = 4 | 0.20 × 0.20 × 0.20 mm |
F(000) = 1760 |
Stoe IPDS-II two-circle diffractometer | 2019 independent reflections |
Radiation source: fine-focus sealed tube | 2014 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.049 |
ω scans | θmax = 29.6°, θmin = 3.1° |
Absorption correction: empirical (using intensity measurements) (MULABS; Spek, 1990; Blessing, 1995) | h = −18→17 |
Tmin = 0.266, Tmax = 0.495 | k = −18→18 |
23871 measured reflections | l = −22→22 |
Refinement on F2 | Hydrogen site location: inferred from neighbouring sites |
Least-squares matrix: full | H-atom parameters constrained |
R[F2 > 2σ(F2)] = 0.058 | w = 1/[σ2(Fo2) + (0.117P)2 + 25.2061P] where P = (Fo2 + 2Fc2)/3 |
wR(F2) = 0.179 | (Δ/σ)max < 0.001 |
S = 1.10 | Δρmax = 1.82 e Å−3 |
2019 reflections | Δρmin = −2.36 e Å−3 |
76 parameters | Extinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
0 restraints | Extinction coefficient: 0.0060 (9) |
Primary atom site location: structure-invariant direct methods | Absolute structure: Flack (1983) |
Secondary atom site location: difference Fourier map | Absolute structure parameter: 0.11 (3) |
(NH4)9Br[Ag(S2O3)4] | Z = 4 |
Mr = 878.55 | Mo Kα radiation |
Tetragonal, I42d | µ = 4.09 mm−1 |
a = 13.2634 (7) Å | T = 173 K |
c = 16.4524 (11) Å | 0.20 × 0.20 × 0.20 mm |
V = 2894.3 (3) Å3 |
Stoe IPDS-II two-circle diffractometer | 2019 independent reflections |
Absorption correction: empirical (using intensity measurements) (MULABS; Spek, 1990; Blessing, 1995) | 2014 reflections with I > 2σ(I) |
Tmin = 0.266, Tmax = 0.495 | Rint = 0.049 |
23871 measured reflections |
R[F2 > 2σ(F2)] = 0.058 | H-atom parameters constrained |
wR(F2) = 0.179 | w = 1/[σ2(Fo2) + (0.117P)2 + 25.2061P] where P = (Fo2 + 2Fc2)/3 |
S = 1.10 | Δρmax = 1.82 e Å−3 |
2019 reflections | Δρmin = −2.36 e Å−3 |
76 parameters | Absolute structure: Flack (1983) |
0 restraints | Absolute structure parameter: 0.11 (3) |
Experimental. ; |
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. |
x | y | z | Uiso*/Ueq | ||
Ag1 | 1.0000 | 0.5000 | 0.2500 | 0.0246 (3) | |
S1 | 0.75466 (11) | 0.52067 (10) | 0.14848 (9) | 0.0230 (3) | |
S2 | 0.85780 (12) | 0.41288 (12) | 0.16837 (11) | 0.0287 (4) | |
O1 | 0.8017 (4) | 0.6066 (4) | 0.1080 (3) | 0.0373 (12) | |
O2 | 0.7116 (4) | 0.5525 (5) | 0.2270 (3) | 0.0368 (12) | |
O3 | 0.6739 (4) | 0.4777 (4) | 0.0979 (4) | 0.0407 (13) | |
Br1 | 0.50586 (14) | 0.2500 | 0.1250 | 0.0593 (4) | |
N1 | 1.0000 | 0.5000 | −0.2500 | 0.0271 (18) | |
H1A | 0.9929 | 0.5562 | −0.2187 | 0.033* | |
N2 | 1.0000 | 0.5000 | −0.0136 (7) | 0.076 (5) | |
H2A | 0.9593 | 0.5355 | −0.0477 | 0.092* | |
H2B | 0.9633 | 0.4579 | 0.0185 | 0.092* | |
N3 | 0.9561 (6) | −0.2500 | 0.1250 | 0.0280 (15) | |
H3A | 0.9159 | −0.2035 | 0.1005 | 0.034* | |
H3B | 0.9959 | −0.2194 | 0.1627 | 0.034* | |
N4 | 0.7283 (5) | 0.1981 (5) | 0.2464 (4) | 0.0381 (13) | |
H4A | 0.7940 | 0.1973 | 0.2622 | 0.046* | |
H4B | 0.7193 | 0.2335 | 0.1996 | 0.046* | |
H4C | 0.7057 | 0.1354 | 0.2332 | 0.046* | |
H4D | 0.6887 | 0.2316 | 0.2826 | 0.046* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Ag1 | 0.0221 (3) | 0.0221 (3) | 0.0297 (4) | 0.000 | 0.000 | 0.000 |
S1 | 0.0197 (6) | 0.0181 (6) | 0.0312 (7) | −0.0016 (4) | −0.0053 (5) | 0.0010 (4) |
S2 | 0.0231 (7) | 0.0236 (7) | 0.0396 (8) | 0.0033 (5) | −0.0084 (6) | −0.0066 (6) |
O1 | 0.034 (2) | 0.035 (2) | 0.043 (3) | −0.009 (2) | −0.011 (2) | 0.018 (2) |
O2 | 0.035 (3) | 0.041 (3) | 0.035 (3) | 0.012 (2) | 0.000 (2) | 0.002 (2) |
O3 | 0.027 (2) | 0.028 (2) | 0.067 (4) | −0.0009 (17) | −0.021 (2) | −0.008 (2) |
Br1 | 0.0458 (7) | 0.0718 (10) | 0.0602 (8) | 0.000 | 0.000 | 0.0039 (7) |
N1 | 0.025 (3) | 0.025 (3) | 0.032 (4) | 0.000 | 0.000 | 0.000 |
N2 | 0.156 (17) | 0.028 (5) | 0.046 (5) | −0.007 (9) | 0.000 | 0.000 |
N3 | 0.033 (4) | 0.023 (3) | 0.029 (3) | 0.000 | 0.000 | 0.002 (3) |
N4 | 0.031 (3) | 0.042 (3) | 0.042 (3) | 0.008 (2) | 0.003 (3) | −0.010 (3) |
Ag1—S2i | 2.5876 (15) | N2—H2A | 0.9100 |
Ag1—S2ii | 2.5877 (15) | N2—H2B | 0.9100 |
Ag1—S2 | 2.5877 (15) | N3—H3A | 0.9100 |
Ag1—S2iii | 2.5877 (15) | N3—H3B | 0.9101 |
S1—O1 | 1.460 (5) | N4—H4A | 0.9100 |
S1—O3 | 1.471 (5) | N4—H4B | 0.9100 |
S1—O2 | 1.474 (6) | N4—H4C | 0.9100 |
S1—S2 | 2.006 (2) | N4—H4D | 0.9100 |
N1—H1A | 0.9100 | ||
S2i—Ag1—S2ii | 117.47 (8) | O2—S1—S2 | 109.0 (2) |
S2i—Ag1—S2 | 105.63 (4) | S1—S2—Ag1 | 105.28 (7) |
S2ii—Ag1—S2 | 105.63 (4) | H2A—N2—H2B | 111.0 |
S2i—Ag1—S2iii | 105.62 (4) | H3A—N3—H3B | 109.9 |
S2ii—Ag1—S2iii | 105.62 (4) | H4A—N4—H4B | 111.9 |
S2—Ag1—S2iii | 117.47 (8) | H4A—N4—H4C | 111.9 |
O1—S1—O3 | 110.8 (3) | H4B—N4—H4C | 103.1 |
O1—S1—O2 | 110.0 (4) | H4A—N4—H4D | 111.9 |
O3—S1—O2 | 108.9 (4) | H4B—N4—H4D | 103.1 |
O1—S1—S2 | 109.8 (2) | H4C—N4—H4D | 114.4 |
O3—S1—S2 | 108.2 (2) | ||
O1—S1—S2—Ag1 | 55.6 (3) | S2i—Ag1—S2—S1 | 29.27 (6) |
O3—S1—S2—Ag1 | 176.7 (3) | S2ii—Ag1—S2—S1 | 154.41 (11) |
O2—S1—S2—Ag1 | −65.0 (3) | S2iii—Ag1—S2—S1 | −88.16 (8) |
Symmetry codes: (i) y+1/2, −x+3/2, −z+1/2; (ii) −y+3/2, x−1/2, −z+1/2; (iii) −x+2, −y+1, z. |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1A···O3iv | 0.91 | 1.92 | 2.829 (5) | 180 |
N2—H2A···O3iv | 0.91 | 2.53 | 3.255 (11) | 138 |
N2—H2A···Br1v | 0.91 | 3.08 | 3.789 (6) | 136 |
N2—H2B···O2vi | 0.91 | 2.36 | 2.896 (6) | 118 |
N2—H2B···S2 | 0.91 | 2.90 | 3.723 (10) | 152 |
N3—H3A···O1vii | 0.91 | 2.10 | 2.808 (8) | 134 |
N3—H3B···O2viii | 0.91 | 1.97 | 2.797 (7) | 151 |
N4—H4A···O2ii | 0.91 | 2.05 | 2.947 (9) | 167 |
N4—H4B···Br1 | 0.91 | 3.09 | 3.628 (7) | 120 |
N4—H4C···O3vii | 0.91 | 2.05 | 2.892 (9) | 153 |
N4—H4D···O1ix | 0.91 | 1.89 | 2.805 (8) | 180 |
Symmetry codes: (ii) −y+3/2, x−1/2, −z+1/2; (iv) y+1/2, x, z−1/4; (v) −y+1, x, −z; (vi) −y+3/2, −x+1, z−1/4; (vii) x, −y+1/2, −z+1/4; (viii) y+1/2, −x+1/2, −z+1/2; (ix) y, x−1/2, z+1/4. |
Experimental details
Crystal data | |
Chemical formula | (NH4)9Br[Ag(S2O3)4] |
Mr | 878.55 |
Crystal system, space group | Tetragonal, I42d |
Temperature (K) | 173 |
a, c (Å) | 13.2634 (7), 16.4524 (11) |
V (Å3) | 2894.3 (3) |
Z | 4 |
Radiation type | Mo Kα |
µ (mm−1) | 4.09 |
Crystal size (mm) | 0.20 × 0.20 × 0.20 |
Data collection | |
Diffractometer | Stoe IPDS-II two-circle diffractometer |
Absorption correction | Empirical (using intensity measurements) (MULABS; Spek, 1990; Blessing, 1995) |
Tmin, Tmax | 0.266, 0.495 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 23871, 2019, 2014 |
Rint | 0.049 |
(sin θ/λ)max (Å−1) | 0.695 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.058, 0.179, 1.10 |
No. of reflections | 2019 |
No. of parameters | 76 |
H-atom treatment | H-atom parameters constrained |
w = 1/[σ2(Fo2) + (0.117P)2 + 25.2061P] where P = (Fo2 + 2Fc2)/3 | |
Δρmax, Δρmin (e Å−3) | 1.82, −2.36 |
Absolute structure | Flack (1983) |
Absolute structure parameter | 0.11 (3) |
Computer programs: X-AREA (Stoe & Cie, 2001), X-AREA, SHELXS97 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997), XP in SHELXTL-Plus (Sheldrick, 1991).
Ag1—S2 | 2.5877 (15) | S1—O2 | 1.474 (6) |
S1—O1 | 1.460 (5) | S1—S2 | 2.006 (2) |
S1—O3 | 1.471 (5) | ||
S2i—Ag1—S2 | 105.63 (4) | S2—Ag1—S2ii | 117.47 (8) |
Symmetry codes: (i) y+1/2, −x+3/2, −z+1/2; (ii) −x+2, −y+1, z. |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1A···O3iii | 0.91 | 1.92 | 2.829 (5) | 179.5 |
N2—H2A···O3iii | 0.91 | 2.53 | 3.255 (11) | 137.5 |
N2—H2A···Br1iv | 0.91 | 3.08 | 3.789 (6) | 136.4 |
N2—H2B···O2v | 0.91 | 2.36 | 2.896 (6) | 117.7 |
N2—H2B···S2 | 0.91 | 2.90 | 3.723 (10) | 151.5 |
N3—H3A···O1vi | 0.91 | 2.10 | 2.808 (8) | 133.8 |
N3—H3B···O2vii | 0.91 | 1.97 | 2.797 (7) | 150.9 |
N4—H4A···O2viii | 0.91 | 2.05 | 2.947 (9) | 167.0 |
N4—H4B···Br1 | 0.91 | 3.09 | 3.628 (7) | 119.5 |
N4—H4C···O3vi | 0.91 | 2.05 | 2.892 (9) | 153.0 |
N4—H4D···O1ix | 0.91 | 1.89 | 2.805 (8) | 179.8 |
Symmetry codes: (iii) y+1/2, x, z−1/4; (iv) −y+1, x, −z; (v) −y+3/2, −x+1, z−1/4; (vi) x, −y+1/2, −z+1/4; (vii) y+1/2, −x+1/2, −z+1/2; (viii) −y+3/2, x−1/2, −z+1/2; (ix) y, x−1/2, z+1/4. |
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Alkaline or ammonium thiosulfates are well known as developing agents in photography. Such complexes belong to a general series which can be formulated as MIX·M'IX·4MI2(S2O3)4, where MI = NH4, K, M'I = Cu, Ag, and X = Cl, Br, I (Ferrari et al., 1952).
The structure of the compound with X = Cl, (NH4)9Cl2[Ag(S2O3)4], has already been determined (Bigoli et al., 1972). The present work deals with the crystal structure of the compound with X = Br, of which crystals were found in solutions during studies of waste photolaboratory solutions. The chemical formula has been confirmed after structure determination to be (NH4)9Br2[Ag(S2O3)4] (Fig. 1). The Cl and the Br compounds are isostructural.
The thiosulfate group adopts an almost tetrahedral conformation (Table 1) and the sulfato group acts as a monodentate ligand, complexing silver. Ag is surrounded by four S2O3 groups in a distorded tetrahedral coordination. The projection of the structure onto the a axis is shown in Fig. 2. The crystal structure can be described as a three-dimensional framework composed of [Ag(S2O3)4]2 pseudo-dimers linked via O···NH4+Br- interactions. Several hydrogen bonds stabilize the crystal packing (Table 2).