The title compound, [PdCl
2(C
7H
9N)
2]·2C
2H
6OS, crystallizes with two molecules of dimethyl sulfoxide (DMSO) in monoclinic space group
P2
1/
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
CCDC reference: 150758
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]·2C2H6OS | F(000) = 560 |
Mr = 547.86 | Dx = 1.556 Mg m−3 |
Monoclinic, P21/n | Mo Kα radiation, λ = 0.71073 Å |
a = 7.242 (2) Å | Cell parameters from 12890 reflections |
b = 16.187 (5) Å | θ = 3–30.6° |
c = 10.596 (3) Å | µ = 1.22 mm−1 |
β = 109.70 (1)° | T = 173 K |
V = 1169.4 (6) Å3 | Plate, yellow |
Z = 2 | 0.38 × 0.23 × 0.12 mm |
Data collection top
Rigaku AFC8/Mercury CCD diffractometer | 3088 independent reflections |
Radiation source: fine-focus sealed tube | 2703 reflections with I > 2σ(I) |
Graphite monochromator | Rint = 0.018 |
ω scans | θmax = 30.6°, θmin = 3.0° |
Absorption correction: analytical (CrystalClear; Rigaku Corporation, 1999) | h = 0→9 |
Tmin = 0.500, Tmax = 0.864 | k = −22→22 |
12890 measured reflections | l = −14→14 |
Refinement top
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)] = 0.026 | H-atom parameters constrained |
wR(F2) = 0.059 | Calculated w = 1/[σ2(Fo2) + (0.015P)2 + 1.2P] where
P = (Fo2 + 2Fc2)/3 |
S = 1.09 | (Δ/σ)max = 0.001 |
3088 reflections | Δρmax = 0.80 e Å−3 |
130 parameters | Δρmin = −0.73 e Å−3 |
0 restraints | Extinction correction: SHELXL93 (Sheldrick, 1993), Fc*=kFc[1+0.001xFc2λ3/sin(2θ)]-1/4 |
Primary atom site location: structure-invariant direct methods | Extinction 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 | x | y | z | Uiso*/Ueq | |
Pd | 0.0000 | 0.0000 | 0.5000 | 0.01804 (8) | |
Cl | 0.14461 (7) | 0.05561 (3) | 0.71091 (5) | 0.02712 (12) | |
N | −0.2573 (2) | 0.05810 (9) | 0.4856 (2) | 0.0204 (3) | |
H1A | −0.2860 | 0.04779 | 0.5603 | 0.033 (3)* | |
H1B | −0.3543 | 0.03678 | 0.4157 | 0.033 (3)* | |
C2 | −0.2506 (3) | 0.14866 (12) | 0.4676 (2) | 0.0236 (4) | |
H2A | −0.2090 | 0.15930 | 0.3922 | 0.033 (3)* | |
H2B | −0.1533 | 0.17154 | 0.5454 | 0.033 (3)* | |
C3 | −0.4421 (3) | 0.19311 (11) | 0.4458 (2) | 0.0210 (3) | |
C4 | −0.5670 (3) | 0.17323 (12) | 0.5166 (2) | 0.0239 (4) | |
H4A | −0.5337 | 0.12874 | 0.5802 | 0.032 (3)* | |
C5 | −0.7397 (3) | 0.21723 (13) | 0.4957 (2) | 0.0283 (4) | |
H5A | −0.8246 | 0.20288 | 0.5451 | 0.032 (3)* | |
C6 | −0.7902 (3) | 0.28194 (13) | 0.4040 (2) | 0.0299 (4) | |
H6A | −0.9102 | 0.31183 | 0.3891 | 0.032 (3)* | |
C7 | −0.6658 (3) | 0.30282 (12) | 0.3344 (2) | 0.0277 (4) | |
H7A | −0.6990 | 0.34773 | 0.2716 | 0.032 (3)* | |
C8 | −0.4932 (3) | 0.25890 (12) | 0.3552 (2) | 0.0241 (4) | |
H8A | −0.4077 | 0.27401 | 0.3067 | 0.032 (3)* | |
S | −0.25387 (9) | −0.02443 (3) | 0.85229 (5) | 0.03160 (13) | |
O | −0.3700 (2) | 0.00169 (9) | 0.71130 (15) | 0.0289 (3) | |
C9 | −0.4180 (4) | −0.0858 (2) | 0.9076 (2) | 0.0425 (6) | |
H9A | −0.5335 | −0.0543 | 0.9001 | 0.062 (4)* | |
H9B | −0.3543 | −0.1016 | 0.9994 | 0.062 (4)* | |
H9C | −0.4541 | −0.1345 | 0.8529 | 0.062 (4)* | |
C10 | −0.0956 (4) | −0.10537 (15) | 0.8374 (3) | 0.0388 (5) | |
H10A | 0.0000 | −0.0835 | 0.8020 | 0.062 (4)* | |
H10B | −0.1714 | −0.1472 | 0.7782 | 0.062 (4)* | |
H10C | −0.0301 | −0.1290 | 0.9241 | 0.062 (4)* | |
Atomic displacement parameters (Å2) top | U11 | U22 | U33 | U12 | U13 | U23 |
Pd | 0.01657 (11) | 0.01723 (11) | 0.01963 (11) | 0.00221 (7) | 0.00519 (7) | 0.00030 (7) |
Cl | 0.0254 (2) | 0.0296 (2) | 0.0239 (2) | 0.0025 (2) | 0.0051 (2) | −0.0044 (2) |
N | 0.0185 (7) | 0.0198 (7) | 0.0231 (7) | 0.0025 (6) | 0.0072 (6) | 0.0003 (6) |
C2 | 0.0206 (9) | 0.0201 (8) | 0.0308 (9) | 0.0010 (7) | 0.0095 (7) | 0.0028 (7) |
C3 | 0.0192 (8) | 0.0181 (8) | 0.0244 (8) | 0.0006 (7) | 0.0056 (7) | −0.0017 (7) |
C4 | 0.0209 (9) | 0.0223 (8) | 0.0275 (9) | 0.0002 (7) | 0.0066 (7) | 0.0033 (7) |
C5 | 0.0220 (9) | 0.0280 (10) | 0.0368 (11) | 0.0004 (8) | 0.0123 (8) | −0.0020 (8) |
C6 | 0.0237 (9) | 0.0263 (9) | 0.0355 (11) | 0.0059 (8) | 0.0045 (8) | −0.0024 (8) |
C7 | 0.0322 (10) | 0.0199 (8) | 0.0257 (9) | 0.0047 (8) | 0.0028 (8) | 0.0010 (7) |
C8 | 0.0271 (9) | 0.0201 (8) | 0.0243 (9) | 0.0000 (7) | 0.0078 (7) | −0.0002 (7) |
S | 0.0404 (3) | 0.0217 (2) | 0.0235 (2) | −0.0029 (2) | −0.0013 (2) | 0.0002 (2) |
O | 0.0256 (7) | 0.0302 (7) | 0.0261 (7) | −0.0009 (6) | 0.0026 (6) | 0.0074 (6) |
C9 | 0.058 (2) | 0.0408 (13) | 0.0317 (11) | 0.0018 (12) | 0.0195 (11) | 0.0056 (10) |
C10 | 0.0324 (12) | 0.0331 (11) | 0.0434 (13) | 0.0027 (9) | 0.0027 (10) | 0.0103 (10) |
Geometric parameters (Å, º) top
Pd—N | 2.046 (2) | C4—C5 | 1.390 (3) |
Pd—Ni | 2.046 (2) | C5—C6 | 1.392 (3) |
Pd—Cl | 2.3072 (7) | C6—C7 | 1.384 (3) |
Pd—Cli | 2.3072 (7) | C7—C8 | 1.390 (3) |
N—C2 | 1.481 (2) | S—O | 1.507 (2) |
C2—C3 | 1.510 (3) | S—C10 | 1.782 (3) |
C3—C4 | 1.393 (3) | S—C9 | 1.793 (3) |
C3—C8 | 1.397 (3) | | |
| | | |
N—Pd—Ni | 180.0 | C8—C3—C2 | 119.0 (2) |
N—Pd—Cl | 89.86 (5) | C5—C4—C3 | 120.6 (2) |
Ni—Pd—Cl | 90.14 (5) | C4—C5—C6 | 120.5 (2) |
N—Pd—Cli | 90.14 (5) | C7—C6—C5 | 119.4 (2) |
Ni—Pd—Cli | 89.86 (5) | C6—C7—C8 | 120.2 (2) |
Cl—Pd—Cli | 180.0 | C7—C8—C3 | 121.0 (2) |
C2—N—Pd | 113.33 (12) | O—S—C10 | 106.21 (11) |
N—C2—C3 | 115.0 (2) | O—S—C9 | 105.65 (12) |
C4—C3—C8 | 118.4 (2) | C10—S—C9 | 97.96 (13) |
C4—C3—C2 | 122.5 (2) | | |
Symmetry code: (i) −x, −y, −z+1. |
Hydrogen-bond geometry (Å, º) top
D—H···A | D—H | H···A | D···A | D—H···A |
N—H1A···O | 0.90 | 2.04 | 2.922 (2) | 168 |
N—H1B···Oii | 0.90 | 2.09 | 2.963 (2) | 163 |
C10—H10A···Cl | 0.90 | 2.79 | 3.631 (3) | 147 |
Symmetry code: (ii) −x+1/2, y+1/2, −z+1/2. |