412
J . Org. Chem. 1998, 63, 412-413
Communications
configuration (Scheme 1, 4A) preferred to have both naph-
thalene rings at 68° and the oxazolines almost orthoganol
to the naphthalenes. The oxazoline rings did not appear to
show any rotation about the connecting C-C bond (Scheme
1A, bond a), for this would place the tert-butyl groups into
the π-face of the naphthalene rings. Since the 3:1 mixture
of 4:5 returns to >98% 4 at room temperature, this supports
the earlier report5 that the activation barrier to atropi-
somerization of many 1,1′,8,8′-binaphthyls is rather low.
This is especially so when sp2 substituents are present at
the 8,8′ position. The barrier is much higher with sp3
substituents OH and OMe, since they present greater
volume during the rotation, and these derivatives have
indeed been resolved into enantiomers.6-8 Fuji4 also re-
ported facile atropisomerization in similar systems contain-
ing phosphorus substituents and attributes the behavior to
distortion from planarity in the naphthalene rings, which
was confirmed by X-ray data. Careful examination of the
X-ray structure of 42 showed no such distortion in the
naphthalene rings so the stability of 4 as the only atropi-
somer at room temperature must be due to other factors
(vide supra).
Th e Un iqu e Beh a vior of a Ch ir a l Bin a p h th yl
Oxa zolin e in th e P r esen ce of Cu (I) a n d Its
Role a s a Ch ir a l Ca ta lyst
A. I. Meyers* and Alan Price
Department of Chemistry, Colorado State University,
Fort Collins, Colorado 80523-1872
Received September 22, 1997
We have been engaged for several years in the acquisition
of chiral binaphthyls from the Ullmann coupling of 1-bromo-
2-oxazolinylnaphthalenes 11 and 8-bromo-1-oxazolinylnaph-
thalenes 3.2 In both cases, the binaphthyl coupling products
2 and 4, respectively, were obtained in high diastereoselec-
tivity (>99%).1,2 In view of the large effort expended by a
Although the low barrier to rotation in 4 to 5 may preclude
its use as a chiral catalyst, we still felt further study was
necessary. We were surprised to learn that when the
Ullmann coupling was performed in DMF in place of
pyridine, th e sole p r od u ct obtained was the aR-atropiso-
mer 5, with none of the aS-derivative detectable by NMR.2
When the copper salts were removed on workup, the aR-
atropisomer was stable as a crystalline solid at room
temperature for several hours and indefinitely at -20 °C.
However, when dissolved in various solvents at room tem-
perature, it was rapidly and completely transformed back
to the aS-isomer 4. Of most interest was the ability to
transform 4 back to 5 only after heating a DMF solution to
90-100 °C containing 1.0 equiv of CuBr. A solution of the
copper complex of 5 in CDCl3 at room temperature was also
found to be stable to atropisomerization indefinitely.
The reasons for this behavior are now more clearly
revealed in light of these data. For example, when 1 was
transformed into 2, only the aS-atropisomer was formed, and
this was explained earlier1 by assuming the Cu was holding
the two ligands (oxazoline nitrogen) in a manner that
minimized all nonbonded interactions. Furthermore, the
barrier for aryl-aryl rotation in 2 is very high so the
kinetically controlled product was the only one formed and
isolated. In the present case of naphthyloxazoline 3, when
the coupling is carried out in pyridine, we were surprised
to find that 4 and not 5 was the product, even though the
latter is capable of readily forming a bidentate oxazoline
complex to copper. We, therefore, attributed the formation
of 4 to buttressing of the tert-butyl groups.1 In light of the
present results, pyridine may compete with the oxazolines
for the copper ion (R-configuration). In the absence of copper
ion, 5 can suffer lone-pair repulsion from both oxazoline
nitrogens, resulting in atropisomerization to 4A. On the
other hand, using DMF to couple 3, the kinetically formed
number of laboratories to utilize chiral binaphthyls, mainly
of the type depicted by 2, as chiral catalysts, we have focused
our recent attention on the more rarely studied4 1,1′,8,8′-
systems, 4. In our recent preliminary report,2 we showed
that the chiral bromo derivative 3 gave, upon heating in
refluxing pyridine containing activated copper powder, the
single diastereomer (aS,S)-4 which was quite stable to
atropisomerism, even after heating for prolonged periods.
Surprisingly, heating 4 for 24 h at 145 °C gave a mixture of
4 and 5 in a 75:25 ratio, only to return to 4 upon standing
at room temperature. An X-ray structure2 of 4 showed that
(1) Nelson, T. D.; Meyers, A. I. J . Org. Chem. 1994, 59, 2655.
(2) Meyers, A. I.; McKennon, M. J . Tetrahedron Lett. 1995, 36, 5869.
(3) For recent reviews see: (a) Rossini, C.; Fannzini, L.; Raffaelli, A.;
Salvadori, P. Synthesis 1992, 503. (b) Narasaka, K. Synthesis 1991, 1. (c)
Tomioka, K. Synthesis 1990, 541.
(4) Fuji, K.; Sakurai, M.; Tohkai, N.; Kuroda, A.; Kawabata, T.; Fuka-
zawa, Y.; Kinoshita, T.; Tada, T. J . Chem. Soc., Chem. Commun. 1996, 1609.
(5) Harris, M. M.; Patel, P. K.; Korp, J . D.; Bernal, I. J . Chem. Soc., Perkin
Trans. 2 1981, 12, 1621 and earlier references cited.
(6) Fabbri, D.; Delogu, G.; DeLucchi, O. J . Org. Chem. 1995, 60, 6599.
(7) Fuji, K.; Kawabata, T.; Kuroda, A.; Taga, T. J . Org. Chem. 1995, 60,
1914.
(8) Artz, S. P.; deGrandpre, M. P.; Cram, D. J . J . Org. Chem. 1985, 50,
1486.
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