metal-organic compounds
Bis[trans-dichloridobis(propane-1,3-diamine-κ2N,N′)chromium(III)] tetrachloridozincate determined using synchrotron radiation
aPohang Accelerator Laboratory, POSTECH, Pohang 790-784, Republic of Korea, bDepartment of Chemistry, Shah Jalal University of Science and Technology, Sylhet, Bangladesh, and cDepartment of Chemistry, Andong National University, Andong 760-749, Republic of Korea
*Correspondence e-mail: jhchoi@andong.ac.kr
In the title compound, [CrCl2(C3H10N2)2]2[ZnCl4], the CrIII atom is coordinated by four N atoms of propane-1,3-diamine (tn) and two Cl atoms in a trans arrangement, displaying a distorted octahedral geometry with crystallographic inversion symmetry; the Zn atom in the [ZnCl4]2− anion lies on a -4 axis. The orientations of the two six-membered chelate rings in the complex cation are in an anti chair–chair conformation with respect to each other. The Cr—N bond lengths are 2.087 (6) and 2.097 (6) Å. The Cr—Cl and Zn—Cl bond lengths are 2.3151 (16) and 2.3255 (13) Å, respectively. Weak intermolecular hydrogen bonds involving the tn NH2 groups as donors and chloride ligands of the anion and cation as acceptors are observed.
Related literature
For the synthesis, see: House (1970). For the structures of trans-[Cr(tn)2L2]ClO4 (L = F, Cl, Br), see: Vaughn & Rogers (1985); Choi & Clegg (2011); Choi et al. (2012). For the structures of trans-[Cr(Me2tn)2Cl2]ClO4 and trans-[Cr(Me2tn)2Cl2]2ZnCl4, see: Choi et al. (2008, 2011).
Experimental
Crystal data
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Refinement
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Data collection: PAL ADSC Quantum-210 ADX Program (Arvai & Nielsen, 1983); cell HKL-3000 (Otwinowski & Minor, 1997); data reduction: HKL-3000; program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL; molecular graphics: DIAMOND (Brandenburg, 2012); software used to prepare material for publication: WinGX (Farrugia, 1999).
Supporting information
10.1107/S1600536812023355/nk2158sup1.cif
contains datablocks I, global. DOI:Structure factors: contains datablock I. DOI: 10.1107/S1600536812023355/nk2158Isup2.hkl
The propane-1,3-diamine was obtained from Aldrich Chemical Co. and used as supplied. All chemicals were reagent grade materials and used without further purification. As starting materials, trans-[Cr(tn)2Cl2]ClO4 was prepared as described in the literature (House, 1970; Choi & Clegg, 2011). The crude chloride salt (0.75 g) was dissolved in 20 ml of 0.1M HCl at 40°C and added 10 ml of 6M HCl containing 1.2 g of solid ZnCl2. The resulting solution was filtered and allowed to stand at room temperature for several days to give green crystals of the tetrachlorozincate(II) salt suitable for X-ray structural analysis.
Non-hydrogen atoms were refined anisotropically; hydrogen atoms were first located in a difference map; N–H hydrogen atoms were freely refined and C–H hydrogen atoms were constrained to ride on the parent carbon atom, with C–H = 0.98 Å and C–H = 0.99 Å and Uiso(H) = 1.2Ueq(C) for methylene groups.
Data collection: PAL ADSC Quantum-210 ADX Program (Arvai & Nielsen, 1983); cell
HKL-3000 (Otwinowski & Minor, 1997); data reduction: HKL-3000 (Otwinowski & Minor, 1997); program(s) used to solve structure: SHELXTL (Sheldrick, 2008); program(s) used to refine structure: SHELXTL (Sheldrick, 2008); molecular graphics: DIAMOND (Brandenburg, 2012); software used to prepare material for publication: WinGX (Farrugia, 1999).Fig. 1. A perspective drawing (30% probability level) of the one complex cation and anion |
[CrCl2(C3H10N2)2]2[ZnCl4] | Dx = 1.691 Mg m−3 |
Mr = 749.49 | Synchrotron radiation, λ = 0.90000 Å |
Tetragonal, P42/n | Cell parameters from 16475 reflections |
a = 15.141 (2) Å | θ = 1.0–33.7° |
c = 6.4220 (13) Å | µ = 4.26 mm−1 |
V = 1472.2 (4) Å3 | T = 95 K |
Z = 2 | Needle, pale blue |
F(000) = 764 | 0.16 × 0.02 × 0.02 mm |
ADSC Q210 CCD area-detector diffractometer | 1225 independent reflections |
Radiation source: PLSII 2D bending magnet | 1157 reflections with I > 2σ(I) |
Si(111) double crystal monochromator | Rint = 0.030 |
ω and kappa scan | θmax = 32.0°, θmin = 2.4° |
Absorption correction: multi-scan (HKL-3000 SCALEPACK; Otwinowski & Minor, 1997) | h = −17→17 |
Tmin = 0.549, Tmax = 0.920 | k = −17→17 |
7735 measured reflections | l = −7→7 |
Refinement on F2 | Secondary atom site location: difference Fourier map |
Least-squares matrix: full | Hydrogen site location: inferred from neighbouring sites |
R[F2 > 2σ(F2)] = 0.066 | H-atom parameters constrained |
wR(F2) = 0.198 | w = 1/[σ2(Fo2) + (0.1185P)2 + 13.7893P] where P = (Fo2 + 2Fc2)/3 |
S = 1.11 | (Δ/σ)max < 0.001 |
1225 reflections | Δρmax = 2.55 e Å−3 |
73 parameters | Δρmin = −1.30 e Å−3 |
0 restraints | Extinction correction: SHELXTL (Sheldrick, 2008), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction coefficient: 0.010 (2) |
[CrCl2(C3H10N2)2]2[ZnCl4] | Z = 2 |
Mr = 749.49 | Synchrotron radiation, λ = 0.90000 Å |
Tetragonal, P42/n | µ = 4.26 mm−1 |
a = 15.141 (2) Å | T = 95 K |
c = 6.4220 (13) Å | 0.16 × 0.02 × 0.02 mm |
V = 1472.2 (4) Å3 |
ADSC Q210 CCD area-detector diffractometer | 1225 independent reflections |
Absorption correction: multi-scan (HKL-3000 SCALEPACK; Otwinowski & Minor, 1997) | 1157 reflections with I > 2σ(I) |
Tmin = 0.549, Tmax = 0.920 | Rint = 0.030 |
7735 measured reflections |
R[F2 > 2σ(F2)] = 0.066 | 0 restraints |
wR(F2) = 0.198 | H-atom parameters constrained |
S = 1.11 | w = 1/[σ2(Fo2) + (0.1185P)2 + 13.7893P] where P = (Fo2 + 2Fc2)/3 |
1225 reflections | Δρmax = 2.55 e Å−3 |
73 parameters | Δρmin = −1.30 e Å−3 |
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 | ||
Cr1 | 0.5000 | 0.5000 | 0.5000 | 0.0176 (6) | |
Cl1 | 0.42602 (11) | 0.55586 (11) | 0.7867 (2) | 0.0219 (6) | |
N1 | 0.4440 (4) | 0.3768 (4) | 0.5622 (10) | 0.0250 (14) | |
H1A | 0.4141 | 0.3811 | 0.6865 | 0.030* | |
H1B | 0.4027 | 0.3657 | 0.4605 | 0.030* | |
N2 | 0.6077 (4) | 0.4700 (4) | 0.6928 (9) | 0.0214 (13) | |
H2A | 0.6528 | 0.5081 | 0.6592 | 0.026* | |
H2B | 0.5914 | 0.4822 | 0.8277 | 0.026* | |
C1 | 0.5033 (5) | 0.2982 (5) | 0.5752 (11) | 0.0249 (16) | |
H1C | 0.5309 | 0.2880 | 0.4375 | 0.030* | |
H1D | 0.4676 | 0.2454 | 0.6100 | 0.030* | |
C2 | 0.5748 (5) | 0.3093 (5) | 0.7361 (11) | 0.0244 (16) | |
H2C | 0.6049 | 0.2518 | 0.7544 | 0.029* | |
H2D | 0.5465 | 0.3245 | 0.8705 | 0.029* | |
C3 | 0.6441 (5) | 0.3786 (5) | 0.6887 (11) | 0.0240 (15) | |
H3A | 0.6923 | 0.3740 | 0.7922 | 0.029* | |
H3B | 0.6696 | 0.3669 | 0.5494 | 0.029* | |
Zn1 | 0.2500 | 0.2500 | 0.2500 | 0.0223 (6) | |
Cl2 | 0.37601 (8) | 0.28336 (9) | 0.0585 (2) | 0.0115 (5) |
U11 | U22 | U33 | U12 | U13 | U23 | |
Cr1 | 0.0199 (9) | 0.0192 (9) | 0.0138 (9) | −0.0007 (5) | −0.0008 (6) | −0.0002 (6) |
Cl1 | 0.0230 (9) | 0.0287 (10) | 0.0141 (9) | 0.0025 (6) | 0.0014 (6) | −0.0007 (6) |
N1 | 0.026 (3) | 0.024 (3) | 0.025 (3) | 0.000 (2) | −0.001 (3) | 0.002 (3) |
N2 | 0.024 (3) | 0.024 (3) | 0.016 (3) | −0.002 (2) | 0.000 (2) | −0.001 (2) |
C1 | 0.031 (4) | 0.020 (3) | 0.023 (4) | 0.001 (3) | −0.002 (3) | −0.002 (3) |
C2 | 0.027 (4) | 0.021 (3) | 0.025 (4) | −0.001 (3) | −0.002 (3) | 0.004 (3) |
C3 | 0.021 (3) | 0.029 (4) | 0.022 (3) | 0.002 (3) | −0.002 (3) | 0.003 (3) |
Zn1 | 0.0223 (7) | 0.0223 (7) | 0.0222 (9) | 0.000 | 0.000 | 0.000 |
Cl2 | 0.0087 (8) | 0.0138 (8) | 0.0119 (8) | −0.0024 (5) | 0.0055 (5) | −0.0009 (5) |
Cr1—N1 | 2.087 (6) | C1—C2 | 1.505 (10) |
Cr1—N1i | 2.087 (6) | C1—H1C | 0.9900 |
Cr1—N2 | 2.097 (6) | C1—H1D | 0.9900 |
Cr1—N2i | 2.097 (6) | C2—C3 | 1.515 (10) |
Cr1—Cl1i | 2.3151 (16) | C2—H2C | 0.9900 |
Cr1—Cl1 | 2.3151 (16) | C2—H2D | 0.9900 |
N1—C1 | 1.494 (9) | C3—H3A | 0.9900 |
N1—H1A | 0.9200 | C3—H3B | 0.9900 |
N1—H1B | 0.9200 | Zn1—Cl2ii | 2.3255 (13) |
N2—C3 | 1.489 (9) | Zn1—Cl2iii | 2.3255 (13) |
N2—H2A | 0.9200 | Zn1—Cl2iv | 2.3255 (13) |
N2—H2B | 0.9200 | Zn1—Cl2 | 2.3255 (13) |
N1—Cr1—N1i | 179.999 (1) | H2A—N2—H2B | 107.1 |
N1—Cr1—N2 | 90.5 (2) | N1—C1—C2 | 112.4 (6) |
N1i—Cr1—N2 | 89.5 (2) | N1—C1—H1C | 109.1 |
N1—Cr1—N2i | 89.5 (2) | C2—C1—H1C | 109.1 |
N1i—Cr1—N2i | 90.5 (2) | N1—C1—H1D | 109.1 |
N2—Cr1—N2i | 179.999 (1) | C2—C1—H1D | 109.1 |
N1—Cr1—Cl1i | 91.27 (18) | H1C—C1—H1D | 107.9 |
N1i—Cr1—Cl1i | 88.73 (18) | C1—C2—C3 | 115.9 (6) |
N2—Cr1—Cl1i | 90.80 (16) | C1—C2—H2C | 108.3 |
N2i—Cr1—Cl1i | 89.20 (16) | C3—C2—H2C | 108.3 |
N1—Cr1—Cl1 | 88.73 (18) | C1—C2—H2D | 108.3 |
N1i—Cr1—Cl1 | 91.27 (18) | C3—C2—H2D | 108.3 |
N2—Cr1—Cl1 | 89.20 (16) | H2C—C2—H2D | 107.4 |
N2i—Cr1—Cl1 | 90.80 (16) | N2—C3—C2 | 112.5 (6) |
Cl1i—Cr1—Cl1 | 180.0 | N2—C3—H3A | 109.1 |
C1—N1—Cr1 | 118.6 (4) | C2—C3—H3A | 109.1 |
C1—N1—H1A | 107.7 | N2—C3—H3B | 109.1 |
Cr1—N1—H1A | 107.7 | C2—C3—H3B | 109.1 |
C1—N1—H1B | 107.7 | H3A—C3—H3B | 107.8 |
Cr1—N1—H1B | 107.7 | Cl2ii—Zn1—Cl2iii | 106.24 (3) |
H1A—N1—H1B | 107.1 | Cl2ii—Zn1—Cl2iv | 106.25 (3) |
C3—N2—Cr1 | 118.6 (4) | Cl2iii—Zn1—Cl2iv | 116.14 (7) |
C3—N2—H2A | 107.7 | Cl2ii—Zn1—Cl2 | 116.14 (7) |
Cr1—N2—H2A | 107.7 | Cl2iii—Zn1—Cl2 | 106.24 (3) |
C3—N2—H2B | 107.7 | Cl2iv—Zn1—Cl2 | 106.25 (3) |
Cr1—N2—H2B | 107.7 |
Symmetry codes: (i) −x+1, −y+1, −z+1; (ii) −x+1/2, −y+1/2, z; (iii) y, −x+1/2, −z+1/2; (iv) −y+1/2, x, −z+1/2. |
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1B···Cl2 | 0.92 | 2.90 | 3.678 (6) | 144 |
N1—H1A···Cl2v | 0.92 | 2.87 | 3.636 (6) | 142 |
N1—H1B···Cl2iv | 0.92 | 2.82 | 3.529 (6) | 134 |
N2—H2A···Cl2vi | 0.92 | 2.72 | 3.641 (6) | 179 |
N2—H2B···Cl1vii | 0.92 | 2.56 | 3.404 (6) | 154 |
Symmetry codes: (iv) −y+1/2, x, −z+1/2; (v) x, y, z+1; (vi) y+1/2, −x+1, z+1/2; (vii) −x+1, −y+1, −z+2. |
Experimental details
Crystal data | |
Chemical formula | [CrCl2(C3H10N2)2]2[ZnCl4] |
Mr | 749.49 |
Crystal system, space group | Tetragonal, P42/n |
Temperature (K) | 95 |
a, c (Å) | 15.141 (2), 6.4220 (13) |
V (Å3) | 1472.2 (4) |
Z | 2 |
Radiation type | Synchrotron, λ = 0.90000 Å |
µ (mm−1) | 4.26 |
Crystal size (mm) | 0.16 × 0.02 × 0.02 |
Data collection | |
Diffractometer | ADSC Q210 CCD area-detector diffractometer |
Absorption correction | Multi-scan (HKL-3000 SCALEPACK; Otwinowski & Minor, 1997) |
Tmin, Tmax | 0.549, 0.920 |
No. of measured, independent and observed [I > 2σ(I)] reflections | 7735, 1225, 1157 |
Rint | 0.030 |
(sin θ/λ)max (Å−1) | 0.588 |
Refinement | |
R[F2 > 2σ(F2)], wR(F2), S | 0.066, 0.198, 1.11 |
No. of reflections | 1225 |
No. of parameters | 73 |
H-atom treatment | H-atom parameters constrained |
w = 1/[σ2(Fo2) + (0.1185P)2 + 13.7893P] where P = (Fo2 + 2Fc2)/3 | |
Δρmax, Δρmin (e Å−3) | 2.55, −1.30 |
Computer programs: PAL ADSC Quantum-210 ADX Program (Arvai & Nielsen, 1983), HKL-3000 (Otwinowski & Minor, 1997), SHELXTL (Sheldrick, 2008), DIAMOND (Brandenburg, 2012), WinGX (Farrugia, 1999).
D—H···A | D—H | H···A | D···A | D—H···A |
N1—H1B···Cl2 | 0.92 | 2.90 | 3.678 (6) | 143.7 |
N1—H1A···Cl2i | 0.92 | 2.87 | 3.636 (6) | 141.8 |
N1—H1B···Cl2ii | 0.92 | 2.82 | 3.529 (6) | 134.4 |
N2—H2A···Cl2iii | 0.92 | 2.72 | 3.641 (6) | 178.6 |
N2—H2B···Cl1iv | 0.92 | 2.56 | 3.404 (6) | 153.5 |
Symmetry codes: (i) x, y, z+1; (ii) −y+1/2, x, −z+1/2; (iii) y+1/2, −x+1, z+1/2; (iv) −x+1, −y+1, −z+2. |
Acknowledgements
This work was supported by a grant from the 2012 Research Fund of Andong National University. MAS thanks the NRF of Korea for a postdoctoral fellowship grant 2010. The experiment at the PLS-II 2D-SMC beamline was supported in part by MEST and POSTECH.
References
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There are two possible conformations with respect to the six-membered rings in the trans-[Cr(tn)2L2]+(tn = propane-1,3-diamine, L = monodentate). The carbon atoms of the two chelate rings of the tn ligands can be located on the same side (syn conformer) or on opposite side (anti conformer) of the equatorial plane. The preference for syn- or anti-conformation in the complex cation is still of interest. The infrared and electronic absorption spectroscopic methods are not useful in distinguishing the syn or anti conformaions of the six-membered chelate rings in the typed transition metal complexes. The different arrangements of the two six-membered chelate rings of tn ligands may be dependent on the packing forces and counter anions in the crystal structure.
In this communication, we report the structure of trans-[Cr(tn)2Cl2]2ZnCl4 in order to obtain more information on the conformation of the two six-membered chelate rings.
Counter anionic species play a very important role in coordination chemistry. This is another example of a trans-[Cr(tn)2Cl2]+ but with different counter anion (Choi et al., 2008). The structural analysis shows that there is only one crystallographically independent CrIII complex cation where the four nitrogen atoms of two tn ligands occupy the equatorial sites and the two chlorine atoms coordinate to the Cr metal centre in trans configuration. The Cr1 moiety of complex cation is half occupancy in the asymmetric unit. An ellipsoid plot (30% probability level) of the one CrIII complex cation and anion in the title compound, together with the atomic labelling, is depicted in Fig. 1.
The two six-membered rings have stable chair conformations. Atom Cr1 is located at a crystallographic centre of symmetry, so the Cr complex cation has molecular Ci symmetry. The two chelate rings in the Cr complex cation adopt same anti chair-chair conformation with respect to each other. The Cr—N(tn) distances of 2.087 (76) and 2.097 (6) Å are good agreement with average Cr—N distance of 2.0884 (19) Å found in trans-[Cr(tn)2Cl2]ClO4 (Choi & Clegg, 2011), and the range of 2.0741 (19) to 2.0981 (18) Å found in trans-[Cr(Me2tn)2Cl2]2ZnCl4 (Me2tn = 2,2-dimethylpropane-1,3-diamine) (Choi, Joshi & Spiccia, 2011). The Cr–Cl distance of 2.315 (2) Å is longer than the 2.085 (4) Å of Cr—F found in trans-[Cr(tn)2F2]ClO4 (Vaughn & Rogers, 1985), but slightly shorter than 2.4681 (4) Å of Cr—Br trans-[Cr(tn)2Br2]ClO4 (Choi et al., 2012). The other N—C and C—C bond distances and Cr—N—C, N—C—C and C—C—C angles are also of usual values for tn ligands in chair conformations. The crystals are held together by weak hydrogen bonds (Table 1) between the NH groups of the tn, Cl ligand and Cl atom of tetrachlorozincate anion. The uncoordinated ZnCl42- anion from chromium(III) ion remains outside the coordination sphere. As expected, the Zn atom in the ZnCl42- has a tetrahedral coordination surrounded by four Cl atoms. The Zn—Cl bond distance of 2.3255 (13) and the Cl—Zn—Cl angles of 106.28 (4)–116.05 (9)° are observed. The coordinate Cl1 atom in Cr1 complex cation also forms one hydrogen bond with one NH group in the neighbouring complex cation. The differences found in the conformations of the two six-membered chelate rings may be attributed to the differences in the hydrogen bonding networks and crystal packing forces between the chromium(III) complex cation and counter anion.