c+404020/91 s3.00+.~
TerrahrdronVol.47.No.41,p~.8139-8~521~1 RmtedinGrelu Britain
RRGIOSELECTIVITY
IN LITHIUM,
0
SODIUM
AND POTASSIDM
AN AS INITIO-TEEORETICAL Carlo
Glauco
Canepa,
Istituto
di Chimica
Via Pietro
and Paolo
Organica
Giuria,
CHLOROALLYL
AND BXPERIMRNTAL
Tonachini
7
dell'
I-10125
1991 Pagamon Press plc
SYSTEMS.
STUDY
Venture110
Universita‘
Torino,
Italy
(Received in UK 28 May 1991)
Abstract The comp;~~$u;tr~;$ural and,electronic features of the title describe the potassium elect%$f%s a?ha~orfhe'n%?~~ous carbonyl regioaelectivity with compounds. Some experimental results con irm this expectation.
;;rnpo;;$s 1ithiA
Introduction In the its reactivity This
system
reacting depending presents Ccl2
gem-dichloroallyl-lithium
last years atudied
has
with
experimentally
been
shown
carbonyl
to
attack
spectrum
to a complete
laboratory,3
providing
Ccl,-selectivity
an
Mauze'
hand
studied of
compounds
(Scheme
1).
when
Indeed,
it
from a complete the reactivity
experimentally
result
and
of attack
atom.
going
On the other
recently
products
carbon
interesting
carbonyl
nucleophile
different
distributions
synthesized
and coworkers.'-2
ambident
carbonylic
attack?
has been the
toward
the
product
CH1
gem-dichloroallyl-potassium
as
yielding
on
of
Seyferth,
behave
compounds,
on the substituents a whole
by
has been
an
of
in this complete
almost
O-M' RR'C=O
+
(C12CCHCH,)-M'
+
RR'&-Ccl=-CH=CHz
FM* CIIC=CH-CH2-CRR'
+
(M=Li,Na,K) Scheme
The rationalization factors
that
properties degree
can
of aggregation and Schleyer
while
allyl-sodium
symmetric, function
results affect
and
of interaction
has
of the counter-ion in principle bonding 8739
such
as:
been
shown
increasing with
from
(i)
the unknown
hy Winchester,
(ii)
allylic
free anion,
where
dimar,
to be present
temperature:
the substituted an almost
situation
electronic
itself
dggregation
of
and
as an asymmetric
been argued
have
structures);q with
by the existence
structural
conditions
allyl-potassium
to a true
the
itself
in the usual
increasing
complicated
is
systems,
these
monomeric,
it ranges
ion pair,
of
(allyl-lithium
of temperature,
in the monomer: separated
of these
to exist
presumably
1
principle
and the behaviour
Bauer
degree
in
(M=Li)
the cation
as
is a the system
a solvent and the
8740
c. CANEPAet al.
anion
would
interact
In the present has been will
assumed
be the
degrees taken
into account
the
molecules, under
the
as a first
study).6
interpretation different
The
lithium,
the
distribution by a hard
and
connection
of the
can be discussed
could
determine with
this
purpose,
also
A comparison
allyl-lithium studied (the
Theoretical
can
also
minima
by complete
parameters
in
first
function
of the
features Their
of the
electron
the possibility
reactions
substituted between
of attack as a factor
mono
systems,
a
to
stable
In
of gem-dichlorobenzaldehydes
that
different
are
and dichlorohave
at the same computational
shows
diffuse
been level
regioselective
using
on
and on a VAX Station
chlorine.
on carbon This will
on an IBM 3090 computer 3200+3150
cluster
shell
been
carried
3-21G
basis
out at set,=O*
atoms
and with
set, containing
neither
be labeled
have been performed
were
and chlorine
basis
have
of the geometrical
computations
split-valence
on the cations,
The computations
of programsll
the
structures
optimization
These
sp functionszob
d functions
nor d functions
this paper.
unconstrained
methods.s
level of theory, with
corresponding
and
by gradient
polarization diffuse
a
of the markedly
the dichloro).*
The energy
augmented
is also
of a soft electrophile.
drawn
paper7
system
attempt
can be examined
of some
be
solvent
shell,
monomers.
with
with
a lithium,
by considering
and electronic
fluoro-substituted
in a previous
to
by
anions,
oxygenated
above)
systems
with
"no
method
determined
the RHF
solvation
attack
the results
gem-difluoroallyl-lithium than
of
-potassium
and the analogous
theoretically
behaviour
series
and
first aims
connection
i.e.
them
with
some
HOMO polarization
are
ally1
with
these
anion
studied
comparing
discussed
structural
the orientation
-sodium
and
dichloroallyl
in
while
allyl-lithium, reported.
substituted
investigation
by
thus
can be modified
a
approximations
potassium
electrophile,
for
are
and
the different
allylic
of the anions
species
shown
investigation
situations,
systems
two
(how this picture
present
on the basis
sodium
extreme
The
association
approximation
(within
two
of deaggregation
Moreover,
the substituted
of
metallated
regioselectivity
counter-ion,
which
cation
of
is under
1,1-dichloropropenide,
from the tight
or potassium
the interaction
just
structures
and
originating
with
interaction".
stable
situation
equilibrium
modelling
"tight
an extreme
communication).6
of the cation
by
and
1-chloropropenide
sodium
study
of a separate
of interaction
determining
significantly.5
(the monomer-dimer
subject
interaction"
those
much more theoretical
using
3-21+Gl*l
at CSI-Piemonte
at the Istituto
throughout
the GAUSSIAN82 (Torino,
di Chimica
and 88 Italy)
Organica.
Regioselectivity in Li, Na and K chloroallyl systems
Results
8741
and discussion
Structural
features
out at this
same
found
be
to
structure.
(Figure
stable
the Ca carbon
1;
CCC planes
the
in
of
is pyramidalized
and reported
to atom
study,' ally1
only in
a
carried
anion
completely
and dichloro
was
planar
ally1
anions
in the gem-disubstituted
anion
Angstrom,
X are defined
in square
of
the mono
lengths
bond
relevant
In a previous unsubstituted
correspondence
structures
RHF/3-21+G[*l
angles
level,
only
The optimized
show that
dihedral
of the free anions.
computational
as angles
angles
in degrees;
between
the XCC and
brackets).
1.062 "_'-'"-._' I.076 1.077 " 122.1
i'
115.3 '14.'
r c
116.6 l.6¶6_,--Cl _--
_
I.366
1.373
\ I.@66
130.1
"
126.5
b
a [170.4] 120.6 116.7 H-s_ '-076 1 H III., I.O76-‘C-c-C 1.072/ I.466 H 122.1 1.331 126.6
116.1
'\ \ \
[-6.0)
\\ I.667 \ \ \ Cl
I.603 106.6 \ [24.611X
(136.1)
122.2
d
104.1 [135.5]
C
Figure
The degree
of pyramidalization
( z angle,
in
description the ally1 system
of the electronic anion
with
of the CClp
is thus
group
leads
for
chloropropenide the CCC plane, bears
some
analytical minimum, to the Ccl2
to a
double
pyramidalized
Hessian
to
This
structure
localized
CC
shows
that
(0.004) is
is dominated less
stable
l,l-dithrough
optimized
critical
geometry
(Fig. Id). The
anion
The Hessian
than
JZ
by the ca-Cp
by reflection
by the
of
the tipical
equivalent
whose
ally1 this
as shown
Two
obtained
and that
delocalized
approximate
structure,
frequencies.
fully
lc the
The pyramidalization
system, that
in Fig.
between
species
atom.
bonds.='
unsubstituted
computation
eigenvalue
carbon
structures,
no imaginary
is reported
difference
of the allylic
lengths,
by a planar the
anion main
of the dichloro
terminal
rather
are connected
showing
group.
of a
and
resemblance
lowest
structure
(1.331 ii) bond
single
The
the desappearance
disubstitution
(1.480 fib and C/?-Q values
in the dichloro
bracketsl.la
round
1
point
is another
eigenvector
inversion
motion
the pyramidal
related of the
(Table
1).
8742
the
In
case
structures, are found center, ally1
close
1-chloropropenide,
with
the CC1 bond
to be planar
features
case of double
length were
some pyramidalixation features
will
was present
of the molecular
be examined
below
’ ally1
anion,
orbitals
in
are 8.
bond
rather Similar
but in the
pyramidalized
too.
electron
The
the free anions.
and
structural
distribution
for both the free and metallated
Total
1.387
was more
in 1-fluoropropenide the
carbon
the Ca-Cg
values
and difluoropropenide,'
both
bond,
at thea
less from that of the
1.379 ii. These
the a carbon
TABLE Free Anions.
depart
the
mono
determine
non-equivalent
to the Cp-Cy
the syn conformation,
in
for
possible respect
not pyramidalized
length
substitution
just discussed
polarization
bond
value
found
fluorine
Being
considering
d and the Cp-Cy
to the CC bond
two
anti with
1-chloropropenide
For instance,
is 1.375
structural
of
the
syn and
(Fig. la,b).
the structures
anion.
length
of
and the
These
effects
anions.
1
and relative
energies.'
E
OE
EOMO polarization.b
P(ca)/
p(q)
I-Chloropropenide
syn planar
la
-572.635579
0.00
1.295
anti planar
lb
-572.631840
2.35
1.156
pyramidal
lc
-1029.473230
0.00
3.906
planar
Id
-1029.466678
4.11
1.705
l,l-Dichloropropenide
a: RHF/3-21+G[*l
energies
b: the polarization squares
of the atomic
have
of
been found
associations
with
bond
lengths
in ingstrom,
atom
X are defined
the
metal
angles
as angles
differences
in kcal mol-z.
for Ca and Cy as the sum of
coefficients.
metallated
for both
an alkali
energy
is computed
orbital
features
Structural
structures
in Hartree,
of the HOMO
anions,
in correspondence
counter-ion
(Figures
in degrees;
between
the
Several
species.
dihedral
stable
to different
2-4; RHF/3-21+G[*l
angles
XCC and CCC planes
relevant
to an
and reported
in
parentheses). The optimized
Lithium.
geometries
for the
while
those
propenide-lithiumlo
system
are shown
in Fig.
2c,d.
2c lithium
to the a allylic
carbon
system
atoms
are
shown
in
is bound
("external"
Fig.
lithium) .
2a,b
On the
lithium for
1-chloropropenide
the
l,l-dichloro-
In the structures
2a and
atom and to one or two chlorine
contrary,
in
the structures
2b and 2d
Regioselectivity inLi,NaandKchloroallylsystems
the Ca
both
bridging
Cy atoms
counter-ion
show that while structure true
in
the
is slightly
dichloro
closer
involved
lithium).
The
system
stable
system.
to that
are more
substantially
monochloro
more
for the dichloro
in general
are
("internal"
than
the
pyramidalized
energies
one, the
and
allyl-lithium, show
longer
ca-cg
with
the
(Table
(or
of the monochloro
unsubstituted
(zvalues)
bonding
"internal"
"external"
The structures
of
in
relative
the
the
8743
2)
bridged) reverse
is
systems
are
while
the
and shorter
bond lengths, respectively. These features (related to a more CB-Cr pronounced localization of the electron distribution to a "double bond zone" and a "lone pair the
"internal"
zone")
one,
are more
for both
evident
in the
the monochloro
[-64.71 120.5
"ex.ternal" structure
and dichloro
than
in
systems.
Li
2.OOS
[175.9] “-120.7 i.oGl--c I.O7S/ H
I.083
119.5 109.7
r
-=-c 1.326 122.1 i-5 .S]
/
i .473 I31
‘\
.S
‘\ 2.04S
I .I381 ‘”
113.1
\
jp:,c1
(130.0)
\
[i22.2'
b
a
Ll
81.0
2.505
[-52.41
2.003 /\
[lse.S]
120.0 I
/
;;_,/‘-ond ‘13.’\,
1
I ::75/ H 109.1 (148.3)
Cl
'\ Cl
t"'61
II8.6\
I.3so,27~QI_4 .-.m _ Z‘zL.U [-21.9]
109.4 [124.S]
-Cl
(131.2)
In the
a structure
\ Cl
li7.0 [158.4] 112.8 [26.S]
d
Figure
optimize
I.767
-.__
I.846
C
Sodium.
144
case with
of
sodium
the counter-ion
the geometry
shown
in Fig.
to the plane
of the allylic
3a, where carbon
the
atoms.
2
1-chloropropenide in an "external" Na-Ca
bond
Attempts
any
attempt
position
is almost
to
yielded
perpendicular
to find a structure
with
C. CANEPAer al. .
8744
sodium
bridging
sodium
appears
defined closer
between
to be stable
for lithium to the
between
latter,
the two
in a position
the
cation
carbon
stable
(Fig. 3b), and
Systems.
Total
Thus
between
those
the situation
bridging
the case
of sodium
found:
the cation
one
and relative
energies.-
EON0 polarization.b P(ca)/
AE
P(q)
I-chloropropenide 2a
-580.071623
1.00
1.527
-580.073224
0.00
1.493
l,l-dichloropropenide
external
2c
-1036.898437
0.00
1.626
internal
2d
-1036.892591
3.67
3.124
I-chloropropenide 1.303
-733.551911
3a
syn
l,l-dichloropropenide
external internal Potassium
3b
-1190.388039
0.00
8.363
3c
-1190.377678
6.50
9.674
I-chloropropenide 4a
syn Potassium
0.977
-1168.745113
l,l-dichloropropenide
external
4b
-1625.502062
0.00
10.773
internal
4c
-1625.492972
5.70
9.552
a: RHF/3-21+G[*l
energies
b: the polarization squares
(apart
cation-Ca-Cfl
in Hartree,
of the HOMO
of the atomic
"external"-Na
structure
structure from
angle:
the ca.
Both
energy
difference
IIinternal" structure,
would
in kcal mol-l.
for CQ and Cy as the sum of
from
for
kcal and
the
Li, molW1
in
mainly
in the
bond
length)
1610
for Na. The two stable
in
favour
large
the
operate
"external"-Li
analogous
ca.
cation-Ca
longer
by ca. 6.5
differences
coefficients.
differs
1340
differ
energy
is computed
orbital
structures this
an
2
2b
Sodium
with
in an "internal"
ayn internal
Sodium
is
as
syn external Lithium
The
In
were
result.
3a.
E
Lithium
although
atoms.
with
to that of Fig.
same
be considered
structures
another
the
is intermediate
cannot
TABLE Metallated
that
"internal";
atom
allylic
two
(Fig. 3c), similar
position
and
sodium
terminal
produced
and 7 carbons
as "external"
l,l-dichloropropenide "external"
the u
Na-Cy
favour
of
of the
"external"
distance
even
one. in the
a Ccl,-regioselective
Regiosekxivity
attack to
by a carbonyl
play
an
inLi,NaandKchloroallylsystems
electrophile,
important
role
if it is assumed
in
stabilizing
that
a
8745
the counter-ion
four-center
has
transition
structure.15 [-B4.6] 109.2
%:;I
Nm
N.
2.213 2.226 I Nf.j;:::~ ,‘.b”,‘4”
/ H
,.0*2
y
::x:i:
-C-C-C I .a34 yz~]
I
I .43a
‘\I
‘30.3
\
.073 H
\
iia.
[ia7
1.841 \
110.4 124.3,
(I33.3)
CI
a
[I74 .o] N-120.4 1.074--c,.072 “0
1.073
N
III.3
t.923 122.3 [*.a]
(143.7)
b Figure
As was the case with
Potassium.
was
found
to be stable
counter-ion carbon
cannot
atoms.
structures with
were
closely
"internal"-K lengths) ca.
found: in
above
Ccl,-regioselective
in
those
obtained
operate
of
the also
by a carbonyl
cation (Fig. for
(apart
for sodium.
(Fig.
between
sodium.
these The
from the different
this
species
electrophile.
stable
results
for
"external"
and
cation-Ca
structures
one.
"external"
two
(Fig. 4b), and another 4c):
The two stable
for
the
4a);
the CU and Cy
1,1-dichloropropenide
position
are similar
favour
bridging
an "external"
"internal"
attack
as
1-chloropropenide
position
"internal"
potassium
one with
optimized
would
an
potassium
sodium,
considered
of
parallel
structures
to those
5.7 kcal molml
discussed
an
in
be
In the case
the cation
potassium
only
again
3
The same in
bond
differ
by
factors
favour
of an
8746
c. CANEPA etal.
[-58.9] 37.4
K
2.633 \ [171.8] "220.4
*,3.4 ,H 111.5
1.073
\
1.074 Ns-ci.s7i-c c I.395 1.074 / 123.6 H 122.3 [-15.0]
103.3 1127.01
(ls3.3)
b Figure
Electronic determine should which case
be sensitive)
of attack
system
structures
the planar
consistent
stable
by the density
the
both
mono
pyramidal
zone"
plot
A similar
system.
appears
structure
and
5,
is
and
rather
The
is
anions of
found (lb,
effect
m
to
orbitala,
importance
of single
distribution
electron
allylic
density
for
the
Id).
On
of leas the
for the more
distribution
appears
stable
planar
contrary,
from a ca "lone pair
in
a ca-cy
zone".
to
For the more
above.
a delocalized
(1~)
(on a
(la and lc), and for
(la), the description
that
of
in the
and double
of them
electron
discussed
features
electrophilea
to it) is plotted
1,1-dichloropropenide
separated
hard
molecular
free anions
features
close
the
the total
parallel
(Id).
description
as clearly
where
of 1-chloro-propenide
dichloro
structure
The
and dichloro
the structural
structure
of
structural
which
be of particular
on the electron
in Figure
of the mono
with
planar
should
The
(to
electrophile.
substitution
dichloro
anions.
polarization
(HOMO)
0.5 i from the CCC plane
stable
of
soft
by a
terminal
free
distribution
the
and
occupied
can be examined
plane
of the
electron
the
the highest
chlorine
be
features
both
4
provided IC allylic structure
the
case
"double
of
bond
8141
Regioselectivity inLi, Na and K chloroallyl systems
Figure
Electrostatic plane
of both
could thea
the
sense
diaubstituted
anion
anion.
and lc structures are shown
and
at
electrophile,
an attractive
and y positions,
monosubstituted
plane,
obtained
-Pa
a hard
show that
"above",
of
potential
approaching
with
a preference
and
for
corresponding
The HOMO
the The
squarea ratio
Table
polarization
for each
1 .
substituted
atom
between
carbon
1-dichloropropenide.
can be
atomic
the Caand
It can be seen atom,
the
from the CCC
allylic
potential
for the former
latter
in
system
from
in correspondence
the
in the case
case
the
of
relevant
to the more
to
distance
of 2.0 ft from the CCC
a
stable
la
6.
X in the
of the HOMO
the
distances
maps,
Figure
defined
different
electrostatic
Two of these
in Figure
5
6
expressed
molecule; orbital
more
the
value
coefficients
Cy P values that
in terms its
belonging
is reported
HOMO
significantly
always
is in
of'a parameter, is given
P(X),
by the sum of to that
in the third polarized
atom.
column toward
1,1-dichloropropenide
of the
than
8748
c. CANEPA et al.
These anion
results
the charge "orbital CClz
show that,
(pyramidalized
distribution,
interaction
terminus
expected
a
have
distribution
On
still This
potential
the CCC plane.
potential this
attractive
potential
effective.
For lithium carbon
attractive
feature
is
overwhelmed
contrary
the
to the allylic
carbon
deeper
becomes
different
features
metallated
at
part
at closer at
namely
from the
the electron
distances
larger the
distances, system
repulsive
least
where
show
field;
two
in
part
the only On the
depressions
obvious
of the
in a
from the that
from the geometries
positions
the less
provided
to the y carbon.16
It is fairly
relative
by the
is much
to the potential
plots
of
R from
generated
and the one originating
distances.
is (as
is the zone of strongly charge)
of
cation
skeleton,
originate
species,
also
potassium
correspondence
anion
7) by a series
different
maps
is in correspondence
and
sodium
three
positive
the
the
the overall
of
(Figure
contribution
by
Although
polarization
these
allylic
to an
toward
and by the P ratios).
again
at
any attractive
zone of the plots
the monochloro
clear
present
sensitive attack
to
hard and soft electrophiles
species.
approaching
the
more
sensitive
contrary,
shown
of
the free dichloro more
their
maps
computed
is
of
a
is
feature
(for an
counterion;
by thea
maps
The dominant
of
to direct
way with
potential
is observable.
electrostatic
the
of the metallated
no net charge,
case
electrophile,
electrophile,
prefer
in a different
features
extreme
soft
would
by the electrostatic
repulsive
the
both a hard
of the molecule.
Electronic systems
and
factor",
to interact
indicated
for
structure),
these of the
acarbon
and
the counterion. The HOMO polarization (third column). exception
It
is reported generally
of 4a); this
is associated
system
important
orbital
electrophile's
In the
interaction
with
rather
energy
the HOMO of the
the electrophile's centered
HOMO's
the
LUMO;
carbonyl
interactions as indicated
schematically
is maximized state.
It
allylic
HOMO
group
in Figure
is polarized
if the alkali can be noted
metal
that
in the direction
of
the
with
the oxygen atoms metal
the carbon
atom
with
Because
approach
this
its a
with
species, the HOMO
interaction
in the transition
significantly bound
the
two orbital
the metallated
atom,
the
have also
interaction Thus
significant.
and oxygen
because
species
whose
on
the more
thus diminishing
ofref7forLi.
toward
the anion
between
The association
energy,
dealing
3
that
the metallated
be
when
in energy)
be
on the counter-ion,
could group have to be considered when
of the carbonyl
to
HOMO.
nucleophile's
high
2
(with the
by a soft electrophile
is rather
expected
terminus
pronounced
of attack
HOMO
for Ca and Cy in Table
substituted
to be more
is
significantly
LUMO,
the
case
interaction
LUMO and the
lowers
as P ratios
appears
(where the allylic
counter-ion
low
feature
to Na or K.
an anionic
again
favours
polarizes
to it, and
the
the LUMO
Regiosele-ctivity in Li, Na and K chloroallyl system
-7-y
:: + :: ::
8749
-
:: _.
: i ; : :
2.2
R(i)
2.0 Figure
7
8750
c. CANEPA ctal.
of the carbonyl orbital8
would
electrophile
group
is
as a consequence
approached
structure,
polarized
as
the
found
Therefore,
factors
in a
favoured
on
the
distribution structural that
and features
carbonyl
addition
indications the HOMO found
but against monochloro
ana
shown
the counter-ion electrophile mostly
involved
(compare
to
attack
Zc,
in
7,
dominant
of metallated
Carbonyl
compd.
P-value case,
repulsive
and
appears This
carbon.
system provided
in some
region
ratiosb
situation
lOO:
o-ClC.H.CHO
p-ClC~H.CHO
(73)
lOO:
with
(70)
(75)
lOO:
(65)
(65)
lOO:
(60)
(68)
lOO:
(67) (63)
o-MeOf&H.CHO
(68)
lOO:
(65)
lOO:
23:77
(75)-
lOO:
(60)
lOO:
(65)
o-MeC,H,CffO
(63)
lOO:
(60)
p-MeCsHeCHO
(68)
lOO:
(68)
3.12 mmol.
f: data
by
from ref.
lOO:
%H n.m.r. product.
(65)
compound,
carbonyl
3; t-BuOK,
a hard
K=
(70)
isolated
for
respect
some carbonyl
lOO:
20 ml; T= -95 OC. b:
maps
is determined
p-MeOCs?i4CA0
THF,
for Na,
and yields".
p-CF&sHJHiO
(25%). c: in parentheses;
be
3
15:85
mmol;
by
surrounding
to discourage
Nag
mmol;
could
the
structures.
PhCHO
2.5
the
are for Li as
potential
feature
Lid
a: 3,3-dichloropropene,
to
for the
pattern
similar
the
(8019
be
electron
less favourable
where
CCla:CEa
those
ratios
Electrostatic
3,3-dichloropropene
compounds:'
the
structures
oppose
all cations
TABLE Reactions
could
related
regioselective
Here
6) by the geometrical
to
the following
attack
for the Li dichloro maps
2).
are for
if the
transition
and 4b (with the possibility
as in the dichloro
for K (Table
systems,
transition
a different
way,
of formaldehyde
discussed,
3b
the
on the substituted
Figure
attack
counter-ion:
just
systems.
(not shown)
is the
the
the frontier
four-center
electrophilic
electrostatic
for Li in Figure
attack
an
atom,
favourable
a
the
On the contrary,
Finally,
attack
systems
that
Figures
monosubstituted
to a CHCl
via
for
closer
from the
polarization.
favourable
in
reaction).
obtained
in the
to those
be
a more
system
polarizations
shown
the counter-ion
way
atom
HOMO
in
carbon
for the Na and K dichloro
sharp
carbon
the
interact
allylic
computationally
methyllithium.15 indicate
toward
2.5
on the crude
d: data
3.12 mmol.
mmol; reaction
from ref. g: total
LDA,
2.5
product
3. e: t-BuONa,
yield.
Regioselectivity inLi,NaandKchloroallylsystems
conclusions
The
experimental
results
various
with
counter-ion attack
of
of some
substituted
when
system
the same
compounds
reactions
with
by treating
tert-butoxide
the reaction
the
in
correspond
with
the
is the
compounds
with
On the
of sodium
to an attack
prepared
have
presence
react
carbonyl
in the presence
derivatives
compounds
lithium
for CH= terminus.
out
products
with
3,3-dichloropropene When
all the tested
LochmannXe
that working
the carbonyl
compared
3).
preference
are carried
and
be
(Table
anion
organolithium
we assume
Similarly,
can
of the metallated
a marked
reactions
SchlosserX7
site.
study
benzaldehydes
or pota'ssium tert-butoxide, the CClz
present
of the gem-dichloroallyl
the allylic
contrary,
the
8751
at
organopotassium
potassium
of sodium
alkoxide.
and potassium
gem-dichloroallyl-sodium
and
respectively.
-potassium,
Experimental The apparatus
and the reaction
reactions
of gem-dichloroallyl-sodium
atmosphere
in flame
diisopropylamine Fluka, The
and were
carbonyl
spectra
IH N.m.r
connected
recorded
with
n-butyllithium
a
sodium
allowed
within
-95 OC. After
a
few
(0.30 g,
the addition
layer was
mixture of
to reach
separated
The combined
the
minutes 3.12
mmol)
THF
was
added
then
stirred
temperature,
and the aqueous organic
phases
Oc!)
solution
ml,
at -95 V,
A mixture
carbonyl under
for 2 h under 3.9 mmol)
then
poured
kashed
of
dissolved
and the apparatus
dropwise
one extracted were
(1 ml) was added
temperature.
was
(0.5
column).
flask was cooled was added
Mass
detector
tert-Butoxide.
in hexanes)
and of the desired
C1Si(CH3)3 room
the
the R-24B
standard.
capillary
(-20
to
selective
THF
cooled
further
Perkin-Elmer
of Sodium
1.6 M solution
equilibrate
anhydrous
The reaction
organic
B mass
anhydrous
previously
without
according
silicone
and from
to the reaction.
as internal
5970
in
(0.27 g, 2.5 mmol)
was allowed
(15 ml).
mmol) a
for 15 min to
mixture
ether
to
After
in 1.0 ml of
5 min.
used
on a Hitachi
methyl
i.e. 2.5 mmol;
tert-butoxide
3,3-dichloropropene (2.5 mmol)
2.5
syringe (1.6 ml,
to stand
were
out with LDA in the Presence
(0.25 g,
in 20 ml of dry THF. then
(cross-linked
prior
TMS
inert
tert-butoxide
synthetized
HP
a
All the
out under
n-Butyllithium
Torr)
and
using
with
THF.
sodium
(0.1
recorded
spectrometer
described.= carried
anhydrous
Aldrich,
was
were
at 70 eV
Carried
Diisopropylamine dropwise
spectra
to a HP 5890 GC
Reaction
likewise
commercial
were
resolution
were
were
vacuum
3,3-Dichloropropene
literature.=-
previously
from
under
compounds
been
with
glassware
purchased
sublimated
purification.
60 MHz high
dried
were
for gem-dichloroallyl-lithium
procedure
has
and gem-dichloroallyl-potassium
twice with
of
compound stirring argon
at
the reaction in water.
The
with
diethyl
brine
(10 ml)
8752
C.CANFLPA~~al.
and dried pressure establish mass
with
anhydrous
Na,SO,.
and the residue the CCla:C&
spectra
ratio.
in agreement
The
was analysed
with
solution
All the obtained those
was condensed
by =H n.m.r.
previously
under
spectroscopy,
compounds
show
reduced
in order
III n.m.r.
to and
reported.'
Aknowledgements This work has been supported by the Minister0 dell'Universita' e della Ricerca Scientifica e Tecnologica, the Italian C.N.R. and CSI-Piemonte. References and notes (a) Seyferth, D.; Simon, R.M.; Sepelak, D.J.; Klein, H.A. J. Org. Chem. 1 (b) Seyferth, D.; Murphy, G.J.; Woodruff, R.A. 1980, 45, 2273-2274. Chem. 1974, 66, C29-32. (cl Seyferth, D.; Murphy, G.J.; J. Organometal. Woodruff, R.A. J. Am. Chem. Sot. 1974, 96, 5011-5012. (d) Mauze', B. J. Organometal.Chem. 1979, 170, 265-279. (e) Mauze'. B. J. Organometal. Chem. 1980, 202, 233-239. (f) Seyferth, D.; Wursthorn, K.R. J. Organometal. Chem. 1979, 182, 455-464. Seyferth, D.; Murphy, G.J.; Mauze', B. J. Am. Chem. Sot. 1977, 99, 5317-5330. Canepa, C.; Cobianco, S.; Degani, I.; Gatti, A.; Venturello, P. Tetrahedron 1991. 47, 1485-1494. Winchester, W.R.; Bauer, W.; Schleyer, P.v.R. J. Chem. Sot., Chem. Commun. 1987, 177-179. on carbanion-cation interactions, see: Smid, J. Angew. For a review Chem., Int. Ed. Engl. 1972, 11, 112-127. in preparation. Canepa, C.; Tonachini, G. manuscript Tonachini. G.: Caneoa. C. Tetrahedron 1989. 45, 5163-5174. Seyferth,.D.;.Simon-, R.M.; Sepelak, D.J.; Klein, H.A. J. Am. Chem. SOC. 1983, 105, 4634-4639. (a) Schlegel, H.B. J. Comput. Chem. 1982, 3, 214-218. (b) Schlegel, Theoretical Organic Chemistry, Csizsmadia, I.G.; H.B. in Computational Daudel, R. Eds. Deidel Publ. Co. 1981, 129-159. (cl Schlegel, H.B. J. Chem. Phys. 1982, 77, 3676-3681. (d) Schlegel, H.B.; Binkley, J.S.; Pople, J.A. J. Chem. Phys. 1984, 80, 1976-1981. J. Am. Chem. Sot. 1980, (a) Binkley, J.S.; Pople, J.A.; Hehre. W.J. 10 102. 939-947. (b) Clark, T.; Jemmis, E.D.; Schlever, P.v.R.; Binkley, Chem. 1,978. 1.50; 1. J.S.; Pople, J. A. J. Organ&met. Binkley, J.S.; Frish, M.J.; DeFrees, D.J.; Krishnan, R.; 11 GAUSSIAN 82: CarnegieWhiteside, R.A.; Schlegel, H.B.; Fluder, E.M.; Pople, J.A.. Mellon Chemistry Publ. Unit. GAUSSIAN 88: Frish, M.J.; Head-Gordon, M.; Schlegel, H.M.; Ragavachari, K.; Binkley, J.S.; Gonzalez, C.; DeFrees, D.J.; Fox, D.J.; Whiteside, R.A.; Seeger, R.; Melius, C.F.; Baker, J.; Martin, R.; Kahn, L.R.; Stewart, J.J.P.; Fluder, E.M.; Topiol, S.; Gaussian Inc., Pittsburgh, PA, 1988. Pople, J.A.. angle z is computed as the angle between the CUC$l 12 The pyramidalization bond and the normal to the CHCl or CClr+ plane (a planar structure has z = 144.70). c =90.00, while a tetrahedral arrangement gives level the CC bond length values for ethane 13 At the same computational and ethene are 1.542 and 1.320 A respectively. Preliminary computations on this system allowed to discuss its regio14 Baima. R.; Canepa, C.; Degani, I.; selectivity: Angeletti, E.; Tetrahedron 1989, 45, 7827-7834. Tonachini, G.; Venturello, P. 15 Kaufmann, E.; Schleyer, P.v.R.; Houk, K.N.; Wu, Y.-D. J. Am. Chem. Sot. The attack of formaldehyde on the a and y 1970, 107, 5560-5562. positions of lithium and sodium 1,1-dichloropropenide is under study. show an Q carbon depression Similar maps for Li-difluoropropenide' 16 deeper than they . 17 Schlosser. M.: Hartmann, J. J. Am. Chem. Sot. 1976, 98, 4674-4676. Lochmann,.L.;.Lim, 18 D. J; Organometal. Chem. 1971, 28, 153-158. King, W.H.; Smith, H.A. J. Am. Chem. Sot. 1950. 72, 3459-3462. 19