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The title compound, [PdCl2(C7H9N)2]·2C2H6OS, crystallizes with two mol­ecules of di­methyl ­sulfoxide (DMSO) in monoclinic space group P21/n. The Pd complex is centrosymmetric and thus the phenyl rings of the benzyl­amine ligands are exo with respect to one another. The crystal packing reveals NH...O and CH...Cl hydrogen bonds between the organometallic mol­ecule and the DMSO mol­ecules, resulting in infinite chains. The distances of the ortho-H atoms on the phenyl ring to the metal center are in the range 4.71–5.34 Å, precluding any significant intramolecular Pd...H interactions.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S0108270100008428/fr1279sup1.cif
Contains datablocks sw000102, I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S0108270100008428/fr1279Isup2.hkl
Contains datablock I

CCDC reference: 150758

Computing details top

Data collection: CrystalClear (Rigaku Corporation, 1999); cell refinement: CrystalClear; data reduction: CrystalClear; program(s) used to solve structure: SHELXS86 (Sheldrick, 1990); program(s) used to refine structure: SHELXL93 (Sheldrick, 1993); molecular graphics: SHELXTL (Sheldrick, 1990); software used to prepare material for publication: SHELXTL.

Trans-Dichlorodibenzylaminepalladium(II) top
Crystal data top
[PdCl2(C7H9N)2]·2C2H6OSF(000) = 560
Mr = 547.86Dx = 1.556 Mg m3
Monoclinic, P21/nMo Kα radiation, λ = 0.71073 Å
a = 7.242 (2) ÅCell parameters from 12890 reflections
b = 16.187 (5) Åθ = 3–30.6°
c = 10.596 (3) ŵ = 1.22 mm1
β = 109.70 (1)°T = 173 K
V = 1169.4 (6) Å3Plate, yellow
Z = 20.38 × 0.23 × 0.12 mm
Data collection top
Rigaku AFC8/Mercury CCD
diffractometer
3088 independent reflections
Radiation source: fine-focus sealed tube2703 reflections with I > 2σ(I)
Graphite monochromatorRint = 0.018
ω scansθmax = 30.6°, θmin = 3.0°
Absorption correction: analytical
(CrystalClear; Rigaku Corporation, 1999)
h = 09
Tmin = 0.500, Tmax = 0.864k = 2222
12890 measured reflectionsl = 1414
Refinement top
Refinement on F2Secondary atom site location: difference Fourier map
Least-squares matrix: fullHydrogen site location: inferred from neighbouring sites
R[F2 > 2σ(F2)] = 0.026H-atom parameters constrained
wR(F2) = 0.059Calculated w = 1/[σ2(Fo2) + (0.015P)2 + 1.2P]
where P = (Fo2 + 2Fc2)/3
S = 1.09(Δ/σ)max = 0.001
3088 reflectionsΔρmax = 0.80 e Å3
130 parametersΔρmin = 0.73 e Å3
0 restraintsExtinction correction: SHELXL93 (Sheldrick, 1993), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4
Primary atom site location: structure-invariant direct methodsExtinction coefficient: 0.0117 (18)
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.

Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
Pd0.00000.00000.50000.01804 (8)
Cl0.14461 (7)0.05561 (3)0.71091 (5)0.02712 (12)
N0.2573 (2)0.05810 (9)0.4856 (2)0.0204 (3)
H1A0.28600.047790.56030.033 (3)*
H1B0.35430.036780.41570.033 (3)*
C20.2506 (3)0.14866 (12)0.4676 (2)0.0236 (4)
H2A0.20900.159300.39220.033 (3)*
H2B0.15330.171540.54540.033 (3)*
C30.4421 (3)0.19311 (11)0.4458 (2)0.0210 (3)
C40.5670 (3)0.17323 (12)0.5166 (2)0.0239 (4)
H4A0.53370.128740.58020.032 (3)*
C50.7397 (3)0.21723 (13)0.4957 (2)0.0283 (4)
H5A0.82460.202880.54510.032 (3)*
C60.7902 (3)0.28194 (13)0.4040 (2)0.0299 (4)
H6A0.91020.311830.38910.032 (3)*
C70.6658 (3)0.30282 (12)0.3344 (2)0.0277 (4)
H7A0.69900.347730.27160.032 (3)*
C80.4932 (3)0.25890 (12)0.3552 (2)0.0241 (4)
H8A0.40770.274010.30670.032 (3)*
S0.25387 (9)0.02443 (3)0.85229 (5)0.03160 (13)
O0.3700 (2)0.00169 (9)0.71130 (15)0.0289 (3)
C90.4180 (4)0.0858 (2)0.9076 (2)0.0425 (6)
H9A0.53350.05430.90010.062 (4)*
H9B0.35430.10160.99940.062 (4)*
H9C0.45410.13450.85290.062 (4)*
C100.0956 (4)0.10537 (15)0.8374 (3)0.0388 (5)
H10A0.00000.08350.80200.062 (4)*
H10B0.17140.14720.77820.062 (4)*
H10C0.03010.12900.92410.062 (4)*
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
Pd0.01657 (11)0.01723 (11)0.01963 (11)0.00221 (7)0.00519 (7)0.00030 (7)
Cl0.0254 (2)0.0296 (2)0.0239 (2)0.0025 (2)0.0051 (2)0.0044 (2)
N0.0185 (7)0.0198 (7)0.0231 (7)0.0025 (6)0.0072 (6)0.0003 (6)
C20.0206 (9)0.0201 (8)0.0308 (9)0.0010 (7)0.0095 (7)0.0028 (7)
C30.0192 (8)0.0181 (8)0.0244 (8)0.0006 (7)0.0056 (7)0.0017 (7)
C40.0209 (9)0.0223 (8)0.0275 (9)0.0002 (7)0.0066 (7)0.0033 (7)
C50.0220 (9)0.0280 (10)0.0368 (11)0.0004 (8)0.0123 (8)0.0020 (8)
C60.0237 (9)0.0263 (9)0.0355 (11)0.0059 (8)0.0045 (8)0.0024 (8)
C70.0322 (10)0.0199 (8)0.0257 (9)0.0047 (8)0.0028 (8)0.0010 (7)
C80.0271 (9)0.0201 (8)0.0243 (9)0.0000 (7)0.0078 (7)0.0002 (7)
S0.0404 (3)0.0217 (2)0.0235 (2)0.0029 (2)0.0013 (2)0.0002 (2)
O0.0256 (7)0.0302 (7)0.0261 (7)0.0009 (6)0.0026 (6)0.0074 (6)
C90.058 (2)0.0408 (13)0.0317 (11)0.0018 (12)0.0195 (11)0.0056 (10)
C100.0324 (12)0.0331 (11)0.0434 (13)0.0027 (9)0.0027 (10)0.0103 (10)
Geometric parameters (Å, º) top
Pd—N2.046 (2)C4—C51.390 (3)
Pd—Ni2.046 (2)C5—C61.392 (3)
Pd—Cl2.3072 (7)C6—C71.384 (3)
Pd—Cli2.3072 (7)C7—C81.390 (3)
N—C21.481 (2)S—O1.507 (2)
C2—C31.510 (3)S—C101.782 (3)
C3—C41.393 (3)S—C91.793 (3)
C3—C81.397 (3)
N—Pd—Ni180.0C8—C3—C2119.0 (2)
N—Pd—Cl89.86 (5)C5—C4—C3120.6 (2)
Ni—Pd—Cl90.14 (5)C4—C5—C6120.5 (2)
N—Pd—Cli90.14 (5)C7—C6—C5119.4 (2)
Ni—Pd—Cli89.86 (5)C6—C7—C8120.2 (2)
Cl—Pd—Cli180.0C7—C8—C3121.0 (2)
C2—N—Pd113.33 (12)O—S—C10106.21 (11)
N—C2—C3115.0 (2)O—S—C9105.65 (12)
C4—C3—C8118.4 (2)C10—S—C997.96 (13)
C4—C3—C2122.5 (2)
Symmetry code: (i) x, y, z+1.
Hydrogen-bond geometry (Å, º) top
D—H···AD—HH···AD···AD—H···A
N—H1A···O0.902.042.922 (2)168
N—H1B···Oii0.902.092.963 (2)163
C10—H10A···Cl0.902.793.631 (3)147
Symmetry code: (ii) x+1/2, y+1/2, z+1/2.
 

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