5136 Organometallics, Vol. 16, No. 24, 1997
Communications
acid to form the corresponding (p-aminophenyl)ruthe-
nium complex.7 Using similar reaction conditions,
excess zinc and hydrochloric acid followed by base,
compound 2 also undergoes reduction to give the η2-acyl
complex Ru(η2-C[O]C6H4NH2-4)Cl(CO)(PPh3)2 (3) (see
Scheme 1). The electron-donating nature of the p-
aminophenyl ligand leads to a weakening of the metal-
carbon bond, and the migratory insertion reaction then
becomes favorable. The solid-state IR spectrum of 3
shows two very weak ν(CO) bands at 2035 and 1955
cm-1 and one strong ν(CO) band at 1910 cm-1
addition, an acyl ν(CO) band of medium intensity is
observed at 1526 cm-1
The solution spectrum, in
. In
.
dichloromethane, suggests that the ratio of the dicar-
bonyl complex to the acyl-monocarbonyl complex is less
1
F igu r e 1. ORTEP diagram of compound 3 (hydrogen
atoms except those on N omitted for clarity). Selected bond
distances (Å) and angles (deg): Ru-C(1), 1.799(3); Ru-
C(2), 1.958(3); Ru-P(2), 2.3691(9); Ru-P(1), 2.3704(9); Ru-
O(2), 2.375(2); Ru-Cl, 2.4786(8); N-C(6), 1.366(5); C(2)-
Ru-O(2), 31.68(9); P(2)-Ru-P(1), 177.21(3).
than 1:15. The amine protons, in the H NMR, appear
as a broad singlet at δ 3.9. This broad signal disappears
upon addition of deuterium oxide. The 13C NMR data
supports a η2-acyl formation. Only two downfield
signals are observed, both as triplets.8 These cor-
respond to the metal-bound carbonyl and acyl carbons,
respectively, which both couple to the phosphorus atoms
of the two mutually trans triphenylphosphine ligands.
The X-ray crystal structure determination of 3 confirms
the η2-coordination mode, and the structure is depicted
in Figure 1.9
When compound 3 is treated with excess HBF4, the
amino group is protonated and thereby becomes electron
withdrawing in nature. As a consequence, the aryl
group migrates back to the metal center, forming the
dicarbonyl complex 4. The solution IR spectrum of 4
shows that only the dicarbonyl complex exists in solu-
tion. Intense ν(CO) bands at 2040 and 1972 cm-1 are
observed. The 13C NMR spectrum of 4 shows three
downfield signals, each of which appears as a triplet.
These arise from the the two carbonyl ligands and the
metal-bound aryl carbon.8
Deprotonation of 4 was easily achieved by treatment
with the strong organic base 1,8-diazabicyclo[5.4.0]-
undec-7-ene (DBU), and the acyl monocarbonyl com-
pound 3 was recovered in excellent yield. This migra-
tory insertion reaction, therefore, could be manipulated
by simply adding acid or base (Scheme 1). In this
reversible process the steric effects remain essentially
constant and so it is the electronic nature of the para
substituent which determines the migratory aptitude
of the aryl ligand. Finally, we note that this facile
migratory insertion is not exhibited by the correspond-
ing osmium system, since Os(C6H4NH2-4)Cl(CO)2-
(PPh3)2 exists exclusively in this dicarbonyl form.10 The
synthesis and further reactions of this compound will
be reported subsequently.
(8) Selected spectroscopic data for 2-4 are as follows. 2: IR (KBr)
ν(CO) 2041 (s) and 1971 (s), ν(NO2) 1435 (ms) and 1339 (s), δ(NO2)
850 (w), δ(CH) 840 (w) cm-1 1H NMR (CDCl3, 400.1 MHz) δ 7.41-
;
7.22 (m, PPh3, C6H4NO2); 13C NMR (CDCl3, 100.6 MHz) δ 198.0 (t,
2J (PC) ) 12.1 Hz, CO), 193.7 (t, 2J (PC) ) 9.1 Hz, CO), 174.2 (t, 2J (PC)
) 12.6 Hz, C1), 144.7 (s, C4), 141.8 (s, C2 or C3), 119.6 (s, C2 or C3),
131.3 (t′11 J (PC) ) 46.3 Hz, PPh3 ipso-C), 134.1 (t′, J (PC) ) 10.1 Hz,
PPh3 m-C), 130.3 (s, PPh3 p-C), 127.9 (t′, J (PC) ) 9.1 Hz, PPh3 o-C). 3:
IR (KBr) ν(NH2) 3462 (w, br) and 3347 (wm, br), ν(CO) 2035 (w), 1955
(w), and 1910 (s), acyl ν(CO) 1526 (m), ν(CN) 1302 (wm) and 918 (ms),
δ(CH) 837 cm-1; 1H NMR (CDCl3, 400.1 MHz) δ 7.59-7.54, 7.36-7.23
(m, PPh3), 6.86 (d, 3J (HH) ) 8.6 Hz, 2,6-C6H4NH2), 6.09 (d, 3J (HH) )
8.6 Hz, 3,5-C6H4NH2), 3.9 (s, br, NH2); 13C NMR (CDCl3, 100.6 MHz)
δ 245.8 (t, 2J (PC) ) 8.0 Hz, η2-CO), 211.4 (t, 2J (PC) ) 16.6 Hz, CO),
150.3 (s, C1), 132.8 (s, C2 or C3), 125.5 (s, C4), 112.8 (s, C2 or C3),
131.9 (t′, J (PC) ) 45.3 Hz, PPh3 ipso-C), δ 134.3 (t′, J (PC) ) 11.1 Hz,
PPh3 m-C), 129.9, (s, PPh3 p-C), 128.0 (t′, J (PC) ) 10.1 Hz, PPh3 o-C).
Ack n ow led gm en t. We thank The University of
Auckland for the award of a Doctoral Scholarship and
The New Zealand Vice-Chancellors Committee for the
award of a William Georgetti Scholarship to V.P.D.Y.
The University of Auckland Research Committee pro-
vided grants-in-aid toward this work.
+
4: IR (KBr) ν(NH3+) 3133 (w, br), NH3 overtone 2590 (w, br), ν(CO)
-
2040 (s) and 1972 (s), δ(NH3+) 1623 (w), BF4 1091 (s, br), δ(CH) 803
cm-1; 1H NMR (CD3COCD3, 400.1 MHz) δ 13.13 (s, br NH3+), δ 7.56-
+
7.34 (mult, PPh3, 2,6-C6H4NH3 or 3,5-C6H4NH3+), 6.73 (d, 3J (HH) )
7.5 Hz, 2,6-C6H4NH3+ or 3,5-C6H4NH3+); 13C NMR (CD3COCD3, 100.6
MHz) δ 199.0 (t, 2J (PC) ) 12.6 Hz, CO), 195.1 (t, 2J (PC) ) 9.1 Hz,
CO), 163.8 (t, 2J (PC) ) 12.6 Hz, C1), 143.4 (s, C2 or C3), δ 131.8 (s,
C4), 121.97 (s, C2 or C3), 132.8 (t′, J (PC) ) 46.3 Hz, PPh3 ipso-C),
135.1, (t′, J (PC) ) 10.1 Hz, PPh3 m-C), 131.6 (s, PPh3 p-C), 128.8 (t′,
J (PC) ) 9.1 Hz, PPh3 o-C).
Su p p or tin g In for m a tion Ava ila ble: A fully labeled
diagram and tables of crystallographic data, data collection,
and solution and refinement details, positional and thermal
parameters, and bond distances and angles for 3 (10 pages).
Ordering information is given on any current masthead page.
(9) Crystals were obtained from CH2Cl2/EtOH by the isopiestic
method. Crystal data for 3 (from 25 reflections, 11.5° < θ < 12.7°):
triclinic, space group P1h, a ) 12.104(1) Å, b ) 13.565(2) Å, c ) 13.700-
(6) Å, R ) 66.17(2)°, â ) 78.85(2)°, γ ) 68.450(10)°, V ) 1911.2(9) Å3;
Z ) 2, Dcalcd ) 1.406 g cm-3, (µ(Mo KR) ) 0.602 mm-1); crystal size
0.29 × 0.19 × 0.14 mm; Enraf-Nonius CAD4 diffractometer, Mo KR
radiation (0.710 69 Å), graphite monochromator, T ) 295(2) K, ω/2θ
scans, maximum 2θ 54°, 8690 reflections measured, 8333 independent
with R(int) ) 0.0369, intensity data corrected for Lorentz and polariza-
tion effects. An empirical absorption correction (ψ scans, transmission
range 0.952-0.998) was applied.12 The structure was solved by direct
methods (SHELXS-86);13 atomic coordinates and anisotropic thermal
parameters were refined by full-matrix least squares on Fo2 (SHELXL-
96).14 Positions of all hydrogen atoms were located crystallographically
and refined with isotropic thermal parameters. R ) 0.0358 for I > 2σ-
(I), wR2 ) 0.0902. R indices (all data): R ) 0.0619, wR2 ) 0.1008;
reflections/restraints/parameters ratio 8333/0/604; residual electron
OM970714R
(10) Roper, W. R.; Wright, L. J .; Yap, V. P. D. To be submitted for
publication.
(11) Maddock, S. M.; Rickard, C. E. F.; Roper, W. R.; Wright, L. J .
Organometallics 1996, 15, 1793.
(12) North, A. C. T.; Phillips, D. C.; Mathews, F. S. Acta Crystallogr.
1968, A24, 351.
(13) Sheldrick, G. M. SHELXS-86. Crystallographic Computing 3;
Sheldrick, G. M., Ed.; Oxford University Press: Oxford, U.K., 1995; p
175.
density +0.848/-0.687 e Å-3. wR2 ) [Σw(Fo - Fc2)2/Σw(Fo2)2]1/2; w-1
(14) Sheldrick, G. M. SHELXL-96; University of Go¨ttingen, Go¨ttin-
gen, Germany, 1996.
2
2
) σ2(Fo2) + (0.0602P)2 + 0.5257P, where P ) (Fo + 2Fc2)/3.