A. Lledꢂs, J. Gimeno et al.
(30 m, 250 mm) column. GC-MS measurements were performed on an
(0.4 mol%, if required) were dissolved in THF or water (20 mL), and the
reaction mixture was stirred at 758C for the time indicated in Table 1
and Table 2. The course of the reaction was monitored every five minutes
by analysis of an aliquot of the mixture by GC. The identity of the resul-
tant saturated carbonyl compounds was assessed by comparison with
commercially available pure samples (Aldrich Chemical Co. or Acros Or-
ganics) and by their fragmentation pattern after GC-MS analysis.
Agilent 6890N instrument coupled to an Agilent 5973 mass detector (EI,
1
70 eV) and fitted with a HP-1 MS column. H and 13C NMR spectra were
recorded on a Bruker DPX-300 instrument at 300 or 75.4 MHz, respec-
tively, with SiMe4 as a standard. DEPT experiments were carried out for
all of the compounds reported. The numbering for the proton and carbon
atoms of the 2,7-dimethylocta-2,6-diene-1,8-diyl skeleton is as follows:
X-Ray crystal structure determination of compounds 1 f and 2c: Crystals
suitable for X-ray diffraction analysis were obtained, in both cases, by
slow diffusion of n-hexane into a saturated solution of the compound in
CH2Cl2. The most relevant crystal and refinement data are collected in
Table S1 (see the Supporting Information).
For 1 f, data collection was performed at 200(2) K on an Oxford Diffrac-
tion Xcalibur Nova single crystal diffractometer by using CuKa radiation
(l=1.5418 ꢈ). Images were collected at a 65 mm fixed crystal–detector
distance (oscillation method) with 18 oscillation and 4 s exposure time
per image. Data collection strategy was calculated with the program Cry-
sAlis Pro CCD.[42] Data reduction and cell refinement was performed
with the program CrysAlis Pro RED.[42] An empirical absorption correc-
tion was applied by using the SCALE3 ABSPACK algorithm as imple-
mented in the program CrysAlis Pro RED.[42]
ESI mass spectrometry: A Quattro LC QhQ (quadrupole–hexapole–
quadrupole) mass spectrometer with an orthogonal Z-spray electrospray
interface (Waters, Manchester, UK) was used. The drying and nebulising
gas was nitrogen at a flow of 300 and 50 Lhꢀ1, respectively. The tempera-
ture of the source block was set to 1008C and the interface to 1208C.
The capillary voltage was set at 3.5 kV in the positive-scan mode and the
cone voltage was adjusted to a low value (typically Uc =5–15 V) to con-
trol the extent of fragmentation in the source region. Solutions of the
sample (cꢁ5ꢇ10ꢀ4 m) in the appropriate solvent were introduced to the
ESI source through a fused-silica capillary by syringe pump at a flow rate
of 10 mLminꢀ1. The chemical composition of each peak obtained in the
full-scan mode was assigned by comparison of the isotope experimental
and theoretical patterns with the MassLynx 4.0 program. Collision-in-
duced dissociation (CID) experiments were performed with argon at var-
ious collision energies (Elab =3–15 eV). The most intense precursor peak
of interest was mass selected with Q1 (isolation width of 1 Da), interact-
ed with argon in the hexapole cell and scanned with Q2 to monitor the
ionic fragments.
For 2c, diffraction data were recorded at RT on a Nonius KappaCCD
single crystal diffractometer by using MoKa radiation (l=0.71073 ꢈ).
Images were collected at a 40 mm fixed crystal–detector distance (oscilla-
tion method) with 18 oscillation and 20 s exposure time per image. Data
collection strategy was calculated with the program Collect.[43] Data re-
duction and cell refinement were performed with the programs HKL
Denzo and Scalepack.[44] A semi-empirical absorption correction was ap-
plied by using the program SORTAV.[45] The software package
WINGX[46] was used for space group determination, structure solution,
and refinement. The structure for the complex 2c was solved by Patter-
son interpretation and phase expansion by using DIRDIF.[47] The crystal
structure of 1 f was solved by direct methods by using the program SIR-
92.[48] Anisotropic least-squares refinement was carried out with
SHELXL-97.[49] All non-hydrogen atoms were anisotropically refined.
The coordinates of the hydrogen atoms for 2c were geometrically located
and their coordinates were refined riding on their parent atoms. The co-
ordinates of the hydrogen atoms for 1 f were found from different Fouri-
Complex 1 f: At RT, a stoichiometric amount of indazole (0.64 mmol)
was added to a solution of complex 1 (0.200 g, 0.32 mmol) in CH2Cl2
(20 mL). The mixture was stirred for 10 min, the solvent was removed
under vacuum and the resultant orange solid was washed with hexane
(3ꢇ10 mL) and dried in vacuo (64%, 175 mg). 1H NMR (300 MHz,
CD2Cl2): d=2.36 (s, 6H; 2ꢇCH3), 2.45 (m, 2H; H4 and H6), 3.12 (m, 2H;
H5 and H7), 4.38 (s, 2H; H2 and H10), 4.50 (s, 2H; H1 and H9), 5.24 (m,
2H; H3 and H8), 7.20 (t, J=7.5 Hz, 1H; H5 L), 7.43 (t, J=7.8 Hz, 1H; H6
L), 7.52 (d, J=7.8 Hz, 1H; H7 L), 7.76 (d, J=7.5 Hz, 1H; H4 L), 8.90 (s,
1H; H3 L), 12.20 ppm (s, 1H; NH); 13C NMR (75 MHz, CD2Cl2): d=21.0
(s; 2ꢇCH3), 36.7 (s; C4 and C5), 77.0 (s; C1 and C8), 95.2 (s; C3 and C6),
109.8 (s; C7 L), 120.6 (s; C5 L), 121.5 (s; C4 L), 123.6 (s; C3a L), 128.0 (s;
C6 L), 130.7 (s; C2 and C7), 138.6 (s; C3 L), 141.0 ppm (s; C7a L); IR
(KBr): n˜ =662 (m) 745 (vs), 867 (m), 950 (s), 1239 (m), 1352 (vs), 1382
(m), 1436 (m), 1506 (m), 1624 (s), 2852 (w), 2913 (m), 3295 cmꢀ1 (s); ele-
mental analysis calcd (%) for RuC17H22Cl2N2: C 47.89, H 5.20, N 6.57;
found: C 47.89, H 5.27, N 6.46.
er maps and included in a refinement with isotropic parameters. The
1
2
2
2
function minimised was ([Sw
(Fo ꢀFc2)/Sw
E
2
AHCTUNGTRENNUNG
(Fo )+(aP)2+bP] (a and b values are collected in Table S1, see the Sup-
2
2(Fo ) from counting statistics and P=(max-
porting Information) with s ACHTGNURTENNUGN
2
AHCTUNGTRENNUNG
(Fo , 0)+2Fc2)/3.
Atomic scattering factors were taken from the International Tables for
X-Ray Crystallography.[50] The crystallographic plots were made with
PLATON.[51]
CCDC-850286 (1 f) and 850287 (2c) contain the supplementary crystallo-
graphic data for this paper. These data can be obtained free of charge
c.uk/data_request/cif.
Computational details: All of the theoretical studies were performed by
DFT calculations. Beckeꢅs three-parameter exchange functional (B3),[52]
in conjunction with the Lee–Yang–Parr correlation functional (LYP),[53]
was employed as implemented in Gaussian 03.[54] In all geometry optimi-
sations the effective core potential LANL2DZ, along with its associated
basis set, complemented by a series of f polarisation functions was em-
ployed for Ru,[55] the 6-31G(d) basis set was used for all of the non-hy-
(h6-C6Me6)}2] (134 mg, 0.2 mmol)
Complex 2c: A mixture of [{RuClACTHNUGTRENNUG(m-Cl)HCATUNGTRENNGUN
and 3,5-dimethylpyrazole (0.64 mmol) in toluene (6 mL) was heated at
reflux temperature for 12 h. The solvent was removed under vacuum and
the resultant orange solid was recrystallised from CH2Cl2/hexane and
dried in vacuo (55%, 94 mg). 1H NMR (300 MHz, CDCl3): d=2.07 (s,
18H; C6Me6), 2.29 (s, 3H; 3-Me), 2.38 (s, 3H; 5-Me), 5.98 (s, 1H; CH),
11.01 ppm (s, 1H; NH); 13C NMR (75 MHz, CDCl3): d=10.7 (s; 3-Me),
14.6 (s; 5-Me), 15.5 (s; 6ꢇCH3), 91.0 (s; 6ꢇCipso), 107.5 (s; CH), 142.6 (s;
C3 L), 153.8 ppm (s; C5 L); IR (KBr): n˜ =553 (w), 614 (w), 659 (m), 696
(m), 740 (w), 799 (s), 833 (w), 1024 (s), 1043 (m), 1069 (m), 1149 (m),
1242 (w), 1274 (vs), 1381 (s), 1419 (m), 1457 (m), 1570 (vs), 2920 (m),
3018 (m), 3135 (m), 3217 cmꢀ1 (vs); elemental analysis calcd (%) for
RuC17H26Cl2N2: C 47.44, H 6.09, N 6.51; found: C 47.29, H 6.01, N 6.47;
drogen atoms, the 6-31GACTHNUTRGNEUGN(d,p) basis set for the hydrogen atoms of the
aqua and pyrazole ligands, as well as the substrates, and the 6-31G basis
set for the rest of the hydrogen atoms.[56] Vibrational frequencies were
computed to characterise the transitions states and the energy minima, as
well for the calculation of gas-phase Gibbs energies. The connections be-
tween transition states and their corresponding reactants and products
were checked by fully optimising structures derived from the transition
states with a small displacement following the transition vector in both
directions.
conductivity (water, 208C): 124 Wꢀ1 cm2 molꢀ1
.
General procedure for the catalytic isomerisation of allylic alcohols into
carbonyl compounds: In a sealed tube, the appropriate allylic alcohol
(4 mmol), ruthenium catalyst precursor (0.2–10 mol%), and co-catalyst
The energies in solution (DEsol) of all species were then estimated by the
application of single-point calculations at the gas-phase optimised sta-
7762
ꢄ 2012 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
Chem. Eur. J. 2012, 18, 7749 – 7765