Supporting information
Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270104002288/sk1675sup1.cif | |
Structure factor file (CIF format) https://doi.org/10.1107/S0108270104002288/sk1675Isup2.hkl |
CCDC reference: 235326
Microcrystals of DABT were obtained in the manner reported by Erlenmeyer (1948). An aqueous solution (20 ml) containing DABT (0.1 g, 0.5 mmol) and CrCl3·6H2O (0.13 g, 0.5 mmol) was mixed with another aqueous solution (10 ml) of IDA (0.07 g, 0.5 mmol) and NaOH (0.04 g, 1 mmol). The mixture was refluxed for 3 h and filtered. After the filtrate was cooled to room temperature, the filtrate was filtered once more. Green single crystals were obtained after 10 d.
H atoms on C atoms were placed in calculated positions, with C—H distances of 0.97 (methylene) and 0.93 Å (aromatic), and included in the final cycles of refinement in a riding model, with Uiso(H) values equal to 1.2Ueq of the carrier atoms. Other H atoms were located in a difference Fourier map and included in structure-factor calculation with fixed positional parameters and Uiso(h) values of 0.05 Å2.
Data collection: PROCESS-AUTO (Rigaku Corporation, 1998); cell refinement: PROCESS-AUTO; data reduction: CrystalStructure (Rigaku/MSC and Rigaku Corporation, 2002); program(s) used to solve structure: SIR92 (Altomare et al., 1993); program(s) used to refine structure: SHELXL97 (Sheldrick, 1997); molecular graphics: ORTEP-3 for Windows (Farrugia, 1997); software used to prepare material for publication: WinGX (Farrugia, 1999).
[Cr(C4H5NO4)(C6H6N4S2)(H2O)]Cl·H2O | Z = 2 |
Mr = 452.86 | F(000) = 462 |
Triclinic, P1 | Dx = 1.746 Mg m−3 |
Hall symbol: -P 1 | Mo Kα radiation, λ = 0.71073 Å |
a = 7.9449 (10) Å | Cell parameters from 3621 reflections |
b = 10.7342 (11) Å | θ = 2.8–23.0° |
c = 10.8835 (12) Å | µ = 1.10 mm−1 |
α = 89.0403 (12)° | T = 295 K |
β = 69.5740 (11)° | Plate, green |
γ = 82.2042 (15)° | 0.41 × 0.32 × 0.13 mm |
V = 861.30 (17) Å3 |
Rigaku R-AXIS RAPID diffractometer | 3069 independent reflections |
Radiation source: fine-focus sealed tube | 2862 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.013 |
Detector resolution: 10.00 pixels mm-1 | θmax = 25.2°, θmin = 1.9° |
ω scans | h = −9→8 |
Absorption correction: multi-scan (ABSCOR; Higashi, 1995) | k = −12→12 |
Tmin = 0.632, Tmax = 0.865 | l = −13→13 |
6761 measured reflections |
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)] = 0.029 | Hydrogen site location: inferred from neighbouring sites |
wR(F2) = 0.084 | H-atom parameters constrained |
S = 1.04 | w = 1/[σ2(Fo2) + (0.0505P)2 + 0.5018P] where P = (Fo2 + 2Fc2)/3 |
3069 reflections | (Δ/σ)max = 0.001 |
226 parameters | Δρmax = 0.30 e Å−3 |
0 restraints | Δρmin = −0.50 e Å−3 |
[Cr(C4H5NO4)(C6H6N4S2)(H2O)]Cl·H2O | γ = 82.2042 (15)° |
Mr = 452.86 | V = 861.30 (17) Å3 |
Triclinic, P1 | Z = 2 |
a = 7.9449 (10) Å | Mo Kα radiation |
b = 10.7342 (11) Å | µ = 1.10 mm−1 |
c = 10.8835 (12) Å | T = 295 K |
α = 89.0403 (12)° | 0.41 × 0.32 × 0.13 mm |
β = 69.5740 (11)° |
Rigaku R-AXIS RAPID diffractometer | 3069 independent reflections |
Absorption correction: multi-scan (ABSCOR; Higashi, 1995) | 2862 reflections with I > 2σ(I) |
Tmin = 0.632, Tmax = 0.865 | Rint = 0.013 |
6761 measured reflections |
R[F2 > 2σ(F2)] = 0.029 | 0 restraints |
wR(F2) = 0.084 | H-atom parameters constrained |
S = 1.04 | Δρmax = 0.30 e Å−3 |
3069 reflections | Δρmin = −0.50 e Å−3 |
226 parameters |
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 | ||
Cr | 0.49717 (4) | 0.21837 (3) | 0.17573 (3) | 0.02755 (11) | |
Cl | 0.93126 (7) | 0.35286 (6) | 0.32254 (6) | 0.04820 (17) | |
S1 | 0.46519 (9) | 0.61351 (6) | 0.34671 (7) | 0.04988 (18) | |
S2 | 0.91435 (8) | 0.33112 (7) | −0.20953 (6) | 0.04665 (17) | |
O1 | 0.3428 (2) | 0.17489 (16) | 0.34687 (16) | 0.0416 (4) | |
O2 | 0.3276 (3) | 0.1410 (2) | 0.55162 (18) | 0.0637 (5) | |
O3 | 0.56157 (19) | 0.04228 (13) | 0.11063 (15) | 0.0332 (3) | |
O4 | 0.7771 (2) | −0.12294 (15) | 0.06443 (18) | 0.0491 (4) | |
O5 | 0.2868 (2) | 0.24608 (15) | 0.11541 (16) | 0.0402 (4) | |
O1W | −0.0386 (4) | 0.1265 (3) | 0.5639 (3) | 0.1019 (9) | |
N1 | 0.4789 (2) | 0.40326 (16) | 0.23256 (18) | 0.0330 (4) | |
N2 | 0.2472 (3) | 0.4381 (2) | 0.4404 (2) | 0.0479 (5) | |
N3 | 0.6699 (2) | 0.28363 (16) | 0.00607 (17) | 0.0315 (4) | |
N4 | 0.7404 (3) | 0.1282 (2) | −0.16230 (19) | 0.0452 (5) | |
N5 | 0.7011 (2) | 0.16649 (16) | 0.25030 (16) | 0.0299 (4) | |
C1 | 0.3856 (3) | 0.4715 (2) | 0.3431 (2) | 0.0366 (5) | |
C2 | 0.6252 (4) | 0.5799 (2) | 0.1930 (3) | 0.0455 (6) | |
H2 | 0.7084 | 0.6326 | 0.1477 | 0.055* | |
C3 | 0.6136 (3) | 0.46720 (19) | 0.1475 (2) | 0.0350 (5) | |
C4 | 0.7181 (3) | 0.4016 (2) | 0.0228 (2) | 0.0350 (5) | |
C5 | 0.8480 (3) | 0.4394 (2) | −0.0808 (2) | 0.0452 (6) | |
H5 | 0.8961 | 0.5141 | −0.0830 | 0.054* | |
C6 | 0.7598 (3) | 0.2365 (2) | −0.1144 (2) | 0.0345 (5) | |
C11 | 0.4142 (3) | 0.1549 (2) | 0.4362 (2) | 0.0415 (5) | |
C12 | 0.6164 (3) | 0.1519 (3) | 0.3929 (2) | 0.0460 (6) | |
H12a | 0.6430 | 0.2189 | 0.4390 | 0.055* | |
H12b | 0.6693 | 0.0725 | 0.4168 | 0.055* | |
C13 | 0.8133 (3) | 0.0509 (2) | 0.1785 (3) | 0.0448 (6) | |
H13a | 0.8492 | −0.0043 | 0.2392 | 0.054* | |
H13b | 0.9225 | 0.0729 | 0.1124 | 0.054* | |
C14 | 0.7113 (3) | −0.0176 (2) | 0.1135 (2) | 0.0340 (5) | |
H | 0.7770 | 0.2276 | 0.2377 | 0.050* | |
H1a | 0.0501 | 0.1638 | 0.5490 | 0.050* | |
H1b | −0.0066 | 0.0559 | 0.6068 | 0.050* | |
H2a | 0.1855 | 0.4853 | 0.5155 | 0.050* | |
H2b | 0.1876 | 0.3750 | 0.4204 | 0.050* | |
H4a | 0.6521 | 0.0858 | −0.1156 | 0.050* | |
H4b | 0.7978 | 0.1068 | −0.2475 | 0.050* | |
H5a | 0.1803 | 0.2629 | 0.1778 | 0.050* | |
H5b | 0.2777 | 0.1961 | 0.0555 | 0.050* |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cr | 0.02625 (18) | 0.02613 (18) | 0.02787 (19) | −0.00490 (13) | −0.00576 (13) | −0.00513 (13) |
Cl | 0.0336 (3) | 0.0531 (4) | 0.0512 (3) | −0.0097 (2) | −0.0041 (2) | −0.0227 (3) |
S1 | 0.0585 (4) | 0.0348 (3) | 0.0604 (4) | −0.0026 (3) | −0.0264 (3) | −0.0188 (3) |
S2 | 0.0429 (3) | 0.0596 (4) | 0.0343 (3) | −0.0194 (3) | −0.0053 (3) | 0.0060 (3) |
O1 | 0.0337 (8) | 0.0471 (9) | 0.0366 (8) | −0.0105 (7) | −0.0010 (7) | 0.0009 (7) |
O2 | 0.0658 (13) | 0.0708 (13) | 0.0355 (10) | −0.0067 (10) | 0.0045 (9) | 0.0094 (9) |
O3 | 0.0324 (7) | 0.0286 (7) | 0.0394 (8) | −0.0062 (6) | −0.0123 (6) | −0.0059 (6) |
O4 | 0.0569 (10) | 0.0366 (9) | 0.0559 (11) | 0.0086 (8) | −0.0270 (9) | −0.0205 (8) |
O5 | 0.0312 (8) | 0.0453 (9) | 0.0420 (9) | 0.0008 (7) | −0.0118 (7) | −0.0159 (7) |
O1W | 0.0735 (16) | 0.148 (3) | 0.0625 (15) | −0.0186 (17) | 0.0058 (13) | −0.0278 (16) |
N1 | 0.0361 (9) | 0.0280 (9) | 0.0346 (9) | −0.0031 (7) | −0.0122 (8) | −0.0060 (7) |
N2 | 0.0441 (11) | 0.0506 (12) | 0.0415 (11) | −0.0021 (9) | −0.0061 (9) | −0.0219 (9) |
N3 | 0.0325 (9) | 0.0304 (9) | 0.0298 (9) | −0.0067 (7) | −0.0079 (7) | −0.0007 (7) |
N4 | 0.0466 (11) | 0.0490 (12) | 0.0322 (10) | −0.0132 (9) | −0.0012 (9) | −0.0109 (8) |
N5 | 0.0311 (8) | 0.0282 (9) | 0.0290 (9) | −0.0076 (7) | −0.0073 (7) | −0.0050 (7) |
C1 | 0.0393 (12) | 0.0321 (11) | 0.0408 (12) | 0.0029 (9) | −0.0194 (10) | −0.0121 (9) |
C2 | 0.0530 (14) | 0.0313 (12) | 0.0559 (15) | −0.0111 (10) | −0.0215 (12) | −0.0023 (10) |
C3 | 0.0409 (11) | 0.0275 (10) | 0.0409 (12) | −0.0058 (9) | −0.0192 (10) | 0.0008 (9) |
C4 | 0.0380 (11) | 0.0309 (11) | 0.0389 (12) | −0.0100 (9) | −0.0151 (10) | 0.0042 (9) |
C5 | 0.0508 (14) | 0.0422 (13) | 0.0458 (13) | −0.0187 (11) | −0.0167 (11) | 0.0078 (11) |
C6 | 0.0326 (11) | 0.0401 (12) | 0.0301 (11) | −0.0070 (9) | −0.0091 (9) | 0.0014 (9) |
C11 | 0.0487 (13) | 0.0314 (11) | 0.0332 (12) | −0.0059 (10) | −0.0001 (10) | −0.0009 (9) |
C12 | 0.0500 (14) | 0.0558 (15) | 0.0298 (11) | −0.0083 (11) | −0.0108 (10) | 0.0010 (10) |
C13 | 0.0375 (12) | 0.0475 (14) | 0.0499 (14) | 0.0059 (10) | −0.0193 (11) | −0.0221 (11) |
C14 | 0.0370 (11) | 0.0320 (11) | 0.0310 (11) | −0.0035 (9) | −0.0098 (9) | −0.0061 (8) |
Cr—O1 | 1.9294 (16) | N2—H2a | 0.912 |
Cr—O3 | 1.9662 (14) | N2—H2b | 0.946 |
Cr—O5 | 1.9843 (15) | N3—C6 | 1.325 (3) |
Cr—N3 | 2.0574 (17) | N3—C4 | 1.404 (3) |
Cr—N1 | 2.0598 (17) | N4—C6 | 1.331 (3) |
Cr—N5 | 2.0620 (18) | N4—H4a | 0.887 |
S1—C2 | 1.719 (3) | N4—H4b | 0.897 |
S1—C1 | 1.734 (2) | N5—C12 | 1.476 (3) |
S2—C5 | 1.722 (3) | N5—C13 | 1.480 (3) |
S2—C6 | 1.740 (2) | N5—H | 0.927 |
O1—C11 | 1.288 (3) | C2—C3 | 1.342 (3) |
O2—C11 | 1.222 (3) | C2—H2 | 0.930 |
O3—C14 | 1.284 (3) | C3—C4 | 1.454 (3) |
O4—C14 | 1.225 (3) | C4—C5 | 1.337 (3) |
O5—H5a | 0.878 | C5—H5 | 0.930 |
O5—H5b | 0.880 | C11—C12 | 1.504 (4) |
O1W—H1a | 0.823 | C12—H12a | 0.970 |
O1W—H1b | 0.936 | C12—H12b | 0.970 |
N1—C1 | 1.339 (3) | C13—C14 | 1.509 (3) |
N1—C3 | 1.400 (3) | C13—H13a | 0.970 |
N2—C1 | 1.319 (3) | C13—H13b | 0.970 |
O1—Cr—O3 | 93.03 (7) | C13—N5—H | 107.2 |
O1—Cr—O5 | 90.70 (7) | Cr—N5—H | 111.6 |
O3—Cr—O5 | 92.79 (6) | N2—C1—N1 | 125.4 (2) |
O1—Cr—N3 | 172.33 (7) | N2—C1—S1 | 122.00 (16) |
O3—Cr—N3 | 93.34 (7) | N1—C1—S1 | 112.58 (17) |
O5—Cr—N3 | 93.25 (7) | C3—C2—S1 | 110.69 (19) |
O1—Cr—N1 | 93.16 (7) | C3—C2—H2 | 124.7 |
O3—Cr—N1 | 169.77 (7) | S1—C2—H2 | 124.7 |
O5—Cr—N1 | 95.27 (7) | C2—C3—N1 | 115.1 (2) |
N3—Cr—N1 | 79.93 (7) | C2—C3—C4 | 130.0 (2) |
O1—Cr—N5 | 83.41 (7) | N1—C3—C4 | 114.91 (18) |
O3—Cr—N5 | 81.81 (6) | C5—C4—N3 | 115.0 (2) |
O5—Cr—N5 | 171.75 (7) | C5—C4—C3 | 129.5 (2) |
N3—Cr—N5 | 93.28 (7) | N3—C4—C3 | 115.36 (18) |
N1—Cr—N5 | 90.82 (7) | C4—C5—S2 | 110.82 (18) |
C2—S1—C1 | 90.48 (11) | C4—C5—H5 | 124.6 |
C5—S2—C6 | 89.97 (11) | S2—C5—H5 | 124.6 |
C11—O1—Cr | 117.65 (14) | N3—C6—N4 | 125.7 (2) |
C14—O3—Cr | 117.62 (13) | N3—C6—S2 | 113.00 (16) |
Cr—O5—H5a | 115.35 | N4—C6—S2 | 121.26 (16) |
Cr—O5—H5b | 121.35 | O2—C11—O1 | 124.0 (2) |
H5a—O5—H5b | 108.98 | O2—C11—C12 | 119.5 (2) |
H1a—O1W—H1b | 101.4 | O1—C11—C12 | 116.51 (19) |
C1—N1—C3 | 111.14 (18) | N5—C12—C11 | 112.72 (19) |
C1—N1—Cr | 134.06 (16) | N5—C12—H12a | 109.0 |
C3—N1—Cr | 113.78 (13) | C11—C12—H12a | 109.0 |
C1—N2—H2a | 124.5 | N5—C12—H12b | 109.0 |
C1—N2—H2b | 116.4 | C11—C12—H12b | 109.0 |
H2a—N2—H2b | 116.5 | H12a—C12—H12b | 107.8 |
C6—N3—C4 | 111.07 (18) | N5—C13—C14 | 111.43 (18) |
C6—N3—Cr | 135.14 (15) | N5—C13—H13a | 109.3 |
C4—N3—Cr | 113.51 (14) | C14—C13—H13a | 109.3 |
C6—N4—H4a | 119.8 | N5—C13—H13b | 109.3 |
C6—N4—H4b | 120.2 | C14—C13—H13b | 109.3 |
H4a—N4—H4b | 118.5 | H13a—C13—H13b | 108.0 |
C12—N5—C13 | 113.95 (19) | O4—C14—O3 | 124.6 (2) |
C12—N5—Cr | 108.06 (14) | O4—C14—C13 | 119.1 (2) |
C13—N5—Cr | 108.38 (13) | O3—C14—C13 | 116.24 (18) |
C12—N5—H | 107.8 |
D—H···A | D—H | H···A | D···A | D—H···A |
N5—H···Cl | 0.93 | 2.33 | 3.1634 (19) | 149 |
O1W—H1a···O2 | 0.82 | 2.20 | 2.891 (4) | 142 |
N2—H2a···Cli | 0.91 | 2.35 | 3.237 (2) | 165 |
N2—H2b···Clii | 0.95 | 2.64 | 3.420 (3) | 140 |
N2—H2b···O1 | 0.95 | 2.33 | 2.927 (3) | 121 |
N4—H4a···O3 | 0.89 | 2.37 | 3.002 (3) | 128 |
N4—H4a···O3iii | 0.89 | 2.31 | 3.104 (3) | 149 |
N4—H4b···O1Wiv | 0.90 | 2.04 | 2.882 (4) | 157 |
O5—H5a···Clii | 0.88 | 2.16 | 3.0230 (18) | 166 |
O5—H5b···O4iii | 0.88 | 1.74 | 2.607 (3) | 168 |
Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) x−1, y, z; (iii) −x+1, −y, −z; (iv) x+1, y, z−1. |
Experimental details
Crystal data | |
Chemical formula | [Cr(C4H5NO4)(C6H6N4S2)(H2O)]Cl·H2O |
Mr | 452.86 |
Crystal system, space group | Triclinic, P1 |
Temperature (K) | 295 |
a, b, c (Å) | 7.9449 (10), 10.7342 (11), 10.8835 (12) |
α, β, γ (°) | 89.0403 (12), 69.5740 (11), 82.2042 (15) |
V (Å3) | 861.30 (17) |
Z | 2 |
Radiation type | Mo Kα |
µ (mm−1) | 1.10 |
Crystal size (mm) | 0.41 × 0.32 × 0.13 |
Data collection | |
Diffractometer | Rigaku R-AXIS RAPID diffractometer |
Absorption correction | Multi-scan (ABSCOR; Higashi, 1995) |
Tmin, Tmax | 0.632, 0.865 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 6761, 3069, 2862 |
Rint | 0.013 |
(sin θ/λ)max (Å−1) | 0.599 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.029, 0.084, 1.04 |
No. of reflections | 3069 |
No. of parameters | 226 |
H-atom treatment | H-atom parameters constrained |
Δρmax, Δρmin (e Å−3) | 0.30, −0.50 |
Computer programs: PROCESS-AUTO (Rigaku Corporation, 1998), PROCESS-AUTO, CrystalStructure (Rigaku/MSC and Rigaku Corporation, 2002), SIR92 (Altomare et al., 1993), SHELXL97 (Sheldrick, 1997), ORTEP-3 for Windows (Farrugia, 1997), WinGX (Farrugia, 1999).
Cr—O1 | 1.9294 (16) | O2—C11 | 1.222 (3) |
Cr—O3 | 1.9662 (14) | O3—C14 | 1.284 (3) |
Cr—O5 | 1.9843 (15) | O4—C14 | 1.225 (3) |
Cr—N3 | 2.0574 (17) | N1—C1 | 1.339 (3) |
Cr—N1 | 2.0598 (17) | N2—C1 | 1.319 (3) |
Cr—N5 | 2.0620 (18) | N3—C6 | 1.325 (3) |
O1—C11 | 1.288 (3) | N4—C6 | 1.331 (3) |
D—H···A | D—H | H···A | D···A | D—H···A |
N5—H···Cl | 0.93 | 2.33 | 3.1634 (19) | 149 |
O1W—H1a···O2 | 0.82 | 2.20 | 2.891 (4) | 142 |
N2—H2a···Cli | 0.91 | 2.35 | 3.237 (2) | 165 |
N2—H2b···Clii | 0.95 | 2.64 | 3.420 (3) | 140 |
N2—H2b···O1 | 0.95 | 2.33 | 2.927 (3) | 121 |
N4—H4a···O3 | 0.89 | 2.37 | 3.002 (3) | 128 |
N4—H4a···O3iii | 0.89 | 2.31 | 3.104 (3) | 149 |
N4—H4b···O1Wiv | 0.90 | 2.04 | 2.882 (4) | 157 |
O5—H5a···Clii | 0.88 | 2.16 | 3.0230 (18) | 166 |
O5—H5b···O4iii | 0.88 | 1.74 | 2.607 (3) | 168 |
Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) x−1, y, z; (iii) −x+1, −y, −z; (iv) x+1, y, z−1. |
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Metal complexes with 2,2'-diamino-4,4'-bi-1,3-thiazole (DABT) have potential applications in several fields. For example, a CoII complex and a NiII complex with DABT have been found to be effective inhibitors of DNA synthesis of tumor cells (Waring, 1981; Fisher et al., 1985). As part of a series of structural investigations of metal complexes with DABT, the title CrIII complex was prepared and its X-ray structure is presented here.
The molecular structure of (I) is shown in Fig. 1. The complex assumes an octahedral coordination geometry, formed by a DABT molecule, an iminodiacetate dianion (IDA) and a coordinated water molecule. The tridentate IDA dianion chelates to the CrIII atom in a facial configuration, which is the common mode for IDA ligands in metal complexes (Mootz & Wunderlich, 1980; Subramaniam et al., 1994). Both chelating five-membered rings of the IDA ion display an envelope conformation, with atom N5 lying in the flap position and out-of the planes formed by the other four atoms by 0.220 (3) and 0.379 (3) Å, respectively. Carboxy groups of the IDA ion coordinate to the CrIII atom in a monodentate manner. The uncoordinated carboxy O atoms are linked to adjacent coordinated water or lattice water molecules via hydrogen bonds, as shown in Fig. 1 and Table 2.
Within the carboxy groups, the C—O(coordinated) distances [1.288 (3) and 1.284 (3) Å] are much longer than the C—O(uncoordinated) distances [1.222 (3) and 1.225 (3) Å; Table 1]. The differences [0.066 (4) and 0.059 (4) Å] are comparable to that found in the neutral carboxyl group of iminodiacetic acid [0.078 (4) Å; Bernstein, 1979]. The differences in C—O distances are are essentially the same as that found in the CrIII complex lithium difluoro(propanediamine-diacetato)chromium(III) [0.059 (4) Å; Bianchini et al., 1986].
The thiazole rings of the DABT molecule are approximately coplanar, the maximum atomic deviation being 0.0743 (12) Å (atom S2). It is notable that the planar DABT molecule chelating to a CrIII atom is inclined to the coordination plane defined by aroms O1, O3, N1, N3 and Cr by a larger dihedral angle [17.23 (7) °]. Hence the CrIII atom lies 0.402 (2) Å out of the DABT mean plane; however, the Cr—N(DABT) distances are normal. Although no geometry data for the DABT complex of CrIII is available for comparison, the Cr—N3 [2.0574 (17) Å] and Cr—N1 [2.0598 (17) Å] distances are similar to the average Cr—N distances found in the 2,2'-bipyridine complex of CrIII [2.064 (3) Å; Swaminathan et al., 1988] and the phenanthroline complex of CrIII [2.065 (8) Å; Ohbo et al., 1983]. The C1—N2 [1.319 (3) Å] and C6—N4 [1.331 (3) Å] distances suggest the existence of electron delocalization between thiazole rings and amino groups.
Extensive hydrogen-bonding interactions occur in the crystal (Table 2). While the amino N atoms of the DABT molecule are intramolecularly hydrogen bonded to the coordinated carboxy O atoms, the Cl− counter-ion and lattice water molecules are linked to the CrIII complex cation via hydrogen bonds (Fig. 1). The Cl− anion is simultaneously hydrogen bonded to the imino group of the IDA ion, the amino group of the DABT molecule and coordinated water molecules of adjacent complex cations, thus formng the hydrogen-bonded supramolecular structure shown in Fig. 2. The lattice water molecules are also involved in the supramolecular structure via hydrogen bonding to the carboxy group of the IDA ion and the amino group of the DABT molecule of neighboring complex cations. Three-centered hydrogen bonds occur in the crystal (Table 2), the sum of three angles about the H atoms being 354 (H2b) and 360 ° (H4a).
The neighboring parallel DABT planes are separated by 3.716 (7) Å, suggesting van der Waals contacts but not π–π stacking between DABT ligands in the crystal. Two symmetry-related O1W water molecules are loosely hydrogen bonded via atom H1B.