geometries, with the sum of the three angles subtended by
nitrogen approaching 360°. The metal center displays two short
zirconium–nitrogen bonds (Zr1–N1 = 2.131(5), Zr1–N3 =
2.043(5) Å) and one longer bond (Zr1–N2 = 2.410(5) Å)
consistent with a diamido-amino ligand. The benzyl groups are
unremarkable (Zr–C–Cbenzyl = 109.2(4), 114.7(4)°), although
1
they are inequivalent by H and 13C NMR spectroscopy. This
implies that the structure observed in the solid state is
maintained in solution, and the benzyl groups are not averaged
by some fluxional process as is observed for tribenzyl 3.
In order to test the generality of this reaction, (Pri2tacn)ZrCl3
1 was reacted with three equiv. of RLi (R = Me, CH2SiMe3,
Ph). The NMR spectra of these products also indicate the
formation of [CH2NCHNCH2CH2N(Pri)CH2CH2NPri]ZrR2
with the elimination of the corresponding alkane. A related
ligand decomposition has been observed for the tantalum
species [N3N]TaMe2 ([N3N] = [N(CH2CH2NSiR3)3]32, R =
Me20, Et21). Thermolysis of the deuterated complex (Pri2-
tacn)Zr(CD2C6D5)3 affords C7D7H, ruling out a-hydrogen
abstraction and a benzylidene intermediate. A more detailed
study of the kinetics and mechanism of this ring-opening
reaction will be reported shortly, along with other examples of
the synthetic utility of (Pri2tacn2).
Fig.
2
ORTEP view of [CH2NCHNCH2CH2N(Pri)CH2CH2N-
Pri]Zr(CH2Ph)2 4 drawn with 50% probability ellipsoids. Selected bond
distances (Å) and angles (°): Zr1–N1 2.131(5), Zr1–N2 2.410(5), Zr1–N3
2.043(5), Zr1–C1 2.289(6), Zr1–C8 2.295(6), C15–C16 1.317(9); N1–Zr1–
N2 71.3(2), N1–Zr1–N3 142.3(2), N1–Zr1–C1 100.5(2), N1–Zr1–C8
94.3(2), N2–Zr1–N3 71.5(4), N2–Zr1–C1 124.3(2), N2–Zr1–C8 125.1(2),
N3–Zr1–C1 105.3(2), N3–Zr1–C8 101.9(2), C1–Zr1–C8 110.2(2), Zr1–
C1–C8 114.7(2), Zr1–C8–C9 109.2(4).
This work was supported by the Department of Energy
contract no. DE-AC03-76SF00098.
Notes and references
† Crystal data: for 3: C33H47N3Zr, M = 576.97, trigonal, a = 39.6517(3),
b = 39.6517(3), c = 9.7469(1) Å, V = 13 271.5(2) Å3, T = 173 K, space
group R-3(h) (no. 148), Z = 18, m(Mo-Ka) = 0.4 mm21, 20082 reflections
measured, 5097 unique (Rint = 0.035), Dcalc = 1.30 g cm23, R = 0.024, Rw
= 0.028. For 4: C26H39N3Zr, M = 484.83, monoclinic, a = 8.881(5), b =
25.936(2), c = 11.7707(7) Å, b = 112.017(1)°, V = 2513.5(6) Å3, T = 164
K, space group P21/c (no. 14), Z = 4, m(Mo-Ka) = 0.45 mm21, 11 204
reflections measured, 4314 unique (Rint = 0.082), Dcalc = 1.28 g cm23, R
cc/b0/b005675h/ for crystallographic files in .cif format.
ligands are positioned with their phenyl rings pointing down-
wards with respect to the tacn ring, while the third has its phenyl
ring pointing upwards, being disposed almost parallel to the
azamacrocycle. Two of the benzyl groups possess normal Zr–
C–C bond angles (113.7(2) and 116.3(2)°) while the third
displays an angle that is larger than expected (Zr1–C15–C16 =
133.5(2)°). The disposition of the benzyl groups is similar to
that found for Cp*Ti(CH2Ph)3, in which a single anomalous Ti–
C–C angle is a consequence of a double agostic CH2–Ti
interaction.19 Owing to the broadness of the peak arising from
the benzylic methylene groups in the {1H}13C NMR spectrum,
we were unable to extract the C–H coupling constant to
determine if any additional interaction was present in our case;
it is likely that this unusually large angle is a result of packing
forces in the crystal.
1 G. J. P. Britovsek, V. C. Gibson and D. F. Wass, Angew. Chem., Int. Ed.,
1999, 38, 428.
2 R. Kempe, Angew. Chem., Int. Ed., 2000, 39, 468.
3 L. H. Gade, Chem. Commun., 2000, 173.
4 J. D. Scollard, D. H. McConville and J. J. Vittal, Organometallics, 1995,
14, 5478.
5 J. D. Scollard, D. H. McConville, N. C. Payne and J. J. Vittal,
Macromolecules, 1996, 29, 5241.
Heating (Pri2tacn)Zr(CH2Ph)3 3 for 24 h at 80 °C results in
elimination of one equiv. of toluene and complete conversion to
1
a new metal complex. The H NMR spectrum reveals a total
6 J. D. Scollard and D. H. McConville, J. Am. Chem. Soc., 1996, 118,
10 008.
lack of symmetry in solution as evidenced by the presence of
four isopropyl methyl doublets and separate multiplets for each
of the methylene protons of the ligand backbone. Particularly
diagnostic of this new species are resonances consistent with a
vinyl group; a doublet of doublets corresponding to one olefinic
proton is present at 7.92 ppm (3JH-HA = 8.4, 3JH-HB = 14.8 Hz)
with the other two protons of the vinyl unit giving rise to two
doublets farther upfield (4.12 ppm, 3JH-H’ = 8.4 Hz; 3.93 ppm,
3JH-H” = 14.8 Hz). These conclusions are supported by
{1H}13C NMR spectroscopy which shows four separate
isopropyl methyl peaks, two isopropyl methine resonances and
distinct peaks for four methylene groups of the ancillary ligand.
13C DEPT experiments allowed the vinyl resonances to be
assigned (143.1 and 79.0 ppm); the presence of a vinyl group is
visible in the IR spectrum which shows a strong absorption in
the olefinic region (ca. 1600 cm21).
7 F. G. N. Cloke, T. J. Geldbach, P. B. Hitchcock and J. B. Love,
J. Organomet. Chem., 1996, 506, 343.
8 C. H. Lee, Y. H. La and J. W. Park, Organometallics, 2000, 19, 344.
9 M. Aizenberg, L. Turculet, W. M. Davis, F. Schattenmann and R. R.
Schrock, Organometallics, 1998, 17, 4795.
10 R. Baumann, W. M. Davis and R. R. Schrock, J. Am. Chem. Soc., 1997,
119, 3830.
11 F. G. N. Cloke, P. B. Hitchcock and J. B. Love, J. Chem. Soc., Dalton
Trans., 1995, 25.
12 F. Guerin, D. H. McConville and J. J. Vittal, Organometallics, 1996, 15,
5586.
13 F. Guerin, D. H. McConville and N. C. Payne, Organometallics, 1996,
15, 5085.
14 F. Guerin, D. H. McConville, J. J. Vittal and G. A. P. Yap,
Organometallics, 1998, 17, 5172.
15 R. R. Schrock, F. Schattenmann, M. Aizenberg and W. M. Davis, Chem.
Commun., 1998, 199.
To further investigate the structure of the thermolysis
product, we turned to X-ray diffraction (Fig. 2).† The ORTEP of
4 shows that the zirconium center is coordinated by two benzyl
groups and a new tacn-derived pincer ligand in which the
original anionic, macrocyclic, diamino-amido ligand has been
transformed into a dianionic, acyclic, diamido-amino moiety.
Additionally, one of the ethylene units of the triazacyclononane
ring has been converted into a vinyl group (C15–C16). The
zirconium center is best described as distorted trigonal bipyr-
amidal, with N1 and N3 occupying the axial sites (N1–Zr1–N3
= 142.3(2)°). Both amido nitrogens in 4 display trigonal planar
16 M. D. Fryzuk, V. Hoffmann, J. E. Kickham, S. J. Rettig and S.
Gambarotta, Inorg. Chem., 1997, 16, 3480.
17 G. R. Giesbrecht, A. Gebauer, A. Shafir and J. Arnold, J. Chem. Soc.,
Dalton Trans., 2000, in press.
18 B Qian, L. M. Henling and J. Peters, Organometallics, 2000, 19,
2805.
19 M. Mena, M. A. Pellinghelli, P. Royo, R. Serrano and A. Tiripicchio,
J. Chem. Soc., Chem. Commun., 1986, 1118.
20 J. S. Freundlich, R. R. Schrock and W. M. Davis, J. Am. Chem. Soc.,
1996, 118, 3643.
21 J. S. Freundlich, R. R. Schrock and W. M. Davis, Organometallics,
1996, 15, 2777.
2136
Chem. Commun., 2000, 2135–2136