B. Quillian et al. / Journal of Organometallic Chemistry 691 (2006) 3765–3770
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C(1)–Al(1)–Br(1) and C(1)–Al(1)–Br(2) bond angles,
117.46(15)° and 120.10(15)°, respectively, are significantly
distorted from classical tetrahedral geometry and are closer
to predicted trigonal planar angles. Conversely, the Br(1)–
Al(1)–O(1) bond angle, 97.94(14)°, is much smaller than
the anticipated 109.5°. An interesting feature of 2 can be
seen along the Al–C(1) vector, which is bent away from
the phenyl ring plane by 15.54°(avg.). This distortion
may be due to packing forces in the crystal lattice, a factor
that allows flexibility in the ionic Al–C bond [20]. Compar-
ison of 2 with (2,6-(4-t-BuC6H4)2C6H3)AlH2(NMe3), 5, is
warranted, as it is the only 2,6-di(4-t-butylphenyl)phenyl-
aluminum compound [10]. The Al(1)–C(1) bond distance
˚
˚
in 2, 1.979(5) A, is shorter than that in 5 (2.018(2) A), but
compares well with the only other reported m-terphenyl
stabilized aluminum bromide etherate, RAlBr2 Æ OEt2,
˚
(R = 2,4,6-Ph3C6H2) (1.983(9) A) [20], and the organoalu-
minum bromide dimer, [RAlBr3Li]2 (R = 2,6-Mes2C6H3),
˚
1.96(2) A [21]. The structure of 2 shows that the Br(2) atom
is almost orthogonal with respect of the central phenyl
ring, and the two outer phenyl rings are tilted to it. The
˚
Al(1)–Br(1) bond distance in 2, 2.3175(17) A, is slightly
longer than the Al(1)–Br(2) bond, 2.3010(16) A, but both
Fig. 3. Molecular structure of (2,6-(4-t-BuC6H4)2C6H3)2GaCl, 3 (thermal
˚
ellipsoids are shown at 35% probability levels). Selected bond distances
are similar to those in RAlBr2 Æ OEt2 (R = 2,4,6-Ph3C6H2),
˚
(A) and angles (°): Ga(1)–C(1), 1.981(3); Ga(1)–C(27), 1.997(3); Ga(1)–
˚
(2.297(3) and 2.302(3) A), but slightly shorter than those in
Cl(1), 2.2537(10); C(1)–Ga(1)–C(27), 137.37(12); C(1)–Ga(1)–Cl(1),
106.69(9); C(27)–Ga(1)–Cl(1), 115.76(9).
˚
[RAlBr3Li]2, (R = 2,6-Mes2C6H3), (mean 2.347 A) [21].
Compound 3 joins a small group of R2GaX compounds,
(R = m-terphenyl, X = halide) [14,16,22], although a series
of analogous hydrides, alkyls, and a hydroxyl have been
reported [17]. The gallium atom in 3 is three-coordinate
in a distorted trigonal planar environment (Fig. 3). Corre-
spondingly, other R2GaX compounds (R = 2,6-Ph2C6H3;
X = I [16], and R = 2,6-Mes2C6H3; X = Cl [22], Br [14]),
all have distorted trigonal planar environments around
the gallium metal center. The C–Ga–Br bond angles in
(2,6-Mes2C6H3)2GaBr, are identical (101.8(2)°). Similarly,
the chloride analogue has C–Ga–Cl bond angles of
103.2(4)° and 103.4(4)°. However, the corresponding
C(1)–Ga(1)–Cl(1) and C(27)–Ga(1)–Cl(1) bond angles in
3, 106.69(9)° and 115.76(9)°, respectively, are asymmetric.
The C(1)–Ga(1)–C(27) bond angle of 3, 137.37(12)°, is lar-
ger than the C(1)–Ga(1)–C(1a) bond angle (134.3(3)°) in
(2,6-Ph2C6H3)2GaI, but expectedly smaller than that of
the ‘‘T shaped’’ (2,6-Mes2C6H3)2GaX (X = Cl, Br) com-
pounds (153.5°). The Ga(1)–C(1) and Ga(1)–C(27) bond
formation of 4 from reaction of RLi and InCl3 in a 1:1
ratio is interesting. The poor solubility of InCl3 may have
been a factor in the preparation of 4. The sharp melting
point and accurate elemental analysis is indicative of 4
being the sole product. Consideration of the X-ray
structure of 4 provides an interesting contrast from the
organo/group 13 halides discussed above (Fig. 4). Com-
pound 4 crystallizes as a monomer with one molecule of
diethyl ether per asymmetric unit. The indium atom in 4
is in a distorted trigonal planar coordination environment
with C–In–C angles of C(1)–In(1)–C(27), 114.77(13)°;
C(1)–In(1)–C(53),
120.34(12)°;
C(27)–In(1)–C(53),
124.83(13)° and are similar to those in trimesitylindium,
Mes3In [29], and triphenylindium, Ph3In [30,31]. However,
a twofold axis was observed for Ph3In that is not evident in
4. The three ligands in 4 are arranged about the indium
atom in a propeller like fashion and are not crystallograph-
ically equivalent due to differing dihedral angles with
respect to the InC3-core plane. The dihedral planes were
found to be 39.84°, 31.95°, and 65.37° for the C(1), C(27)
and C(53) central phenyl ring planes, respectively. The
˚
lengths in 3, 1.981(3) and 1.997(3) A, respectively, compare
well with other reported diarylgallium halides, while the
˚
Ga(1)–Cl(1) bond length in 3, 2.2537(10) A, is somewhat
˚
longer than that in (2,6-Mes2C6H3)2GaCl, 2.177(5) A.
˚
In–C bonds in 4 (In(1)–C(1), 2.200(3) A; In(1)–C(27),
With the growing utility of triorganoindium compounds
for fundamental organic transformations such as conjugate
addition [23], cross-coupling [24–26], and allylic substitu-
tion reactions [27,28], and the ubiquitous use of m-terphe-
nyl ligands in organometallic-group 13 chemistry, it is
noteworthy that there are no reports of tris(m-terphe-
nyl)indium compounds. Compound 4, the first tris
(m-terphenyl)group 13 compound, is noteworthy. The
˚
˚
2.199(3) A; In(1)–C(53), 2.193(3) A) are comparable to
˚
˚
˚
those in Mes3In (2.170(5) A; 2.170(5) A; 2.163(5) A), Ph3In
(2.111(14) A; 2.155(14) A), and (2,6-Mes2C6H3)2InBr
(2.171(25) A; 2.166(26) A) [32]. These values for 4 are com-
parable to those in [(2,6-Mes2C6H3)InCl2]2 (2.138(8) A)
˚
˚
˚
˚
˚
˚
[33] and [(2,6-(2,4,6-i-Pr3C6H2)2C6H3)InCl2]2 (2.129(5) A)
[15].