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Acta Crystallographica Section E: Structure Reports Online logoLink to Acta Crystallographica Section E: Structure Reports Online
. 2010 Dec 15;67(Pt 1):m84. doi: 10.1107/S1600536810051780

Bis{benzyl 3-[(1H-indol-3-yl)methyl­idene]dithio­carbazato-κ2 N 3,S}palladium(II) N,N-dimethyl­formamide disolvate

Hamid Khaledi a,*, Hapipah Mohd Ali a
PMCID: PMC3050367  PMID: 21522600

Abstract

In the title compound, [Pd(C17H14N3S2)2]·2C3H7NO, the deprotonated Schiff base ligand acts as an N,S-bidentate chelate, forming a five-membered ring with the metal atom. The PdII ion, located on an inversion center, is four-coordinated by two of the Schiff base ligands in a square-planar geometry. In the crystal, the indolic NH groups are bonded to the dimethyl­formamide (DMF) solvent mol­ecules via an N—H⋯O inter­action. In addition, C—H⋯S inter­actions are observed.

Related literature

For the crystal structure of the ligand, see: Khaledi et al. (2008 ▶). For the isotypic Cu(II) analog, see: Khaledi et al. (2009 ▶). For the PdII complex of the acetone Schiff base of S-methyl­dithio­carbazate, see: Ali et al. (2002 ▶).graphic file with name e-67-00m84-scheme1.jpg

Experimental

Crystal data

  • [Pd(C17H14N3S2)2]·2C3H7NO

  • M r = 901.46

  • Monoclinic, Inline graphic

  • a = 10.509 (4) Å

  • b = 20.320 (7) Å

  • c = 10.925 (4) Å

  • β = 117.577 (5)°

  • V = 2067.8 (12) Å3

  • Z = 2

  • Mo Kα radiation

  • μ = 0.70 mm−1

  • T = 296 K

  • 0.30 × 0.15 × 0.03 mm

Data collection

  • Bruker APEXII CCD diffractometer

  • Absorption correction: multi-scan (SADABS; Sheldrick, 1996 ▶) T min = 0.818, T max = 0.979

  • 11353 measured reflections

  • 4486 independent reflections

  • 3411 reflections with I > 2σ(I)

  • R int = 0.024

Refinement

  • R[F 2 > 2σ(F 2)] = 0.030

  • wR(F 2) = 0.074

  • S = 1.02

  • 4486 reflections

  • 255 parameters

  • 1 restraint

  • H atoms treated by a mixture of independent and constrained refinement

  • Δρmax = 0.27 e Å−3

  • Δρmin = −0.31 e Å−3

Data collection: APEX2 (Bruker, 2007 ▶); cell refinement: SAINT (Bruker, 2007 ▶); data reduction: SAINT; program(s) used to solve structure: SHELXS97 (Sheldrick, 2008 ▶); program(s) used to refine structure: SHELXL97 (Sheldrick, 2008 ▶); molecular graphics: X-SEED (Barbour, 2001 ▶); software used to prepare material for publication: SHELXL97 and publCIF (Westrip, 2010 ▶).

Supplementary Material

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810051780/pv2368sup1.cif

e-67-00m84-sup1.cif (19.1KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810051780/pv2368Isup2.hkl

e-67-00m84-Isup2.hkl (219.8KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report

Table 1. Hydrogen-bond geometry (Å, °).

D—H⋯A D—H H⋯A D⋯A D—H⋯A
N1—H1N⋯O1 0.84 (2) 1.91 (2) 2.749 (3) 174 (3)
C9—H9⋯S1i 0.93 2.60 3.279 (2) 130

Symmetry code: (i) Inline graphic.

Acknowledgments

The authors thank University of Malaya for funding this study (UMRG grant RG024/09BIO).

supplementary crystallographic information

Comment

The title compound is isostructural with the CuII complex of the Schiff base ligand (Khaledi et al., 2009). The palladium(II) ion is four-coordinated by two azomethine nitrogen and two thioamide sulfur atoms in a trans-square planar geometry. It has been suggested that the square planar geometry of the Schiff bases of S-alkyldithiocarbazate is trans when they are derived from aldehydes, whereas the ketone derivatives show cis geometry (Ali et al., 2002). Similar to the analogous CuII complex, the indole amino groups in the present structure are hydrogen bonded to the co-crystallized DMF molecules. Moreover, non-classical hydrogen bonds, C—H···N, C—H···O and C—H···S, are observed in the structure.

Experimental

The Schiff base ligand was prepared as reported previously (Khaledi et al., 2008). A solution of palladium(II) acetate (0.224 g, 1 mmol) in ethanol (30 ml) was added to an ethanolic solution (30 ml) of the ligand (0.65 g, 2 mmol) containing a few drops of triethylamine. The mixture was refluxed for an hour, then cooled to room temperature. The resulting brown solid was filtered, washed with cold ethanol and dried over siliga-gel. The title crystals were obtained by slow evaporation of a solution of the solid in DMF.

Refinement

The C-bound H atoms were placed at calculated positions (C–H 0.93–0.97 Å) and were treated as riding on their parent C atoms. The N-bound H atom was located in a difference Fourier map, and was refined with a distance restraint of N–H 0.86±0.02. For all H atoms, Uiso(H) was set to 1.2–1.5 Ueq(carrier atom).

Figures

Fig. 1.

Fig. 1.

Thermal ellipsoid plot of the title compound at the 30% probability level. Hydrogen atoms are drawn as spheres of arbitrary radius.

Crystal data

[Pd(C17H14N3S2)2]·2C3H7NO F(000) = 928
Mr = 901.46 Dx = 1.448 Mg m−3
Monoclinic, P21/c Mo Kα radiation, λ = 0.71073 Å
Hall symbol: -P 2ybc Cell parameters from 3977 reflections
a = 10.509 (4) Å θ = 2.3–29.4°
b = 20.320 (7) Å µ = 0.70 mm−1
c = 10.925 (4) Å T = 296 K
β = 117.577 (5)° Plate, red
V = 2067.8 (12) Å3 0.30 × 0.15 × 0.03 mm
Z = 2

Data collection

Bruker APEXII CCD diffractometer 4486 independent reflections
Radiation source: fine-focus sealed tube 3411 reflections with I > 2σ(I)
graphite Rint = 0.024
φ and ω scans θmax = 27.0°, θmin = 2.0°
Absorption correction: multi-scan (SADABS; Sheldrick, 1996) h = −13→12
Tmin = 0.818, Tmax = 0.979 k = −25→25
11353 measured reflections l = −11→13

Refinement

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)] = 0.030 Hydrogen site location: inferred from neighbouring sites
wR(F2) = 0.074 H atoms treated by a mixture of independent and constrained refinement
S = 1.02 w = 1/[σ2(Fo2) + (0.0332P)2 + 0.5126P] where P = (Fo2 + 2Fc2)/3
4486 reflections (Δ/σ)max = 0.001
255 parameters Δρmax = 0.27 e Å−3
1 restraint Δρmin = −0.31 e Å−3

Special details

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)

x y z Uiso*/Ueq
Pd1 0.5000 0.5000 1.0000 0.03881 (8)
S1 0.50770 (7) 0.38703 (3) 1.00654 (7) 0.05372 (16)
S2 0.60819 (8) 0.29517 (3) 0.86690 (7) 0.05937 (18)
N1 0.7185 (2) 0.50542 (10) 0.5369 (2) 0.0550 (5)
H1N 0.753 (3) 0.4818 (12) 0.496 (3) 0.066*
N2 0.56951 (19) 0.48716 (8) 0.85694 (19) 0.0422 (4)
N3 0.60342 (19) 0.42432 (8) 0.82622 (19) 0.0438 (4)
C1 0.6788 (3) 0.48235 (11) 0.6292 (3) 0.0517 (6)
H1 0.6771 0.4381 0.6505 0.062*
C2 0.6405 (2) 0.53413 (10) 0.6881 (2) 0.0438 (5)
C3 0.6598 (2) 0.59335 (10) 0.6243 (2) 0.0434 (5)
C4 0.6429 (3) 0.66054 (11) 0.6388 (3) 0.0547 (6)
H4 0.6111 0.6755 0.7005 0.066*
C5 0.6739 (3) 0.70436 (13) 0.5604 (3) 0.0667 (7)
H5 0.6642 0.7493 0.5703 0.080*
C6 0.7198 (3) 0.68253 (13) 0.4660 (3) 0.0692 (8)
H6 0.7388 0.7132 0.4134 0.083*
C7 0.7374 (3) 0.61730 (13) 0.4495 (3) 0.0595 (6)
H7 0.7678 0.6029 0.3865 0.071*
C8 0.7080 (2) 0.57292 (11) 0.5304 (2) 0.0479 (5)
C9 0.5902 (2) 0.53485 (11) 0.7881 (2) 0.0449 (5)
H9 0.5681 0.5765 0.8081 0.054*
C10 0.5759 (2) 0.37785 (10) 0.8902 (2) 0.0424 (5)
C11 0.6598 (3) 0.29661 (12) 0.7301 (3) 0.0587 (6)
H11A 0.6411 0.2533 0.6880 0.070*
H11B 0.5969 0.3273 0.6602 0.070*
C12 0.8120 (3) 0.31475 (10) 0.7668 (3) 0.0514 (6)
C13 0.8432 (3) 0.32943 (13) 0.6598 (3) 0.0641 (7)
H13 0.7699 0.3284 0.5694 0.077*
C14 0.9801 (3) 0.34555 (15) 0.6844 (4) 0.0792 (9)
H14 0.9987 0.3548 0.6108 0.095*
C15 1.0875 (3) 0.34793 (16) 0.8149 (4) 0.0858 (10)
H15 1.1798 0.3595 0.8316 0.103*
C16 1.0600 (3) 0.33329 (16) 0.9226 (4) 0.0884 (10)
H16 1.1340 0.3348 1.0126 0.106*
C17 0.9222 (3) 0.31618 (14) 0.8987 (3) 0.0706 (7)
H17 0.9050 0.3057 0.9726 0.085*
O1 0.8241 (4) 0.43495 (13) 0.3888 (3) 0.1248 (10)
N4 0.9096 (2) 0.42640 (11) 0.2347 (2) 0.0634 (6)
C18 0.8601 (4) 0.45922 (17) 0.3077 (4) 0.0946 (11)
H18 0.8520 0.5046 0.2964 0.113*
C19 0.9457 (3) 0.45852 (16) 0.1364 (3) 0.0827 (9)
H19A 0.9369 0.5053 0.1420 0.124*
H19B 0.8815 0.4438 0.0448 0.124*
H19C 1.0426 0.4477 0.1574 0.124*
C20 0.9206 (3) 0.35570 (14) 0.2455 (3) 0.0785 (8)
H20A 0.9153 0.3418 0.3269 0.118*
H20B 1.0106 0.3420 0.2511 0.118*
H20C 0.8432 0.3363 0.1656 0.118*

Atomic displacement parameters (Å2)

U11 U22 U33 U12 U13 U23
Pd1 0.04047 (13) 0.04106 (13) 0.04411 (14) 0.00056 (10) 0.02740 (11) 0.00044 (11)
S1 0.0737 (4) 0.0436 (3) 0.0685 (4) −0.0004 (3) 0.0537 (4) 0.0015 (3)
S2 0.0807 (4) 0.0410 (3) 0.0797 (5) −0.0021 (3) 0.0569 (4) −0.0023 (3)
N1 0.0705 (13) 0.0540 (12) 0.0608 (13) −0.0030 (10) 0.0477 (11) −0.0044 (10)
N2 0.0469 (10) 0.0428 (10) 0.0467 (10) 0.0017 (7) 0.0301 (9) −0.0002 (8)
N3 0.0503 (10) 0.0407 (9) 0.0511 (11) 0.0002 (8) 0.0325 (9) −0.0031 (8)
C1 0.0656 (15) 0.0462 (12) 0.0603 (15) −0.0024 (11) 0.0434 (13) 0.0003 (11)
C2 0.0495 (12) 0.0444 (12) 0.0480 (13) 0.0014 (10) 0.0314 (11) 0.0026 (10)
C3 0.0426 (11) 0.0470 (12) 0.0466 (12) 0.0015 (10) 0.0257 (10) 0.0046 (10)
C4 0.0573 (14) 0.0507 (13) 0.0664 (16) 0.0053 (11) 0.0374 (13) 0.0056 (12)
C5 0.0681 (17) 0.0505 (14) 0.089 (2) 0.0026 (12) 0.0431 (16) 0.0135 (14)
C6 0.0660 (17) 0.0691 (17) 0.082 (2) −0.0025 (13) 0.0426 (16) 0.0267 (15)
C7 0.0599 (15) 0.0741 (17) 0.0586 (16) −0.0024 (13) 0.0394 (13) 0.0115 (13)
C8 0.0475 (12) 0.0546 (13) 0.0490 (13) −0.0030 (10) 0.0287 (11) 0.0032 (11)
C9 0.0513 (13) 0.0404 (11) 0.0528 (14) 0.0030 (10) 0.0323 (12) 0.0018 (10)
C10 0.0432 (11) 0.0430 (11) 0.0487 (13) −0.0026 (9) 0.0278 (11) −0.0040 (10)
C11 0.0702 (16) 0.0537 (14) 0.0667 (16) −0.0089 (12) 0.0440 (14) −0.0186 (12)
C12 0.0610 (15) 0.0404 (11) 0.0645 (16) 0.0026 (10) 0.0389 (14) −0.0099 (11)
C13 0.0680 (17) 0.0654 (16) 0.0694 (17) 0.0005 (13) 0.0409 (15) −0.0041 (14)
C14 0.076 (2) 0.082 (2) 0.101 (3) 0.0005 (17) 0.059 (2) 0.0081 (19)
C15 0.0625 (19) 0.082 (2) 0.122 (3) 0.0053 (16) 0.050 (2) 0.009 (2)
C16 0.0637 (19) 0.095 (2) 0.089 (2) 0.0093 (17) 0.0210 (18) −0.0057 (19)
C17 0.0734 (19) 0.0774 (18) 0.0687 (19) 0.0053 (15) 0.0393 (17) −0.0040 (15)
O1 0.202 (3) 0.120 (2) 0.1058 (19) 0.0498 (19) 0.116 (2) 0.0098 (16)
N4 0.0643 (13) 0.0729 (14) 0.0570 (13) 0.0028 (11) 0.0315 (12) −0.0111 (11)
C18 0.136 (3) 0.080 (2) 0.086 (2) 0.026 (2) 0.067 (2) −0.0029 (19)
C19 0.079 (2) 0.095 (2) 0.083 (2) −0.0068 (17) 0.0451 (19) −0.0070 (18)
C20 0.090 (2) 0.0727 (19) 0.073 (2) 0.0108 (16) 0.0386 (18) −0.0092 (16)

Geometric parameters (Å, °)

Pd1—N2i 2.0252 (18) C9—H9 0.9300
Pd1—N2 2.0252 (18) C11—C12 1.505 (3)
Pd1—S1 2.2969 (10) C11—H11A 0.9700
Pd1—S1i 2.2969 (10) C11—H11B 0.9700
S1—C10 1.735 (2) C12—C17 1.369 (4)
S2—C10 1.755 (2) C12—C13 1.384 (3)
S2—C11 1.810 (2) C13—C14 1.376 (4)
N1—C1 1.342 (3) C13—H13 0.9300
N1—C8 1.375 (3) C14—C15 1.349 (4)
N1—H1N 0.840 (16) C14—H14 0.9300
N2—C9 1.305 (3) C15—C16 1.368 (4)
N2—N3 1.407 (2) C15—H15 0.9300
N3—C10 1.285 (3) C16—C17 1.391 (4)
C1—C2 1.387 (3) C16—H16 0.9300
C1—H1 0.9300 C17—H17 0.9300
C2—C9 1.417 (3) O1—C18 1.218 (4)
C2—C3 1.451 (3) N4—C18 1.317 (4)
C3—C4 1.395 (3) N4—C20 1.442 (3)
C3—C8 1.401 (3) N4—C19 1.449 (4)
C4—C5 1.375 (3) C18—H18 0.9300
C4—H4 0.9300 C19—H19A 0.9600
C5—C6 1.398 (4) C19—H19B 0.9600
C5—H5 0.9300 C19—H19C 0.9600
C6—C7 1.362 (4) C20—H20A 0.9600
C6—H6 0.9300 C20—H20B 0.9600
C7—C8 1.394 (3) C20—H20C 0.9600
C7—H7 0.9300
N2i—Pd1—N2 179.999 (1) S1—C10—S2 112.47 (12)
N2i—Pd1—S1 97.17 (5) C12—C11—S2 118.18 (19)
N2—Pd1—S1 82.83 (5) C12—C11—H11A 107.8
N2i—Pd1—S1i 82.83 (5) S2—C11—H11A 107.8
N2—Pd1—S1i 97.17 (5) C12—C11—H11B 107.8
S1—Pd1—S1i 180.0 S2—C11—H11B 107.8
C10—S1—Pd1 96.04 (7) H11A—C11—H11B 107.1
C10—S2—C11 104.82 (11) C17—C12—C13 118.0 (2)
C1—N1—C8 109.95 (19) C17—C12—C11 124.2 (2)
C1—N1—H1N 123.9 (19) C13—C12—C11 117.8 (2)
C8—N1—H1N 125.9 (19) C14—C13—C12 121.4 (3)
C9—N2—N3 114.08 (17) C14—C13—H13 119.3
C9—N2—Pd1 124.40 (15) C12—C13—H13 119.3
N3—N2—Pd1 121.50 (12) C15—C14—C13 120.2 (3)
C10—N3—N2 113.06 (17) C15—C14—H14 119.9
N1—C1—C2 110.0 (2) C13—C14—H14 119.9
N1—C1—H1 125.0 C14—C15—C16 119.6 (3)
C2—C1—H1 125.0 C14—C15—H15 120.2
C1—C2—C9 131.1 (2) C16—C15—H15 120.2
C1—C2—C3 105.77 (19) C15—C16—C17 120.6 (3)
C9—C2—C3 123.12 (19) C15—C16—H16 119.7
C4—C3—C8 118.8 (2) C17—C16—H16 119.7
C4—C3—C2 134.7 (2) C12—C17—C16 120.2 (3)
C8—C3—C2 106.49 (18) C12—C17—H17 119.9
C5—C4—C3 118.9 (2) C16—C17—H17 119.9
C5—C4—H4 120.5 C18—N4—C20 119.6 (3)
C3—C4—H4 120.5 C18—N4—C19 122.2 (3)
C4—C5—C6 121.1 (2) C20—N4—C19 118.1 (2)
C4—C5—H5 119.5 O1—C18—N4 125.4 (3)
C6—C5—H5 119.5 O1—C18—H18 117.3
C7—C6—C5 121.4 (2) N4—C18—H18 117.3
C7—C6—H6 119.3 N4—C19—H19A 109.5
C5—C6—H6 119.3 N4—C19—H19B 109.5
C6—C7—C8 117.5 (2) H19A—C19—H19B 109.5
C6—C7—H7 121.2 N4—C19—H19C 109.5
C8—C7—H7 121.2 H19A—C19—H19C 109.5
N1—C8—C7 129.9 (2) H19B—C19—H19C 109.5
N1—C8—C3 107.81 (18) N4—C20—H20A 109.5
C7—C8—C3 122.3 (2) N4—C20—H20B 109.5
N2—C9—C2 131.1 (2) H20A—C20—H20B 109.5
N2—C9—H9 114.4 N4—C20—H20C 109.5
C2—C9—H9 114.4 H20A—C20—H20C 109.5
N3—C10—S1 126.36 (16) H20B—C20—H20C 109.5
N3—C10—S2 121.17 (16)

Symmetry codes: (i) −x+1, −y+1, −z+2.

Hydrogen-bond geometry (Å, °)

D—H···A D—H H···A D···A D—H···A
N1—H1N···O1 0.84 (2) 1.91 (2) 2.749 (3) 174 (3)
C1—H1···N3 0.93 2.40 2.869 (3) 111.
C17—H17···S2 0.93 2.79 3.183 (3) 107.
C20—H20A···O1 0.96 2.36 2.747 (3) 104.
C9—H9···S1i 0.93 2.60 3.279 (2) 130.

Symmetry codes: (i) −x+1, −y+1, −z+2.

Footnotes

Supplementary data and figures for this paper are available from the IUCr electronic archives (Reference: PV2368).

References

  1. Ali, M. A., Mirza, A. H., Butcher, R. J., Tarafder, M. T. H., Keat, T. B. & Ali, A. M. (2002). J. Inorg. Biochem. 92, 141–148. [DOI] [PubMed]
  2. Barbour, L. J. (2001). J. Supramol. Chem. 1, 189–191.
  3. Bruker (2007). APEX2 and SAINT Bruker AXS Inc., Madison, Wisconsin, USA.
  4. Khaledi, H., Mohd Ali, H. & Ng, S. W. (2008). Acta Cryst. E64, o2107. [DOI] [PMC free article] [PubMed]
  5. Khaledi, H., Mohd Ali, H. & Ng, S. W. (2009). Acta Cryst. E65, m139. [DOI] [PMC free article] [PubMed]
  6. Sheldrick, G. M. (1996). SADABS University of Göttingen, Germany.
  7. Sheldrick, G. M. (2008). Acta Cryst. A64, 112–122. [DOI] [PubMed]
  8. Westrip, S. P. (2010). J. Appl. Cryst. 43, 920–925.

Associated Data

This section collects any data citations, data availability statements, or supplementary materials included in this article.

Supplementary Materials

Crystal structure: contains datablocks I, global. DOI: 10.1107/S1600536810051780/pv2368sup1.cif

e-67-00m84-sup1.cif (19.1KB, cif)

Structure factors: contains datablocks I. DOI: 10.1107/S1600536810051780/pv2368Isup2.hkl

e-67-00m84-Isup2.hkl (219.8KB, hkl)

Additional supplementary materials: crystallographic information; 3D view; checkCIF report


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