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Crystals of the title compound, [Cr(C4H5NO4)(C6H6N4S2)(H2O)]Cl·H2O, consist of CrIII complex cations, Cl- counter-ions and lattice water mol­ecules. The complex cation assumes an octahedral coordination geometry, formed by a tridentate imino­di­acetate dianion (IDA), a di­amino­bi­thia­zole (DABT) mol­ecule and a water mol­ecule. The planar DABT group chelates the CrIII ion with normal Cr-N distances [2.0574 (17) and 2.0598 (17) Å], but the DABT mol­ecule is inclined to the coordination plane by a dihedral angle of 17.23 (7)°. In the monodentate carboxylate groups of the IDA ion, the coordinated C-O bonds [1.288 (3) and 1.284 (3) Å] are much longer than the uncoordinated C-O bonds [1.222 (3) and 1.225 (3) Å].

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270104002288/sk1675sup1.cif
Contains datablocks I, global

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270104002288/sk1675Isup2.hkl
Contains datablock I

CCDC reference: 235326

Comment top

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 ππ stacking between DABT ligands in the crystal. Two symmetry-related O1W water molecules are loosely hydrogen bonded via atom H1B.

Experimental top

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.

Refinement top

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.

Computing details top

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).

Figures top
[Figure 1]
[Figure 2]
[Figure 3]
Fig. 1. The molecular structure of (I), with 30% probability displacement ellipsoids. Dashed lines indicate hydrogen bonding. [Symmetric code: (iii) 1 − x,-y,-z.]

Fig. 2. The hydrogen-bonding network between complex cations. [Symmetric codes: (i)1 − x,1 − y,1 − z; (v)1 + x,y,z; (vi)-1 + x,y, 1 + z.]
(I) top
Crystal data top
[Cr(C4H5NO4)(C6H6N4S2)(H2O)]Cl·H2OZ = 2
Mr = 452.86F(000) = 462
Triclinic, P1Dx = 1.746 Mg m3
Hall symbol: -P 1Mo Kα radiation, λ = 0.71073 Å
a = 7.9449 (10) ÅCell parameters from 3621 reflections
b = 10.7342 (11) Åθ = 2.8–23.0°
c = 10.8835 (12) ŵ = 1.10 mm1
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
Data collection top
Rigaku R-AXIS RAPID
diffractometer
3069 independent reflections
Radiation source: fine-focus sealed tube2862 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.013
Detector resolution: 10.00 pixels mm-1θmax = 25.2°, θmin = 1.9°
ω scansh = 98
Absorption correction: multi-scan
(ABSCOR; Higashi, 1995)
k = 1212
Tmin = 0.632, Tmax = 0.865l = 1313
6761 measured reflections
Refinement top
Refinement on F2Primary atom site location: structure-invariant direct methods
Least-squares matrix: fullSecondary atom site location: difference Fourier map
R[F2 > 2σ(F2)] = 0.029Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.084H-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 parametersΔρmax = 0.30 e Å3
0 restraintsΔρmin = 0.50 e Å3
Crystal data top
[Cr(C4H5NO4)(C6H6N4S2)(H2O)]Cl·H2Oγ = 82.2042 (15)°
Mr = 452.86V = 861.30 (17) Å3
Triclinic, P1Z = 2
a = 7.9449 (10) ÅMo Kα radiation
b = 10.7342 (11) ŵ = 1.10 mm1
c = 10.8835 (12) ÅT = 295 K
α = 89.0403 (12)°0.41 × 0.32 × 0.13 mm
β = 69.5740 (11)°
Data collection top
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 = 0.865Rint = 0.013
6761 measured reflections
Refinement top
R[F2 > 2σ(F2)] = 0.0290 restraints
wR(F2) = 0.084H-atom parameters constrained
S = 1.04Δρmax = 0.30 e Å3
3069 reflectionsΔρmin = 0.50 e Å3
226 parameters
Special details top

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
Cr0.49717 (4)0.21837 (3)0.17573 (3)0.02755 (11)
Cl0.93126 (7)0.35286 (6)0.32254 (6)0.04820 (17)
S10.46519 (9)0.61351 (6)0.34671 (7)0.04988 (18)
S20.91435 (8)0.33112 (7)0.20953 (6)0.04665 (17)
O10.3428 (2)0.17489 (16)0.34687 (16)0.0416 (4)
O20.3276 (3)0.1410 (2)0.55162 (18)0.0637 (5)
O30.56157 (19)0.04228 (13)0.11063 (15)0.0332 (3)
O40.7771 (2)0.12294 (15)0.06443 (18)0.0491 (4)
O50.2868 (2)0.24608 (15)0.11541 (16)0.0402 (4)
O1W0.0386 (4)0.1265 (3)0.5639 (3)0.1019 (9)
N10.4789 (2)0.40326 (16)0.23256 (18)0.0330 (4)
N20.2472 (3)0.4381 (2)0.4404 (2)0.0479 (5)
N30.6699 (2)0.28363 (16)0.00607 (17)0.0315 (4)
N40.7404 (3)0.1282 (2)0.16230 (19)0.0452 (5)
N50.7011 (2)0.16649 (16)0.25030 (16)0.0299 (4)
C10.3856 (3)0.4715 (2)0.3431 (2)0.0366 (5)
C20.6252 (4)0.5799 (2)0.1930 (3)0.0455 (6)
H20.70840.63260.14770.055*
C30.6136 (3)0.46720 (19)0.1475 (2)0.0350 (5)
C40.7181 (3)0.4016 (2)0.0228 (2)0.0350 (5)
C50.8480 (3)0.4394 (2)0.0808 (2)0.0452 (6)
H50.89610.51410.08300.054*
C60.7598 (3)0.2365 (2)0.1144 (2)0.0345 (5)
C110.4142 (3)0.1549 (2)0.4362 (2)0.0415 (5)
C120.6164 (3)0.1519 (3)0.3929 (2)0.0460 (6)
H12a0.64300.21890.43900.055*
H12b0.66930.07250.41680.055*
C130.8133 (3)0.0509 (2)0.1785 (3)0.0448 (6)
H13a0.84920.00430.23920.054*
H13b0.92250.07290.11240.054*
C140.7113 (3)0.0176 (2)0.1135 (2)0.0340 (5)
H0.77700.22760.23770.050*
H1a0.05010.16380.54900.050*
H1b0.00660.05590.60680.050*
H2a0.18550.48530.51550.050*
H2b0.18760.37500.42040.050*
H4a0.65210.08580.11560.050*
H4b0.79780.10680.24750.050*
H5a0.18030.26290.17780.050*
H5b0.27770.19610.05550.050*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Cr0.02625 (18)0.02613 (18)0.02787 (19)0.00490 (13)0.00576 (13)0.00513 (13)
Cl0.0336 (3)0.0531 (4)0.0512 (3)0.0097 (2)0.0041 (2)0.0227 (3)
S10.0585 (4)0.0348 (3)0.0604 (4)0.0026 (3)0.0264 (3)0.0188 (3)
S20.0429 (3)0.0596 (4)0.0343 (3)0.0194 (3)0.0053 (3)0.0060 (3)
O10.0337 (8)0.0471 (9)0.0366 (8)0.0105 (7)0.0010 (7)0.0009 (7)
O20.0658 (13)0.0708 (13)0.0355 (10)0.0067 (10)0.0045 (9)0.0094 (9)
O30.0324 (7)0.0286 (7)0.0394 (8)0.0062 (6)0.0123 (6)0.0059 (6)
O40.0569 (10)0.0366 (9)0.0559 (11)0.0086 (8)0.0270 (9)0.0205 (8)
O50.0312 (8)0.0453 (9)0.0420 (9)0.0008 (7)0.0118 (7)0.0159 (7)
O1W0.0735 (16)0.148 (3)0.0625 (15)0.0186 (17)0.0058 (13)0.0278 (16)
N10.0361 (9)0.0280 (9)0.0346 (9)0.0031 (7)0.0122 (8)0.0060 (7)
N20.0441 (11)0.0506 (12)0.0415 (11)0.0021 (9)0.0061 (9)0.0219 (9)
N30.0325 (9)0.0304 (9)0.0298 (9)0.0067 (7)0.0079 (7)0.0007 (7)
N40.0466 (11)0.0490 (12)0.0322 (10)0.0132 (9)0.0012 (9)0.0109 (8)
N50.0311 (8)0.0282 (9)0.0290 (9)0.0076 (7)0.0073 (7)0.0050 (7)
C10.0393 (12)0.0321 (11)0.0408 (12)0.0029 (9)0.0194 (10)0.0121 (9)
C20.0530 (14)0.0313 (12)0.0559 (15)0.0111 (10)0.0215 (12)0.0023 (10)
C30.0409 (11)0.0275 (10)0.0409 (12)0.0058 (9)0.0192 (10)0.0008 (9)
C40.0380 (11)0.0309 (11)0.0389 (12)0.0100 (9)0.0151 (10)0.0042 (9)
C50.0508 (14)0.0422 (13)0.0458 (13)0.0187 (11)0.0167 (11)0.0078 (11)
C60.0326 (11)0.0401 (12)0.0301 (11)0.0070 (9)0.0091 (9)0.0014 (9)
C110.0487 (13)0.0314 (11)0.0332 (12)0.0059 (10)0.0001 (10)0.0009 (9)
C120.0500 (14)0.0558 (15)0.0298 (11)0.0083 (11)0.0108 (10)0.0010 (10)
C130.0375 (12)0.0475 (14)0.0499 (14)0.0059 (10)0.0193 (11)0.0221 (11)
C140.0370 (11)0.0320 (11)0.0310 (11)0.0035 (9)0.0098 (9)0.0061 (8)
Geometric parameters (Å, º) top
Cr—O11.9294 (16)N2—H2a0.912
Cr—O31.9662 (14)N2—H2b0.946
Cr—O51.9843 (15)N3—C61.325 (3)
Cr—N32.0574 (17)N3—C41.404 (3)
Cr—N12.0598 (17)N4—C61.331 (3)
Cr—N52.0620 (18)N4—H4a0.887
S1—C21.719 (3)N4—H4b0.897
S1—C11.734 (2)N5—C121.476 (3)
S2—C51.722 (3)N5—C131.480 (3)
S2—C61.740 (2)N5—H0.927
O1—C111.288 (3)C2—C31.342 (3)
O2—C111.222 (3)C2—H20.930
O3—C141.284 (3)C3—C41.454 (3)
O4—C141.225 (3)C4—C51.337 (3)
O5—H5a0.878C5—H50.930
O5—H5b0.880C11—C121.504 (4)
O1W—H1a0.823C12—H12a0.970
O1W—H1b0.936C12—H12b0.970
N1—C11.339 (3)C13—C141.509 (3)
N1—C31.400 (3)C13—H13a0.970
N2—C11.319 (3)C13—H13b0.970
O1—Cr—O393.03 (7)C13—N5—H107.2
O1—Cr—O590.70 (7)Cr—N5—H111.6
O3—Cr—O592.79 (6)N2—C1—N1125.4 (2)
O1—Cr—N3172.33 (7)N2—C1—S1122.00 (16)
O3—Cr—N393.34 (7)N1—C1—S1112.58 (17)
O5—Cr—N393.25 (7)C3—C2—S1110.69 (19)
O1—Cr—N193.16 (7)C3—C2—H2124.7
O3—Cr—N1169.77 (7)S1—C2—H2124.7
O5—Cr—N195.27 (7)C2—C3—N1115.1 (2)
N3—Cr—N179.93 (7)C2—C3—C4130.0 (2)
O1—Cr—N583.41 (7)N1—C3—C4114.91 (18)
O3—Cr—N581.81 (6)C5—C4—N3115.0 (2)
O5—Cr—N5171.75 (7)C5—C4—C3129.5 (2)
N3—Cr—N593.28 (7)N3—C4—C3115.36 (18)
N1—Cr—N590.82 (7)C4—C5—S2110.82 (18)
C2—S1—C190.48 (11)C4—C5—H5124.6
C5—S2—C689.97 (11)S2—C5—H5124.6
C11—O1—Cr117.65 (14)N3—C6—N4125.7 (2)
C14—O3—Cr117.62 (13)N3—C6—S2113.00 (16)
Cr—O5—H5a115.35N4—C6—S2121.26 (16)
Cr—O5—H5b121.35O2—C11—O1124.0 (2)
H5a—O5—H5b108.98O2—C11—C12119.5 (2)
H1a—O1W—H1b101.4O1—C11—C12116.51 (19)
C1—N1—C3111.14 (18)N5—C12—C11112.72 (19)
C1—N1—Cr134.06 (16)N5—C12—H12a109.0
C3—N1—Cr113.78 (13)C11—C12—H12a109.0
C1—N2—H2a124.5N5—C12—H12b109.0
C1—N2—H2b116.4C11—C12—H12b109.0
H2a—N2—H2b116.5H12a—C12—H12b107.8
C6—N3—C4111.07 (18)N5—C13—C14111.43 (18)
C6—N3—Cr135.14 (15)N5—C13—H13a109.3
C4—N3—Cr113.51 (14)C14—C13—H13a109.3
C6—N4—H4a119.8N5—C13—H13b109.3
C6—N4—H4b120.2C14—C13—H13b109.3
H4a—N4—H4b118.5H13a—C13—H13b108.0
C12—N5—C13113.95 (19)O4—C14—O3124.6 (2)
C12—N5—Cr108.06 (14)O4—C14—C13119.1 (2)
C13—N5—Cr108.38 (13)O3—C14—C13116.24 (18)
C12—N5—H107.8
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N5—H···Cl0.932.333.1634 (19)149
O1W—H1a···O20.822.202.891 (4)142
N2—H2a···Cli0.912.353.237 (2)165
N2—H2b···Clii0.952.643.420 (3)140
N2—H2b···O10.952.332.927 (3)121
N4—H4a···O30.892.373.002 (3)128
N4—H4a···O3iii0.892.313.104 (3)149
N4—H4b···O1Wiv0.902.042.882 (4)157
O5—H5a···Clii0.882.163.0230 (18)166
O5—H5b···O4iii0.881.742.607 (3)168
Symmetry codes: (i) x+1, y+1, z+1; (ii) x1, y, z; (iii) x+1, y, z; (iv) x+1, y, z1.

Experimental details

Crystal data
Chemical formula[Cr(C4H5NO4)(C6H6N4S2)(H2O)]Cl·H2O
Mr452.86
Crystal system, space groupTriclinic, 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)
V3)861.30 (17)
Z2
Radiation typeMo Kα
µ (mm1)1.10
Crystal size (mm)0.41 × 0.32 × 0.13
Data collection
DiffractometerRigaku R-AXIS RAPID
diffractometer
Absorption correctionMulti-scan
(ABSCOR; Higashi, 1995)
Tmin, Tmax0.632, 0.865
No. of measured, independent and
observed [I > 2σ(I)] reflections
6761, 3069, 2862
Rint0.013
(sin θ/λ)max1)0.599
Refinement
R[F2 > 2σ(F2)], wR(F2), S 0.029, 0.084, 1.04
No. of reflections3069
No. of parameters226
H-atom treatmentH-atom parameters constrained
Δρmax, Δρmin (e Å3)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).

Selected bond lengths (Å) top
Cr—O11.9294 (16)O2—C111.222 (3)
Cr—O31.9662 (14)O3—C141.284 (3)
Cr—O51.9843 (15)O4—C141.225 (3)
Cr—N32.0574 (17)N1—C11.339 (3)
Cr—N12.0598 (17)N2—C11.319 (3)
Cr—N52.0620 (18)N3—C61.325 (3)
O1—C111.288 (3)N4—C61.331 (3)
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N5—H···Cl0.932.333.1634 (19)149
O1W—H1a···O20.822.202.891 (4)142
N2—H2a···Cli0.912.353.237 (2)165
N2—H2b···Clii0.952.643.420 (3)140
N2—H2b···O10.952.332.927 (3)121
N4—H4a···O30.892.373.002 (3)128
N4—H4a···O3iii0.892.313.104 (3)149
N4—H4b···O1Wiv0.902.042.882 (4)157
O5—H5a···Clii0.882.163.0230 (18)166
O5—H5b···O4iii0.881.742.607 (3)168
Symmetry codes: (i) x+1, y+1, z+1; (ii) x1, y, z; (iii) x+1, y, z; (iv) x+1, y, z1.
 

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