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Crystals of (NH4)9Br2[Ag(S2O3)4] have been found to be isostructural with those of (NH4)9Cl2[Ag(S2O3)4], previously reported by Bigoli, Tiripicchio & Tiripicchio Camellini [Acta Cryst. (1972), B28, 2079-2083].

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600536802007614/br6048sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600536802007614/br6048Isup2.hkl
Contains datablock I

Key indicators

  • Single-crystal X-ray study
  • T = 173 K
  • Mean [sigma](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


Red Alert 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.
Amber Alert 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.
Yellow Alert 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

Comment top

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).

Experimental top

Crystals of the title compound were found in solutions during studies of waste photolaboratory solutions.

Computing details top

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).

Figures top
[Figure 1] Fig. 1. Perspective view of the title compound with the atom numbering. Displacement ellipsoids are at the 50% probability level.
[Figure 2] Fig. 2. Packing diagram of the title compound, viewed along the a axis, red = Br, blue = NH4, violet = AgS4 and yellow = S2O3.
(I) top
Crystal data top
(NH4)9Br[Ag(S2O3)4]Dx = 2.016 Mg m3
Mr = 878.55Mo Kα radiation, λ = 0.71073 Å
Tetragonal, I42dCell parameters from 72726 reflections
Hall symbol: I -4 2bwθ = 2.8–29.7°
a = 13.2634 (7) ŵ = 4.09 mm1
c = 16.4524 (11) ÅT = 173 K
V = 2894.3 (3) Å3Block, colourless
Z = 40.20 × 0.20 × 0.20 mm
F(000) = 1760
Data collection top
Stoe IPDS-II two-circle
diffractometer
2019 independent reflections
Radiation source: fine-focus sealed tube2014 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.049
ω scansθmax = 29.6°, θmin = 3.1°
Absorption correction: empirical (using intensity measurements)
(MULABS; Spek, 1990; Blessing, 1995)
h = 1817
Tmin = 0.266, Tmax = 0.495k = 1818
23871 measured reflectionsl = 2222
Refinement top
Refinement on F2Hydrogen site location: inferred from neighbouring sites
Least-squares matrix: fullH-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 = 1.10Δρmax = 1.82 e Å3
2019 reflectionsΔρmin = 2.36 e Å3
76 parametersExtinction correction: SHELXL97, Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
0 restraintsExtinction coefficient: 0.0060 (9)
Primary atom site location: structure-invariant direct methodsAbsolute structure: Flack (1983)
Secondary atom site location: difference Fourier mapAbsolute structure parameter: 0.11 (3)
Crystal data top
(NH4)9Br[Ag(S2O3)4]Z = 4
Mr = 878.55Mo Kα radiation
Tetragonal, I42dµ = 4.09 mm1
a = 13.2634 (7) ÅT = 173 K
c = 16.4524 (11) Å0.20 × 0.20 × 0.20 mm
V = 2894.3 (3) Å3
Data collection top
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 = 0.495Rint = 0.049
23871 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.058H-atom parameters constrained
wR(F2) = 0.179 w = 1/[σ2(Fo2) + (0.117P)2 + 25.2061P]
where P = (Fo2 + 2Fc2)/3
S = 1.10Δρmax = 1.82 e Å3
2019 reflectionsΔρmin = 2.36 e Å3
76 parametersAbsolute structure: Flack (1983)
0 restraintsAbsolute structure parameter: 0.11 (3)
Special details top

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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Ag11.00000.50000.25000.0246 (3)
S10.75466 (11)0.52067 (10)0.14848 (9)0.0230 (3)
S20.85780 (12)0.41288 (12)0.16837 (11)0.0287 (4)
O10.8017 (4)0.6066 (4)0.1080 (3)0.0373 (12)
O20.7116 (4)0.5525 (5)0.2270 (3)0.0368 (12)
O30.6739 (4)0.4777 (4)0.0979 (4)0.0407 (13)
Br10.50586 (14)0.25000.12500.0593 (4)
N11.00000.50000.25000.0271 (18)
H1A0.99290.55620.21870.033*
N21.00000.50000.0136 (7)0.076 (5)
H2A0.95930.53550.04770.092*
H2B0.96330.45790.01850.092*
N30.9561 (6)0.25000.12500.0280 (15)
H3A0.91590.20350.10050.034*
H3B0.99590.21940.16270.034*
N40.7283 (5)0.1981 (5)0.2464 (4)0.0381 (13)
H4A0.79400.19730.26220.046*
H4B0.71930.23350.19960.046*
H4C0.70570.13540.23320.046*
H4D0.68870.23160.28260.046*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Ag10.0221 (3)0.0221 (3)0.0297 (4)0.0000.0000.000
S10.0197 (6)0.0181 (6)0.0312 (7)0.0016 (4)0.0053 (5)0.0010 (4)
S20.0231 (7)0.0236 (7)0.0396 (8)0.0033 (5)0.0084 (6)0.0066 (6)
O10.034 (2)0.035 (2)0.043 (3)0.009 (2)0.011 (2)0.018 (2)
O20.035 (3)0.041 (3)0.035 (3)0.012 (2)0.000 (2)0.002 (2)
O30.027 (2)0.028 (2)0.067 (4)0.0009 (17)0.021 (2)0.008 (2)
Br10.0458 (7)0.0718 (10)0.0602 (8)0.0000.0000.0039 (7)
N10.025 (3)0.025 (3)0.032 (4)0.0000.0000.000
N20.156 (17)0.028 (5)0.046 (5)0.007 (9)0.0000.000
N30.033 (4)0.023 (3)0.029 (3)0.0000.0000.002 (3)
N40.031 (3)0.042 (3)0.042 (3)0.008 (2)0.003 (3)0.010 (3)
Geometric parameters (Å, º) top
Ag1—S2i2.5876 (15)N2—H2A0.9100
Ag1—S2ii2.5877 (15)N2—H2B0.9100
Ag1—S22.5877 (15)N3—H3A0.9100
Ag1—S2iii2.5877 (15)N3—H3B0.9101
S1—O11.460 (5)N4—H4A0.9100
S1—O31.471 (5)N4—H4B0.9100
S1—O21.474 (6)N4—H4C0.9100
S1—S22.006 (2)N4—H4D0.9100
N1—H1A0.9100
S2i—Ag1—S2ii117.47 (8)O2—S1—S2109.0 (2)
S2i—Ag1—S2105.63 (4)S1—S2—Ag1105.28 (7)
S2ii—Ag1—S2105.63 (4)H2A—N2—H2B111.0
S2i—Ag1—S2iii105.62 (4)H3A—N3—H3B109.9
S2ii—Ag1—S2iii105.62 (4)H4A—N4—H4B111.9
S2—Ag1—S2iii117.47 (8)H4A—N4—H4C111.9
O1—S1—O3110.8 (3)H4B—N4—H4C103.1
O1—S1—O2110.0 (4)H4A—N4—H4D111.9
O3—S1—O2108.9 (4)H4B—N4—H4D103.1
O1—S1—S2109.8 (2)H4C—N4—H4D114.4
O3—S1—S2108.2 (2)
O1—S1—S2—Ag155.6 (3)S2i—Ag1—S2—S129.27 (6)
O3—S1—S2—Ag1176.7 (3)S2ii—Ag1—S2—S1154.41 (11)
O2—S1—S2—Ag165.0 (3)S2iii—Ag1—S2—S188.16 (8)
Symmetry codes: (i) y+1/2, x+3/2, z+1/2; (ii) y+3/2, x1/2, z+1/2; (iii) x+2, y+1, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1A···O3iv0.911.922.829 (5)180
N2—H2A···O3iv0.912.533.255 (11)138
N2—H2A···Br1v0.913.083.789 (6)136
N2—H2B···O2vi0.912.362.896 (6)118
N2—H2B···S20.912.903.723 (10)152
N3—H3A···O1vii0.912.102.808 (8)134
N3—H3B···O2viii0.911.972.797 (7)151
N4—H4A···O2ii0.912.052.947 (9)167
N4—H4B···Br10.913.093.628 (7)120
N4—H4C···O3vii0.912.052.892 (9)153
N4—H4D···O1ix0.911.892.805 (8)180
Symmetry codes: (ii) y+3/2, x1/2, z+1/2; (iv) y+1/2, x, z1/4; (v) y+1, x, z; (vi) y+3/2, x+1, z1/4; (vii) x, y+1/2, z+1/4; (viii) y+1/2, x+1/2, z+1/2; (ix) y, x1/2, z+1/4.

Experimental details

Crystal data
Chemical formula(NH4)9Br[Ag(S2O3)4]
Mr878.55
Crystal system, space groupTetragonal, I42d
Temperature (K)173
a, c (Å)13.2634 (7), 16.4524 (11)
V3)2894.3 (3)
Z4
Radiation typeMo Kα
µ (mm1)4.09
Crystal size (mm)0.20 × 0.20 × 0.20
Data collection
DiffractometerStoe IPDS-II two-circle
diffractometer
Absorption correctionEmpirical (using intensity measurements)
(MULABS; Spek, 1990; Blessing, 1995)
Tmin, Tmax0.266, 0.495
No. of measured, independent and
observed [I > 2σ(I)] reflections
23871, 2019, 2014
Rint0.049
(sin θ/λ)max1)0.695
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.058, 0.179, 1.10
No. of reflections2019
No. of parameters76
H-atom treatmentH-atom parameters constrained
w = 1/[σ2(Fo2) + (0.117P)2 + 25.2061P]
where P = (Fo2 + 2Fc2)/3
Δρmax, Δρmin (e Å3)1.82, 2.36
Absolute structureFlack (1983)
Absolute structure parameter0.11 (3)

Computer programs: X-AREA (Stoe & Cie, 2001), X-AREA, SHELXS97 (Sheldrick, 1990), SHELXL97 (Sheldrick, 1997), XP in SHELXTL-Plus (Sheldrick, 1991).

Selected geometric parameters (Å, º) top
Ag1—S22.5877 (15)S1—O21.474 (6)
S1—O11.460 (5)S1—S22.006 (2)
S1—O31.471 (5)
S2i—Ag1—S2105.63 (4)S2—Ag1—S2ii117.47 (8)
Symmetry codes: (i) y+1/2, x+3/2, z+1/2; (ii) x+2, y+1, z.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N1—H1A···O3iii0.911.922.829 (5)179.5
N2—H2A···O3iii0.912.533.255 (11)137.5
N2—H2A···Br1iv0.913.083.789 (6)136.4
N2—H2B···O2v0.912.362.896 (6)117.7
N2—H2B···S20.912.903.723 (10)151.5
N3—H3A···O1vi0.912.102.808 (8)133.8
N3—H3B···O2vii0.911.972.797 (7)150.9
N4—H4A···O2viii0.912.052.947 (9)167.0
N4—H4B···Br10.913.093.628 (7)119.5
N4—H4C···O3vi0.912.052.892 (9)153.0
N4—H4D···O1ix0.911.892.805 (8)179.8
Symmetry codes: (iii) y+1/2, x, z1/4; (iv) y+1, x, z; (v) y+3/2, x+1, z1/4; (vi) x, y+1/2, z+1/4; (vii) y+1/2, x+1/2, z+1/2; (viii) y+3/2, x1/2, z+1/2; (ix) y, x1/2, z+1/4.
 

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