Reactions of ZnR2 Compounds with Dibenzoyl
FULL PAPER
Diffusivity measurement: Application of diffusion-ordered spectroscopy
(DOSY), which has happened to become a very routine NMR technique
lately, provided us with a reliable evidence of approximate size of the
species existing in solution. As already discussed in antecedent works[13]
the molecular weight can be straightforwardly obtained by combining
Stokes–Einstein equation [Eq. (1)] and the relationship between molecu-
lar weight M and molar radius [Eq. (2)]. It has also been shown that
these quantities are much alike for small molecules, which is the case in
our system. DOSY measurements were performed in dry and degassed
[D8]toluene as we exploited the fact that the physical properties of the
diluted solution, namely density and viscosity, deviate only slightly from
the properties of the pure solvent.[13] Solutions were prepared so that the
concentration of the resulting species emerging in the course of the reac-
tion was approximately 0.01m. A pulsed field gradient double-stimulated
echo convection-compensated sequence with total of 15 diffusion encod-
ing gradients (ranging from 3–45 Gcmꢀ1, sine shaped, equal steps in gra-
dient squared) was used and the total width of the gradient pulse was op-
timised to achieve attenuation of about 90% of the initial intensity of the
signals. Overall, the key acquisition parameters were as follows: total
length of gradient encoding pulses gradient: 2 ms, diffusion delay: 50 ms,
gradient recovery delay: 1 ms, relaxation delay: 2 s. Steady-state scans in
number of 16 were performed prior to data acquisition. The sample was
allowed to equilibrate in the set temperature (298 K), controlled by a VT
module. Spinner was turned off. Raw data were processed with a power-
ful DOSY toolbox, which is extensively described in the literature.[21]
(m, 18H; CACHTUNGTREU(NNG CH3)3), 7.51 (m, 4H; CHAr), 7.69 (m, 2H; CHAr), 7.97 ppm
(m, 4H; CHAr).
Low temperature reaction of dibenzoyl with Et2Zn (2): Et2Zn (0.09 mL,
0.111 g, 0.90 mmol) was added to a yellowish solution of dibenzoyl
(0.189 g, 0.90 mmol) in diethyl ether (6 mL) at ꢀ208C. The reaction mix-
ture was slowly warmed up to room temperature over 1 h and the reac-
tion mixture was stirred for further 36 h at room temperature. The sol-
vent was removed from the resulting intensively yellow reaction mixture
under reduced pressure to give the crude product 2 as a white solid.
1H NMR (500 MHz, [D8]toluene, ꢀ308C): d=0.40 (2H; Zn(1)CH2), 0.60
(brs, 2H; Zn(2)CH2), 0.92 (brs, 3H; Zn(2)CH2CH3), 1.10 (3H;
Zn(1)CH2CH3), 1.64 (3H; O(1)CH2CH3), 1.70 (brs, 3H; O(2)CH2CH3), 3.54
(brs, 2H; O(2)CH2CH3), 3.67 (2H; O(1)CH2CH3), 6.70–8.20 ppm (m, 10H;
CHAr); 13C NMR (500 MHz, [D8]toluene, 208C): d=0.01 (br), 6.22 (br),
6.90, 10.49 (br), 13.37 (br), 15.16, 65.84, 80.69, 133.6, 133.8, 134.3 (d),
137.4, 139.4, 139.7, 142.0, 146.6, 208.8, 209.8 ppm. Then NaHCO3 was
added to the crude product and the resulting mixture was stirred for
30 min. Toluene (5 mL) was added and after evaporation of the solvents
under reduced pressure the organic residue was analysed by 1H NMR
spectroscopy (for the data description see the text below and Figure S1a
in the Supporting Information).
Room-temperature reaction of dibenzoyl with Et2Zn (2 and 2’): Et2Zn
(0.09 mL, 0.111 g, 0.90 mmol) was added to a yellowish solution of diben-
zoyl (0.189 g, 0.90 mmol) in diethyl ether (6 mL) at room temperature
and the reaction mixture was stirred for 36 h. The solvent was removed
from the resulting intensively yellow reaction mixture under reduced
pressure to give a mixture of crude product 2 and 2’ as a white solid. The
1H NMR spectrum of the reaction mixture was complicated and not in-
formative, the alkylation products were identified spectroscopically after
hydrolysis: NaHCO3 was added to the crude product and the resulting
mixture was stirred for 30 min. Toluene (5 mL) was added and after
evaporation of solvents under reduced pressure the organic residue was
analysed by 1H NMR spectroscopy (for the data description see the text
below and Figure S1b in the Supporting Information). The resulting
1H NMR spectra of the organic residue obtained from hydrolysis of reac-
tion mixture confirm the anticipated O-alkylated and C-alkylated prod-
ucts: 2-hydroxy-1,2-diphenylbutan-1-one (2) and 2-ethoxy-1,2-diphenyl-
Computational details: The geometry of all molecules was optimised by
density functional theory[22] by using the Gaussian 09[23] package. Geome-
try optimisations were carried out by using standard gradient methods
(Berny algorithm) with the M06-2X functional[24] and the Dunning-like
aug-cc-pVDZ[25] double-zeta basis set. Optimisations were performed
without constrains apart from the s-cis conformation of dibenzoyl, where
the O-C-C-O dihedral angle was frozen (0.08) (as a consequence, this ge-
ometry does not correspond to a minimum at the potential energy sur-
face). To validate locations of stationary points, all freely optimised geo-
metries were subjected to frequency calculations (by using analytical
methods) at the same level of theory and in the same basis set as optimi-
sations were performed. As a result, zero-point energies for all species
apart from the s-cis conformation of dibenzoyl, were obtained. For all
freely optimised geometries nuclear hessian had only positive eigenvalues
(corresponding to energy minima). To improve the accuracy of the ener-
getic results, single point DFT energy recalculations were performed on
previously optimised structures by using the same exchange–correlation
functional but with extension of the basis set to triple zeta quality—aug-
cc-pVTZ.[25] These re-calculations were performed by using automatic
correction for BSSE (basis set superposition error) with a counterpoise
(Boys–Bernardi) method.[26, 27] During all optimisations the aug-cc-pVDZ
basis set was used. Spherical harmonics basis set functions were used
throughout and the linear dependence of the basis set functions was not
observed. To provide reliable results of both geometry optimisations and
energy calculations grid used for numerical integration of the DFT equa-
tions (both self-consistent field and gradient/hessian) was extended to
126 radial points and 770 angular points per atom (which roughly corre-
sponds to extension by a factor of two compared to the default Gaussi-
an 09 options). At the stage of geometry optimisations, no correction for
BSSE was introduced. This approximation is fully justified by further
single-point energy re-calculations corrected for BSSE—in all cases
BSSE was small (usually less than 4 kJmolꢀ1), so its influence on the re-
sulting geometries is clearly insignificant. Final energetic relations were
obtained by using results from re-calculations at the aug-cc-pVTZ level
(corrected for BSSE) and ZPE computed at aug-cc-pVDZ level. Solvent
effects were not included at any stage of the calculations (for the results
of the DFT calculations see the Supporting Information).
AHCTUNGERTGeNNUN thanone (2’). The latter compound exists in a keto–enol equilibrium in a
ratio of 1:1.5. 2-hydroxy-1,2-diphenylbutan-1-one (2): 1H NMR
(400 MHz, [D6]benzene, 208C): d=0.80 (t, J=7.3 Hz, 3H; CH3), 2.24 (m,
2H; CH2), 4.34 (brs, 1H; OH), 6.50–7.30 ppm (m, 10H; CHAr); 2-
ethoxy-1,2-diphenylethanone (2’), keto form: 1H NMR ([400 MHz,
3
[D6]benzene, 208C): d=1.05 (t, J
N
CH2), 5.41 (s, 1H; CH) 6.50–7.30 ppm (m, 10H; CHAr); enol form:
1H NMR (400 MHz, [D6]benzene, 208C): d=0.99 (t, 3J
(H,H)=7.3 Hz,
3H; CH3), 4.10 (q, 3J
(H,H)=7.3 Hz, 2H; CH2), 5.77 (brs, 1H; OH),
6.50–7.30 ppm (m, 10H; CHAr).
{[12][1,2-bis(4-pyridyl)ethane]}n (3): Et2Zn (0.45 mL, 0.90 mmol, 2m solu-
AHCTUNGTRENNUNG
AHCTUNGTRENNUNG
AHCTUNGTRENNUNG
tion in THF) was added to a solution of dibenzoyl (0.189 g, 0.90 mmol)
and 1,2-bis(4-pyridyl)ethane (0.083 g, 0.45 mmol) in THF (5 mL) at
ꢀ788C . The reaction mixture was warmed up to room temperature.
During this time precipitation of light yellow crystals was observed. The
reaction mixture was stirred at room temperature for 2 h. The solvents
were removed under reduced pressure. The Remaining solid was dis-
solved in THF (1.5 mL) and hexane (1 mL) was added. The solution was
left for crystallisation at room temperature. Colourless crystals suitable
for X-ray analysis were obtained after 24 h in 75% yield. 1H NMR
(400 MHz, CDCl3, 208C): d=0.85 (4H; ZnCH2CH3), 1.26 (6H;
ZnCH2CH3), 1.30 (6H; OCH2CH3), 2.97 (m, 4H; CH2CH2), 3.88 (4H;
OCH2CH3), 7.10 (m, 8H; CHAr), 7.11 (m, 4H; CHpyridyl), 7.13 (m, 4H;
CHAr), 7.45 (m, 8H; CHAr), 8.46 ppm (m, 4H; CHpyridyl).
X-ray structure determination: The data were collected at 100(2) K on a
Nonius Kappa CCD diffractometer[28] by using graphite monochromated
MoKa radiation (l=0.71073 ꢁ). The crystals were mounted in a nylon
loop in a drop of silicon oil to prevent the possibility of decay of the crys-
tals during data collection. The unit cell parameters were determined
from ten frames, then refined on all data. The data were processed with
DENZO and SCALEPACK (HKL2000 package).[29] The structure was
ACHTUNGTRENNUNG[tBuZnACHTUNGTRENNUNG{PhC(O)CACHTUNGTRENNUNG(OtBu)Ph}] (1): tBu2Zn (87.7 mg, 0.49 mmol) in THF
(0.35 mL) was added to a solution of dibenzoyl (0.104 g, 0.49 mmol) in
THF (5 mL) at ꢀ788C. The reaction mixture was left to warm up to
room temperature and stirred for 2 h. After 24 h of crystallisation from
THF/hexane at ꢀ158C colourless crystals suitable for X-ray analysis
were obtained in 70% yield. 1H NMR (400 MHz, CDCl3, 208C): d=1.28
Chem. Eur. J. 2011, 17, 12713 – 12721
ꢀ 2011 Wiley-VCH Verlag GmbH & Co. KGaA, Weinheim
12719